Machine Learning Enabled Computational Screening of Inorganic Solid Electrolytes for Suppression of Dendrite Formation in Lithium Metal AnodesClick to copy article linkArticle link copied!
- Zeeshan AhmadZeeshan AhmadDepartment of Mechanical Engineering, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, United StatesMore by Zeeshan Ahmad
- Tian XieTian XieDepartment of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United StatesMore by Tian Xie
- Chinmay MaheshwariChinmay MaheshwariDepartment of Mechanical Engineering, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, United StatesMore by Chinmay Maheshwari
- Jeffrey C. GrossmanJeffrey C. GrossmanDepartment of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United StatesMore by Jeffrey C. Grossman
- Venkatasubramanian Viswanathan*Venkatasubramanian Viswanathan*E-mail: [email protected]Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, United StatesDepartment of Physics, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, United StatesMore by Venkatasubramanian Viswanathan
Abstract
Next generation batteries based on lithium (Li) metal anodes have been plagued by the dendritic electrodeposition of Li metal on the anode during cycling, resulting in short circuit and capacity loss. Suppression of dendritic growth through the use of solid electrolytes has emerged as one of the most promising strategies for enabling the use of Li metal anodes. We perform a computational screening of over 12 000 inorganic solids based on their ability to suppress dendrite initiation in contact with Li metal anode. Properties for mechanically isotropic and anisotropic interfaces that can be used in stability criteria for determining the propensity of dendrite initiation are usually obtained from computationally expensive first-principles methods. In order to obtain a large data set for screening, we use machine-learning models to predict the mechanical properties of several new solid electrolytes. The machine-learning models are trained on purely structural features of the material, which do not require any first-principles calculations. We train a graph convolutional neural network on the shear and bulk moduli because of the availability of a large training data set with low noise due to low uncertainty in their first-principles-calculated values. We use gradient boosting regressor and kernel ridge regression to train the elastic constants, where the choice of the model depends on the size of the training data and the noise that it can handle. The material stiffness is found to increase with an increase in mass density and ratio of Li and sublattice bond ionicity, and decrease with increase in volume per atom and sublattice electronegativity. Cross-validation/test performance suggests our models generalize well. We predict over 20 mechanically anisotropic interfaces between Li metal and four solid electrolytes which can be used to suppress dendrite growth. Our screened candidates are generally soft and highly anisotropic, and present opportunities for simultaneously obtaining dendrite suppression and high ionic conductivity in solid electrolytes.
Synopsis
Driven by machine-learning methods, we perform a large-scale screening of ∼13 000 materials for their use as solid electrolytes in Li metal anode-based batteries.
Introduction
Results and Discussion
Isotropic Material Screening




Figure 1
Figure 1. Parity plots comparing the elastic properties: (a) shear modulus G, and elastic constants (b) C11, (c) C12, and (d) C44 predicted by the machine-learning models to the DFT-calculated values. The shear modulus is predicted using CGCNN, and the elastic constants C11 and C44 are predicted using gradient boosting regression while C12 is predicted using kernel ridge regression. The parity plot for shear modulus is on 680 test data points while that for the elastic constants contains all available data (170 points) where each prediction is a cross-validated value.
method | log(G) RMSE | log(K) RMSE |
---|---|---|
this work | 0.1268 | 0.1013 |
de Jong et al. (49) | 0.1378 | 0.0750 |
Figure 2
Figure 2. Contribution of hydrostatic stress, deviatoric stress, and surface tension to the stability parameter as a function of surface roughness wavenumber. The surface tension term starts dominating at high k and ultimately stabilizes the interface after k = kcrit. The contributions are plotted for a material with shear modulus ratio G/GLi = 1 and Poisson’s ratio ν = 0.33 which is not stable (χ > 0) at k = 108 m–1. The red line shows the fraction of surface tension contribution to the stability parameter obtained by dividing the absolute value of its contribution by the sum of absolute values of all components.
Figure 3
Figure 3. Results of isotropic screening for 12 950 Li-containing compounds. Distribution of ensemble averaged (a) stability parameter for isotropic Li–solid electrolyte interfaces at k = 108 m–1 and (b) critical wavelength of surface roughness required for stability. None of the materials in the database can be stabilized without the aid of surface tension. The required critical surface roughness wavenumber depends on the contribution of the stress term in the stability parameter.
Figure 4
Figure 4. Isotropic stability diagram showing the position of all solid electrolytes involved in the screening. GLi is the shear modulus of Li = 3.4 GPa. The critical G/GLi line separating the stable and unstable regions depends weakly on the Poisson’s ratio, so the lines corresponding to νs = 0.33 and 0.5 are good indicators for assessment of stability. The darker regions indicate more number of materials in the region.
low k | high k | ||||||
---|---|---|---|---|---|---|---|
formula | space group | MP id | χ | Ps | χ | Ps | λcrit (nm) |
Li2WS4 | P4̅2m | mp-867695 | 0.62 | –109.26 | 3.64 | ||
Li2WS4 | I4̅2m | mp-753195 | 1.75 | –38.54 | 1.34 | ||
LiBH4 | P1̅ | mp-675926 | 1.98 | –40.13 | 1.32 | ||
LiAuI4 | P21/c | mp-29520 | 2.7 ± 0.9 | 0 | 16.1 ± 55.2 | 0.43 | 1.02 ± 0.40 |
LiGaI4 | P21/c | mp-567967 | 3.2 ± 1.1 | 0 | 48.6 ± 67.0 | 0.28 | 0.85 ± 0.29 |
LiWCl6 | R3 | mp-570512 | 3.2 ± 0.9 | 0 | 51.3 ± 56.6 | 0.17 | 0.82 ± 0.27 |
Cs3LiI4 | P21/m | mp-569238 | 3.1 ± 0.7 | 0 | 46.9 ± 43.4 | 0.15 | 0.80 ± 0.17 |
LiInI4 | P21/c | mp-541001 | 3.5 ± 1.0 | 0 | 68.5 ± 62.8 | 0.12 | 0.74 ± 0.20 |
Cs2Li3I5 | C2 | mp-608311 | 3.6 ± 0.9 | 0 | 77.2 ± 59.0 | 0.05 | 0.71 ± 0.17 |
Ba19Na29Li35 | F4̅3m | mp-569025 | 4.2 ± 1.3 | 0 | 101.9 ± 81.3 | 0.08 | 0.68 ± 0.19 |
Ba38Na58Li26N | F4̅3m | mp-570185 | 4.2 ± 1.3 | 0 | 104.5 ± 82.3 | 0.08 | 0.67 ± 0.20 |
Li2UI6 | P3̅1c | mp-570813 | 4.2 ± 1.4 | 0 | 111.5 ± 86.8 | 0.11 | 0.66 ± 0.29 |
χ is the stability parameter in kJ/(mol nm) which needs to be negative for stability, and k = 2π/λ is the surface roughness wavenumber. Low k corresponds to k = 108 m–1 while high k corresponds to a wavelength λ = 2π/k = 1 nm. Only materials with probability of stability Ps > 0.05 at high k are shown. Uncertainties in χ and λcrit (standard deviation of their distributions) and Ps are only shown for materials whose properties were predicted using CGCNN and not for those whose properties were available in training data.
Anisotropic Material Screening
interface normal | ||||||
---|---|---|---|---|---|---|
formula | space group | MP id | Li | electrolyte | χ at k = 108 m–1 (kJ/(mol nm)) | AU |
Li2WS4 | P4̅2m | mp-867695 | [1 1 1] | [0 0 1] | –1.92 | 31.30 |
Li2WS4 | P4̅2m | mp-867695 | [2 1 1] | [0 0 1] | –1.87 | 31.30 |
Li2WS4 | P4̅2m | mp-867695 | [0 1 0] | [0 0 1] | –1.68 | 31.30 |
Li2WS4 | I4̅2m | mp-753195 | [0 1 0] | [0 0 1] | –1.23 | 12.84 |
LiBH4 | P1̅ | mp-675926 | [0 1 0] | [0 1 0] | –1.12 | 13.65 |
Li2WS4 | I4̅2m | mp-753195 | [1 1 1] | [1 0 1] | –1.00 | 12.84 |
LiOH | P4/nmm | mp-23856 | [0 1 0] | [0 0 1] | –1.00 | 113.29 |
Li2WS4 | I4̅2m | mp-753195 | [1 1 1] | [0 0 1] | –1.00 | 12.84 |
LiOH | P4/nmm | mp-23856 | [2 1 1] | [0 0 1] | –0.99 | 113.29 |
LiOH | P4/nmm | mp-23856 | [1 1 1] | [0 0 1] | –0.98 | 113.29 |
Li2WS4 | I4̅2m | mp-753195 | [2 1 1] | [0 0 1] | –0.89 | 12.84 |
Li2WS4 | I4̅2m | mp-753195 | [0 1 0] | [1 0 1] | –0.79 | 12.84 |
LiBH4 | P1̅ | mp-675926 | [1 1 1] | [1 1 0] | –0.77 | 13.65 |
LiBH4 | P1̅ | mp-675926 | [1 1 1] | [0 1 0] | –0.75 | 13.65 |
Li2WS4 | I4̅2m | mp-753195 | [0 1 0] | [0 1 1] | –0.49 | 13.84 |
LiBH4 | P1̅ | mp-675926 | [0 1 0] | [1 1 0] | –0.47 | 13.65 |
Li2WS4 | P4̅2m | mp-867695 | [1 1 0] | [0 0 1] | –0.40 | 31.30 |
Li2WS4 | P4̅2m | mp-867695 | [1 1 1] | [1 0 1] | –0.28 | 31.30 |
Li2WS4 | P4̅2m | mp-867695 | [0 1 0] | [1 0 1] | –0.17 | 31.30 |
Li2WS4 | I4̅2m | mp-753195 | [2 1 1] | [1 0 1] | –0.07 | 13.84 |
Other Considerations for Screened Electrolytes
formula | space group | MP id | Pion | band gap (eV) | energy above hull per atom (eV) |
---|---|---|---|---|---|
LiOH | P4/nmm | mp-23856 | 0.05 | 6.34 | 0.000 |
LiAuI4 | P21/c | mp-29520 | 0.94 | 1.92 | 0.000 |
LiGaI4 | P21/c | mp-567967 | 0.18 | 4.33 | 0.000 |
LiBH4 | P1̅ | mp-675926 | 0.27 | 8.57 | 0.071 |
Li2WS4 | I4̅2m | mp-753195 | 0.15 | 3.61 | 0.032 |
Li2WS4 | P4̅2m | mp-867695 | 0.23 | 3.52 | 0.037 |
Cs3LiI4 | P21/m | mp-569238 | 0.01 | 6.07 | 0.018 |
LiInI4 | P21/c | mp-541001 | 0.13 | 3.96 | 0.000 |
Cs2Li3I5 | C2 | mp-608311 | 0.33 | 6.58 | 0.000 |
Ba19Na29Li35 | F4̅3m | mp-569025 | 0.00 | 0.94 | 0.000 |
Ba38Na58Li26N | F4̅3m | mp-570185 | 1.00 | 0.96 | 0.009 |
Li2UI6 | P3̅1c | mp-570813 | 0.26 | 1.17 | 0.000 |
Ionic conductivity is quantified through Pion, the probability of superionic conduction; electronic conductivity through the band gap; and thermodynamic stability through energy per atom above the convex hull.
Ionic Conductivity
Thermodynamic Stability
Electronic Conductivity
Conclusions
Supporting Information
The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acscentsci.8b00229.
Details of machine-learning models and additional figures including schematics and visualizations, shear modulus values, and stability parameter values (PDF)
Anisotropic stability parameter for training data (XLSX)
Shear modulus of 60 648 compounds predicted using CGCNN (XLSX)
Anisotropic stability parameter for predicted data (XLSX)
Bulk modulus of 60 648 compounds predicted using CGCNN (XLSX)
Terms & Conditions
Most electronic Supporting Information files are available without a subscription to ACS Web Editions. Such files may be downloaded by article for research use (if there is a public use license linked to the relevant article, that license may permit other uses). Permission may be obtained from ACS for other uses through requests via the RightsLink permission system: http://pubs.acs.org/page/copyright/permissions.html.
Acknowledgments
Z.A. thanks A. Sendek for sharing data on features of Li-containing compounds, and S. Shekhar, C. Hwu, L. Kara, J. Montoya, and K. Thomas-Alyea for helpful discussions. Z.A. acknowledges support from the Advanced Research Projects Agency—Energy (ARPA-E) Integration and Optimization of Novel Ion Conducting Solids (IONICS) program under Grant DE-AR0000774. V.V. gratefully acknowledges support from the U.S. Department of Energy, Energy Efficiency and Renewable Energy Vehicle Technologies Office under Award DE-EE0007810. This work used the Extreme Science and Engineering Discovery Environment (XSEDE), (96) which is supported by National Science Foundation Grant OCI-1053575. Specifically, it used Grant MSS170010P on the Bridges system, (97) which is supported by NSF Award ACI-1445606, at the Pittsburgh Supercomputing Center (PSC).
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- 10Aurbach, D.; Zinigrad, E.; Cohen, Y.; Teller, H. A short review of failure mechanisms of lithium metal and lithiated graphite anodes in liquid electrolyte solutions. Solid State Ionics 2002, 148, 405– 416, DOI: 10.1016/S0167-2738(02)00080-2Google Scholar10https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD38XktVWgurY%253D&md5=24417ffbcd25ad6ffaba30ab7d00e3d4A short review of failure mechanisms of lithium metal and lithiated graphite anodes in liquid electrolyte solutionsAurbach, Doron; Zinigrad, Ella; Cohen, Yaron; Teller, HananSolid State Ionics (2002), 148 (3,4), 405-416CODEN: SSIOD3; ISSN:0167-2738. (Elsevier Science B.V.)A review. Li electrodes in any relevant electrolyte soln. (i.e., polar aprotic) are covered by surface films of a very complicated structure. It was found that even in cases where the surface films formed on lithium contain elastomers, or where the lithium metal reactivity is reduced by doping with elements such as N, As, Al, Mg, Ca, etc., it is impossible to achieve sufficient passivation with lithium electrodes and liq. solns. Passivation is considerably worsened when Li electrodes are operated at high rates (esp. at high charging, Li deposition rates). Thus, there is no way that rechargeable Li batteries can compete with Li-ion batteries in any application that requires high charging rates (e.g., in powering portable electronic devices). The electrochem. behavior of lithiated graphite electrodes also depends on passivation phenomena. The surface films formed on lithiated graphite are similar to those formed on Li metal in the same solns. The vol. changes of graphite electrodes during Li insertion-deinsertion are small enough to enable their reasonable passivation in a variety of electrolyte solns. A crit. factor that dets. the stability of graphite electrodes is their morphol. It was found that the shape of graphite particles plays a key role in their application as active mass in anodes for Li-ion batteries.
- 11Steiger, J.; Kramer, D.; Mönig, R. Mechanisms of dendritic growth investigated by in situ light microscopy during electrodeposition and dissolution of lithium. J. Power Sources 2014, 261, 112– 119, DOI: 10.1016/j.jpowsour.2014.03.029Google Scholar11https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXnsl2murc%253D&md5=2db8d2782ea70c21bf11b86d6c3618fdMechanisms of dendritic growth investigated by in situ light microscopy during electrodeposition and dissolution of lithiumSteiger, Jens; Kramer, Dominik; Moenig, ReinerJournal of Power Sources (2014), 261 (), 112-119CODEN: JPSODZ; ISSN:0378-7753. (Elsevier B.V.)Batteries with metallic lithium anodes offer improved volumetric and gravimetric energy densities; therefore, future batteries including the promising lithium-sulfur and lithium-air systems would benefit from them. The electrodeposition of lithium metal - which is an unwanted incident in lithium ion systems - often results in fine filaments or moss, called dendritic lithium, which leads to strong capacity fading and the danger of internal short circuiting. To study the mechanisms of dendritic growth and the behavior during lithium dissoln., lithium deposits have been obsd. in situ in 1 M LiPF6 in EC:DMC by light microscopy. The high resoln. optical microscopy provided information on the growth and electrodissoln. of single lithium filaments. The growth areas could be identified in detail: The lithium wires can grow either from the substrate-lithium interface, at kinks or in a region at or close to the tip. Based on these observations, we suggest a growth model for lithium filaments predicated on defect-based insertion of lithium at the aforementioned locations. This type of growth is not compatible with previous models of dendritic growth, for example, it is hardly influenced by elec. fields at the tip and does not depend on the direction of the elec. field.
- 12Albertus, P.; Babinec, S.; Litzelman, S.; Newman, A. Status and challenges in enabling the lithium metal electrode for high-energy and low-cost rechargeable batteries. Nat. Energy 2018, 3, 16– 21, DOI: 10.1038/s41560-017-0047-2Google Scholar12https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXitVehurY%253D&md5=569e6865fb3a225323353f9e9f39fddbStatus and challenges in enabling the lithium metal electrode for high-energy and low-cost rechargeable batteriesAlbertus, Paul; Babinec, Susan; Litzelman, Scott; Newman, AronNature Energy (2018), 3 (1), 16-21CODEN: NEANFD; ISSN:2058-7546. (Nature Research)Enabling the reversible lithium metal electrode is essential for surpassing the energy content of today's lithium-ion cells. Although lithium metal cells for niche applications have been developed already, efforts are underway to create rechargeable lithium metal batteries that can significantly advance vehicle electrification and grid energy storage. In this Perspective, we focus on three tasks to guide and further advance the reversible lithium metal electrode. First, we summarize the state of research and com. efforts in terms of four key performance parameters, and identify addnl. performance parameters of interest. We then advocate for the use of limited lithium (≤30 μm) to ensure early identification of tech. challenges assocd. with stable and dendrite-free cycling and a more rapid transition to com. relevant designs. Finally, we provide a cost target and outline material costs and manufg. methods that could allow lithium metal cells to reach 100 US$ kWh-1.
- 13Aurbach, D.; Markovsky, B.; Shechter, A.; Ein-Eli, Y.; Cohen, H. A Comparative Study of Synthetic Graphite and Li Electrodes in Electrolyte Solutions Based on Ethylene Carbonate-Dimethyl Carbonate Mixtures. J. Electrochem. Soc. 1996, 143, 3809– 3820, DOI: 10.1149/1.1837300Google Scholar13https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK2sXhsFehsg%253D%253D&md5=02e52a156683cedd7ca6901f81eb7313A comparative study of synthetic graphite and Li electrodes in electrolyte solutions based on ethylene carbonate-dimethyl carbonate mixturesAurbach, D.; Markovsky, B.; Shechter, A.; Ein-Eli, Y.; Cohen, H.Journal of the Electrochemical Society (1996), 143 (12), 3809-3820CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)This work entails a comparative study of both Li and synthetic graphite electrodes in electrolyte solns. based on ethylene and di-Me carbonates (EC-DMC) and the impact of the salt used [LiAsF6, LiClO4, LiPF6, LiBF4, and LiN(SO2CF3)2]. The presence of some additives in solns. (e.g., Li2CO3, CO2, tributylamine) and the effect of the particle size of the carbon on the behavior of the electrode were studied. The correlation between the surface chem., the morphol., and the performance of Li and graphite electrodes was explored using surface sensitive FTIR and x-ray and photoelectron spectroscopies, impedance spectroscopy, x-ray diffraction and SEM in conjunction with std. electrochem. techniques. Synthetic graphite anodes could be cycled (Li intercalation-deintercalation) hundreds of times at a capacity close to the optimal (x → 1 in LixC6) in EC-DMC solns. due to the formation of highly stable and passivating surface films in which EC redn. products such as (CH2OCO2Li)2 are the major constituents. The cycling efficiency of Li metal anodes in these solns., however, is lower than that obtained in ethereal solns. and seems to be too low for Li-metal liq. electrolyte, rechargeable battery application. The connection between the soln. compn. and the electrode's performance is discussed.
- 14Hirai, T.; Yoshimatsu, I.; Yamaki, J. Effect of Additives on Lithium Cycling Efficiency. J. Electrochem. Soc. 1994, 141, 2300– 2305, DOI: 10.1149/1.2055116Google Scholar14https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK2cXmtlCls7o%253D&md5=9125cb1237f464f238f6507a83b742acEffect of additives on lithium cycling efficiencyHirai, Toshiro; Yoshimatsu, Isamu; Yamaki, Jun-ichiJournal of the Electrochemical Society (1994), 141 (9), 2300-5CODEN: JESOAN; ISSN:0013-4651.Li cycling efficiency was evaluated for LiAsF6-ethylene carbonate/2-methyltetrahydrofuran mixed-solvent electrolyte (LiAsF6-EC/2MeTHF) contg. additives of tetraalkylammonium chlorides with a long n-alkyl chain and three Me groups. The tetraalkylammonium chloride with n-alkyl group longer than n-C12H25 increased Li cycling efficiency. Cetyltrimethylammonium chloride (CTAC) produced the best improvement in Li cycling efficiency. A figure of merit (FOM) of Li for 0.01M CTAC was 46, which was 1.5 times the FOM for the corresponding additive-free electrolyte. The LiAsF6-EC/2MeTHF with CTAC showed an increase in FOM with stack pressure, but the effect was less than that for the additive-free LiAsF6-EC/2MeTHF. SEM observation showed that the addn. of CTAC decreased the needle-like Li deposition and increased particulate Li deposition. This deposition morphol. may be the main cause of the increase in FOM. The additive had no effect on rate capability for cell cycling at 3 mA/cm2 discharge and 1 mA/cm2 charge.
- 15Ding, F.; Xu, W.; Graff, G. L.; Zhang, J.; Sushko, M. L.; Chen, X.; Shao, Y.; Engelhard, M. H.; Nie, Z.; Xiao, J.; Liu, X.; Sushko, P. V.; Liu, J.; Zhang, J.-G. Dendrite-Free Lithium Deposition via Self-Healing Electrostatic Shield Mechanism. J. Am. Chem. Soc. 2013, 135, 4450– 4456, DOI: 10.1021/ja312241yGoogle Scholar15https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXjtlWgsLs%253D&md5=be89c1fc31e4b3293c7f0fb4e6b55407Dendrite-Free Lithium Deposition via Self-Healing Electrostatic Shield MechanismDing, Fei; Xu, Wu; Graff, Gordon L.; Zhang, Jian; Sushko, Maria L.; Chen, Xilin; Shao, Yuyan; Engelhard, Mark H.; Nie, Zimin; Xiao, Jie; Liu, Xingjiang; Sushko, Peter V.; Liu, Jun; Zhang, Ji-GuangJournal of the American Chemical Society (2013), 135 (11), 4450-4456CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Rechargeable Li metal batteries are of great importance. Unfortunately, uncontrollable dendritic Li growth inherent in these batteries (upon repeated charge/discharge cycling) has prevented their practical application over the past 40 years. The authors show a novel mechanism that can fundamentally alter dendrite formation. At low concns., selected cations (such as Cs or Rb ions) exhibit an effective redn. potential below the std. redn. potential of Li ions. During Li deposition, these additive cations form a pos. charged electrostatic shield around the initial growth tip of the protuberances without redn. and deposition of the additives. This forces further deposition of Li to adjacent regions of the anode and eliminates dendrite formation in Li metal batteries. This strategy may also prevent dendrite growth in Li-ion batteries as well as other metal batteries and transform the surface uniformity of coatings deposited in many general electrodeposition processes.
- 16Qian, J.; Henderson, W. A.; Xu, W.; Bhattacharya, P.; Engelhard, M.; Borodin, O.; Zhang, J.-G. High rate and stable cycling of lithium metal anode. Nat. Commun. 2015, 6, 6362, DOI: 10.1038/ncomms7362Google Scholar16https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtF2itrrI&md5=9bde3388626c7f3d31618a2d934a90cfHigh rate and stable cycling of lithium metal anodeQian, Jiangfeng; Henderson, Wesley A.; Xu, Wu; Bhattacharya, Priyanka; Engelhard, Mark; Borodin, Oleg; Zhang, Ji-GuangNature Communications (2015), 6 (), 6362CODEN: NCAOBW; ISSN:2041-1723. (Nature Publishing Group)Lithium metal is an ideal battery anode. However, dendrite growth and limited Coulombic efficiency during cycling have prevented its practical application in rechargeable batteries. Herein, we report that the use of highly concd. electrolytes composed of ether solvents and the lithium bis(fluorosulfonyl)imide salt enables the high-rate cycling of a lithium metal anode at high Coulombic efficiency (up to 99.1%) without dendrite growth. With 4 M lithium bis(fluorosulfonyl)imide in 1,2-dimethoxyethane as the electrolyte, a lithium|lithium cell can be cycled at 10 mA cm-2 for more than 6,000 cycles, and a copper|lithium cell can be cycled at 4 mA cm-2 for more than 1,000 cycles with an av. Coulombic efficiency of 98.4%. These excellent performances can be attributed to the increased solvent coordination and increased availability of lithium ion concn. in the electrolyte. Further development of this electrolyte may enable practical applications for lithium metal anode in rechargeable batteries.
- 17Suo, L.; Hu, Y.-S.; Li, H.; Armand, M.; Chen, L. A new class of Solvent-in-Salt electrolyte for high-energy rechargeable metallic lithium batteries. Nat. Commun. 2013, 4, 1481, DOI: 10.1038/ncomms2513Google Scholar17https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC3sznslKgtA%253D%253D&md5=cb719ace996906c08eadedf61644e3dcA new class of Solvent-in-Salt electrolyte for high-energy rechargeable metallic lithium batteriesSuo Liumin; Hu Yong-Sheng; Li Hong; Armand Michel; Chen LiquanNature communications (2013), 4 (), 1481 ISSN:.Liquid electrolyte plays a key role in commercial lithium-ion batteries to allow conduction of lithium-ion between cathode and anode. Traditionally, taking into account the ionic conductivity, viscosity and dissolubility of lithium salt, the salt concentration in liquid electrolytes is typically less than 1.2 mol l(-1). Here we show a new class of 'Solvent-in-Salt' electrolyte with ultrahigh salt concentration and high lithium-ion transference number (0.73), in which salt holds a dominant position in the lithium-ion transport system. It remarkably enhances cyclic and safety performance of next-generation high-energy rechargeable lithium batteries via an effective suppression of lithium dendrite growth and shape change in the metallic lithium anode. Moreover, when used in lithium-sulphur battery, the advantage of this electrolyte is further demonstrated that lithium polysulphide dissolution is inhibited, thus overcoming one of today's most challenging technological hurdles, the 'polysulphide shuttle phenomenon'. Consequently, a coulombic efficiency nearing 100% and long cycling stability are achieved.
- 18Lu, Y.; Tu, Z.; Archer, L. A. Stable lithium electrodeposition in liquid and nanoporous solid electrolytes. Nat. Mater. 2014, 13, 961, DOI: 10.1038/nmat4041Google Scholar18https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhtlahu77J&md5=72567640c740e4e4b584b1e838d4d9d8Stable lithium electrodeposition in liquid and nanoporous solid electrolytesLu, Yingying; Tu, Zhengyuan; Archer, Lynden A.Nature Materials (2014), 13 (10), 961-969CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Rechargeable lithium, sodium and aluminum metal-based batteries are among the most versatile platforms for high-energy, cost-effective electrochem. energy storage. Non-uniform metal deposition and dendrite formation on the neg. electrode during repeated cycles of charge and discharge are major hurdles to commercialization of energy-storage devices based on each of these chemistries. A long-held view is that unstable electrodeposition is a consequence of inherent characteristics of these metals and their inability to form uniform electrodeposits on surfaces with inevitable defects. We report on electrodeposition of lithium in simple liq. electrolytes and in nanoporous solids infused with liq. electrolytes. We find that simple liq. electrolytes reinforced with halogenated salt blends exhibit stable long-term cycling at room temp., often with no signs of deposition instabilities over hundreds of cycles of charge and discharge and thousands of operating hours. We rationalize these observations with the help of surface energy data for the electrolyte/lithium interface and impedance anal. of the interface during different stages of cell operation. Our findings provide support for an important recent theor. prediction that the surface mobility of lithium is significantly enhanced in the presence of lithium halide salts. Our results also show that a high electrolyte modulus is unnecessary for stable electrodeposition of lithium.
- 19Zhang, X.; Cheng, X.; Chen, X.; Yan, C.; Zhang, Q. Fluoroethylene Carbonate Additives to Render Uniform Li Deposits in Lithium Metal Batteries. Adv. Funct. Mater. 2017, 27, 1605989, DOI: 10.1002/adfm.201605989Google ScholarThere is no corresponding record for this reference.
- 20Wang, D.; Zhang, W.; Zheng, W.; Cui, X.; Rojo, T.; Zhang, Q. Towards High-Safe Lithium Metal Anodes: Suppressing Lithium Dendrites via Tuning Surface Energy. Adv. Sci. 2017, 4, 1600168, DOI: 10.1002/advs.201600168Google Scholar20https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC1c7nsFektg%253D%253D&md5=97708cfbe6ea7cd34edab1a667521da1Towards High-Safe Lithium Metal Anodes: Suppressing Lithium Dendrites via Tuning Surface EnergyWang Dong; Zheng Weitao; Cui Xiaoqiang; Zhang Wei; Rojo Teofilo; Zhang QiangAdvanced science (Weinheim, Baden-Wurttemberg, Germany) (2017), 4 (1), 1600168 ISSN:2198-3844.The formation of lithium dendrites induces the notorious safety issue and poor cycling life of energy storage devices, such as lithium-sulfur and lithium-air batteries. We propose a surface energy model to describe the complex interface between the lithium anode and electrolyte. A universal strategy of hindering formation of lithium dendrites via tuning surface energy of the relevant thin film growth is suggested. The merit of the novel motif lies not only fundamentally a perfect correlation between electrochemistry and thin film fields, but also significantly promotes larger-scale application of lithium-sulfur and lithium-air batteries, as well as other metal batteries (e.g., Zn, Na, K, Cu, Ag, and Sn).
- 21Zhang, Y.; Qian, J.; Xu, W.; Russell, S. M.; Chen, X.; Nasybulin, E.; Bhattacharya, P.; Engelhard, M. H.; Mei, D.; Cao, R.; Ding, F.; Cresce, A. V.; Xu, K.; Zhang, J.-G. Dendrite-Free Lithium Deposition with Self-Aligned Nanorod Structure. Nano Lett. 2014, 14, 6889– 6896, DOI: 10.1021/nl5039117Google Scholar21https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhvFOjs7zN&md5=568690f8c450f7a6ff90166875481674Dendrite-Free Lithium Deposition with Self-Aligned Nanorod StructureZhang, Yaohui; Qian, Jiangfeng; Xu, Wu; Russell, Selena M.; Chen, Xilin; Nasybulin, Eduard; Bhattacharya, Priyanka; Engelhard, Mark H.; Mei, Donghai; Cao, Ruiguo; Ding, Fei; Cresce, Arthur V.; Xu, Kang; Zhang, Ji-GuangNano Letters (2014), 14 (12), 6889-6896CODEN: NALEFD; ISSN:1530-6984. (American Chemical Society)Suppressing Li dendrite growth is one of the most crit. challenges for the development of Li metal batteries. Here, the authors report for the 1st time the growth of dendrite-free Li films with a self-aligned and highly compacted nanorod structure when the film was deposited in the electrolyte consisting of 1.0M LiPF6 in propylene carbonate with 0.05M CsPF6 as an additive. Evolution of both the surface and the cross-sectional morphologies of the Li films during repeated Li deposition/stripping processes were studied. The formation of the compact Li nanorod structure is preceded by a solid electrolyte interphase (SEI) layer formed on the surface of the substrate. Electrochem. anal. indicates that an initial redn. process occurred at ∼2.05 V vs. Li/Li+ before Li deposition is responsible for the formation of the initial SEI, while the XPS indicates that the presence of CsPF6 additive can largely enhance the formation of LiF in this initial SEI. Hence, the smooth Li deposition in Cs+-contg. electrolyte is the result of a synergistic effect of Cs+ additive and preformed SEI layer. A fundamental understanding on the compn., internal structure, and evolution of Li metal films may lead to new approaches to stabilize the long-term cycling stability of Li metal and other metal anodes for energy storage applications.
- 22Mayers, M. Z.; Kaminski, J. W.; Miller, T. F. Suppression of Dendrite Formation via Pulse Charging in Rechargeable Lithium Metal Batteries. J. Phys. Chem. C 2012, 116, 26214– 26221, DOI: 10.1021/jp309321wGoogle Scholar22https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC38Xhs12mtrzE&md5=e17f74971b90114acb68bb36063c52ceSuppression of Dendrite Formation via Pulse Charging in Rechargeable Lithium Metal BatteriesMayers, Matthew Z.; Kaminski, Jakub W.; Miller, Thomas F.Journal of Physical Chemistry C (2012), 116 (50), 26214-26221CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)We introduce a coarse-grained simulation model for the reductive deposition of lithium cations in secondary lithium batteries. The model accounts for the heterogeneous and nonequil. nature of the electrodeposition dynamics, and it enables simulation of the long timescales and lengthscales assocd. with metal dendrite formation. We investigate the effects of applied overpotential and material properties on early-stage dendrite formation, as well as the mol. mechanisms that govern this process. The model confirms that dendrite formation propensity increases with the applied electrode overpotential, and it demonstrates that application of the electrode overpotential in time-dependent pulses leads to dramatic suppression of dendrite formation while reducing the accumulated electrode on-time by as much as 96%. Moreover, the model predicts that time dependence of the applied electrode overpotential can lead to pos., neg., or zero correlation between cation diffusivity in the solid-electrolyte interphase (SEI) and dendrite formation propensity. Anal. of the simulation trajectories reveals that dendrite formation emerges from a competition between the timescales for cation diffusion and redn. at the anode/SEI interface, with lower applied overpotentials and shorter electrode pulse durations shifting this competition in favor of lower dendrite formation propensity. This work provides a mol. basis for understanding and designing pulsing waveforms that mitigate dendrite formation while minimally affecting battery charging times.
- 23Aryanfar, A.; Brooks, D.; Merinov, B. V.; Goddard, W. A.; Colussi, A. J.; Hoffmann, M. R. Dynamics of Lithium Dendrite Growth and Inhibition: Pulse Charging Experiments and Monte Carlo Calculations. J. Phys. Chem. Lett. 2014, 5, 1721– 1726, DOI: 10.1021/jz500207aGoogle Scholar23https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXntFOmurw%253D&md5=a49ca2f7ec9d6e627017e04994a96429Dynamics of Lithium Dendrite Growth and Inhibition: Pulse Charging Experiments and Monte Carlo CalculationsAryanfar, Asghar; Brooks, Daniel; Merinov, Boris V.; Goddard, William A.; Colussi, Agustin J.; Hoffmann, Michael R.Journal of Physical Chemistry Letters (2014), 5 (10), 1721-1726CODEN: JPCLCD; ISSN:1948-7185. (American Chemical Society)Short-circuiting via dendrites compromises the reliability of Li-metal batteries. Dendrites ensue from instabilities inherent to electrodeposition that should be amenable to dynamic control. Here, the authors report that by charging a scaled coin-cell prototype with 1 ms pulses followed by 3 ms rest periods the av. dendrite length is shortened ∼2.5 times relative to those grown under continuous charging. Monte Carlo simulations dealing with Li+ diffusion and electromigration reveal that expts. involving 20 ms pulses were ineffective because Li+ migration in the strong elec. fields converging to dendrite tips generates extended depleted layers that cannot be replenished by diffusion during rest periods. Because the application of pulses much shorter than the characteristic time τc approx. O(∼1 ms) for polarizing elec. double layers in the system would approach d.c. charging, probably dendrite propagation can should be inhibited (albeit not suppressed) by pulse charging within appropriate frequency ranges.
- 24Liu, Q.; Xu, J.; Yuan, S.; Chang, Z.; Xu, D.; Yin, Y.; Li, L.; Zhong, H.; Jiang, Y.; Yan, J.; Zhang, X. Artificial Protection Film on Lithium Metal Anode toward Long-Cycle-Life Lithium-Oxygen Batteries. Adv. Mater. 2015, 27, 5241– 5247, DOI: 10.1002/adma.201501490Google Scholar24https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtlWgsL%252FN&md5=e7d030229d8bda40d111e25dbce59847Artificial Protection Film on Lithium Metal Anode toward Long-Cycle-Life Lithium-Oxygen BatteriesLiu, Qing-Chao; Xu, Ji-Jing; Yuan, Shuang; Chang, Zhi-Wen; Xu, Dan; Yin, Yan-Bin; Li, Lin; Zhong, Hai-Xia; Jiang, Yin-Shan; Yan, Jun-Min; Zhang, Xin-BoAdvanced Materials (Weinheim, Germany) (2015), 27 (35), 5241-5247CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)A facile and effective strategy was developed to protect the lithium anode of a secondary lithium battery through fabrication of a protection film on the metal Li anode, in which a fluoroethylene carbonate (I) additive plays a key role in the crucial film-forming additive. As a proof-of-concept expt., even when using conventional Super P (carbon black) cathode, the obtained I-treated Li metal anode endowed Li-O2 batteries with superior cycle stability of >100 stable cycles with a fixed capacity of 1000 mA-h/g at a c.d. of 300 mA/g was obtained, which is more than three times that of the cells with a pristine Li metal anode and Li metal anode treated without I. The significantly improved cycling stability could be attributed to the protective film derived from I decompn.,.
- 25Yan, K.; Lee, H.-W.; Gao, T.; Zheng, G.; Yao, H.; Wang, H.; Lu, Z.; Zhou, Y.; Liang, Z.; Liu, Z.; Chu, S.; Cui, Y. Ultrathin Two-Dimensional Atomic Crystals as Stable Interfacial Layer for Improvement of Lithium Metal Anode. Nano Lett. 2014, 14, 6016– 6022, DOI: 10.1021/nl503125uGoogle Scholar25https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhsVekt7jJ&md5=b7cf8adb44da1aedf75c2a104d259fb2Ultrathin Two-Dimensional Atomic Crystals as Stable Interfacial Layer for Improvement of Lithium Metal AnodeYan, Kai; Lee, Hyun-Wook; Gao, Teng; Zheng, Guangyuan; Yao, Hongbin; Wang, Haotian; Lu, Zhenda; Zhou, Yu; Liang, Zheng; Liu, Zhongfan; Chu, Steven; Cui, YiNano Letters (2014), 14 (10), 6016-6022CODEN: NALEFD; ISSN:1530-6984. (American Chemical Society)Stable cycling of lithium metal anode is challenging due to the dendritic lithium formation and high chem. reactivity of lithium with electrolyte and nearly all the materials. Here, we demonstrate a promising novel electrode design by growing two-dimensional (2D) at. crystal layers including hexagonal boron nitride (h-BN) and graphene directly on Cu metal current collectors. Lithium ions were able to penetrate through the point and line defects of the 2D layers during the electrochem. deposition, leading to sandwiched lithium metal between ultrathin 2D layers and Cu. The 2D layers afford an excellent interfacial protection of Li metal due to their remarkable chem. stability as well as mech. strength and flexibility, resulting from the strong intralayer bonds and ultrathin thickness. Smooth Li metal deposition without dendritic and mossy Li formation was realized. We showed stable cycling over 50 cycles with Coulombic efficiency ∼97% in org. carbonate electrolyte with c.d. and areal capacity up to the practical value of 2.0 mA/cm2and 5.0 mAh/cm2, resp., which is a significant improvement over the unprotected electrodes in the same electrolyte.
- 26Liu, Y.; Lin, D.; Yuen, P. Y.; Liu, K.; Xie, J.; Dauskardt, R. H.; Cui, Y. An Artificial Solid Electrolyte Interphase with High Li-Ion Conductivity, Mechanical Strength, and Flexibility for Stable Lithium Metal Anodes. Adv. Mater. 2017, 29, 1605531, DOI: 10.1002/adma.201605531Google ScholarThere is no corresponding record for this reference.
- 27Khurana, R.; Schaefer, J. L.; Archer, L. A.; Coates, G. W. Suppression of Lithium Dendrite Growth Using Cross-Linked Polyethylene/Poly(ethylene oxide) Electrolytes: A New Approach for Practical Lithium-Metal Polymer Batteries. J. Am. Chem. Soc. 2014, 136, 7395– 7402, DOI: 10.1021/ja502133jGoogle Scholar27https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXmsFWnsrc%253D&md5=71960add56cf11e7e9d858a50b0c6d1cSuppression of Lithium Dendrite Growth Using Cross-Linked Polyethylene/Poly(ethylene oxide) Electrolytes: A New Approach for Practical Lithium-Metal Polymer BatteriesKhurana, Rachna; Schaefer, Jennifer L.; Archer, Lynden A.; Coates, Geoffrey W.Journal of the American Chemical Society (2014), 136 (20), 7395-7402CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Solid polymer electrolyte (SPE) membranes are a crit. component of high specific energy rechargeable Li-metal polymer (LMP) batteries. SPEs exhibit low volatility and thus increase the safety of Li-based batteries compared to current state-of-the-art Li-ion batteries that use flammable small-mol. electrolytes. However, most SPEs exhibit low ionic cond. at room temp., and often allow the growth of lithium dendrites that short-circuit the batteries. Both of these deficiencies are significant barriers to the commercialization of LMP batteries. Herein a cross-linked polyethylene/poly(ethylene oxide) SPE is reported with both high ionic cond. (> 1.0 × 10-4 S/cm at 25°) and excellent resistance to dendrite growth. It has been proposed that SPEs with shear moduli of the same order of magnitude as lithium could be used to suppress dendrite growth, leading to increased lifetime and safety for LMP batteries. In contrast to the theor. predictions, the low-modulus (G' ≈ 1.0 × 105 Pa at 90°) cross-linked SPEs reported herein exhibit remarkable dendrite growth resistance. These results suggest that a high-modulus SPE is not a requirement for the control of dendrite proliferation.
- 28Stone, G. M.; Mullin, S. A.; Teran, A. A.; Hallinan, D. T.; Minor, A. M.; Hexemer, A.; Balsara, N. P. Resolution of the Modulus versus Adhesion Dilemma in Solid Polymer Electrolytes for Rechargeable Lithium Metal Batteries. J. Electrochem. Soc. 2012, 159, A222– A227, DOI: 10.1149/2.030203jesGoogle Scholar28https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC38XnvVSnsg%253D%253D&md5=45d31f648114ce418df69b70a8b1ab72Resolution of the Modulus versus Adhesion Dilemma in Solid Polymer Electrolytes for Rechargeable Lithium Metal BatteriesStone, G. M.; Mullin, S. A.; Teran, A. A.; Hallinan, D. T., Jr.; Minor, A. M.; Hexemer, A.; Balsara, N. P.Journal of the Electrochemical Society (2012), 159 (3), A222-A227CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)The authors present a solid electrolyte that adheres to the Li surface and resists dendrite growth, both of which are needed for the development of high specific energy rechargeable batteries with Li anodes. Nanostructured lamellar block copolymer electrolytes exhibit solid-like properties in the bulk, due to the presence of a randomly oriented granular structure, and liq.-like surface properties due to the formation of perpendicularly oriented lamellae at the Li-electrolyte interface. The amt. of charge that can be passed before short-circuit in a sym. Li-polymer-Li cell with nanostructured polystyrene-block-poly(ethylene oxide) electrolytes is larger than that obtained with homopolymer poly(ethylene oxide) electrolytes by a factor of 11 to 48. Grazing incident small angle x-ray scattering confirms that the microstructure of the block copolymer near the Li-polymer interface has a perpendicular orientation. This orientation leads to a liq.-like behavior of the polymer at the interface due to the liq. cryst. symmetry of block copolymers. This combination of bulk and surface properties enhances the resistance to dendrites while maintaining electrode-electrolyte contact.
- 29Yue, L.; Ma, J.; Zhang, J.; Zhao, J.; Dong, S.; Liu, Z.; Cui, G.; Chen, L. All solid-state polymer electrolytes for high-performance lithium ion batteries. Energy Storage Mater. 2016, 5, 139– 164, DOI: 10.1016/j.ensm.2016.07.003Google ScholarThere is no corresponding record for this reference.
- 30Janek, J.; Zeier, W. G. A solid future for battery development. Nat. Energy 2016, 1, 16141, DOI: 10.1038/nenergy.2016.141Google ScholarThere is no corresponding record for this reference.
- 31Li, J.; Ma, C.; Chi, M.; Liang, C.; Dudney, N. J. Solid Electrolyte: the Key for High-Voltage Lithium Batteries. Adv. Energy Mater. 2015, 5, 1401408, DOI: 10.1002/aenm.201401408Google ScholarThere is no corresponding record for this reference.
- 32Suzuki, Y.; Kami, K.; Watanabe, K.; Watanabe, A.; Saito, N.; Ohnishi, T.; Takada, K.; Sudo, R.; Imanishi, N. Transparent cubic garnet-type solid electrolyte of Al2O3-doped Li7La3Zr2O12. Solid State Ionics 2015, 278, 172– 176, DOI: 10.1016/j.ssi.2015.06.009Google Scholar32https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtVKmsbrP&md5=7fd10b6e096b6cc875cc5495c59477c7Transparent cubic garnet-type solid electrolyte of Al2O3-doped Li7La3Zr2O12Suzuki, Yosuke; Kami, K.; Watanabe, K.; Watanabe, A.; Saito, N.; Ohnishi, T.; Takada, K.; Sudo, R.; Imanishi, N.Solid State Ionics (2015), 278 (), 172-176CODEN: SSIOD3; ISSN:0167-2738. (Elsevier B.V.)A transparent garnet-type lithium-ion conducting solid electrolyte of 1.0 wt. % Al2O3-doped Li7La3Zr2O12 (A-LLZ) was prepd. using hot isostatic pressing (HIP). The A-LLZ pellet sintered at 1180°C for 36 h was followed by HIP treatment at 127 MPa and 1180°C under an Ar atm. The bulk cond. of the HIP treated A-LLZ was 9.9 × 10-4 S cm-1 at 25°C. The Li/HIP treated A-LLZ/Li cell showed no short-circuit due to lithium dendrite formation at 0.5 mA cm- 2.
- 33Manthiram, A.; Yu, X.; Wang, S. Lithium battery chemistries enabled by solid-state electrolytes. Nat. Rev. Mater. 2017, 2, 16103, DOI: 10.1038/natrevmats.2016.103Google Scholar33https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXislGitr0%253D&md5=be4704bc600127083842361f9e75c578Lithium battery chemistries enabled by solid-state electrolytesManthiram, Arumugam; Yu, Xingwen; Wang, ShaofeiNature Reviews Materials (2017), 2 (3), 16103CODEN: NRMADL; ISSN:2058-8437. (Nature Publishing Group)Solid-state electrolytes are attracting increasing interest for electrochem. energy storage technologies. In this Review, we provide a background overview and discuss the state of the art, ion-transport mechanisms and fundamental properties of solid-state electrolyte materials of interest for energy storage applications. We focus on recent advances in various classes of battery chemistries and systems that are enabled by solid electrolytes, including all-solid-state lithium-ion batteries and emerging solid-electrolyte lithium batteries that feature cathodes with liq. or gaseous active materials (for example, lithium-air, lithium-sulfur and lithium-bromine systems). A low-cost, safe, aq. electrochem. energy storage concept with a 'mediator-ion' solid electrolyte is also discussed. Advanced battery systems based on solid electrolytes would revitalize the rechargeable battery field because of their safety, excellent stability, long cycle lives and low cost. However, great effort will be needed to implement solid-electrolyte batteries as viable energy storage systems. In this context, we discuss the main issues that must be addressed, such as achieving acceptable ionic cond., electrochem. stability and mech. properties of the solid electrolytes, as well as a compatible electrolyte/electrode interface.
- 34Kamaya, N.; Homma, K.; Yamakawa, Y.; Hirayama, M.; Kanno, R.; Yonemura, M.; Kamiyama, T.; Kato, Y.; Hama, S.; Kawamoto, K.; Mitsui, A. A lithium superionic conductor. Nat. Mater. 2011, 10, 682– 686, DOI: 10.1038/nmat3066Google Scholar34https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3MXpsFaisLc%253D&md5=30637e2968f742a3e1da5f7fa4250644A lithium superionic conductorKamaya, Noriaki; Homma, Kenji; Yamakawa, Yuichiro; Hirayama, Masaaki; Kanno, Ryoji; Yonemura, Masao; Kamiyama, Takashi; Kato, Yuki; Hama, Shigenori; Kawamoto, Koji; Mitsui, AkioNature Materials (2011), 10 (9), 682-686CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Batteries are a key technol. in modern society. They are used to power elec. and hybrid elec. vehicles and to store wind and solar energy in smart grids. Electrochem. devices with high energy and power densities can currently be powered only by batteries with org. liq. electrolytes. However, such batteries require relatively stringent safety precautions, making large-scale systems complicated and expensive. The application of solid electrolytes is currently limited because they attain practically useful conductivities (10-2 S/cm) only at 50-80°, which is one order of magnitude lower than those of org. liq. electrolytes. Here, the authors report a Li superionic conductor, Li10GeP2S12 that has a new 3-dimensional framework structure. It exhibits an extremely high Li ionic cond. of 12 mS/cm at room temp. This represents the highest cond. achieved in a solid electrolyte, exceeding even those of liq. org. electrolytes. This new solid-state battery electrolyte has many advantages in terms of device fabrication (facile shaping, patterning and integration), stability (non-volatile), safety (non-explosive) and excellent electrochem. properties (high cond. and wide potential window).
- 35Kato, Y.; Hori, S.; Saito, T.; Suzuki, K.; Hirayama, M.; Mitsui, A.; Yonemura, M.; Iba, H.; Kanno, R. High-power all-solid-state batteries using sulfide superionic conductors. Nat. Energy 2016, 1, 16030, DOI: 10.1038/nenergy.2016.30Google Scholar35https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVekurs%253D&md5=cc1210221e70bc3e6c06e015effc70deHigh-power all-solid-state batteries using sulfide superionic conductorsKato, Yuki; Hori, Satoshi; Saito, Toshiya; Suzuki, Kota; Hirayama, Masaaki; Mitsui, Akio; Yonemura, Masao; Iba, Hideki; Kanno, RyojiNature Energy (2016), 1 (4), 16030CODEN: NEANFD; ISSN:2058-7546. (Nature Publishing Group)Compared with Li-ion batteries with liq. electrolytes, all-solid-state batteries offer an attractive option owing to their potential in improving the safety and achieving both high power and high energy densities. Despite extensive research efforts, the development of all-solid-state batteries still falls short of expectation largely because of the lack of suitable candidate materials for the electrolyte required for practical applications. Here the authors report Li superionic conductors with an exceptionally high cond. (25 mS cm-1 for Li9.54Si1.74P1.44S11.7Cl0.3), as well as high stability ( ∼0 V vs. Li metal for Li9.6P3S12). A fabricated all-solid-state cell based on this Li conductor has very small internal resistance, esp. at 100 oC. The cell possesses high specific power that is superior to that of conventional cells with liq. electrolytes. Stable cycling with a high c.d. of 18 C (charging/discharging in just 3 min; where C is the C-rate) is also demonstrated.
- 36Kerman, K.; Luntz, A.; Viswanathan, V.; Chiang, Y.-M.; Chen, Z. Review-Practical Challenges Hindering the Development of Solid State Li Ion Batteries. J. Electrochem. Soc. 2017, 164, A1731– A1744, DOI: 10.1149/2.1571707jesGoogle Scholar36https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVCitLvI&md5=99cf3345659e25c91eb25ed7090d1403Review-Practical Challenges Hindering the Development of Solid State Li Ion BatteriesKerman, Kian; Luntz, Alan; Viswanathan, Venkatasubramanian; Chiang, Yet-Ming; Chen, ZheboJournal of the Electrochemical Society (2017), 164 (7), A1731-A1744CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Solid state electrolyte systems boasting Li+ cond. of >10 mS cm-1 at room temp. have opened the potential for developing a solid state battery with power and energy densities that are competitive with conventional liq. electrolyte systems. The primary focus of this review is twofold. First, differences in Li penetration resistance in solid state systems are discussed, and kinetic limitations of the solid state interface are highlighted. Second, technol. challenges assocd. with processing such systems in relevant form factors are elucidated, and architectures needed for cell level devices in the context of product development are reviewed. Specific research vectors that provide high value to advancing solid state batteries are outlined and discussed.
- 37Sharafi, A.; Yu, S.; Naguib, M.; Lee, M.; Ma, C.; Meyer, H. M.; Nanda, J.; Chi, M.; Siegel, D. J.; Sakamoto, J. Impact of air exposure and surface chemistry on Li-Li7La3Zr2O12 interfacial resistance. J. Mater. Chem. A 2017, 5, 13475– 13487, DOI: 10.1039/C7TA03162AGoogle Scholar37https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVWmtrnE&md5=ba7e873b21db6b50f59e450c3d6f6ec2Impact of air exposure and surface chemistry on Li-Li7La3Zr2O12 interfacial resistanceSharafi, Asma; Yu, Seungho; Naguib, Michael; Lee, Marcus; Ma, Cheng; Meyer, Harry M.; Nanda, Jagjit; Chi, Maiofang; Siegel, Donald J.; Sakamoto, JeffJournal of Materials Chemistry A: Materials for Energy and Sustainability (2017), 5 (26), 13475-13487CODEN: JMCAET; ISSN:2050-7496. (Royal Society of Chemistry)Li7La3Zr2O12 (LLZO) is a promising solid-state electrolyte that could enable solid-state-batteries (SSB) using metallic Li anodes. For a SSB to be viable, the stability and charge transfer kinetics at the Li-LLZO interface should foster facile plating and stripping of Li. Contrary to these goals, recent studies have reported high Li-LLZO interfacial resistance which was attributed to a contamination layer that forms upon exposure of LLZO to air. This study clarifies the mechanisms and consequences assocd. with air exposure of LLZO; addnl., strategies to minimize these effects are described. First-principles calcns. reveal that LLZO readily reacts with humid air; the most favorable reaction pathway involves protonation of LLZO and formation of Li2CO3. XPS, SEM, Raman spectroscopy, and transmission electron microscopy were used to characterize the surface and subsurface chem. of LLZO as a function of relative humidity and exposure time. Electrochem. impedance spectroscopy was used to measure the Li-LLZO interfacial resistance as a function of surface contamination. These data indicate that air exposure-induced contamination impacts the interfacial resistance significantly, when exposure time exceeds 24 h. The results of this study provide valuable insight into the sensitivity of LLZO to air and how the effects of air contamination can be reversed.
- 38Sharafi, A.; Haslam, C. G.; Kerns, R. D.; Wolfenstine, J.; Sakamoto, J. Controlling and correlating the effect of grain size with the mechanical and electrochemical properties of Li7La3Zr2O12 solid-state electrolyte. J. Mater. Chem. A 2017, 5, 21491– 21504, DOI: 10.1039/C7TA06790AGoogle Scholar38https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhs1Sksb%252FP&md5=eccb1f1d8cfb3d13b2237d27793aa772Controlling and correlating the effect of grain size with the mechanical and electrochemical properties of Li7La3Zr2O12 solid-state electrolyteSharafi, Asma; Haslam, Catherine G.; Kerns, Robert D.; Wolfenstine, Jeff; Sakamoto, JeffJournal of Materials Chemistry A: Materials for Energy and Sustainability (2017), 5 (40), 21491-21504CODEN: JMCAET; ISSN:2050-7496. (Royal Society of Chemistry)Li7La3Zr2O12 (LLZO) solid-state electrolyte is garnering interest due to its potential to enable solid-state batteries (SSBs) using metallic Li anodes. However, Li metal propagates along LLZO grain boundaries at high Li plating current densities (above the crit. c.d., CCD). In the present study, we examd. whether microstructural aspects, such as grain size, could influence mech. and electrochem. properties thereby affecting the CCD. A unique densification technique (heating between 1100 and 1300 °C) was used to control grain size. Electron backscatter diffraction detd. that the grain size and the misorientation angle varied from 5 to 600 μm and 20 to 40°, resp. Vickers indentation was used to characterize the mech. properties and revealed that hardness decreased (9.9-6.8 GPa) with increasing grain size, but the fracture toughness was invariant (0.6 MPa m-1/2) at grain sizes ≥40 μm. DC and AC techniques were used to measure and correlate the CCD with grain size and showed that the CCD increased with increasing grain size achieving a max. of 0.6 mA cm-2. We believe the implications of this work could be far-reaching in that they represent a significant step towards understanding the mechanism(s) that control the stability of the Li-LLZO interface and a rational approach to increase the CCD in SSBs.
- 39Monroe, C.; Newman, J. The Impact of Elastic Deformation on Deposition Kinetics at Lithium/Polymer Interfaces. J. Electrochem. Soc. 2005, 152, A396– A404, DOI: 10.1149/1.1850854Google Scholar39https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2MXhs1KktLc%253D&md5=e878820c6a811396757bd7435bdb40adThe impact of elastic deformation on deposition kinetics at lithium/polymer interfacesMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2005), 152 (2), A396-A404CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Past theories of electrode stability assume that the surface tension resists the amplification of surface roughness at cathodes and show that instability at lithium/liq. interfaces cannot be prevented by surface forces alone. This work treats interfacial stability in lithium/polymer systems where the electrolyte is solid. Linear elasticity theory is employed to compute the addnl. effect of bulk mech. forces on electrode stability. The lithium and polymer are treated as Hookean elastic materials, characterized by their shear moduli and Poisson's ratios. Two-dimensional displacement distributions that satisfy force balances across a periodically deforming interface are derived; these allow computation of the stress and surface-tension forces. The incorporation of elastic effects into a kinetic model demonstrates regimes of electrolyte mech. properties where amplification of surface roughness can be inhibited. For a polymer material with Poisson's ratio similar to poly(ethylene oxide), interfacial roughening is mech. suppressed when the separator shear modulus is about twice that of lithium.
- 40Ahmad, Z.; Viswanathan, V. Stability of Electrodeposition at Solid-Solid Interfaces and Implications for Metal Anodes. Phys. Rev. Lett. 2017, 119, 056003, DOI: 10.1103/PhysRevLett.119.056003Google Scholar40https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXhs1SrtbrP&md5=b71331ba73f970ec5c45f52cdc08ecadStability of electrodeposition at solid-solid interfaces and implications for metal anodesAhmad, Zeeshan; Viswanathan, VenkatasubramanianPhysical Review Letters (2017), 119 (5), 056003/1-056003/6CODEN: PRLTAO; ISSN:1079-7114. (American Physical Society)We generalize the conditions for stable electrodeposition at isotropic solid-solid interfaces using a kinetic model which incorporates the effects of stresses and surface tension at the interface. We develop a stability diagram that shows two regimes of stability: a previously known pressure-driven mechanism and a new d.-driven stability mechanism that is governed by the relative d. of metal in the two phases. We show that inorg. solids and solid polymers generally do not lead to stable electrodeposition, and provide design guidelines for achieving stable electrodeposition.
- 41Diggle, J. W.; Despic, A. R.; Bockris, J. O. The Mechanism of the Dendritic Electrocrystallization of Zinc. J. Electrochem. Soc. 1969, 116, 1503– 1514, DOI: 10.1149/1.2411588Google Scholar41https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaE3cXos1yl&md5=48077f26ea20fa76b2cc78e39c4f1309Mechanism of the dendritic electrocrystallization of zincDiggle, J. W.; Despic, A. R.; Bockris, J. O'M.Journal of the Electrochemical Society (1969), 116 (11), 1503-14CODEN: JESOAN; ISSN:0013-4651.Measurements were made of the growth rate of Zn dendrites in alk. zincate solns. as a function of overpotential (η), concn. (c), and temp. (T). The tip radii were measured by electron microscopy. At const. potential, an initiation time of between 5 and 100 min is observed, depending on η, c, and T. The total current to base and dendrite was independent of time until a time *aui, where τi < τd (the time for initiation obtained from the growth rate vs. time relation). Thereafter, i is proportional to t2. A crit. overpotential was detd., -75 mv. >ηcrit> -85 mv. Below this ηcrit, sponge was formed. Dendrites were observed up to η = -160 mv.; above this the deposition was heavy sponge. At a given c, the growth rate of a given dendrite increased with η according to an exponential law. The growing tip is parabolic, where 10-5 < γtip < 10-4 cm. No twinning was observed. The basic model used depended on the increase in c.d. possible for an electrodic reaction when the diffusion current depends on a radius of curvature of the substrate, rather than the linear diffusion layer thickness, δ. When the tip of a dendrite-precursor attains this condition, its growth is released from the diffusion control characteristic of it in the predendrite situation, and it grows further under predominantly activation control at a rate far greater than that possible in any other direction, where the radii of curvature are much greater. The Gibbs radius-dependent overpotential term is also present, although it has a minimized influence. The initiation of the dendrite is treated in terms of growing pyramids on the substrate surface. At 1st the growth is linear-diffusion controlled, but the rotation of the spiral, within the linear diffusion boundary surrounding the sphere, gives rise to a decrease of the effective radius (γ) of curvature of the dendrite tip until the value γ<0.1 δ is attained, which is effectively the condition for the dendrite initiation. The theory of the propagation in terms of the activation, diffusion, and Gibbs overpotential is consistent, in terms of τd, with expt. A derived growth-time line is also numerically consistent with expt. The dendrite growth rate as a function of c and η are numerically calcd. with reasonable consistency. The tip radius can also be approx. calcd. in terms of the present model.
- 42Monroe, C.; Newman, J. Dendrite Growth in Lithium/Polymer Systems: A Propagation Model for Liquid Electrolytes under Galvanostatic Conditions. J. Electrochem. Soc. 2003, 150, A1377– A1384, DOI: 10.1149/1.1606686Google Scholar42https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD3sXnt1OmtLw%253D&md5=178ec3a3e854d05aede7708d68c7957aDendrite Growth in Lithium/Polymer SystemsMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2003), 150 (10), A1377-A1384CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Dendrite growth in a parallel-electrode Li/polymer battery during galvanostatic charging was modeled. The growth model is surface-energy controlled, incorporating the effect of dendrite tip curvature into the dendrite growth kinetics. Using data representative of the oxymethylene-linked poly(ethylene oxide)/LiTFSI system, dendrites accelerate across cells under all conditions, and growth is always slowed by lowering the c.d. Cell shorting occurs during typical charges at current densities >75% of the limiting current. Increased interelectrode distance slows failure, but the advantages decrease as distance increases. A factor of 1000 increase in surface forces delays cell failure by only 6%. While larger diffusion coeffs. usually extend the time to cell failure, this trend is not consistent at high transference nos.
- 43Monroe, C.; Newman, J. The Effect of Interfacial Deformation on Electrodeposition Kinetics. J. Electrochem. Soc. 2004, 151, A880– A886, DOI: 10.1149/1.1710893Google Scholar43https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2cXktVGkt70%253D&md5=22ed18c5cf280522d5d26e2bc30cb6bcThe Effect of Interfacial Deformation on Electrodeposition KineticsMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2004), 151 (6), A880-A886CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Mullins-Sekerka linear stability anal. and the Barton and Bockris dendrite-propagation model are popular methods used to describe cathodic roughening and dendritic growth. These commonly cited theories employ kinetic relations that differ in math. form, but both contain the effects of surface tension and local concn. deviations induced by surface roughening. Here, a kinetic model is developed which addnl. includes mech. forces such as elasticity, viscous drag, and pressure, showing their effect on exchange current densities and potentials at roughening interfaces. The proposed expression describes the c.d. in terms of applied overpotential at deformed interfaces with arbitrary three-dimensional interfacial geometry. Both the Mullins-Sekerka and the Barton-Bockris kinetics can be derived as special cases of the general expression, thereby validating the proposed model and elucidating the fundamental assumptions on which the 2 previous theories rely.
- 44Curtarolo, S.; Hart, G. L. W.; Nardelli, M. B.; Mingo, N.; Sanvito, S.; Levy, O. The high-throughput highway to computational materials design. Nat. Mater. 2013, 12, 191, DOI: 10.1038/nmat3568Google Scholar44https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXislWju7c%253D&md5=5e116fbafda8e8437ccd0fdf7304d939The high-throughput highway to computational materials designCurtarolo, Stefano; Hart, Gus L. W.; Nardelli, Marco Buongiorno; Mingo, Natalio; Sanvito, Stefano; Levy, OhadNature Materials (2013), 12 (3), 191-201CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)A review. High-throughput computational materials design is an emerging area of materials science. By combining advanced thermodn. and electronic-structure methods with intelligent data mining and database construction, and exploiting the power of current supercomputer architectures, scientists generate, manage and analyze enormous data repositories for the discovery of novel materials. In this Review we provide a current snapshot of this rapidly evolving field, and highlight the challenges and opportunities that lie ahead.
- 45Saal, J. E.; Kirklin, S.; Aykol, M.; Meredig, B.; Wolverton, C. Materials Design and Discovery with High-Throughput Density Functional Theory: The Open Quantum Materials Database (OQMD). JOM 2013, 65, 1501– 1509, DOI: 10.1007/s11837-013-0755-4Google Scholar45https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhsFentbzK&md5=feaac43dc6ff4c2d7a7a4c94f0b58c2bMaterials Design and Discovery with High-Throughput Density Functional Theory: The Open Quantum Materials Database (OQMD)Saal, James E.; Kirklin, Scott; Aykol, Muratahan; Meredig, Bryce; Wolverton, C.JOM (2013), 65 (11), 1501-1509CODEN: JOMMER; ISSN:1047-4838. (Springer)A review. High-throughput d. functional theory (HT DFT) is fast becoming a powerful tool for accelerating materials design and discovery by the amassing tens and even hundreds of thousands of DFT calcns. in large databases. Complex materials problems can be approached much more efficiently and broadly through the sheer quantity of structures and chemistries available in such databases. Our HT DFT database, the Open Quantum Materials Database (OQMD), contains over 200,000 DFT calcd. crystal structures and will be freely available for public use at http://oqmd.org. In this review, we describe the OQMD and its use in five materials problems, spanning a wide range of applications and materials types: (I) Li-air battery combination catalyst/electrodes, (II) Li-ion battery anodes, (III) Li-ion battery cathode coatings reactive with HF, (IV) Mg-alloy long-period stacking ordered (LPSO) strengthening ppts., and (V) training a machine learning model to predict new stable ternary compds.
- 46Pilania, G.; Wang, C.; Jiang, X.; Rajasekaran, S.; Ramprasad, R. Accelerating materials property predictions using machine learning. Sci. Rep. 2013, 3, 2810, DOI: 10.1038/srep02810Google Scholar46https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC2c%252FltlCqtQ%253D%253D&md5=3475edb4dda3d93baae0d552d482b187Accelerating materials property predictions using machine learningPilania Ghanshyam; Wang Chenchen; Jiang Xun; Rajasekaran Sanguthevar; Ramprasad RamamurthyScientific reports (2013), 3 (), 2810 ISSN:.The materials discovery process can be significantly expedited and simplified if we can learn effectively from available knowledge and data. In the present contribution, we show that efficient and accurate prediction of a diverse set of properties of material systems is possible by employing machine (or statistical) learning methods trained on quantum mechanical computations in combination with the notions of chemical similarity. Using a family of one-dimensional chain systems, we present a general formalism that allows us to discover decision rules that establish a mapping between easily accessible attributes of a system and its properties. It is shown that fingerprints based on either chemo-structural (compositional and configurational information) or the electronic charge density distribution can be used to make ultra-fast, yet accurate, property predictions. Harnessing such learning paradigms extends recent efforts to systematically explore and mine vast chemical spaces, and can significantly accelerate the discovery of new application-specific materials.
- 47Liu, Y.; Zhao, T.; Ju, W.; Shi, S. Materials discovery and design using machine learning. J. Materiomics 2017, 3, 159– 177, DOI: 10.1016/j.jmat.2017.08.002Google ScholarThere is no corresponding record for this reference.
- 48Gómez-Bombarelli, R.; Wei, J. N.; Duvenaud, D.; Hernández-Lobato, J. M.; Sánchez-Lengeling, B.; Sheberla, D.; Aguilera-Iparraguirre, J.; Hirzel, T. D.; Adams, R. P.; Aspuru-Guzik, A. Automatic Chemical Design Using a Data-Driven Continuous Representation of Molecules. ACS Cent. Sci. 2018, 4, 268– 276, DOI: 10.1021/acscentsci.7b00572Google Scholar48https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXntlWquw%253D%253D&md5=322d9ff569fc9c8831e91d915104d985Automatic Chemical Design Using a Data-Driven Continuous Representation of MoleculesGomez-Bombarelli, Rafael; Wei, Jennifer N.; Duvenaud, David; Hernandez-Lobato, Jose Miguel; Sanchez-Lengeling, Benjamin; Sheberla, Dennis; Aguilera-Iparraguirre, Jorge; Hirzel, Timothy D.; Adams, Ryan P.; Aspuru-Guzik, AlanACS Central Science (2018), 4 (2), 268-276CODEN: ACSCII; ISSN:2374-7951. (American Chemical Society)We report a method to convert discrete representations of mols. to and from a multidimensional continuous representation. This model allows us to generate new mols. for efficient exploration and optimization through open-ended spaces of chem. compds. A deep neural network was trained on hundreds of thousands of existing chem. structures to construct three coupled functions: an encoder, a decoder, and a predictor. The encoder converts the discrete representation of a mol. into a real-valued continuous vector, and the decoder converts these continuous vectors back to discrete mol. representations. The predictor ests. chem. properties from the latent continuous vector representation of the mol. Continuous representations of mols. allow us to automatically generate novel chem. structures by performing simple operations in the latent space, such as decoding random vectors, perturbing known chem. structures, or interpolating between mols. Continuous representations also allow the use of powerful gradient-based optimization to efficiently guide the search for optimized functional compds. We demonstrate our method in the domain of drug-like mols. and also in a set of mols. with fewer that nine heavy atoms.
- 49de Jong, M.; Chen, W.; Notestine, R.; Persson, K.; Ceder, G.; Jain, A.; Asta, M.; Gamst, A. A Statistical Learning Framework for Materials Science: Application to Elastic Moduli of k-nary Inorganic Polycrystalline Compounds. Sci. Rep. 2016, 6, 34256, DOI: 10.1038/srep34256Google Scholar49https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28Xhs1amtL%252FO&md5=dbe3625fe35277822c6ae92c7dcbfee7A Statistical Learning Framework for Materials Science: Application to Elastic Moduli of k-nary Inorganic Polycrystalline Compoundsde Jong, Maarten; Chen, Wei; Notestine, Randy; Persson, Kristin; Ceder, Gerbrand; Jain, Anubhav; Asta, Mark; Gamst, AnthonyScientific Reports (2016), 6 (), 34256CODEN: SRCEC3; ISSN:2045-2322. (Nature Publishing Group)Materials scientists increasingly employ machine or statistical learning (SL) techniques to accelerate materials discovery and design. Such pursuits benefit from pooling training data across, and thus being able to generalize predictions over, k-nary compds. of diverse chemistries and structures. This work presents a SL framework that addresses challenges in materials science applications, where datasets are diverse but of modest size, and extreme values are often of interest. Our advances include the application of power or Holder means to construct descriptors that generalize over chem. and crystal structure, and the incorporation of multivariate local regression within a gradient boosting framework. The approach is demonstrated by developing SL models to predict bulk and shear moduli (K and G, resp.) for polycryst. inorg. compds., using 1,940 compds. from a growing database of calcd. elastic moduli for metals, semiconductors and insulators. The usefulness of the models is illustrated by screening for superhard materials.
- 50Isayev, O.; Oses, C.; Toher, C.; Gossett, E.; Curtarolo, S.; Tropsha, A. Universal fragment descriptors for predicting properties of inorganic crystals. Nat. Commun. 2017, 8, 15679, DOI: 10.1038/ncomms15679Google Scholar50https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXpt1Oksb8%253D&md5=543e2069263b9b1b1a121667866e2c5aUniversal fragment descriptors for predicting properties of inorganic crystalsIsayev, Olexandr; Oses, Corey; Toher, Cormac; Gossett, Eric; Curtarolo, Stefano; Tropsha, AlexanderNature Communications (2017), 8 (), 15679CODEN: NCAOBW; ISSN:2041-1723. (Nature Publishing Group)A review. Although historically materials discovery has been driven by a laborious trial-and-error process, knowledge-driven materials design can now be enabled by the rational combination of Machine Learning methods and materials databases. Here, data from the AFLOW repository for ab initio calcns. is combined with Quant. Materials Structure-Property Relationship models to predict important properties: metal/insulator classification, band gap energy, bulk/shear moduli, Debye temp. and heat capacities. The prediction's accuracy compares well with the quality of the training data for virtually any stoichiometric inorg. cryst. material, reciprocating the available thermomech. exptl. data. The universality of the approach is attributed to the construction of the descriptors: Property-Labeled Materials Fragments. The representations require only minimal structural input allowing straightforward implementations of simple heuristic design rules.
- 51Fujimura, K.; Seko, A.; Koyama, Y.; Kuwabara, A.; Kishida, I.; Shitara, K.; Fisher, C. A. J.; Moriwake, H.; Tanaka, I. Accelerated Materials Design of Lithium Superionic Conductors Based on First-Principles Calculations and Machine Learning Algorithms. Adv. Energy Mater. 2013, 3, 980– 985, DOI: 10.1002/aenm.201300060Google Scholar51https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtlWhsbzM&md5=4ec409403b25e39e04cc760523694fa3Accelerated materials design of lithium superionic conductors based on first-principles calculations and machine learning algorithmsFujimura, Koji; Seko, Atsuto; Koyama, Yukinori; Kuwabara, Akihide; Kishida, Ippei; Shitara, Kazuki; Fisher, Craig A. J.; Moriwake, Hiroki; Tanaka, IsaoAdvanced Energy Materials (2013), 3 (8), 980-985CODEN: ADEMBC; ISSN:1614-6840. (Wiley-Blackwell)In this article, results of systematic sets of first-principles calcns. based on the cluster expansion method, as well as first-principles mol. dynamics (FPMD) simulations carried out to calc. lithium-ion conductivities at high temp., for a diverse range of compns. is studied. A machine-learning technique is used to combine theor. and exptl. datasets to predict the cond. of each compn. at 373 K. The insights obtained show that an iterative combination of first-principles calcns. and focused expts. can greatly accelerate the materials design process by enabling a wide compositional and structural phase space to be examd. efficiently.
- 52Sendek, A. D.; Yang, Q.; Cubuk, E. D.; Duerloo, K.-A. N.; Cui, Y.; Reed, E. J. Holistic computational structure screening of more than 12000 candidates for solid lithium-ion conductor materials. Energy Environ. Sci. 2017, 10, 306– 320, DOI: 10.1039/C6EE02697DGoogle Scholar52https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XhvFymtbrP&md5=97cc808518346d0a599f623a2b35b7e4Holistic computational structure screening of more than 12 000 candidates for solid lithium-ion conductor materialsSendek, Austin D.; Yang, Qian; Cubuk, Ekin D.; Duerloo, Karel-Alexander N.; Cui, Yi; Reed, Evan J.Energy & Environmental Science (2017), 10 (1), 306-320CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)We present a new type of large-scale computational screening approach for identifying promising candidate materials for solid state electrolytes for lithium ion batteries that is capable of screening all known lithium contg. solids. To be useful for batteries, high performance solid state electrolyte materials must satisfy many requirements at once, an optimization that is difficult to perform exptl. or with computationally expensive ab initio techniques. We first screen 12 831 lithium contg. cryst. solids for those with high structural and chem. stability, low electronic cond., and low cost. We then develop a data-driven ionic cond. classification model using logistic regression for identifying which candidate structures are likely to exhibit fast lithium conduction based on exptl. measurements reported in the literature. The screening reduces the list of candidate materials from 12 831 down to 21 structures that show promise as electrolytes, few of which have been examd. exptl. We discover that none of our simple atomistic descriptor functions alone provide predictive power for ionic cond., but a multi-descriptor model can exhibit a useful degree of predictive power. We also find that screening for structural stability, chem. stability and low electronic cond. eliminates 92.2% of all Li-contg. materials and screening for high ionic cond. eliminates a further 93.3% of the remainder. Our screening utilizes structures and electronic information contained in the Materials Project database.
- 53Evans, J. D.; Coudert, F.-X. Predicting the Mechanical Properties of Zeolite Frameworks by Machine Learning. Chem. Mater. 2017, 29, 7833– 7839, DOI: 10.1021/acs.chemmater.7b02532Google Scholar53https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtl2lsLfK&md5=5745ca383f3204d7c606d9eec2953d22Predicting the Mechanical Properties of Zeolite Frameworks by Machine LearningEvans, Jack D.; Coudert, Francois-XavierChemistry of Materials (2017), 29 (18), 7833-7839CODEN: CMATEX; ISSN:0897-4756. (American Chemical Society)We show here that machine learning is a powerful new tool for predicting the elastic response of zeolites. We built our machine learning approach relying on geometric features only, which are related to local geometry, structure, and porosity of a zeolite, to predict bulk and shear moduli of zeolites with an accuracy exceeding that of force field approaches. The development of this model has illustrated clear correlations between characteristic features of a zeolite and elastic moduli, providing exceptional insight into the mechanics of zeolitic frameworks. Finally, we employ this methodol. to predict the elastic response of 590,448 hypothetical zeolites, and the results of this massive database provide clear evidence of stability trends in porous materials.
- 54Ahmad, Z.; Viswanathan, V. Role of anisotropy in determining stability of electrodeposition at solid-solid interfaces. Phys. Rev. Materials 2017, 1, 055403, DOI: 10.1103/PhysRevMaterials.1.055403Google ScholarThere is no corresponding record for this reference.
- 55Xu, C.; Ahmad, Z.; Aryanfar, A.; Viswanathan, V.; Greer, J. R. Enhanced strength and temperature dependence of mechanical properties of Li at small scales and its implications for Li metal anodes. Proc. Natl. Acad. Sci. U. S. A. 2017, 114, 57– 61, DOI: 10.1073/pnas.1615733114Google Scholar55https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XitFWls7fM&md5=65404fc79b4b340710a0a4c287094cf0Enhanced strength and temperature dependence of mechanical properties of Li at small scales and its implications for Li metal anodesXu, Chen; Ahmad, Zeeshan; Aryanfar, Asghar; Viswanathan, Venkatasubramanian; Greer, Julia R.Proceedings of the National Academy of Sciences of the United States of America (2017), 114 (1), 57-61CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Most next-generation Li ion battery chemistries require a functioning lithium metal (Li) anode. However, its application in secondary batteries has been inhibited because of uncontrollable dendrite growth during cycling. Mech. suppression of dendrite growth through solid polymer electrolytes (SPEs) or through robust separators has shown the most potential for alleviating this problem. Studies of the mech. behavior of Li at any length scale and temp. are limited because of its extreme reactivity, which renders sample prepn., transfer, microstructure characterization, and mech. testing extremely challenging. We conduct nanomech. expts. in an in situ scanning electron microscope and show that micrometer-sized Li attains extremely high strengths of 105 MPa at room temp. and of 35 MPa at 90 °C. We demonstrate that single-cryst. Li exhibits a power-law size effect at the micrometer and submicrometer length scales, with the strengthening exponent of -0.68 at room temp. and of -1.00 at 90 °C. We also report the elastic and shear moduli as a function of crystallog. orientation gleaned from expts. and first-principles calcns., which show a high level of anisotropy up to the m.p., where the elastic and shear moduli vary by a factor of ∼4 between the stiffest and most compliant orientations. The emergence of such high strengths in small-scale Li and sensitivity of this metal's stiffness to crystallog. orientation help explain why the existing methods of dendrite suppression have been mainly unsuccessful and have significant implications for practical design of future-generation batteries.
- 56Shi, F.; Pei, A.; Vailionis, A.; Xie, J.; Liu, B.; Zhao, J.; Gong, Y.; Cui, Y. Strong texturing of lithium metal in batteries. Proc. Natl. Acad. Sci. U. S. A. 2017, 114, 12138– 12143, DOI: 10.1073/pnas.1708224114Google Scholar56https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhslemsrjO&md5=ca7238bf137ef10cd147f88226c28000Strong texturing of lithium metal in batteriesShi, Feifei; Pei, Allen; Vailionis, Arturas; Xie, Jin; Liu, Bofei; Zhao, Jie; Gong, Yongji; Cui, YiProceedings of the National Academy of Sciences of the United States of America (2017), 114 (46), 12138-12143CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Lithium, with its high theor. specific capacity and lowest electrochem. potential, was recognized as the ultimate neg. electrode material for next-generation lithium-based high-energy-d. batteries. However, a key challenge that has yet to be overcome is the inferior reversibility of Li plating and stripping, typically thought to be related to the uncontrollable morphol. evolution of the Li anode during cycling. Here we show that Li-metal texturing (preferential crystallog. orientation) occurs during electrochem. deposition, which governs the morphol. change of the Li anode. X-ray diffraction pole-figure anal. demonstrates that the texture of Li deposits is primarily dependent on the type of additive or cross-over mol. from the cathode side. With adsorbed additives, like LiNO3 and polysulfide, the lithium deposits are strongly textured, with Li (110) planes parallel to the substrate, and thus exhibit uniform, rounded morphol. A growth diagram of lithium deposits is given to connect various texture and morphol. scenarios for different battery electrolytes. This understanding of lithium electrocrystn. from the crystallog. point of view provides significant insight for future lithium anode materials design in high-energy-d. batteries.
- 57Wang, Y.; Richards, W. D.; Ong, S. P.; Miara, L. J.; Kim, J. C.; Mo, Y.; Ceder, G. Design principles for solid-state lithium superionic conductors. Nat. Mater. 2015, 14, 1026– 1031, DOI: 10.1038/nmat4369Google Scholar57https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtlCksb%252FI&md5=114ad3946493cf35ef3ee5d65e37c2d7Design principles for solid-state lithium superionic conductorsWang, Yan; Richards, William Davidson; Ong, Shyue Ping; Miara, Lincoln J.; Kim, Jae Chul; Mo, Yifei; Ceder, GerbrandNature Materials (2015), 14 (10), 1026-1031CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Lithium solid electrolytes can potentially address two key limitations of the org. electrolytes used in today's lithium-ion batteries, namely, their flammability and limited electrochem. stability. However, achieving a Li+ cond. in the solid state comparable to existing liq. electrolytes (>1 mS cm-1) is particularly challenging. In this work, we reveal a fundamental relationship between anion packing and ionic transport in fast Li-conducting materials and expose the desirable structural attributes of good Li-ion conductors. We find that an underlying body-centered cubic-like anion framework, which allows direct Li hops between adjacent tetrahedral sites, is most desirable for achieving high ionic cond., and that indeed this anion arrangement is present in several known fast Li-conducting materials and other fast ion conductors. These findings provide important insight towards the understanding of ionic transport in Li-ion conductors and serve as design principles for future discovery and design of improved electrolytes for Li-ion batteries.
- 58Shannon, R. D. Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Crystallogr., Sect. A: Cryst. Phys., Diffr., Theor. Gen. Crystallogr. 1976, 32, 751– 767, DOI: 10.1107/S0567739476001551Google ScholarThere is no corresponding record for this reference.
- 59Gotoh, K.; Finney, J. L. Statistical geometrical approach to random packing density of equal spheres. Nature 1974, 252, 202, DOI: 10.1038/252202a0Google ScholarThere is no corresponding record for this reference.
- 60Stepanyuk, V.; Szasz, A.; Katsnelson, A.; Trushin, O.; Müller, H.; Kirchmayr, H. Microstructure and its relaxation in FeB amorphous system simulated by moleculular dynamics. J. Non-Cryst. Solids 1993, 159, 80– 87, DOI: 10.1016/0022-3093(93)91284-AGoogle ScholarThere is no corresponding record for this reference.
- 61Ong, S. P.; Richards, W. D.; Jain, A.; Hautier, G.; Kocher, M.; Cholia, S.; Gunter, D.; Chevrier, V. L.; Persson, K. A.; Ceder, G. Python Materials Genomics (pymatgen): A robust, open-source python library for materials analysis. Comput. Mater. Sci. 2013, 68, 314– 319, DOI: 10.1016/j.commatsci.2012.10.028Google Scholar61https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhsVGjt7g%253D&md5=104f567dbd8f4199911ded91bc42100ePython Materials Genomics (pymatgen): A robust, open-source python library for materials analysisOng, Shyue Ping; Richards, William Davidson; Jain, Anubhav; Hautier, Geoffroy; Kocher, Michael; Cholia, Shreyas; Gunter, Dan; Chevrier, Vincent L.; Persson, Kristin A.; Ceder, GerbrandComputational Materials Science (2013), 68 (), 314-319CODEN: CMMSEM; ISSN:0927-0256. (Elsevier B.V.)We present the Python Materials Genomics (pymatgen) library, a robust, open-source Python library for materials anal. A key enabler in high-throughput computational materials science efforts is a robust set of software tools to perform initial setup for the calcns. (e.g., generation of structures and necessary input files) and post-calcn. anal. to derive useful material properties from raw calcd. data. The pymatgen library aims to meet these needs by (1) defining core Python objects for materials data representation, (2) providing a well-tested set of structure and thermodn. analyses relevant to many applications, and (3) establishing an open platform for researchers to collaboratively develop sophisticated analyses of materials data obtained both from first principles calcns. and expts. The pymatgen library also provides convenient tools to obtain useful materials data via the Materials Project's REpresentational State Transfer (REST) Application Programming Interface (API). As an example, using pymatgen's interface to the Materials Project's RESTful API and phase diagram package, we demonstrate how the phase and electrochem. stability of a recently synthesized material, Li4SnS4, can be analyzed using a min. of computing resources. We find that Li4SnS4 is a stable phase in the Li-Sn-S phase diagram (consistent with the fact that it can be synthesized), but the narrow range of lithium chem. potentials for which it is predicted to be stable would suggest that it is not intrinsically stable against typical electrodes used in lithium-ion batteries.
- 62Pannikkat, A.; Raj, R. Measurement of an electrical potential induced by normal stress applied to the interface of an ionic material at elevated temperatures. Acta Mater. 1999, 47, 3423– 3431, DOI: 10.1016/S1359-6454(99)00206-2Google Scholar62https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK1MXmvVaku78%253D&md5=929fe736a48797d25a19d934c8079ebfMeasurement of an electrical potential induced by normal stress applied to the interface of an ionic material at elevated temperaturesPannikkat, A. K.; Raj, R.Acta Materialia (1999), 47 (12), 3423-3431CODEN: ACMAFD; ISSN:1359-6454. (Elsevier Science Ltd.)The measurement of a p.d. between 2 surfaces of ZrO2 is reported, when a normal stress is applied to one surface, leaving the other surface stress free. The p.d. is proportional to the applied stress over a wide range. The proportionality const. represents a new thermodn. measurement of the interfacial state because the measurement is reversible and independent of temp. In ZrO2, the proportionality const. is related to the vol. and the charge on the O ion by considering thermodn. equil. among the electrochem. potentials of the O ion at the stressed and unstressed interfaces. The agreement with theory is within 10% for specimens made of polycryst. ZrO2, or single crystal cubic ZrO2 of (100) orientation. The proportionality const. changes by up to 20% for other orientations of the single crystal; this change is attributed to differences in the effective charge on the O ion on different surface orientations. The kinetics of the voltage response was also investigated in detail; it is consistent with the diffusion of the O ion along the interface formed between the metal electrode and the ZrO2 surface. The present measurements provide the first exptl. confirmation of the fundamental relationship between the chem. potential, the normal traction, and the at. vol. of species at interfaces of cryst. materials. The measurement has implications in further understanding of diffusional creep, creep cavitation, and sintering in ionic (or partially ionic) solids.
- 63Xie, T.; Grossman, J. C. Crystal Graph Convolutional Neural Networks for an Accurate and Interpretable Prediction of Material Properties. Phys. Rev. Lett. 2018, 120, 145301, DOI: 10.1103/PhysRevLett.120.145301Google Scholar63https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1MXltFSnu7c%253D&md5=93beb5675af86cf95e07c82c136f3511Crystal Graph Convolutional Neural Networks for an Accurate and Interpretable Prediction of Material PropertiesXie, Tian; Grossman, Jeffrey C.Physical Review Letters (2018), 120 (14), 145301CODEN: PRLTAO; ISSN:1079-7114. (American Physical Society)The use of machine learning methods for accelerating the design of cryst. materials usually requires manually constructed feature vectors or complex transformation of atom coordinates to input the crystal structure, which either constrains the model to certain crystal types or makes it difficult to provide chem. insights. Here, we develop a crystal graph convolutional neural networks framework to directly learn material properties from the connection of atoms in the crystal, providing a universal and interpretable representation of cryst. materials. Our method provides a highly accurate prediction of d. functional theory calcd. properties for eight different properties of crystals with various structure types and compns. after being trained with 104 data points. Further, our framework is interpretable because one can ext. the contributions from local chem. environments to global properties. Using an example of perovskites, we show how this information can be utilized to discover empirical rules for materials design.
- 64Jain, A.; Ong, S. P.; Hautier, G.; Chen, W.; Richards, W. D.; Dacek, S.; Cholia, S.; Gunter, D.; Skinner, D.; Ceder, G.; Persson, K. A. The Materials Project: A materials genome approach to accelerating materials innovation. APL Mater. 2013, 1, 011002, DOI: 10.1063/1.4812323Google Scholar64https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtlyktLjF&md5=88cb8642abed05e6b34a2191519b3ff3Commentary: The Materials Project: A materials genome approach to accelerating materials innovationJain, Anubhav; Ong, Shyue Ping; Hautier, Geoffroy; Chen, Wei; Richards, William Davidson; Dacek, Stephen; Cholia, Shreyas; Gunter, Dan; Skinner, David; Ceder, Gerbrand; Persson, Kristin A.APL Materials (2013), 1 (1), 011002/1-011002/11CODEN: AMPADS; ISSN:2166-532X. (American Institute of Physics)Accelerating the discovery of advanced materials is essential for human welfare and sustainable, clean energy. In this paper, we introduce the Materials Project (www.materialsproject.org), a core program of the Materials Genome Initiative that uses high-throughput computing to uncover the properties of all known inorg. materials. This open dataset can be accessed through multiple channels for both interactive exploration and data mining. The Materials Project also seeks to create open-source platforms for developing robust, sophisticated materials analyses. Future efforts will enable users to perform rapid-prototyping'' of new materials in silico, and provide researchers with new avenues for cost-effective, data-driven materials design. (c) 2013 American Institute of Physics.
- 65de Jong, M.; Chen, W.; Angsten, T.; Jain, A.; Notestine, R.; Gamst, A.; Sluiter, M.; Krishna Ande, C.; van der Zwaag, S.; Plata, J. J.; Toher, C.; Curtarolo, S.; Ceder, G.; Persson, K. A.; Asta, M. Charting the complete elastic properties of inorganic crystalline compounds. Sci. Data 2015, 2, 150009, DOI: 10.1038/sdata.2015.9Google Scholar65https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXoslOku74%253D&md5=0479a0c29355429904fd5fe14ca08cd8Charting the complete elastic properties of inorganic crystalline compoundsde Jong, Maarten; Chen, Wei; Angsten, Thomas; Jain, Anubhav; Notestine, Randy; Gamst, Anthony; Sluiter, Marcel; Krishna Ande, Chaitanya; van der Zwaag, Sybrand; Plata, Jose J.; Toher, Cormac; Curtarolo, Stefano; Ceder, Gerbrand; Persson, Kristin A.; Asta, MarkScientific Data (2015), 2 (), 150009CODEN: SDCABS; ISSN:2052-4463. (Nature Publishing Group)The elastic const. tensor of an inorg. compd. provides a complete description of the response of the material to external stresses in the elastic limit. It thus provides fundamental insight into the nature of the bonding in the material, and it is known to correlate with many mech. properties. Despite the importance of the elastic const. tensor, it has been measured for a very small fraction of all known inorg. compds., a situation that limits the ability of materials scientists to develop new materials with targeted mech. responses. To address this deficiency, we present here the largest database of calcd. elastic properties for inorg. compds. to date. The database currently contains full elastic information for 1,181 inorg. compds., and this no. is growing steadily. The methods used to develop the database are described, as are results of tests that establish the accuracy of the data. In addn., we document the database format and describe the different ways it can be accessed and analyzed in efforts related to materials discovery and design.
- 66Perdew, J. P.; Burke, K.; Ernzerhof, M. Generalized gradient approximation made simple. Phys. Rev. Lett. 1996, 77, 3865, DOI: 10.1103/PhysRevLett.77.3865Google Scholar66https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK28XmsVCgsbs%253D&md5=55943538406ee74f93aabdf882cd4630Generalized gradient approximation made simplePerdew, John P.; Burke, Kieron; Ernzerhof, MatthiasPhysical Review Letters (1996), 77 (18), 3865-3868CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)Generalized gradient approxns. (GGA's) for the exchange-correlation energy improve upon the local spin d. (LSD) description of atoms, mols., and solids. We present a simple derivation of a simple GGA, in which all parameters (other than those in LSD) are fundamental consts. Only general features of the detailed construction underlying the Perdew-Wang 1991 (PW91) GGA are invoked. Improvements over PW91 include an accurate description of the linear response of the uniform electron gas, correct behavior under uniform scaling, and a smoother potential.
- 67Paszke, A.; Gross, S.; Chintala, S.; Chanan, G.; Yang, E.; DeVito, Z.; Lin, Z.; Desmaison, A.; Antiga, L.; Lerer, A. Automatic differentiation in PyTorch , NIPS-W, 2017.Google ScholarThere is no corresponding record for this reference.
- 68Tikekar, M. D.; Archer, L. A.; Koch, D. L. Stabilizing electrodeposition in elastic solid electrolytes containing immobilized anions. Sci. Adv. 2016, 2, 1600320, DOI: 10.1126/sciadv.1600320Google Scholar68https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXkslKrtLo%253D&md5=63591374b78e8f147b116ede066d3fa7Stabilizing electrodeposition in elastic solid electrolytes containing immobilized anionsTikekar, Mukul D.; Archer, Lynden A.; Koch, Donald L.Science Advances (2016), 2 (7), e1600320/1-e1600320/15CODEN: SACDAF; ISSN:2375-2548. (American Association for the Advancement of Science)Ion transport - driven instabilities in electrodeposition of metals that lead to morphol. instabilities and dendrites are receiving renewed attention because mitigation strategies are needed for improving recharge-ability and safety of lithium batteries. The growth rate of these morphol. instabilities can be slowed by immobilizing a fraction of anions within the electrolyte to reduce the elec. field at the metal electrode. We analyze the role of elastic deformation of the solid electrolyte with immobilized anions and present theory combining the roles of separator elasticity and modified transport to evaluate the factors affecting the stability of planar deposition over a wide range of current densities. We find that stable electrodeposition can be easily achieved even at relatively high current densities in electrolytes/separators with moderate polymer-like mech. moduli, provided a small fraction of anions are immobilized in the separator.
- 69Seino, Y.; Ota, T.; Takada, K.; Hayashi, A.; Tatsumisago, M. A sulphide lithium super ion conductor is superior to liquid ion conductors for use in rechargeable batteries. Energy Environ. Sci. 2014, 7, 627– 631, DOI: 10.1039/C3EE41655KGoogle Scholar69https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhsFakt7Y%253D&md5=bdd225e1bf4147f70baf646869b2c4f7A sulphide lithium super ion conductor is superior to liquid ion conductors for use in rechargeable batteriesSeino, Yoshikatsu; Ota, Tsuyoshi; Takada, Kazunori; Hayashi, Akitoshi; Tatsumisago, MasahiroEnergy & Environmental Science (2014), 7 (2), 627-631CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)We report that a heat-treated Li2S-P2S5 glass-ceramic conductor has an extremely high ionic cond. of 1.7 × 10-2 S cm-1 and the lowest conduction activation energy of 17 kJ mol-1 at room temp. among lithium-ion conductors reported to date. The optimum conditions of the heat treatment reduce the grain boundary resistance, and the influence of voids, to increase the Li+ ionic cond. of the solid electrolyte so that it is greater than the conductivities of liq. electrolytes, when the transport no. of lithium ions in the inorg. electrolyte is unity.
- 70Li, Y.; Li, Y.; Pei, A.; Yan, K.; Sun, Y.; Wu, C.-L.; Joubert, L.-M.; Chin, R.; Koh, A. L.; Yu, Y.; Perrino, J.; Butz, B.; Chu, S.; Cui, Y. Atomic structure of sensitive battery materials and interfaces revealed by cryo–electron microscopy. Science 2017, 358, 506– 510, DOI: 10.1126/science.aam6014Google Scholar70https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhslSgsb7O&md5=313b19162d2034ecf59cdef499b39565Atomic structure of sensitive battery materials and interfaces revealed by cryo-electron microscopyLi, Yuzhang; Li, Yanbin; Pei, Allen; Yan, Kai; Sun, Yongming; Wu, Chun-Lan; Joubert, Lydia-Marie; Chin, Richard; Koh, Ai Leen; Yu, Yi; Perrino, John; Butz, Benjamin; Chu, Steven; Cui, YiScience (Washington, DC, United States) (2017), 358 (6362), 506-510CODEN: SCIEAS; ISSN:0036-8075. (American Association for the Advancement of Science)Whereas std. transmission electron microscopy studies are unable to preserve the native state of chem. reactive and beam-sensitive battery materials after operation, such materials remain pristine at cryogenic conditions. It is then possible to atomically resolve individual Li metal atoms and their interface with the solid electrolyte interphase (SEI). We observe that dendrites in carbonate-based electrolytes grow along the <111> (preferred), <110>, or <211> directions as faceted, single-cryst. nanowires. These growth directions can change at kinks with no observable crystallog. defect. We reveal distinct SEI nanostructures formed in different electrolytes.
- 71Stroh, A. N. Dislocations and Cracks in Anisotropic Elasticity. Philos. Mag. 1958, 3, 625– 646, DOI: 10.1080/14786435808565804Google Scholar71https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaG1MXitV2ltQ%253D%253D&md5=4195bf838814988673bec6632a6b1dc8Dislocations and cracks in anisotropic elasticityStroh, A. N.Philosophical Magazine (1798-1977) (1958), 3 (), 625-46CODEN: PHMAA4; ISSN:0031-8086.The solution of the elastic equations is considered for the case in which the state of the solid is independent of 1 of the 3 Cartesian co.ovrddot.ordinates. The stresses due to a dislocation, a wall of parallel dislocations, and a crack in an arbitrary nonuniform stress field are obtained. The results hold for the most general anisotropy in which no symmetry elements of the crystal are assumed.
- 72Stroh, A. N. Steady State Problems in Anisotropic Elasticity. J. Math. Phys. 1962, 41, 77– 103, DOI: 10.1002/sapm196241177Google ScholarThere is no corresponding record for this reference.
- 73Hall, S. R.; Allen, F. H.; Brown, I. D. The crystallographic information file (CIF): a new standard archive file for crystallography. Acta Crystallogr., Sect. A: Found. Crystallogr. 1991, 47, 655– 685, DOI: 10.1107/S010876739101067XGoogle ScholarThere is no corresponding record for this reference.
- 74Mouhat, F.; Coudert, F. m. c.-X. Necessary and sufficient elastic stability conditions in various crystal systems. Phys. Rev. B: Condens. Matter Mater. Phys. 2014, 90, 224104, DOI: 10.1103/PhysRevB.90.224104Google Scholar74https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXivVGkur0%253D&md5=d8f5d43f831b6e45962e567bee94a008Necessary and sufficient elastic stability conditions in various crystal systemsMouhat, Felix; Coudert, Francois-XavierPhysical Review B: Condensed Matter and Materials Physics (2014), 90 (22), 224104/1-224104/4, 4 pp.CODEN: PRBMDO; ISSN:1098-0121. (American Physical Society)While the Born elastic stability criteria are well known for cubic crystals, there is some confusion in the literature about the form they should take for lower-symmetry crystal classes. Here we present closed form necessary and sufficient conditions for elastic stability in all crystal classes, as a concise and pedagogical ref. to stability criteria in noncubic materials.
- 75Ahmad, Z.; Viswanathan, V. Quantification of uncertainty in first-principles predicted mechanical properties of solids: Application to solid ion conductors. Phys. Rev. B: Condens. Matter Mater. Phys. 2016, 94, 064105, DOI: 10.1103/PhysRevB.94.064105Google ScholarThere is no corresponding record for this reference.
- 76Friedman, J. H. Greedy Function Approximation: A Gradient Boosting Machine. Ann. Stat. 2001, 29, 1189– 1232, DOI: 10.1214/aos/1013203451Google ScholarThere is no corresponding record for this reference.
- 77Friedman, J. H.; Hastie, T.; Tibshirani, R. The elements of statistical learning; Springer series in statistics: New York, 2001; Vol. 1.Google ScholarThere is no corresponding record for this reference.
- 78Freund, Y.; Schapire, R. E. A Decision-Theoretic Generalization of On-Line Learning and an Application to Boosting. J. Comput. Syst. Sci. 1997, 55, 119– 139, DOI: 10.1006/jcss.1997.1504Google ScholarThere is no corresponding record for this reference.
- 79Drucker, H. Improving Regressors Using Boosting Techniques , Proceedings of the Fourteenth International Conference on Machine Learning, San Francisco, CA, United States, 1997; pp 107– 115.Google ScholarThere is no corresponding record for this reference.
- 80Smola, A. J.; Schülkopf, B. A tutorial on support vector regression. Statistics and Computing 2004, 14, 199– 222, DOI: 10.1023/B:STCO.0000035301.49549.88Google ScholarThere is no corresponding record for this reference.
- 81MacKay, D. J. C. Bayesian Interpolation. Neural Comput. 1992, 4, 415– 447, DOI: 10.1162/neco.1992.4.3.415Google ScholarThere is no corresponding record for this reference.
- 82Pedregosa, F. Scikit-learn: Machine Learning in Python. J. Mach. Learn. Res. 2011, 12, 2825– 2830Google ScholarThere is no corresponding record for this reference.
- 83Deng, Z.; Wang, Z.; Chu, I.-H.; Luo, J.; Ong, S. P. Elastic Properties of Alkali Superionic Conductor Electrolytes from First Principles Calculations. J. Electrochem. Soc. 2016, 163, A67– A74, DOI: 10.1149/2.0061602jesGoogle Scholar83https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhvFylurvI&md5=b8172c27880503a159ab9fe8a1a7c6c3Elastic Properties of Alkali Superionic Conductor Electrolytes from First Principles CalculationsDeng, Zhi; Wang, Zhenbin; Chu, Iek-Heng; Luo, Jian; Ong, Shyue PingJournal of the Electrochemical Society (2016), 163 (2), A67-A74CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)In this work, we present a comprehensive investigation of the elastic properties (the full elastic tensor, bulk, shear and Young's moduli, and Poisson's ratio) of 23 well-known ceramic alkali superionic conductor electrolytes (SICEs) using first principles calcns. We find that the computed elastic moduli are in good agreement with exptl. data (wherever available) and chem. bonding nature. The anion species and structural framework have a significant influence on the elastic properties, and the relative elastic moduli of the various classes of SICEs follow the order thiophosphate < antiperovskite < phosphate < NASICON < garnet < perovskite. Within the same framework structure, we observe that Na SICEs are softer than their Li analogs. We discuss the implications of these findings in the context of fabrication, battery operation, and enabling a Li metal anode. The data computed in this work will also serve as a useful ref. for future expts. as well as theor. modeling of SICEs for rechargeable alkali-ion batteries.
- 84Ranganathan, S. I.; Ostoja-Starzewski, M. Universal Elastic Anisotropy Index. Phys. Rev. Lett. 2008, 101, 055504, DOI: 10.1103/PhysRevLett.101.055504Google Scholar84https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1cXhtVSju7nN&md5=40a1e4eb5d42153f25575b60665ccab9Universal elastic anisotropy indexRanganathan, Shivakumar I.; Ostoja-Starzewski, MartinPhysical Review Letters (2008), 101 (5), 055504/1-055504/4CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)Practically all elastic single crystals are anisotropic, which calls for an appropriate universal measure to quantify the extent of anisotropy. A review of the existing anisotropy measures in the literature leads to a conclusion that they lack universality in the sense that they are nonunique and ignore contributions from the bulk part of the elastic stiffness (or compliance) tensor. Proceeding from extremal principles of elasticity, the authors introduce a new universal anisotropy index that overcomes the above limitations. Also, the authors establish special relations between the proposed anisotropy index and the existing anisotropy measures for special cases. A new elastic anisotropy diagram is constructed for over 100 different crystals (from cubic through triclinic), demonstrating that the proposed anisotropy measure is applicable to all types of elastic single crystals, and thus fills an important void in the existing literature.
- 85Lu, Z.; Ciucci, F. Metal Borohydrides as Electrolytes for Solid-State Li, Na, Mg, and Ca Batteries: A First-Principles Study. Chem. Mater. 2017, 29, 9308– 9319, DOI: 10.1021/acs.chemmater.7b03284Google Scholar85https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhs1Sks77I&md5=4f24aceeeec626b708e8a2546488d8c9Metal Borohydrides as Electrolytes for Solid-State Li, Na, Mg, and Ca Batteries: A First-Principles StudyLu, Ziheng; Ciucci, FrancescoChemistry of Materials (2017), 29 (21), 9308-9319CODEN: CMATEX; ISSN:0897-4756. (American Chemical Society)Metal borohydrides are a family of materials that were recently discovered to have extraordinary ionic conductivities, making them promising candidates as electrolytes for solid-state batteries (SSBs). In fact, various groups have measured the ionic conductivities and assembled batteries using specific borohydrides. However, there are no comprehensive studies assessing the thermodn. properties or discussing the suitability of metal borohydrides as electrolytes in SSBs, esp. for beyond-lithium applications. In this work, we investigate the electrochem. stability, interfacial characteristics, mech. properties, and ionic conductivities of Li, Na, Ca, and Mg borohydrides using first-principles calcns. Our results suggest that Li and Na borohydrides are unstable at high voltages. However, the corresponding decompn. products, i.e., B12H122--contg. phases, have wide electrochem. windows which protect the electrolyte, leading to large electrochem. windows as wide as 5 V. In addn., our simulations indicate that metal borohydrides are ductile, suggesting facile processing. However, their low shear moduli may result in metal dendrite formation. For Ca and Mg borohydrides, while they possess reasonably good electrochem. stability, the low cationic diffusivity may impede their practical use. Finally, the anion rotation barrier was shown to correlate with the superionic phase transition temp., suggesting that anion mixing may be a potential approach to achieve room-temp. superionic cond.
- 86Varley, J. B.; Kweon, K.; Mehta, P.; Shea, P.; Heo, T. W.; Udovic, T. J.; Stavila, V.; Wood, B. C. Understanding Ionic Conductivity Trends in Polyborane Solid Electrolytes from Ab Initio Molecular Dynamics. ACS Energy Lett. 2017, 2, 250– 255, DOI: 10.1021/acsenergylett.6b00620Google Scholar86https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XitFektb3P&md5=10bc784c32c1869968e8c1ae8ab49401Understanding Ionic Conductivity Trends in Polyborane Solid Electrolytes from Ab Initio Molecular DynamicsVarley, Joel B.; Kweon, Kyoung; Mehta, Prateek; Shea, Patrick; Heo, Tae Wook; Udovic, Terrence J.; Stavila, Vitalie; Wood, Brandon C.ACS Energy Letters (2017), 2 (1), 250-255CODEN: AELCCP; ISSN:2380-8195. (American Chemical Society)Polyborane salts based on B12H122-, B10H102-, CB11H12-, and CB9H10- demonstrate high Li and Na superionic cond. that makes them attractive as electrolytes in all-solid-state batteries. Their chem. and structural diversity creates a versatile design space that could be used to optimize materials with higher cond. at lower temps.; however, many mechanistic details remain enigmatic, including reasons why certain known modifications lead to improved performance. We use extensive ab initio mol. dynamics simulations to explore the dependence of ionic cond. on cation/anion pair combinations for Li and Na polyborane salts. Further simulations are used to probe the influence of local modifications to chem., stoichiometry, and compn. Carbon doping, anion alloying, and cation off-stoichiometry are found to favorably introduce intrinsic disorder, facilitating local deviation from the expected cation population. Lattice expansion likewise has a pos. effect by aiding anion reorientations that are crit. for conduction. Implications for engineering polyboranes for improved ionic cond. are discussed.
- 87Tang, W. S.; Matsuo, M.; Wu, H.; Stavila, V.; Zhou, W.; Talin, A. A.; Soloninin, A. V.; Skoryunov, R. V.; Babanova, O. A.; Skripov, A. V.; Unemoto, A.; Orimo, S.; Udovic, T. J. Liquid-Like Ionic Conduction in Solid Lithium and Sodium Monocarba-closo-Decaborates Near or at Room Temperature. Adv. Energy Mater. 2016, 6, 1502237, DOI: 10.1002/aenm.201502237Google ScholarThere is no corresponding record for this reference.
- 88Tang, W. S.; Unemoto, A.; Zhou, W.; Stavila, V.; Matsuo, M.; Wu, H.; Orimo, S.-i.; Udovic, T. J. Unparalleled lithium and sodium superionic conduction in solid electrolytes with large monovalent cage-like anions. Energy Environ. Sci. 2015, 8, 3637– 3645, DOI: 10.1039/C5EE02941DGoogle Scholar88https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhs1amsr%252FL&md5=6ce33938ab3579da7ee531eb41f73964Unparalleled lithium and sodium superionic conduction in solid electrolytes with large monovalent cage-like anionsTang, Wan Si; Unemoto, Atsushi; Zhou, Wei; Stavila, Vitalie; Matsuo, Motoaki; Wu, Hui; Orimo, Shin-ichi; Udovic, Terrence J.Energy & Environmental Science (2015), 8 (12), 3637-3645CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)Solid electrolytes with sufficiently high conductivities and stabilities are the elusive answer to the inherent shortcomings of org. liq. electrolytes prevalent in today's rechargeable batteries. We recently revealed a novel fast-ion-conducting sodium salt, Na2B12H12, which contains large, icosahedral, divalent B12H122- anions that enable impressive superionic cond., albeit only above its 529 K phase transition. Its lithium congener, Li2B12H12, possesses an even more technol. prohibitive transition temp. above 600 K. Here we show that the chem. related LiCB11H12 and NaCB11H12 salts, which contain icosahedral, monovalent CB11H12- anions, both exhibit much lower transition temps. near 400 K and 380 K, resp., and truly stellar ionic conductivities (>0.1 S cm-1) unmatched by any other known polycryst. materials at these temps. With proper modifications, we are confident that room-temp.-stabilized superionic salts incorporating such large polyhedral anion building blocks are attainable, thus enhancing their future prospects as practical electrolyte materials in next-generation, all-solid-state batteries.
- 89Malmgren, S.; Ciosek, K.; Lindblad, R.; Plogmaker, S.; Kühn, J.; Rensmo, H.; Edström, K.; Hahlin, M. Consequences of air exposure on the lithiated graphite SEI. Electrochim. Acta 2013, 105, 83– 91, DOI: 10.1016/j.electacta.2013.04.118Google Scholar89https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtVehsbvE&md5=6475c40a670e813d2a8de45c21003e64Consequences of air exposure on the lithiated graphite SEIMalmgren, Sara; Ciosek, Katarzyna; Lindblad, Rebecka; Plogmaker, Stefan; Kuhn, Julius; Rensmo, Haakan; Edstroem, Kristina; Hahlin, MariaElectrochimica Acta (2013), 105 (), 83-91CODEN: ELCAAV; ISSN:0013-4686. (Elsevier Ltd.)Consequences of air exposure on the surface compn. of one of the most reactive Li-ion battery components, the lithiated graphite, was studied using 280-835 eV soft XPS (SOXPES) as well as 1486.7 eV XPS (∼2 and ∼10 nm probing depth, resp.). Different depth regions of the solid electrolyte interphase (SEI) of graphite cycled vs. LiFePO4 were thereby examd. Also, the air sensitivity of samples subject to four different combinations of pre-treatments (washed/unwashed and exposed to air before or after vacuum treatment) was explored. The samples showed important changes after exposure to air, which are largely dependent on sample pre-treatment. Changes after exposure of unwashed samples exposed before vacuum treatment were attributed to reactions involving volatile species. On washed, air exposed samples, as well as unwashed samples exposed after vacuum treatment, effects attributed to LiOH formation in the innermost SEI were obsd. and suggested to be assocd. with partial delithiation of the surface region of the lithiated graphite electrode. Also, effects that can be attributed to LiPF6 decompn. were obsd. However, these effects were less pronounced than those attributed to reactions involving solvent species and the lithiated graphite.
- 90Tasaki, K.; Goldberg, A.; Lian, J.-J.; Walker, M.; Timmons, A.; Harris, S. Solubility of Lithium Salts Formed on the Lithium-Ion Battery Negative Electrode Surface in Organic Solvents. J. Electrochem. Soc. 2009, 156, A1019– A1027, DOI: 10.1149/1.3239850Google Scholar90https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1MXhtlCmsbzN&md5=433ac8ee99379a475c1e174d35423704Solubility of Lithium Salts Formed on the Lithium-Ion Battery Negative Electrode Surface in Organic SolventsTasaki, Ken; Goldberg, Alex; Lian, Jian-Jie; Walker, Merry; Timmons, Adam; Harris, Stephen J.Journal of the Electrochemical Society (2009), 156 (12), A1019-A1027CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)The soly. of lithium salts in di-Me carbonate (DMC) found in solid electrolyte interface films was detd. The salt-DMC solns. were evapd., and the salts were transferred into water for ion cond. measurements. The salts examd. included Li2CO3, lithium oxalate [(LiCO2)2], LiF, LiOH, lithium Me carbonate (LiOCO2CH3), and lithium Et carbonate (LiOCO2C2H5). The salt molarity in DMC ranged from 9.6 × 10-4 mol/L (LiOCO2CH3) to 9 × 10-5 mol/L (Li2CO3) in the order of LiOCO2CH3 > LiOCO2C2H5 > LiOH > LiF > (LiCO2)2 > Li2CO3. XPS measurements on solid electrolyte interface films on the surface of the anode taken from a com. battery after soaking in DMC for 1 h suggested that the films can dissolve. Sep., the heat of dissoln. of the salts was calcd. from computer simulations for the same salts, including Li2O, lithium methoxide (LiOCH3), and dilithium ethylene glycol dicarbonate [(CH2OCO2Li)2:LiEDC] in both DMC and ethylene carbonate. The results from the computer simulations suggested that the order in which the salt was likely to dissolve in both DMC and ethylene carbonate was LiEDC > LiOCO2CH3 > LiOH > LiOCO2C2H5 > LiOCH3 > LiF > (LiCO2)2 > Li2CO3 > Li2O. This order agreed with the expt. in DMC within the exptl. error. Both expt. and computer simulations showed that the org. salts are more likely to dissolve in DMC than the inorg. salts. The calcns. also predicted that the salts dissolve more likely in ethylene carbonate than in DMC, in general. Moreover, the results from the study were used to discuss the capacity fading mechanism during the storage of lithium-ion batteries.
- 91Matsuo, M.; Nakamori, Y.; ichi Orimo, S.; Maekawa, H.; Takamura, H. Lithium superionic conduction in lithium borohydride accompanied by structural transition. Appl. Phys. Lett. 2007, 91, 224103, DOI: 10.1063/1.2817934Google Scholar91https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2sXhsVequ7zJ&md5=8949f5d9d2da1f61bf6ad230dac90749Lithium superionic conduction in lithium borohydride accompanied by structural transitionMatsuo, Motoaki; Nakamori, Yuko; Orimo, Shin-ichi; Maekawa, Hideki; Takamura, HitoshiApplied Physics Letters (2007), 91 (22), 224103/1-224103/3CODEN: APPLAB; ISSN:0003-6951. (American Institute of Physics)The elec. cond. of LiBH4 measured by a.c. complex impedance increased by 3 orders of magnitude due to structural transition from orthorhombic to hexagonal at ∼390 K. The hexagonal phase exhibited a high elec. cond. of about 10-3 S/cm. The cond. calcd. from the Nernst-Einstein equation using the correlation time obtained from 7Li NMR agreed with the measured elec. cond. The elec. cond. in the hexagonal phase is due to Li superionic conduction.
- 92Johnson, R.; Biefeld, R.; Keck, J. Ionic conductivity in Li5AlO4 and LiOH. Mater. Res. Bull. 1977, 12, 577– 587, DOI: 10.1016/0025-5408(77)90066-6Google Scholar92https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaE2sXkslKqs7k%253D&md5=49b9b53cd2c56638c6e2539226cf0764Ionic conductivity in lithium aluminum oxide (Li5AlO4) and lithium hydroxideJohnson, R. T., Jr.; Biefeld, R. M.; Keck, J. D.Materials Research Bulletin (1977), 12 (6), 577-87CODEN: MRBUAC; ISSN:0025-5408.The ionic cond. and thermal properties of Li5AlO4 and LiOH were measured in wet and dry environments. An endothehrmic reaction at ∼415°C and an assocd. large increase in cond. were obsd. both in Li5AlO4, in wet environment, and in LiOH. The large cond. increase in Li5AlO4 results from LiOH retained within the material. The reaction(s) for formation of LiOH within Li5AlO4 ad the assocd. elec. changes appear to be reversible as the environment switches from wet to dry at high temps. There is a significant (>1%) electronic contribution to the cond. in these materials.
- 93Maekawa, H.; Matsuo, M.; Takamura, H.; Ando, M.; Noda, Y.; Karahashi, T.; Orimo, S.-i. Halide-Stabilized LiBH4, a Room-Temperature Lithium Fast-Ion Conductor. J. Am. Chem. Soc. 2009, 131, 894– 895, DOI: 10.1021/ja807392kGoogle Scholar93https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1MXisValtQ%253D%253D&md5=7602a4b2a0f259ac649e6ce4dfe8e53bHalide-Stabilized LiBH4, a Room-Temperature Lithium Fast-Ion ConductorMaekawa, Hideki; Matsuo, Motoaki; Takamura, Hitoshi; Ando, Mariko; Noda, Yasuto; Karahashi, Taiki; Orimo, Shin-ichiJournal of the American Chemical Society (2009), 131 (3), 894-895CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)A review on development of lithium superionic conductors based on LiBH4 and lithium halides. Using these compds., room-temp. high lithium ion cond. was imparted to a hydride system that had not been considered a lithium ion electrolyte. The electrochem. measurements showed a great advantage of this material as an extremely lightwt. lithium electrolyte for high energy d. batteries. Versatile properties of these materials make them suitable for use in all-solid-state batteries.
- 94Das, S.; Ngene, P.; Norby, P.; Vegge, T.; de Jongh, P. E.; Blanchard, D. All-Solid-State Lithium-Sulfur Battery Based on a Nanoconfined LiBH4 Electrolyte. J. Electrochem. Soc. 2016, 163, A2029– A2034, DOI: 10.1149/2.0771609jesGoogle Scholar94https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28Xht1Krsr%252FP&md5=ee1106f5cdf799cd3505e1078501696fAll-Solid-State Lithium-Sulfur Battery Based on a Nanoconfined LiBH4 ElectrolyteDas, Supti; Ngene, Peter; Norby, Poul; Vegge, Tejs; de Jongh, Petra E.; Blanchard, DidierJournal of the Electrochemical Society (2016), 163 (9), A2029-A2034CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)In this work we characterize all-solid-state lithium-sulfur batteries based on nano-confined LiBH4 in mesoporous silica as solid electrolytes. The nano-confined LiBH4 has fast ionic lithium cond. at room temp., 0.1 mScm-1, negligible electronic cond. and its cationic transport no. (t+ = 0.96), close to unity, demonstrates a purely cationic conductor. The electrolyte has an excellent stability against lithium metal. The behavior of the batteries is studied by cyclic voltammetry and repeated charge/discharge cycles in galvanostatic conditions. The batteries show good performance, delivering high capacities vs. sulfur mass, typically 1220 mAhg-1 after 40 cycles at moderate temp. (55°), 0.03 C rates and working voltage of 2 V.
- 95Morales-García, A.; Valero, R.; Illas, F. An Empirical, yet Practical Way To Predict the Band Gap in Solids by Using Density Functional Band Structure Calculations. J. Phys. Chem. C 2017, 121, 18862– 18866, DOI: 10.1021/acs.jpcc.7b07421Google Scholar95https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXht12mtLnE&md5=b0a676344af3832e6ff75461b9232229An empirical, yet practical way to predict the band gap in solids by using density functional band structure calculationsMorales-Garcia, Angel; Valero, Rosendo; Illas, FrancescJournal of Physical Chemistry C (2017), 121 (34), 18862-18866CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)Band structure calcns. based on d. functional theory (DFT) with local or gradient-cor. exchange-correlation potentials are known to severely underestimate the band gap of semiconducting and insulating materials. Alternative approaches have been proposed: from semiempirical setups, such as the so-called DFT+U, to hybrid d. functionals using a fraction of nonlocal Fock exchange, to modifications of semilocal d. functionals. However, the resulting methods appear to be material dependent and lack theor. rigor. The rigorous many-body perturbation theory based on GW methods provides accurate results but at a very high computational cost. Hereby, we show that a linear correlation between the electronic band gaps obtained from std. DFT and GW approaches exists for most materials and argue that (1) this is a strong indication that the problem of predicting band gaps from std. DFT calcn. arises from the assignment of a phys. meaning to the Kohn-Sham energy levels rather than from intrinsic errors of the DFT methods and (2) it provides a practical way to obtain GW-like quality results from std. DFT calcns. The latter will be esp. useful for systems where the unit cell involves a large no. of atoms as in the case of doped or defect-contg. materials for which GW calcns. become unfeasible.
- 96Towns, J.; Cockerill, T.; Dahan, M.; Foster, I.; Gaither, K.; Grimshaw, A.; Hazlewood, V.; Lathrop, S.; Lifka, D.; Peterson, G. D.; Roskies, R.; Scott, J. R.; Wilkins-Diehr, N. XSEDE: Accelerating Scientific Discovery. Comput. Sci. Eng. 2014, 16, 62– 74, DOI: 10.1109/MCSE.2014.80Google ScholarThere is no corresponding record for this reference.
- 97Nystrom, N. A.; Levine, M. J.; Roskies, R. Z.; Scott, J. R. Bridges: A Uniquely Flexible HPC Resource for New Communities and Data Analytics. Proceedings of the 2015 XSEDE Conference: Scientific Achievements Enabled by Enhanced Cyberinfrastructure 2015, 1– 8, DOI: 10.1145/2792745.2792775Google ScholarThere is no corresponding record for this reference.
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Abstract
Figure 1
Figure 1. Parity plots comparing the elastic properties: (a) shear modulus G, and elastic constants (b) C11, (c) C12, and (d) C44 predicted by the machine-learning models to the DFT-calculated values. The shear modulus is predicted using CGCNN, and the elastic constants C11 and C44 are predicted using gradient boosting regression while C12 is predicted using kernel ridge regression. The parity plot for shear modulus is on 680 test data points while that for the elastic constants contains all available data (170 points) where each prediction is a cross-validated value.
Figure 2
Figure 2. Contribution of hydrostatic stress, deviatoric stress, and surface tension to the stability parameter as a function of surface roughness wavenumber. The surface tension term starts dominating at high k and ultimately stabilizes the interface after k = kcrit. The contributions are plotted for a material with shear modulus ratio G/GLi = 1 and Poisson’s ratio ν = 0.33 which is not stable (χ > 0) at k = 108 m–1. The red line shows the fraction of surface tension contribution to the stability parameter obtained by dividing the absolute value of its contribution by the sum of absolute values of all components.
Figure 3
Figure 3. Results of isotropic screening for 12 950 Li-containing compounds. Distribution of ensemble averaged (a) stability parameter for isotropic Li–solid electrolyte interfaces at k = 108 m–1 and (b) critical wavelength of surface roughness required for stability. None of the materials in the database can be stabilized without the aid of surface tension. The required critical surface roughness wavenumber depends on the contribution of the stress term in the stability parameter.
Figure 4
Figure 4. Isotropic stability diagram showing the position of all solid electrolytes involved in the screening. GLi is the shear modulus of Li = 3.4 GPa. The critical G/GLi line separating the stable and unstable regions depends weakly on the Poisson’s ratio, so the lines corresponding to νs = 0.33 and 0.5 are good indicators for assessment of stability. The darker regions indicate more number of materials in the region.
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- 6Christensen, J.; Albertus, P.; Sanchez-Carrera, R. S.; Lohmann, T.; Kozinsky, B.; Liedtke, R.; Ahmed, J.; Kojic, A. A Critical Review of Li/Air Batteries. J. Electrochem. Soc. 2011, 159, R1– R30, DOI: 10.1149/2.086202jesThere is no corresponding record for this reference.
- 7Xu, W.; Wang, J.; Ding, F.; Chen, X.; Nasybulin, E.; Zhang, Y.; Zhang, J.-G. Lithium metal anodes for rechargeable batteries. Energy Environ. Sci. 2014, 7, 513– 537, DOI: 10.1039/C3EE40795K7https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhsFaktL8%253D&md5=3813f919eb7ca4218cfb562f54c9382aLithium metal anodes for rechargeable batteriesXu, Wu; Wang, Jiulin; Ding, Fei; Chen, Xilin; Nasybulin, Eduard; Zhang, Yaohui; Zhang, Ji-GuangEnergy & Environmental Science (2014), 7 (2), 513-537CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)A review. Lithium (Li) metal is an ideal anode material for rechargeable batteries due to its extremely high theor. specific capacity (3860 mA h g-1), low d. (0.59 g cm-3) and the lowest neg. electrochem. potential (-3.040 V vs. the std. hydrogen electrode). Unfortunately, uncontrollable dendritic Li growth and limited Coulombic efficiency during Li deposition/stripping inherent in these batteries have prevented their practical applications over the past 40 years. With the emergence of post-Li-ion batteries, safe and efficient operation of Li metal anodes has become an enabling technol. which may det. the fate of several promising candidates for the next generation energy storage systems, including rechargeable Li-air batteries, Li-S batteries, and Li metal batteries which utilize intercalation compds. as cathodes. In this paper, various factors that affect the morphol. and Coulombic efficiency of Li metal anodes have been analyzed. Technologies utilized to characterize the morphol. of Li deposition and the results obtained by modeling of Li dendrite growth have also been reviewed. Finally, recent development and urgent need in this field are discussed.
- 8Tikekar, M. D.; Choudhury, S.; Tu, Z.; Archer, L. A. Design principles for electrolytes and interfaces for stable lithium-metal batteries. Nat. Energy 2016, 1, 16114, DOI: 10.1038/nenergy.2016.1148https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVersL8%253D&md5=3627028eaacfbf47fd2a8691cfddcef1Design principles for electrolytes and interfaces for stable lithium-metal batteriesTikekar, Mukul D.; Choudhury, Snehashis; Tu, Zhengyuan; Archer, Lynden A.Nature Energy (2016), 1 (9), 16114CODEN: NEANFD; ISSN:2058-7546. (Nature Publishing Group)A review. The future of electrochem. energy storage hinges on the advancement of science and technol. that enables rechargeable batteries that utilize reactive metals as anodes. With specific capacity more than ten times that of the LiC6 anode used in present-day lithium-ion batteries, cells based on Li-metal anodes are of particular interest. Effective strategies for stabilizing the anode in such cells are now understood to be a requirement for progress on exceptional storage technologies, including Li-S and Li-O2 batteries. Multiple challenges-parasitic reactions of Li-metal with liq. electrolytes, unstable and dendritic electrodeposition, and dendrite-induced short circuits-derailed early efforts to commercialize such lithium-metal batteries. Here we consider approaches for rationally designing electrolytes and Li-metal/electrolyte interfaces for stable, dendrite-free operation of lithium-metal batteries. On the basis of fundamental understanding of the failure modes of reactive metal anodes, we discuss the key variables that govern the stability of electrodeposition at the Li anode and propose a universal framework for designing stable electrolytes and interfaces for lithium-metal batteries.
- 9Aurbach, D.; Zinigrad, E.; Teller, H.; Dan, P. Factors Which Limit the Cycle Life of Rechargeable Lithium (Metal) Batteries. J. Electrochem. Soc. 2000, 147, 1274– 1279, DOI: 10.1149/1.13933499https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD3cXisVygtLo%253D&md5=9c7dc9d384db266edbddf0a3ae3d6f0cFactors which limit the cycle life of rechargeable lithium (metal) batteriesAurbach, D.; Zinigrad, E.; Teller, H.; Dan, P.Journal of the Electrochemical Society (2000), 147 (4), 1274-1279CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Failure mechanisms due to high charging rates of rechargeable lithium batteries comprised of Li anodes, Li0.3MnO2 cathodes (tunneled structure), and electrolyte solns. based on the combination of 1,3-dioxolane, LiAsF6, and tributylamine (antipolymn. stabilizer) were explored with the aid of postmortem anal. It was found that at high charging rates, lithium deposition produces small grains, which are too reactive toward the electrolyte soln., in spite of the excellent passivation of lithium in this soln. In practical batteries such as AA cells with spirally wound configurations, the amt. of soln. is relatively small, and the soln. is spread throughout the battery in a thin layer. Therefore, upon cycling, the Li-soln. reactions deplete the amt. of the soln. below a crit. value, so that only part of the active materials continues to function. This leads to a pronounced increase in the internal resistance of these batteries, which fail as a result of their high impedance and the decrease in the effective working electrodes area. Another failure mechanism relates to the extremely high charge-discharge current densities developed as the active electrode area decreases. These high currents, developed after prolonged cycling, lead to the formation of dendrites that short-circuit the battery, thus terminating its life.
- 10Aurbach, D.; Zinigrad, E.; Cohen, Y.; Teller, H. A short review of failure mechanisms of lithium metal and lithiated graphite anodes in liquid electrolyte solutions. Solid State Ionics 2002, 148, 405– 416, DOI: 10.1016/S0167-2738(02)00080-210https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD38XktVWgurY%253D&md5=24417ffbcd25ad6ffaba30ab7d00e3d4A short review of failure mechanisms of lithium metal and lithiated graphite anodes in liquid electrolyte solutionsAurbach, Doron; Zinigrad, Ella; Cohen, Yaron; Teller, HananSolid State Ionics (2002), 148 (3,4), 405-416CODEN: SSIOD3; ISSN:0167-2738. (Elsevier Science B.V.)A review. Li electrodes in any relevant electrolyte soln. (i.e., polar aprotic) are covered by surface films of a very complicated structure. It was found that even in cases where the surface films formed on lithium contain elastomers, or where the lithium metal reactivity is reduced by doping with elements such as N, As, Al, Mg, Ca, etc., it is impossible to achieve sufficient passivation with lithium electrodes and liq. solns. Passivation is considerably worsened when Li electrodes are operated at high rates (esp. at high charging, Li deposition rates). Thus, there is no way that rechargeable Li batteries can compete with Li-ion batteries in any application that requires high charging rates (e.g., in powering portable electronic devices). The electrochem. behavior of lithiated graphite electrodes also depends on passivation phenomena. The surface films formed on lithiated graphite are similar to those formed on Li metal in the same solns. The vol. changes of graphite electrodes during Li insertion-deinsertion are small enough to enable their reasonable passivation in a variety of electrolyte solns. A crit. factor that dets. the stability of graphite electrodes is their morphol. It was found that the shape of graphite particles plays a key role in their application as active mass in anodes for Li-ion batteries.
- 11Steiger, J.; Kramer, D.; Mönig, R. Mechanisms of dendritic growth investigated by in situ light microscopy during electrodeposition and dissolution of lithium. J. Power Sources 2014, 261, 112– 119, DOI: 10.1016/j.jpowsour.2014.03.02911https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXnsl2murc%253D&md5=2db8d2782ea70c21bf11b86d6c3618fdMechanisms of dendritic growth investigated by in situ light microscopy during electrodeposition and dissolution of lithiumSteiger, Jens; Kramer, Dominik; Moenig, ReinerJournal of Power Sources (2014), 261 (), 112-119CODEN: JPSODZ; ISSN:0378-7753. (Elsevier B.V.)Batteries with metallic lithium anodes offer improved volumetric and gravimetric energy densities; therefore, future batteries including the promising lithium-sulfur and lithium-air systems would benefit from them. The electrodeposition of lithium metal - which is an unwanted incident in lithium ion systems - often results in fine filaments or moss, called dendritic lithium, which leads to strong capacity fading and the danger of internal short circuiting. To study the mechanisms of dendritic growth and the behavior during lithium dissoln., lithium deposits have been obsd. in situ in 1 M LiPF6 in EC:DMC by light microscopy. The high resoln. optical microscopy provided information on the growth and electrodissoln. of single lithium filaments. The growth areas could be identified in detail: The lithium wires can grow either from the substrate-lithium interface, at kinks or in a region at or close to the tip. Based on these observations, we suggest a growth model for lithium filaments predicated on defect-based insertion of lithium at the aforementioned locations. This type of growth is not compatible with previous models of dendritic growth, for example, it is hardly influenced by elec. fields at the tip and does not depend on the direction of the elec. field.
- 12Albertus, P.; Babinec, S.; Litzelman, S.; Newman, A. Status and challenges in enabling the lithium metal electrode for high-energy and low-cost rechargeable batteries. Nat. Energy 2018, 3, 16– 21, DOI: 10.1038/s41560-017-0047-212https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXitVehurY%253D&md5=569e6865fb3a225323353f9e9f39fddbStatus and challenges in enabling the lithium metal electrode for high-energy and low-cost rechargeable batteriesAlbertus, Paul; Babinec, Susan; Litzelman, Scott; Newman, AronNature Energy (2018), 3 (1), 16-21CODEN: NEANFD; ISSN:2058-7546. (Nature Research)Enabling the reversible lithium metal electrode is essential for surpassing the energy content of today's lithium-ion cells. Although lithium metal cells for niche applications have been developed already, efforts are underway to create rechargeable lithium metal batteries that can significantly advance vehicle electrification and grid energy storage. In this Perspective, we focus on three tasks to guide and further advance the reversible lithium metal electrode. First, we summarize the state of research and com. efforts in terms of four key performance parameters, and identify addnl. performance parameters of interest. We then advocate for the use of limited lithium (≤30 μm) to ensure early identification of tech. challenges assocd. with stable and dendrite-free cycling and a more rapid transition to com. relevant designs. Finally, we provide a cost target and outline material costs and manufg. methods that could allow lithium metal cells to reach 100 US$ kWh-1.
- 13Aurbach, D.; Markovsky, B.; Shechter, A.; Ein-Eli, Y.; Cohen, H. A Comparative Study of Synthetic Graphite and Li Electrodes in Electrolyte Solutions Based on Ethylene Carbonate-Dimethyl Carbonate Mixtures. J. Electrochem. Soc. 1996, 143, 3809– 3820, DOI: 10.1149/1.183730013https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK2sXhsFehsg%253D%253D&md5=02e52a156683cedd7ca6901f81eb7313A comparative study of synthetic graphite and Li electrodes in electrolyte solutions based on ethylene carbonate-dimethyl carbonate mixturesAurbach, D.; Markovsky, B.; Shechter, A.; Ein-Eli, Y.; Cohen, H.Journal of the Electrochemical Society (1996), 143 (12), 3809-3820CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)This work entails a comparative study of both Li and synthetic graphite electrodes in electrolyte solns. based on ethylene and di-Me carbonates (EC-DMC) and the impact of the salt used [LiAsF6, LiClO4, LiPF6, LiBF4, and LiN(SO2CF3)2]. The presence of some additives in solns. (e.g., Li2CO3, CO2, tributylamine) and the effect of the particle size of the carbon on the behavior of the electrode were studied. The correlation between the surface chem., the morphol., and the performance of Li and graphite electrodes was explored using surface sensitive FTIR and x-ray and photoelectron spectroscopies, impedance spectroscopy, x-ray diffraction and SEM in conjunction with std. electrochem. techniques. Synthetic graphite anodes could be cycled (Li intercalation-deintercalation) hundreds of times at a capacity close to the optimal (x → 1 in LixC6) in EC-DMC solns. due to the formation of highly stable and passivating surface films in which EC redn. products such as (CH2OCO2Li)2 are the major constituents. The cycling efficiency of Li metal anodes in these solns., however, is lower than that obtained in ethereal solns. and seems to be too low for Li-metal liq. electrolyte, rechargeable battery application. The connection between the soln. compn. and the electrode's performance is discussed.
- 14Hirai, T.; Yoshimatsu, I.; Yamaki, J. Effect of Additives on Lithium Cycling Efficiency. J. Electrochem. Soc. 1994, 141, 2300– 2305, DOI: 10.1149/1.205511614https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK2cXmtlCls7o%253D&md5=9125cb1237f464f238f6507a83b742acEffect of additives on lithium cycling efficiencyHirai, Toshiro; Yoshimatsu, Isamu; Yamaki, Jun-ichiJournal of the Electrochemical Society (1994), 141 (9), 2300-5CODEN: JESOAN; ISSN:0013-4651.Li cycling efficiency was evaluated for LiAsF6-ethylene carbonate/2-methyltetrahydrofuran mixed-solvent electrolyte (LiAsF6-EC/2MeTHF) contg. additives of tetraalkylammonium chlorides with a long n-alkyl chain and three Me groups. The tetraalkylammonium chloride with n-alkyl group longer than n-C12H25 increased Li cycling efficiency. Cetyltrimethylammonium chloride (CTAC) produced the best improvement in Li cycling efficiency. A figure of merit (FOM) of Li for 0.01M CTAC was 46, which was 1.5 times the FOM for the corresponding additive-free electrolyte. The LiAsF6-EC/2MeTHF with CTAC showed an increase in FOM with stack pressure, but the effect was less than that for the additive-free LiAsF6-EC/2MeTHF. SEM observation showed that the addn. of CTAC decreased the needle-like Li deposition and increased particulate Li deposition. This deposition morphol. may be the main cause of the increase in FOM. The additive had no effect on rate capability for cell cycling at 3 mA/cm2 discharge and 1 mA/cm2 charge.
- 15Ding, F.; Xu, W.; Graff, G. L.; Zhang, J.; Sushko, M. L.; Chen, X.; Shao, Y.; Engelhard, M. H.; Nie, Z.; Xiao, J.; Liu, X.; Sushko, P. V.; Liu, J.; Zhang, J.-G. Dendrite-Free Lithium Deposition via Self-Healing Electrostatic Shield Mechanism. J. Am. Chem. Soc. 2013, 135, 4450– 4456, DOI: 10.1021/ja312241y15https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXjtlWgsLs%253D&md5=be89c1fc31e4b3293c7f0fb4e6b55407Dendrite-Free Lithium Deposition via Self-Healing Electrostatic Shield MechanismDing, Fei; Xu, Wu; Graff, Gordon L.; Zhang, Jian; Sushko, Maria L.; Chen, Xilin; Shao, Yuyan; Engelhard, Mark H.; Nie, Zimin; Xiao, Jie; Liu, Xingjiang; Sushko, Peter V.; Liu, Jun; Zhang, Ji-GuangJournal of the American Chemical Society (2013), 135 (11), 4450-4456CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Rechargeable Li metal batteries are of great importance. Unfortunately, uncontrollable dendritic Li growth inherent in these batteries (upon repeated charge/discharge cycling) has prevented their practical application over the past 40 years. The authors show a novel mechanism that can fundamentally alter dendrite formation. At low concns., selected cations (such as Cs or Rb ions) exhibit an effective redn. potential below the std. redn. potential of Li ions. During Li deposition, these additive cations form a pos. charged electrostatic shield around the initial growth tip of the protuberances without redn. and deposition of the additives. This forces further deposition of Li to adjacent regions of the anode and eliminates dendrite formation in Li metal batteries. This strategy may also prevent dendrite growth in Li-ion batteries as well as other metal batteries and transform the surface uniformity of coatings deposited in many general electrodeposition processes.
- 16Qian, J.; Henderson, W. A.; Xu, W.; Bhattacharya, P.; Engelhard, M.; Borodin, O.; Zhang, J.-G. High rate and stable cycling of lithium metal anode. Nat. Commun. 2015, 6, 6362, DOI: 10.1038/ncomms736216https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtF2itrrI&md5=9bde3388626c7f3d31618a2d934a90cfHigh rate and stable cycling of lithium metal anodeQian, Jiangfeng; Henderson, Wesley A.; Xu, Wu; Bhattacharya, Priyanka; Engelhard, Mark; Borodin, Oleg; Zhang, Ji-GuangNature Communications (2015), 6 (), 6362CODEN: NCAOBW; ISSN:2041-1723. (Nature Publishing Group)Lithium metal is an ideal battery anode. However, dendrite growth and limited Coulombic efficiency during cycling have prevented its practical application in rechargeable batteries. Herein, we report that the use of highly concd. electrolytes composed of ether solvents and the lithium bis(fluorosulfonyl)imide salt enables the high-rate cycling of a lithium metal anode at high Coulombic efficiency (up to 99.1%) without dendrite growth. With 4 M lithium bis(fluorosulfonyl)imide in 1,2-dimethoxyethane as the electrolyte, a lithium|lithium cell can be cycled at 10 mA cm-2 for more than 6,000 cycles, and a copper|lithium cell can be cycled at 4 mA cm-2 for more than 1,000 cycles with an av. Coulombic efficiency of 98.4%. These excellent performances can be attributed to the increased solvent coordination and increased availability of lithium ion concn. in the electrolyte. Further development of this electrolyte may enable practical applications for lithium metal anode in rechargeable batteries.
- 17Suo, L.; Hu, Y.-S.; Li, H.; Armand, M.; Chen, L. A new class of Solvent-in-Salt electrolyte for high-energy rechargeable metallic lithium batteries. Nat. Commun. 2013, 4, 1481, DOI: 10.1038/ncomms251317https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC3sznslKgtA%253D%253D&md5=cb719ace996906c08eadedf61644e3dcA new class of Solvent-in-Salt electrolyte for high-energy rechargeable metallic lithium batteriesSuo Liumin; Hu Yong-Sheng; Li Hong; Armand Michel; Chen LiquanNature communications (2013), 4 (), 1481 ISSN:.Liquid electrolyte plays a key role in commercial lithium-ion batteries to allow conduction of lithium-ion between cathode and anode. Traditionally, taking into account the ionic conductivity, viscosity and dissolubility of lithium salt, the salt concentration in liquid electrolytes is typically less than 1.2 mol l(-1). Here we show a new class of 'Solvent-in-Salt' electrolyte with ultrahigh salt concentration and high lithium-ion transference number (0.73), in which salt holds a dominant position in the lithium-ion transport system. It remarkably enhances cyclic and safety performance of next-generation high-energy rechargeable lithium batteries via an effective suppression of lithium dendrite growth and shape change in the metallic lithium anode. Moreover, when used in lithium-sulphur battery, the advantage of this electrolyte is further demonstrated that lithium polysulphide dissolution is inhibited, thus overcoming one of today's most challenging technological hurdles, the 'polysulphide shuttle phenomenon'. Consequently, a coulombic efficiency nearing 100% and long cycling stability are achieved.
- 18Lu, Y.; Tu, Z.; Archer, L. A. Stable lithium electrodeposition in liquid and nanoporous solid electrolytes. Nat. Mater. 2014, 13, 961, DOI: 10.1038/nmat404118https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhtlahu77J&md5=72567640c740e4e4b584b1e838d4d9d8Stable lithium electrodeposition in liquid and nanoporous solid electrolytesLu, Yingying; Tu, Zhengyuan; Archer, Lynden A.Nature Materials (2014), 13 (10), 961-969CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Rechargeable lithium, sodium and aluminum metal-based batteries are among the most versatile platforms for high-energy, cost-effective electrochem. energy storage. Non-uniform metal deposition and dendrite formation on the neg. electrode during repeated cycles of charge and discharge are major hurdles to commercialization of energy-storage devices based on each of these chemistries. A long-held view is that unstable electrodeposition is a consequence of inherent characteristics of these metals and their inability to form uniform electrodeposits on surfaces with inevitable defects. We report on electrodeposition of lithium in simple liq. electrolytes and in nanoporous solids infused with liq. electrolytes. We find that simple liq. electrolytes reinforced with halogenated salt blends exhibit stable long-term cycling at room temp., often with no signs of deposition instabilities over hundreds of cycles of charge and discharge and thousands of operating hours. We rationalize these observations with the help of surface energy data for the electrolyte/lithium interface and impedance anal. of the interface during different stages of cell operation. Our findings provide support for an important recent theor. prediction that the surface mobility of lithium is significantly enhanced in the presence of lithium halide salts. Our results also show that a high electrolyte modulus is unnecessary for stable electrodeposition of lithium.
- 19Zhang, X.; Cheng, X.; Chen, X.; Yan, C.; Zhang, Q. Fluoroethylene Carbonate Additives to Render Uniform Li Deposits in Lithium Metal Batteries. Adv. Funct. Mater. 2017, 27, 1605989, DOI: 10.1002/adfm.201605989There is no corresponding record for this reference.
- 20Wang, D.; Zhang, W.; Zheng, W.; Cui, X.; Rojo, T.; Zhang, Q. Towards High-Safe Lithium Metal Anodes: Suppressing Lithium Dendrites via Tuning Surface Energy. Adv. Sci. 2017, 4, 1600168, DOI: 10.1002/advs.20160016820https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC1c7nsFektg%253D%253D&md5=97708cfbe6ea7cd34edab1a667521da1Towards High-Safe Lithium Metal Anodes: Suppressing Lithium Dendrites via Tuning Surface EnergyWang Dong; Zheng Weitao; Cui Xiaoqiang; Zhang Wei; Rojo Teofilo; Zhang QiangAdvanced science (Weinheim, Baden-Wurttemberg, Germany) (2017), 4 (1), 1600168 ISSN:2198-3844.The formation of lithium dendrites induces the notorious safety issue and poor cycling life of energy storage devices, such as lithium-sulfur and lithium-air batteries. We propose a surface energy model to describe the complex interface between the lithium anode and electrolyte. A universal strategy of hindering formation of lithium dendrites via tuning surface energy of the relevant thin film growth is suggested. The merit of the novel motif lies not only fundamentally a perfect correlation between electrochemistry and thin film fields, but also significantly promotes larger-scale application of lithium-sulfur and lithium-air batteries, as well as other metal batteries (e.g., Zn, Na, K, Cu, Ag, and Sn).
- 21Zhang, Y.; Qian, J.; Xu, W.; Russell, S. M.; Chen, X.; Nasybulin, E.; Bhattacharya, P.; Engelhard, M. H.; Mei, D.; Cao, R.; Ding, F.; Cresce, A. V.; Xu, K.; Zhang, J.-G. Dendrite-Free Lithium Deposition with Self-Aligned Nanorod Structure. Nano Lett. 2014, 14, 6889– 6896, DOI: 10.1021/nl503911721https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhvFOjs7zN&md5=568690f8c450f7a6ff90166875481674Dendrite-Free Lithium Deposition with Self-Aligned Nanorod StructureZhang, Yaohui; Qian, Jiangfeng; Xu, Wu; Russell, Selena M.; Chen, Xilin; Nasybulin, Eduard; Bhattacharya, Priyanka; Engelhard, Mark H.; Mei, Donghai; Cao, Ruiguo; Ding, Fei; Cresce, Arthur V.; Xu, Kang; Zhang, Ji-GuangNano Letters (2014), 14 (12), 6889-6896CODEN: NALEFD; ISSN:1530-6984. (American Chemical Society)Suppressing Li dendrite growth is one of the most crit. challenges for the development of Li metal batteries. Here, the authors report for the 1st time the growth of dendrite-free Li films with a self-aligned and highly compacted nanorod structure when the film was deposited in the electrolyte consisting of 1.0M LiPF6 in propylene carbonate with 0.05M CsPF6 as an additive. Evolution of both the surface and the cross-sectional morphologies of the Li films during repeated Li deposition/stripping processes were studied. The formation of the compact Li nanorod structure is preceded by a solid electrolyte interphase (SEI) layer formed on the surface of the substrate. Electrochem. anal. indicates that an initial redn. process occurred at ∼2.05 V vs. Li/Li+ before Li deposition is responsible for the formation of the initial SEI, while the XPS indicates that the presence of CsPF6 additive can largely enhance the formation of LiF in this initial SEI. Hence, the smooth Li deposition in Cs+-contg. electrolyte is the result of a synergistic effect of Cs+ additive and preformed SEI layer. A fundamental understanding on the compn., internal structure, and evolution of Li metal films may lead to new approaches to stabilize the long-term cycling stability of Li metal and other metal anodes for energy storage applications.
- 22Mayers, M. Z.; Kaminski, J. W.; Miller, T. F. Suppression of Dendrite Formation via Pulse Charging in Rechargeable Lithium Metal Batteries. J. Phys. Chem. C 2012, 116, 26214– 26221, DOI: 10.1021/jp309321w22https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC38Xhs12mtrzE&md5=e17f74971b90114acb68bb36063c52ceSuppression of Dendrite Formation via Pulse Charging in Rechargeable Lithium Metal BatteriesMayers, Matthew Z.; Kaminski, Jakub W.; Miller, Thomas F.Journal of Physical Chemistry C (2012), 116 (50), 26214-26221CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)We introduce a coarse-grained simulation model for the reductive deposition of lithium cations in secondary lithium batteries. The model accounts for the heterogeneous and nonequil. nature of the electrodeposition dynamics, and it enables simulation of the long timescales and lengthscales assocd. with metal dendrite formation. We investigate the effects of applied overpotential and material properties on early-stage dendrite formation, as well as the mol. mechanisms that govern this process. The model confirms that dendrite formation propensity increases with the applied electrode overpotential, and it demonstrates that application of the electrode overpotential in time-dependent pulses leads to dramatic suppression of dendrite formation while reducing the accumulated electrode on-time by as much as 96%. Moreover, the model predicts that time dependence of the applied electrode overpotential can lead to pos., neg., or zero correlation between cation diffusivity in the solid-electrolyte interphase (SEI) and dendrite formation propensity. Anal. of the simulation trajectories reveals that dendrite formation emerges from a competition between the timescales for cation diffusion and redn. at the anode/SEI interface, with lower applied overpotentials and shorter electrode pulse durations shifting this competition in favor of lower dendrite formation propensity. This work provides a mol. basis for understanding and designing pulsing waveforms that mitigate dendrite formation while minimally affecting battery charging times.
- 23Aryanfar, A.; Brooks, D.; Merinov, B. V.; Goddard, W. A.; Colussi, A. J.; Hoffmann, M. R. Dynamics of Lithium Dendrite Growth and Inhibition: Pulse Charging Experiments and Monte Carlo Calculations. J. Phys. Chem. Lett. 2014, 5, 1721– 1726, DOI: 10.1021/jz500207a23https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXntFOmurw%253D&md5=a49ca2f7ec9d6e627017e04994a96429Dynamics of Lithium Dendrite Growth and Inhibition: Pulse Charging Experiments and Monte Carlo CalculationsAryanfar, Asghar; Brooks, Daniel; Merinov, Boris V.; Goddard, William A.; Colussi, Agustin J.; Hoffmann, Michael R.Journal of Physical Chemistry Letters (2014), 5 (10), 1721-1726CODEN: JPCLCD; ISSN:1948-7185. (American Chemical Society)Short-circuiting via dendrites compromises the reliability of Li-metal batteries. Dendrites ensue from instabilities inherent to electrodeposition that should be amenable to dynamic control. Here, the authors report that by charging a scaled coin-cell prototype with 1 ms pulses followed by 3 ms rest periods the av. dendrite length is shortened ∼2.5 times relative to those grown under continuous charging. Monte Carlo simulations dealing with Li+ diffusion and electromigration reveal that expts. involving 20 ms pulses were ineffective because Li+ migration in the strong elec. fields converging to dendrite tips generates extended depleted layers that cannot be replenished by diffusion during rest periods. Because the application of pulses much shorter than the characteristic time τc approx. O(∼1 ms) for polarizing elec. double layers in the system would approach d.c. charging, probably dendrite propagation can should be inhibited (albeit not suppressed) by pulse charging within appropriate frequency ranges.
- 24Liu, Q.; Xu, J.; Yuan, S.; Chang, Z.; Xu, D.; Yin, Y.; Li, L.; Zhong, H.; Jiang, Y.; Yan, J.; Zhang, X. Artificial Protection Film on Lithium Metal Anode toward Long-Cycle-Life Lithium-Oxygen Batteries. Adv. Mater. 2015, 27, 5241– 5247, DOI: 10.1002/adma.20150149024https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtlWgsL%252FN&md5=e7d030229d8bda40d111e25dbce59847Artificial Protection Film on Lithium Metal Anode toward Long-Cycle-Life Lithium-Oxygen BatteriesLiu, Qing-Chao; Xu, Ji-Jing; Yuan, Shuang; Chang, Zhi-Wen; Xu, Dan; Yin, Yan-Bin; Li, Lin; Zhong, Hai-Xia; Jiang, Yin-Shan; Yan, Jun-Min; Zhang, Xin-BoAdvanced Materials (Weinheim, Germany) (2015), 27 (35), 5241-5247CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)A facile and effective strategy was developed to protect the lithium anode of a secondary lithium battery through fabrication of a protection film on the metal Li anode, in which a fluoroethylene carbonate (I) additive plays a key role in the crucial film-forming additive. As a proof-of-concept expt., even when using conventional Super P (carbon black) cathode, the obtained I-treated Li metal anode endowed Li-O2 batteries with superior cycle stability of >100 stable cycles with a fixed capacity of 1000 mA-h/g at a c.d. of 300 mA/g was obtained, which is more than three times that of the cells with a pristine Li metal anode and Li metal anode treated without I. The significantly improved cycling stability could be attributed to the protective film derived from I decompn.,.
- 25Yan, K.; Lee, H.-W.; Gao, T.; Zheng, G.; Yao, H.; Wang, H.; Lu, Z.; Zhou, Y.; Liang, Z.; Liu, Z.; Chu, S.; Cui, Y. Ultrathin Two-Dimensional Atomic Crystals as Stable Interfacial Layer for Improvement of Lithium Metal Anode. Nano Lett. 2014, 14, 6016– 6022, DOI: 10.1021/nl503125u25https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhsVekt7jJ&md5=b7cf8adb44da1aedf75c2a104d259fb2Ultrathin Two-Dimensional Atomic Crystals as Stable Interfacial Layer for Improvement of Lithium Metal AnodeYan, Kai; Lee, Hyun-Wook; Gao, Teng; Zheng, Guangyuan; Yao, Hongbin; Wang, Haotian; Lu, Zhenda; Zhou, Yu; Liang, Zheng; Liu, Zhongfan; Chu, Steven; Cui, YiNano Letters (2014), 14 (10), 6016-6022CODEN: NALEFD; ISSN:1530-6984. (American Chemical Society)Stable cycling of lithium metal anode is challenging due to the dendritic lithium formation and high chem. reactivity of lithium with electrolyte and nearly all the materials. Here, we demonstrate a promising novel electrode design by growing two-dimensional (2D) at. crystal layers including hexagonal boron nitride (h-BN) and graphene directly on Cu metal current collectors. Lithium ions were able to penetrate through the point and line defects of the 2D layers during the electrochem. deposition, leading to sandwiched lithium metal between ultrathin 2D layers and Cu. The 2D layers afford an excellent interfacial protection of Li metal due to their remarkable chem. stability as well as mech. strength and flexibility, resulting from the strong intralayer bonds and ultrathin thickness. Smooth Li metal deposition without dendritic and mossy Li formation was realized. We showed stable cycling over 50 cycles with Coulombic efficiency ∼97% in org. carbonate electrolyte with c.d. and areal capacity up to the practical value of 2.0 mA/cm2and 5.0 mAh/cm2, resp., which is a significant improvement over the unprotected electrodes in the same electrolyte.
- 26Liu, Y.; Lin, D.; Yuen, P. Y.; Liu, K.; Xie, J.; Dauskardt, R. H.; Cui, Y. An Artificial Solid Electrolyte Interphase with High Li-Ion Conductivity, Mechanical Strength, and Flexibility for Stable Lithium Metal Anodes. Adv. Mater. 2017, 29, 1605531, DOI: 10.1002/adma.201605531There is no corresponding record for this reference.
- 27Khurana, R.; Schaefer, J. L.; Archer, L. A.; Coates, G. W. Suppression of Lithium Dendrite Growth Using Cross-Linked Polyethylene/Poly(ethylene oxide) Electrolytes: A New Approach for Practical Lithium-Metal Polymer Batteries. J. Am. Chem. Soc. 2014, 136, 7395– 7402, DOI: 10.1021/ja502133j27https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXmsFWnsrc%253D&md5=71960add56cf11e7e9d858a50b0c6d1cSuppression of Lithium Dendrite Growth Using Cross-Linked Polyethylene/Poly(ethylene oxide) Electrolytes: A New Approach for Practical Lithium-Metal Polymer BatteriesKhurana, Rachna; Schaefer, Jennifer L.; Archer, Lynden A.; Coates, Geoffrey W.Journal of the American Chemical Society (2014), 136 (20), 7395-7402CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Solid polymer electrolyte (SPE) membranes are a crit. component of high specific energy rechargeable Li-metal polymer (LMP) batteries. SPEs exhibit low volatility and thus increase the safety of Li-based batteries compared to current state-of-the-art Li-ion batteries that use flammable small-mol. electrolytes. However, most SPEs exhibit low ionic cond. at room temp., and often allow the growth of lithium dendrites that short-circuit the batteries. Both of these deficiencies are significant barriers to the commercialization of LMP batteries. Herein a cross-linked polyethylene/poly(ethylene oxide) SPE is reported with both high ionic cond. (> 1.0 × 10-4 S/cm at 25°) and excellent resistance to dendrite growth. It has been proposed that SPEs with shear moduli of the same order of magnitude as lithium could be used to suppress dendrite growth, leading to increased lifetime and safety for LMP batteries. In contrast to the theor. predictions, the low-modulus (G' ≈ 1.0 × 105 Pa at 90°) cross-linked SPEs reported herein exhibit remarkable dendrite growth resistance. These results suggest that a high-modulus SPE is not a requirement for the control of dendrite proliferation.
- 28Stone, G. M.; Mullin, S. A.; Teran, A. A.; Hallinan, D. T.; Minor, A. M.; Hexemer, A.; Balsara, N. P. Resolution of the Modulus versus Adhesion Dilemma in Solid Polymer Electrolytes for Rechargeable Lithium Metal Batteries. J. Electrochem. Soc. 2012, 159, A222– A227, DOI: 10.1149/2.030203jes28https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC38XnvVSnsg%253D%253D&md5=45d31f648114ce418df69b70a8b1ab72Resolution of the Modulus versus Adhesion Dilemma in Solid Polymer Electrolytes for Rechargeable Lithium Metal BatteriesStone, G. M.; Mullin, S. A.; Teran, A. A.; Hallinan, D. T., Jr.; Minor, A. M.; Hexemer, A.; Balsara, N. P.Journal of the Electrochemical Society (2012), 159 (3), A222-A227CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)The authors present a solid electrolyte that adheres to the Li surface and resists dendrite growth, both of which are needed for the development of high specific energy rechargeable batteries with Li anodes. Nanostructured lamellar block copolymer electrolytes exhibit solid-like properties in the bulk, due to the presence of a randomly oriented granular structure, and liq.-like surface properties due to the formation of perpendicularly oriented lamellae at the Li-electrolyte interface. The amt. of charge that can be passed before short-circuit in a sym. Li-polymer-Li cell with nanostructured polystyrene-block-poly(ethylene oxide) electrolytes is larger than that obtained with homopolymer poly(ethylene oxide) electrolytes by a factor of 11 to 48. Grazing incident small angle x-ray scattering confirms that the microstructure of the block copolymer near the Li-polymer interface has a perpendicular orientation. This orientation leads to a liq.-like behavior of the polymer at the interface due to the liq. cryst. symmetry of block copolymers. This combination of bulk and surface properties enhances the resistance to dendrites while maintaining electrode-electrolyte contact.
- 29Yue, L.; Ma, J.; Zhang, J.; Zhao, J.; Dong, S.; Liu, Z.; Cui, G.; Chen, L. All solid-state polymer electrolytes for high-performance lithium ion batteries. Energy Storage Mater. 2016, 5, 139– 164, DOI: 10.1016/j.ensm.2016.07.003There is no corresponding record for this reference.
- 30Janek, J.; Zeier, W. G. A solid future for battery development. Nat. Energy 2016, 1, 16141, DOI: 10.1038/nenergy.2016.141There is no corresponding record for this reference.
- 31Li, J.; Ma, C.; Chi, M.; Liang, C.; Dudney, N. J. Solid Electrolyte: the Key for High-Voltage Lithium Batteries. Adv. Energy Mater. 2015, 5, 1401408, DOI: 10.1002/aenm.201401408There is no corresponding record for this reference.
- 32Suzuki, Y.; Kami, K.; Watanabe, K.; Watanabe, A.; Saito, N.; Ohnishi, T.; Takada, K.; Sudo, R.; Imanishi, N. Transparent cubic garnet-type solid electrolyte of Al2O3-doped Li7La3Zr2O12. Solid State Ionics 2015, 278, 172– 176, DOI: 10.1016/j.ssi.2015.06.00932https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtVKmsbrP&md5=7fd10b6e096b6cc875cc5495c59477c7Transparent cubic garnet-type solid electrolyte of Al2O3-doped Li7La3Zr2O12Suzuki, Yosuke; Kami, K.; Watanabe, K.; Watanabe, A.; Saito, N.; Ohnishi, T.; Takada, K.; Sudo, R.; Imanishi, N.Solid State Ionics (2015), 278 (), 172-176CODEN: SSIOD3; ISSN:0167-2738. (Elsevier B.V.)A transparent garnet-type lithium-ion conducting solid electrolyte of 1.0 wt. % Al2O3-doped Li7La3Zr2O12 (A-LLZ) was prepd. using hot isostatic pressing (HIP). The A-LLZ pellet sintered at 1180°C for 36 h was followed by HIP treatment at 127 MPa and 1180°C under an Ar atm. The bulk cond. of the HIP treated A-LLZ was 9.9 × 10-4 S cm-1 at 25°C. The Li/HIP treated A-LLZ/Li cell showed no short-circuit due to lithium dendrite formation at 0.5 mA cm- 2.
- 33Manthiram, A.; Yu, X.; Wang, S. Lithium battery chemistries enabled by solid-state electrolytes. Nat. Rev. Mater. 2017, 2, 16103, DOI: 10.1038/natrevmats.2016.10333https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXislGitr0%253D&md5=be4704bc600127083842361f9e75c578Lithium battery chemistries enabled by solid-state electrolytesManthiram, Arumugam; Yu, Xingwen; Wang, ShaofeiNature Reviews Materials (2017), 2 (3), 16103CODEN: NRMADL; ISSN:2058-8437. (Nature Publishing Group)Solid-state electrolytes are attracting increasing interest for electrochem. energy storage technologies. In this Review, we provide a background overview and discuss the state of the art, ion-transport mechanisms and fundamental properties of solid-state electrolyte materials of interest for energy storage applications. We focus on recent advances in various classes of battery chemistries and systems that are enabled by solid electrolytes, including all-solid-state lithium-ion batteries and emerging solid-electrolyte lithium batteries that feature cathodes with liq. or gaseous active materials (for example, lithium-air, lithium-sulfur and lithium-bromine systems). A low-cost, safe, aq. electrochem. energy storage concept with a 'mediator-ion' solid electrolyte is also discussed. Advanced battery systems based on solid electrolytes would revitalize the rechargeable battery field because of their safety, excellent stability, long cycle lives and low cost. However, great effort will be needed to implement solid-electrolyte batteries as viable energy storage systems. In this context, we discuss the main issues that must be addressed, such as achieving acceptable ionic cond., electrochem. stability and mech. properties of the solid electrolytes, as well as a compatible electrolyte/electrode interface.
- 34Kamaya, N.; Homma, K.; Yamakawa, Y.; Hirayama, M.; Kanno, R.; Yonemura, M.; Kamiyama, T.; Kato, Y.; Hama, S.; Kawamoto, K.; Mitsui, A. A lithium superionic conductor. Nat. Mater. 2011, 10, 682– 686, DOI: 10.1038/nmat306634https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3MXpsFaisLc%253D&md5=30637e2968f742a3e1da5f7fa4250644A lithium superionic conductorKamaya, Noriaki; Homma, Kenji; Yamakawa, Yuichiro; Hirayama, Masaaki; Kanno, Ryoji; Yonemura, Masao; Kamiyama, Takashi; Kato, Yuki; Hama, Shigenori; Kawamoto, Koji; Mitsui, AkioNature Materials (2011), 10 (9), 682-686CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Batteries are a key technol. in modern society. They are used to power elec. and hybrid elec. vehicles and to store wind and solar energy in smart grids. Electrochem. devices with high energy and power densities can currently be powered only by batteries with org. liq. electrolytes. However, such batteries require relatively stringent safety precautions, making large-scale systems complicated and expensive. The application of solid electrolytes is currently limited because they attain practically useful conductivities (10-2 S/cm) only at 50-80°, which is one order of magnitude lower than those of org. liq. electrolytes. Here, the authors report a Li superionic conductor, Li10GeP2S12 that has a new 3-dimensional framework structure. It exhibits an extremely high Li ionic cond. of 12 mS/cm at room temp. This represents the highest cond. achieved in a solid electrolyte, exceeding even those of liq. org. electrolytes. This new solid-state battery electrolyte has many advantages in terms of device fabrication (facile shaping, patterning and integration), stability (non-volatile), safety (non-explosive) and excellent electrochem. properties (high cond. and wide potential window).
- 35Kato, Y.; Hori, S.; Saito, T.; Suzuki, K.; Hirayama, M.; Mitsui, A.; Yonemura, M.; Iba, H.; Kanno, R. High-power all-solid-state batteries using sulfide superionic conductors. Nat. Energy 2016, 1, 16030, DOI: 10.1038/nenergy.2016.3035https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVekurs%253D&md5=cc1210221e70bc3e6c06e015effc70deHigh-power all-solid-state batteries using sulfide superionic conductorsKato, Yuki; Hori, Satoshi; Saito, Toshiya; Suzuki, Kota; Hirayama, Masaaki; Mitsui, Akio; Yonemura, Masao; Iba, Hideki; Kanno, RyojiNature Energy (2016), 1 (4), 16030CODEN: NEANFD; ISSN:2058-7546. (Nature Publishing Group)Compared with Li-ion batteries with liq. electrolytes, all-solid-state batteries offer an attractive option owing to their potential in improving the safety and achieving both high power and high energy densities. Despite extensive research efforts, the development of all-solid-state batteries still falls short of expectation largely because of the lack of suitable candidate materials for the electrolyte required for practical applications. Here the authors report Li superionic conductors with an exceptionally high cond. (25 mS cm-1 for Li9.54Si1.74P1.44S11.7Cl0.3), as well as high stability ( ∼0 V vs. Li metal for Li9.6P3S12). A fabricated all-solid-state cell based on this Li conductor has very small internal resistance, esp. at 100 oC. The cell possesses high specific power that is superior to that of conventional cells with liq. electrolytes. Stable cycling with a high c.d. of 18 C (charging/discharging in just 3 min; where C is the C-rate) is also demonstrated.
- 36Kerman, K.; Luntz, A.; Viswanathan, V.; Chiang, Y.-M.; Chen, Z. Review-Practical Challenges Hindering the Development of Solid State Li Ion Batteries. J. Electrochem. Soc. 2017, 164, A1731– A1744, DOI: 10.1149/2.1571707jes36https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVCitLvI&md5=99cf3345659e25c91eb25ed7090d1403Review-Practical Challenges Hindering the Development of Solid State Li Ion BatteriesKerman, Kian; Luntz, Alan; Viswanathan, Venkatasubramanian; Chiang, Yet-Ming; Chen, ZheboJournal of the Electrochemical Society (2017), 164 (7), A1731-A1744CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Solid state electrolyte systems boasting Li+ cond. of >10 mS cm-1 at room temp. have opened the potential for developing a solid state battery with power and energy densities that are competitive with conventional liq. electrolyte systems. The primary focus of this review is twofold. First, differences in Li penetration resistance in solid state systems are discussed, and kinetic limitations of the solid state interface are highlighted. Second, technol. challenges assocd. with processing such systems in relevant form factors are elucidated, and architectures needed for cell level devices in the context of product development are reviewed. Specific research vectors that provide high value to advancing solid state batteries are outlined and discussed.
- 37Sharafi, A.; Yu, S.; Naguib, M.; Lee, M.; Ma, C.; Meyer, H. M.; Nanda, J.; Chi, M.; Siegel, D. J.; Sakamoto, J. Impact of air exposure and surface chemistry on Li-Li7La3Zr2O12 interfacial resistance. J. Mater. Chem. A 2017, 5, 13475– 13487, DOI: 10.1039/C7TA03162A37https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtVWmtrnE&md5=ba7e873b21db6b50f59e450c3d6f6ec2Impact of air exposure and surface chemistry on Li-Li7La3Zr2O12 interfacial resistanceSharafi, Asma; Yu, Seungho; Naguib, Michael; Lee, Marcus; Ma, Cheng; Meyer, Harry M.; Nanda, Jagjit; Chi, Maiofang; Siegel, Donald J.; Sakamoto, JeffJournal of Materials Chemistry A: Materials for Energy and Sustainability (2017), 5 (26), 13475-13487CODEN: JMCAET; ISSN:2050-7496. (Royal Society of Chemistry)Li7La3Zr2O12 (LLZO) is a promising solid-state electrolyte that could enable solid-state-batteries (SSB) using metallic Li anodes. For a SSB to be viable, the stability and charge transfer kinetics at the Li-LLZO interface should foster facile plating and stripping of Li. Contrary to these goals, recent studies have reported high Li-LLZO interfacial resistance which was attributed to a contamination layer that forms upon exposure of LLZO to air. This study clarifies the mechanisms and consequences assocd. with air exposure of LLZO; addnl., strategies to minimize these effects are described. First-principles calcns. reveal that LLZO readily reacts with humid air; the most favorable reaction pathway involves protonation of LLZO and formation of Li2CO3. XPS, SEM, Raman spectroscopy, and transmission electron microscopy were used to characterize the surface and subsurface chem. of LLZO as a function of relative humidity and exposure time. Electrochem. impedance spectroscopy was used to measure the Li-LLZO interfacial resistance as a function of surface contamination. These data indicate that air exposure-induced contamination impacts the interfacial resistance significantly, when exposure time exceeds 24 h. The results of this study provide valuable insight into the sensitivity of LLZO to air and how the effects of air contamination can be reversed.
- 38Sharafi, A.; Haslam, C. G.; Kerns, R. D.; Wolfenstine, J.; Sakamoto, J. Controlling and correlating the effect of grain size with the mechanical and electrochemical properties of Li7La3Zr2O12 solid-state electrolyte. J. Mater. Chem. A 2017, 5, 21491– 21504, DOI: 10.1039/C7TA06790A38https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhs1Sksb%252FP&md5=eccb1f1d8cfb3d13b2237d27793aa772Controlling and correlating the effect of grain size with the mechanical and electrochemical properties of Li7La3Zr2O12 solid-state electrolyteSharafi, Asma; Haslam, Catherine G.; Kerns, Robert D.; Wolfenstine, Jeff; Sakamoto, JeffJournal of Materials Chemistry A: Materials for Energy and Sustainability (2017), 5 (40), 21491-21504CODEN: JMCAET; ISSN:2050-7496. (Royal Society of Chemistry)Li7La3Zr2O12 (LLZO) solid-state electrolyte is garnering interest due to its potential to enable solid-state batteries (SSBs) using metallic Li anodes. However, Li metal propagates along LLZO grain boundaries at high Li plating current densities (above the crit. c.d., CCD). In the present study, we examd. whether microstructural aspects, such as grain size, could influence mech. and electrochem. properties thereby affecting the CCD. A unique densification technique (heating between 1100 and 1300 °C) was used to control grain size. Electron backscatter diffraction detd. that the grain size and the misorientation angle varied from 5 to 600 μm and 20 to 40°, resp. Vickers indentation was used to characterize the mech. properties and revealed that hardness decreased (9.9-6.8 GPa) with increasing grain size, but the fracture toughness was invariant (0.6 MPa m-1/2) at grain sizes ≥40 μm. DC and AC techniques were used to measure and correlate the CCD with grain size and showed that the CCD increased with increasing grain size achieving a max. of 0.6 mA cm-2. We believe the implications of this work could be far-reaching in that they represent a significant step towards understanding the mechanism(s) that control the stability of the Li-LLZO interface and a rational approach to increase the CCD in SSBs.
- 39Monroe, C.; Newman, J. The Impact of Elastic Deformation on Deposition Kinetics at Lithium/Polymer Interfaces. J. Electrochem. Soc. 2005, 152, A396– A404, DOI: 10.1149/1.185085439https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2MXhs1KktLc%253D&md5=e878820c6a811396757bd7435bdb40adThe impact of elastic deformation on deposition kinetics at lithium/polymer interfacesMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2005), 152 (2), A396-A404CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Past theories of electrode stability assume that the surface tension resists the amplification of surface roughness at cathodes and show that instability at lithium/liq. interfaces cannot be prevented by surface forces alone. This work treats interfacial stability in lithium/polymer systems where the electrolyte is solid. Linear elasticity theory is employed to compute the addnl. effect of bulk mech. forces on electrode stability. The lithium and polymer are treated as Hookean elastic materials, characterized by their shear moduli and Poisson's ratios. Two-dimensional displacement distributions that satisfy force balances across a periodically deforming interface are derived; these allow computation of the stress and surface-tension forces. The incorporation of elastic effects into a kinetic model demonstrates regimes of electrolyte mech. properties where amplification of surface roughness can be inhibited. For a polymer material with Poisson's ratio similar to poly(ethylene oxide), interfacial roughening is mech. suppressed when the separator shear modulus is about twice that of lithium.
- 40Ahmad, Z.; Viswanathan, V. Stability of Electrodeposition at Solid-Solid Interfaces and Implications for Metal Anodes. Phys. Rev. Lett. 2017, 119, 056003, DOI: 10.1103/PhysRevLett.119.05600340https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXhs1SrtbrP&md5=b71331ba73f970ec5c45f52cdc08ecadStability of electrodeposition at solid-solid interfaces and implications for metal anodesAhmad, Zeeshan; Viswanathan, VenkatasubramanianPhysical Review Letters (2017), 119 (5), 056003/1-056003/6CODEN: PRLTAO; ISSN:1079-7114. (American Physical Society)We generalize the conditions for stable electrodeposition at isotropic solid-solid interfaces using a kinetic model which incorporates the effects of stresses and surface tension at the interface. We develop a stability diagram that shows two regimes of stability: a previously known pressure-driven mechanism and a new d.-driven stability mechanism that is governed by the relative d. of metal in the two phases. We show that inorg. solids and solid polymers generally do not lead to stable electrodeposition, and provide design guidelines for achieving stable electrodeposition.
- 41Diggle, J. W.; Despic, A. R.; Bockris, J. O. The Mechanism of the Dendritic Electrocrystallization of Zinc. J. Electrochem. Soc. 1969, 116, 1503– 1514, DOI: 10.1149/1.241158841https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaE3cXos1yl&md5=48077f26ea20fa76b2cc78e39c4f1309Mechanism of the dendritic electrocrystallization of zincDiggle, J. W.; Despic, A. R.; Bockris, J. O'M.Journal of the Electrochemical Society (1969), 116 (11), 1503-14CODEN: JESOAN; ISSN:0013-4651.Measurements were made of the growth rate of Zn dendrites in alk. zincate solns. as a function of overpotential (η), concn. (c), and temp. (T). The tip radii were measured by electron microscopy. At const. potential, an initiation time of between 5 and 100 min is observed, depending on η, c, and T. The total current to base and dendrite was independent of time until a time *aui, where τi < τd (the time for initiation obtained from the growth rate vs. time relation). Thereafter, i is proportional to t2. A crit. overpotential was detd., -75 mv. >ηcrit> -85 mv. Below this ηcrit, sponge was formed. Dendrites were observed up to η = -160 mv.; above this the deposition was heavy sponge. At a given c, the growth rate of a given dendrite increased with η according to an exponential law. The growing tip is parabolic, where 10-5 < γtip < 10-4 cm. No twinning was observed. The basic model used depended on the increase in c.d. possible for an electrodic reaction when the diffusion current depends on a radius of curvature of the substrate, rather than the linear diffusion layer thickness, δ. When the tip of a dendrite-precursor attains this condition, its growth is released from the diffusion control characteristic of it in the predendrite situation, and it grows further under predominantly activation control at a rate far greater than that possible in any other direction, where the radii of curvature are much greater. The Gibbs radius-dependent overpotential term is also present, although it has a minimized influence. The initiation of the dendrite is treated in terms of growing pyramids on the substrate surface. At 1st the growth is linear-diffusion controlled, but the rotation of the spiral, within the linear diffusion boundary surrounding the sphere, gives rise to a decrease of the effective radius (γ) of curvature of the dendrite tip until the value γ<0.1 δ is attained, which is effectively the condition for the dendrite initiation. The theory of the propagation in terms of the activation, diffusion, and Gibbs overpotential is consistent, in terms of τd, with expt. A derived growth-time line is also numerically consistent with expt. The dendrite growth rate as a function of c and η are numerically calcd. with reasonable consistency. The tip radius can also be approx. calcd. in terms of the present model.
- 42Monroe, C.; Newman, J. Dendrite Growth in Lithium/Polymer Systems: A Propagation Model for Liquid Electrolytes under Galvanostatic Conditions. J. Electrochem. Soc. 2003, 150, A1377– A1384, DOI: 10.1149/1.160668642https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD3sXnt1OmtLw%253D&md5=178ec3a3e854d05aede7708d68c7957aDendrite Growth in Lithium/Polymer SystemsMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2003), 150 (10), A1377-A1384CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Dendrite growth in a parallel-electrode Li/polymer battery during galvanostatic charging was modeled. The growth model is surface-energy controlled, incorporating the effect of dendrite tip curvature into the dendrite growth kinetics. Using data representative of the oxymethylene-linked poly(ethylene oxide)/LiTFSI system, dendrites accelerate across cells under all conditions, and growth is always slowed by lowering the c.d. Cell shorting occurs during typical charges at current densities >75% of the limiting current. Increased interelectrode distance slows failure, but the advantages decrease as distance increases. A factor of 1000 increase in surface forces delays cell failure by only 6%. While larger diffusion coeffs. usually extend the time to cell failure, this trend is not consistent at high transference nos.
- 43Monroe, C.; Newman, J. The Effect of Interfacial Deformation on Electrodeposition Kinetics. J. Electrochem. Soc. 2004, 151, A880– A886, DOI: 10.1149/1.171089343https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2cXktVGkt70%253D&md5=22ed18c5cf280522d5d26e2bc30cb6bcThe Effect of Interfacial Deformation on Electrodeposition KineticsMonroe, Charles; Newman, JohnJournal of the Electrochemical Society (2004), 151 (6), A880-A886CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)Mullins-Sekerka linear stability anal. and the Barton and Bockris dendrite-propagation model are popular methods used to describe cathodic roughening and dendritic growth. These commonly cited theories employ kinetic relations that differ in math. form, but both contain the effects of surface tension and local concn. deviations induced by surface roughening. Here, a kinetic model is developed which addnl. includes mech. forces such as elasticity, viscous drag, and pressure, showing their effect on exchange current densities and potentials at roughening interfaces. The proposed expression describes the c.d. in terms of applied overpotential at deformed interfaces with arbitrary three-dimensional interfacial geometry. Both the Mullins-Sekerka and the Barton-Bockris kinetics can be derived as special cases of the general expression, thereby validating the proposed model and elucidating the fundamental assumptions on which the 2 previous theories rely.
- 44Curtarolo, S.; Hart, G. L. W.; Nardelli, M. B.; Mingo, N.; Sanvito, S.; Levy, O. The high-throughput highway to computational materials design. Nat. Mater. 2013, 12, 191, DOI: 10.1038/nmat356844https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXislWju7c%253D&md5=5e116fbafda8e8437ccd0fdf7304d939The high-throughput highway to computational materials designCurtarolo, Stefano; Hart, Gus L. W.; Nardelli, Marco Buongiorno; Mingo, Natalio; Sanvito, Stefano; Levy, OhadNature Materials (2013), 12 (3), 191-201CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)A review. High-throughput computational materials design is an emerging area of materials science. By combining advanced thermodn. and electronic-structure methods with intelligent data mining and database construction, and exploiting the power of current supercomputer architectures, scientists generate, manage and analyze enormous data repositories for the discovery of novel materials. In this Review we provide a current snapshot of this rapidly evolving field, and highlight the challenges and opportunities that lie ahead.
- 45Saal, J. E.; Kirklin, S.; Aykol, M.; Meredig, B.; Wolverton, C. Materials Design and Discovery with High-Throughput Density Functional Theory: The Open Quantum Materials Database (OQMD). JOM 2013, 65, 1501– 1509, DOI: 10.1007/s11837-013-0755-445https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhsFentbzK&md5=feaac43dc6ff4c2d7a7a4c94f0b58c2bMaterials Design and Discovery with High-Throughput Density Functional Theory: The Open Quantum Materials Database (OQMD)Saal, James E.; Kirklin, Scott; Aykol, Muratahan; Meredig, Bryce; Wolverton, C.JOM (2013), 65 (11), 1501-1509CODEN: JOMMER; ISSN:1047-4838. (Springer)A review. High-throughput d. functional theory (HT DFT) is fast becoming a powerful tool for accelerating materials design and discovery by the amassing tens and even hundreds of thousands of DFT calcns. in large databases. Complex materials problems can be approached much more efficiently and broadly through the sheer quantity of structures and chemistries available in such databases. Our HT DFT database, the Open Quantum Materials Database (OQMD), contains over 200,000 DFT calcd. crystal structures and will be freely available for public use at http://oqmd.org. In this review, we describe the OQMD and its use in five materials problems, spanning a wide range of applications and materials types: (I) Li-air battery combination catalyst/electrodes, (II) Li-ion battery anodes, (III) Li-ion battery cathode coatings reactive with HF, (IV) Mg-alloy long-period stacking ordered (LPSO) strengthening ppts., and (V) training a machine learning model to predict new stable ternary compds.
- 46Pilania, G.; Wang, C.; Jiang, X.; Rajasekaran, S.; Ramprasad, R. Accelerating materials property predictions using machine learning. Sci. Rep. 2013, 3, 2810, DOI: 10.1038/srep0281046https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A280%3ADC%252BC2c%252FltlCqtQ%253D%253D&md5=3475edb4dda3d93baae0d552d482b187Accelerating materials property predictions using machine learningPilania Ghanshyam; Wang Chenchen; Jiang Xun; Rajasekaran Sanguthevar; Ramprasad RamamurthyScientific reports (2013), 3 (), 2810 ISSN:.The materials discovery process can be significantly expedited and simplified if we can learn effectively from available knowledge and data. In the present contribution, we show that efficient and accurate prediction of a diverse set of properties of material systems is possible by employing machine (or statistical) learning methods trained on quantum mechanical computations in combination with the notions of chemical similarity. Using a family of one-dimensional chain systems, we present a general formalism that allows us to discover decision rules that establish a mapping between easily accessible attributes of a system and its properties. It is shown that fingerprints based on either chemo-structural (compositional and configurational information) or the electronic charge density distribution can be used to make ultra-fast, yet accurate, property predictions. Harnessing such learning paradigms extends recent efforts to systematically explore and mine vast chemical spaces, and can significantly accelerate the discovery of new application-specific materials.
- 47Liu, Y.; Zhao, T.; Ju, W.; Shi, S. Materials discovery and design using machine learning. J. Materiomics 2017, 3, 159– 177, DOI: 10.1016/j.jmat.2017.08.002There is no corresponding record for this reference.
- 48Gómez-Bombarelli, R.; Wei, J. N.; Duvenaud, D.; Hernández-Lobato, J. M.; Sánchez-Lengeling, B.; Sheberla, D.; Aguilera-Iparraguirre, J.; Hirzel, T. D.; Adams, R. P.; Aspuru-Guzik, A. Automatic Chemical Design Using a Data-Driven Continuous Representation of Molecules. ACS Cent. Sci. 2018, 4, 268– 276, DOI: 10.1021/acscentsci.7b0057248https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXntlWquw%253D%253D&md5=322d9ff569fc9c8831e91d915104d985Automatic Chemical Design Using a Data-Driven Continuous Representation of MoleculesGomez-Bombarelli, Rafael; Wei, Jennifer N.; Duvenaud, David; Hernandez-Lobato, Jose Miguel; Sanchez-Lengeling, Benjamin; Sheberla, Dennis; Aguilera-Iparraguirre, Jorge; Hirzel, Timothy D.; Adams, Ryan P.; Aspuru-Guzik, AlanACS Central Science (2018), 4 (2), 268-276CODEN: ACSCII; ISSN:2374-7951. (American Chemical Society)We report a method to convert discrete representations of mols. to and from a multidimensional continuous representation. This model allows us to generate new mols. for efficient exploration and optimization through open-ended spaces of chem. compds. A deep neural network was trained on hundreds of thousands of existing chem. structures to construct three coupled functions: an encoder, a decoder, and a predictor. The encoder converts the discrete representation of a mol. into a real-valued continuous vector, and the decoder converts these continuous vectors back to discrete mol. representations. The predictor ests. chem. properties from the latent continuous vector representation of the mol. Continuous representations of mols. allow us to automatically generate novel chem. structures by performing simple operations in the latent space, such as decoding random vectors, perturbing known chem. structures, or interpolating between mols. Continuous representations also allow the use of powerful gradient-based optimization to efficiently guide the search for optimized functional compds. We demonstrate our method in the domain of drug-like mols. and also in a set of mols. with fewer that nine heavy atoms.
- 49de Jong, M.; Chen, W.; Notestine, R.; Persson, K.; Ceder, G.; Jain, A.; Asta, M.; Gamst, A. A Statistical Learning Framework for Materials Science: Application to Elastic Moduli of k-nary Inorganic Polycrystalline Compounds. Sci. Rep. 2016, 6, 34256, DOI: 10.1038/srep3425649https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28Xhs1amtL%252FO&md5=dbe3625fe35277822c6ae92c7dcbfee7A Statistical Learning Framework for Materials Science: Application to Elastic Moduli of k-nary Inorganic Polycrystalline Compoundsde Jong, Maarten; Chen, Wei; Notestine, Randy; Persson, Kristin; Ceder, Gerbrand; Jain, Anubhav; Asta, Mark; Gamst, AnthonyScientific Reports (2016), 6 (), 34256CODEN: SRCEC3; ISSN:2045-2322. (Nature Publishing Group)Materials scientists increasingly employ machine or statistical learning (SL) techniques to accelerate materials discovery and design. Such pursuits benefit from pooling training data across, and thus being able to generalize predictions over, k-nary compds. of diverse chemistries and structures. This work presents a SL framework that addresses challenges in materials science applications, where datasets are diverse but of modest size, and extreme values are often of interest. Our advances include the application of power or Holder means to construct descriptors that generalize over chem. and crystal structure, and the incorporation of multivariate local regression within a gradient boosting framework. The approach is demonstrated by developing SL models to predict bulk and shear moduli (K and G, resp.) for polycryst. inorg. compds., using 1,940 compds. from a growing database of calcd. elastic moduli for metals, semiconductors and insulators. The usefulness of the models is illustrated by screening for superhard materials.
- 50Isayev, O.; Oses, C.; Toher, C.; Gossett, E.; Curtarolo, S.; Tropsha, A. Universal fragment descriptors for predicting properties of inorganic crystals. Nat. Commun. 2017, 8, 15679, DOI: 10.1038/ncomms1567950https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXpt1Oksb8%253D&md5=543e2069263b9b1b1a121667866e2c5aUniversal fragment descriptors for predicting properties of inorganic crystalsIsayev, Olexandr; Oses, Corey; Toher, Cormac; Gossett, Eric; Curtarolo, Stefano; Tropsha, AlexanderNature Communications (2017), 8 (), 15679CODEN: NCAOBW; ISSN:2041-1723. (Nature Publishing Group)A review. Although historically materials discovery has been driven by a laborious trial-and-error process, knowledge-driven materials design can now be enabled by the rational combination of Machine Learning methods and materials databases. Here, data from the AFLOW repository for ab initio calcns. is combined with Quant. Materials Structure-Property Relationship models to predict important properties: metal/insulator classification, band gap energy, bulk/shear moduli, Debye temp. and heat capacities. The prediction's accuracy compares well with the quality of the training data for virtually any stoichiometric inorg. cryst. material, reciprocating the available thermomech. exptl. data. The universality of the approach is attributed to the construction of the descriptors: Property-Labeled Materials Fragments. The representations require only minimal structural input allowing straightforward implementations of simple heuristic design rules.
- 51Fujimura, K.; Seko, A.; Koyama, Y.; Kuwabara, A.; Kishida, I.; Shitara, K.; Fisher, C. A. J.; Moriwake, H.; Tanaka, I. Accelerated Materials Design of Lithium Superionic Conductors Based on First-Principles Calculations and Machine Learning Algorithms. Adv. Energy Mater. 2013, 3, 980– 985, DOI: 10.1002/aenm.20130006051https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtlWhsbzM&md5=4ec409403b25e39e04cc760523694fa3Accelerated materials design of lithium superionic conductors based on first-principles calculations and machine learning algorithmsFujimura, Koji; Seko, Atsuto; Koyama, Yukinori; Kuwabara, Akihide; Kishida, Ippei; Shitara, Kazuki; Fisher, Craig A. J.; Moriwake, Hiroki; Tanaka, IsaoAdvanced Energy Materials (2013), 3 (8), 980-985CODEN: ADEMBC; ISSN:1614-6840. (Wiley-Blackwell)In this article, results of systematic sets of first-principles calcns. based on the cluster expansion method, as well as first-principles mol. dynamics (FPMD) simulations carried out to calc. lithium-ion conductivities at high temp., for a diverse range of compns. is studied. A machine-learning technique is used to combine theor. and exptl. datasets to predict the cond. of each compn. at 373 K. The insights obtained show that an iterative combination of first-principles calcns. and focused expts. can greatly accelerate the materials design process by enabling a wide compositional and structural phase space to be examd. efficiently.
- 52Sendek, A. D.; Yang, Q.; Cubuk, E. D.; Duerloo, K.-A. N.; Cui, Y.; Reed, E. J. Holistic computational structure screening of more than 12000 candidates for solid lithium-ion conductor materials. Energy Environ. Sci. 2017, 10, 306– 320, DOI: 10.1039/C6EE02697D52https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XhvFymtbrP&md5=97cc808518346d0a599f623a2b35b7e4Holistic computational structure screening of more than 12 000 candidates for solid lithium-ion conductor materialsSendek, Austin D.; Yang, Qian; Cubuk, Ekin D.; Duerloo, Karel-Alexander N.; Cui, Yi; Reed, Evan J.Energy & Environmental Science (2017), 10 (1), 306-320CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)We present a new type of large-scale computational screening approach for identifying promising candidate materials for solid state electrolytes for lithium ion batteries that is capable of screening all known lithium contg. solids. To be useful for batteries, high performance solid state electrolyte materials must satisfy many requirements at once, an optimization that is difficult to perform exptl. or with computationally expensive ab initio techniques. We first screen 12 831 lithium contg. cryst. solids for those with high structural and chem. stability, low electronic cond., and low cost. We then develop a data-driven ionic cond. classification model using logistic regression for identifying which candidate structures are likely to exhibit fast lithium conduction based on exptl. measurements reported in the literature. The screening reduces the list of candidate materials from 12 831 down to 21 structures that show promise as electrolytes, few of which have been examd. exptl. We discover that none of our simple atomistic descriptor functions alone provide predictive power for ionic cond., but a multi-descriptor model can exhibit a useful degree of predictive power. We also find that screening for structural stability, chem. stability and low electronic cond. eliminates 92.2% of all Li-contg. materials and screening for high ionic cond. eliminates a further 93.3% of the remainder. Our screening utilizes structures and electronic information contained in the Materials Project database.
- 53Evans, J. D.; Coudert, F.-X. Predicting the Mechanical Properties of Zeolite Frameworks by Machine Learning. Chem. Mater. 2017, 29, 7833– 7839, DOI: 10.1021/acs.chemmater.7b0253253https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhtl2lsLfK&md5=5745ca383f3204d7c606d9eec2953d22Predicting the Mechanical Properties of Zeolite Frameworks by Machine LearningEvans, Jack D.; Coudert, Francois-XavierChemistry of Materials (2017), 29 (18), 7833-7839CODEN: CMATEX; ISSN:0897-4756. (American Chemical Society)We show here that machine learning is a powerful new tool for predicting the elastic response of zeolites. We built our machine learning approach relying on geometric features only, which are related to local geometry, structure, and porosity of a zeolite, to predict bulk and shear moduli of zeolites with an accuracy exceeding that of force field approaches. The development of this model has illustrated clear correlations between characteristic features of a zeolite and elastic moduli, providing exceptional insight into the mechanics of zeolitic frameworks. Finally, we employ this methodol. to predict the elastic response of 590,448 hypothetical zeolites, and the results of this massive database provide clear evidence of stability trends in porous materials.
- 54Ahmad, Z.; Viswanathan, V. Role of anisotropy in determining stability of electrodeposition at solid-solid interfaces. Phys. Rev. Materials 2017, 1, 055403, DOI: 10.1103/PhysRevMaterials.1.055403There is no corresponding record for this reference.
- 55Xu, C.; Ahmad, Z.; Aryanfar, A.; Viswanathan, V.; Greer, J. R. Enhanced strength and temperature dependence of mechanical properties of Li at small scales and its implications for Li metal anodes. Proc. Natl. Acad. Sci. U. S. A. 2017, 114, 57– 61, DOI: 10.1073/pnas.161573311455https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XitFWls7fM&md5=65404fc79b4b340710a0a4c287094cf0Enhanced strength and temperature dependence of mechanical properties of Li at small scales and its implications for Li metal anodesXu, Chen; Ahmad, Zeeshan; Aryanfar, Asghar; Viswanathan, Venkatasubramanian; Greer, Julia R.Proceedings of the National Academy of Sciences of the United States of America (2017), 114 (1), 57-61CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Most next-generation Li ion battery chemistries require a functioning lithium metal (Li) anode. However, its application in secondary batteries has been inhibited because of uncontrollable dendrite growth during cycling. Mech. suppression of dendrite growth through solid polymer electrolytes (SPEs) or through robust separators has shown the most potential for alleviating this problem. Studies of the mech. behavior of Li at any length scale and temp. are limited because of its extreme reactivity, which renders sample prepn., transfer, microstructure characterization, and mech. testing extremely challenging. We conduct nanomech. expts. in an in situ scanning electron microscope and show that micrometer-sized Li attains extremely high strengths of 105 MPa at room temp. and of 35 MPa at 90 °C. We demonstrate that single-cryst. Li exhibits a power-law size effect at the micrometer and submicrometer length scales, with the strengthening exponent of -0.68 at room temp. and of -1.00 at 90 °C. We also report the elastic and shear moduli as a function of crystallog. orientation gleaned from expts. and first-principles calcns., which show a high level of anisotropy up to the m.p., where the elastic and shear moduli vary by a factor of ∼4 between the stiffest and most compliant orientations. The emergence of such high strengths in small-scale Li and sensitivity of this metal's stiffness to crystallog. orientation help explain why the existing methods of dendrite suppression have been mainly unsuccessful and have significant implications for practical design of future-generation batteries.
- 56Shi, F.; Pei, A.; Vailionis, A.; Xie, J.; Liu, B.; Zhao, J.; Gong, Y.; Cui, Y. Strong texturing of lithium metal in batteries. Proc. Natl. Acad. Sci. U. S. A. 2017, 114, 12138– 12143, DOI: 10.1073/pnas.170822411456https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhslemsrjO&md5=ca7238bf137ef10cd147f88226c28000Strong texturing of lithium metal in batteriesShi, Feifei; Pei, Allen; Vailionis, Arturas; Xie, Jin; Liu, Bofei; Zhao, Jie; Gong, Yongji; Cui, YiProceedings of the National Academy of Sciences of the United States of America (2017), 114 (46), 12138-12143CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Lithium, with its high theor. specific capacity and lowest electrochem. potential, was recognized as the ultimate neg. electrode material for next-generation lithium-based high-energy-d. batteries. However, a key challenge that has yet to be overcome is the inferior reversibility of Li plating and stripping, typically thought to be related to the uncontrollable morphol. evolution of the Li anode during cycling. Here we show that Li-metal texturing (preferential crystallog. orientation) occurs during electrochem. deposition, which governs the morphol. change of the Li anode. X-ray diffraction pole-figure anal. demonstrates that the texture of Li deposits is primarily dependent on the type of additive or cross-over mol. from the cathode side. With adsorbed additives, like LiNO3 and polysulfide, the lithium deposits are strongly textured, with Li (110) planes parallel to the substrate, and thus exhibit uniform, rounded morphol. A growth diagram of lithium deposits is given to connect various texture and morphol. scenarios for different battery electrolytes. This understanding of lithium electrocrystn. from the crystallog. point of view provides significant insight for future lithium anode materials design in high-energy-d. batteries.
- 57Wang, Y.; Richards, W. D.; Ong, S. P.; Miara, L. J.; Kim, J. C.; Mo, Y.; Ceder, G. Design principles for solid-state lithium superionic conductors. Nat. Mater. 2015, 14, 1026– 1031, DOI: 10.1038/nmat436957https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhtlCksb%252FI&md5=114ad3946493cf35ef3ee5d65e37c2d7Design principles for solid-state lithium superionic conductorsWang, Yan; Richards, William Davidson; Ong, Shyue Ping; Miara, Lincoln J.; Kim, Jae Chul; Mo, Yifei; Ceder, GerbrandNature Materials (2015), 14 (10), 1026-1031CODEN: NMAACR; ISSN:1476-1122. (Nature Publishing Group)Lithium solid electrolytes can potentially address two key limitations of the org. electrolytes used in today's lithium-ion batteries, namely, their flammability and limited electrochem. stability. However, achieving a Li+ cond. in the solid state comparable to existing liq. electrolytes (>1 mS cm-1) is particularly challenging. In this work, we reveal a fundamental relationship between anion packing and ionic transport in fast Li-conducting materials and expose the desirable structural attributes of good Li-ion conductors. We find that an underlying body-centered cubic-like anion framework, which allows direct Li hops between adjacent tetrahedral sites, is most desirable for achieving high ionic cond., and that indeed this anion arrangement is present in several known fast Li-conducting materials and other fast ion conductors. These findings provide important insight towards the understanding of ionic transport in Li-ion conductors and serve as design principles for future discovery and design of improved electrolytes for Li-ion batteries.
- 58Shannon, R. D. Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Crystallogr., Sect. A: Cryst. Phys., Diffr., Theor. Gen. Crystallogr. 1976, 32, 751– 767, DOI: 10.1107/S0567739476001551There is no corresponding record for this reference.
- 59Gotoh, K.; Finney, J. L. Statistical geometrical approach to random packing density of equal spheres. Nature 1974, 252, 202, DOI: 10.1038/252202a0There is no corresponding record for this reference.
- 60Stepanyuk, V.; Szasz, A.; Katsnelson, A.; Trushin, O.; Müller, H.; Kirchmayr, H. Microstructure and its relaxation in FeB amorphous system simulated by moleculular dynamics. J. Non-Cryst. Solids 1993, 159, 80– 87, DOI: 10.1016/0022-3093(93)91284-AThere is no corresponding record for this reference.
- 61Ong, S. P.; Richards, W. D.; Jain, A.; Hautier, G.; Kocher, M.; Cholia, S.; Gunter, D.; Chevrier, V. L.; Persson, K. A.; Ceder, G. Python Materials Genomics (pymatgen): A robust, open-source python library for materials analysis. Comput. Mater. Sci. 2013, 68, 314– 319, DOI: 10.1016/j.commatsci.2012.10.02861https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhsVGjt7g%253D&md5=104f567dbd8f4199911ded91bc42100ePython Materials Genomics (pymatgen): A robust, open-source python library for materials analysisOng, Shyue Ping; Richards, William Davidson; Jain, Anubhav; Hautier, Geoffroy; Kocher, Michael; Cholia, Shreyas; Gunter, Dan; Chevrier, Vincent L.; Persson, Kristin A.; Ceder, GerbrandComputational Materials Science (2013), 68 (), 314-319CODEN: CMMSEM; ISSN:0927-0256. (Elsevier B.V.)We present the Python Materials Genomics (pymatgen) library, a robust, open-source Python library for materials anal. A key enabler in high-throughput computational materials science efforts is a robust set of software tools to perform initial setup for the calcns. (e.g., generation of structures and necessary input files) and post-calcn. anal. to derive useful material properties from raw calcd. data. The pymatgen library aims to meet these needs by (1) defining core Python objects for materials data representation, (2) providing a well-tested set of structure and thermodn. analyses relevant to many applications, and (3) establishing an open platform for researchers to collaboratively develop sophisticated analyses of materials data obtained both from first principles calcns. and expts. The pymatgen library also provides convenient tools to obtain useful materials data via the Materials Project's REpresentational State Transfer (REST) Application Programming Interface (API). As an example, using pymatgen's interface to the Materials Project's RESTful API and phase diagram package, we demonstrate how the phase and electrochem. stability of a recently synthesized material, Li4SnS4, can be analyzed using a min. of computing resources. We find that Li4SnS4 is a stable phase in the Li-Sn-S phase diagram (consistent with the fact that it can be synthesized), but the narrow range of lithium chem. potentials for which it is predicted to be stable would suggest that it is not intrinsically stable against typical electrodes used in lithium-ion batteries.
- 62Pannikkat, A.; Raj, R. Measurement of an electrical potential induced by normal stress applied to the interface of an ionic material at elevated temperatures. Acta Mater. 1999, 47, 3423– 3431, DOI: 10.1016/S1359-6454(99)00206-262https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK1MXmvVaku78%253D&md5=929fe736a48797d25a19d934c8079ebfMeasurement of an electrical potential induced by normal stress applied to the interface of an ionic material at elevated temperaturesPannikkat, A. K.; Raj, R.Acta Materialia (1999), 47 (12), 3423-3431CODEN: ACMAFD; ISSN:1359-6454. (Elsevier Science Ltd.)The measurement of a p.d. between 2 surfaces of ZrO2 is reported, when a normal stress is applied to one surface, leaving the other surface stress free. The p.d. is proportional to the applied stress over a wide range. The proportionality const. represents a new thermodn. measurement of the interfacial state because the measurement is reversible and independent of temp. In ZrO2, the proportionality const. is related to the vol. and the charge on the O ion by considering thermodn. equil. among the electrochem. potentials of the O ion at the stressed and unstressed interfaces. The agreement with theory is within 10% for specimens made of polycryst. ZrO2, or single crystal cubic ZrO2 of (100) orientation. The proportionality const. changes by up to 20% for other orientations of the single crystal; this change is attributed to differences in the effective charge on the O ion on different surface orientations. The kinetics of the voltage response was also investigated in detail; it is consistent with the diffusion of the O ion along the interface formed between the metal electrode and the ZrO2 surface. The present measurements provide the first exptl. confirmation of the fundamental relationship between the chem. potential, the normal traction, and the at. vol. of species at interfaces of cryst. materials. The measurement has implications in further understanding of diffusional creep, creep cavitation, and sintering in ionic (or partially ionic) solids.
- 63Xie, T.; Grossman, J. C. Crystal Graph Convolutional Neural Networks for an Accurate and Interpretable Prediction of Material Properties. Phys. Rev. Lett. 2018, 120, 145301, DOI: 10.1103/PhysRevLett.120.14530163https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1MXltFSnu7c%253D&md5=93beb5675af86cf95e07c82c136f3511Crystal Graph Convolutional Neural Networks for an Accurate and Interpretable Prediction of Material PropertiesXie, Tian; Grossman, Jeffrey C.Physical Review Letters (2018), 120 (14), 145301CODEN: PRLTAO; ISSN:1079-7114. (American Physical Society)The use of machine learning methods for accelerating the design of cryst. materials usually requires manually constructed feature vectors or complex transformation of atom coordinates to input the crystal structure, which either constrains the model to certain crystal types or makes it difficult to provide chem. insights. Here, we develop a crystal graph convolutional neural networks framework to directly learn material properties from the connection of atoms in the crystal, providing a universal and interpretable representation of cryst. materials. Our method provides a highly accurate prediction of d. functional theory calcd. properties for eight different properties of crystals with various structure types and compns. after being trained with 104 data points. Further, our framework is interpretable because one can ext. the contributions from local chem. environments to global properties. Using an example of perovskites, we show how this information can be utilized to discover empirical rules for materials design.
- 64Jain, A.; Ong, S. P.; Hautier, G.; Chen, W.; Richards, W. D.; Dacek, S.; Cholia, S.; Gunter, D.; Skinner, D.; Ceder, G.; Persson, K. A. The Materials Project: A materials genome approach to accelerating materials innovation. APL Mater. 2013, 1, 011002, DOI: 10.1063/1.481232364https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtlyktLjF&md5=88cb8642abed05e6b34a2191519b3ff3Commentary: The Materials Project: A materials genome approach to accelerating materials innovationJain, Anubhav; Ong, Shyue Ping; Hautier, Geoffroy; Chen, Wei; Richards, William Davidson; Dacek, Stephen; Cholia, Shreyas; Gunter, Dan; Skinner, David; Ceder, Gerbrand; Persson, Kristin A.APL Materials (2013), 1 (1), 011002/1-011002/11CODEN: AMPADS; ISSN:2166-532X. (American Institute of Physics)Accelerating the discovery of advanced materials is essential for human welfare and sustainable, clean energy. In this paper, we introduce the Materials Project (www.materialsproject.org), a core program of the Materials Genome Initiative that uses high-throughput computing to uncover the properties of all known inorg. materials. This open dataset can be accessed through multiple channels for both interactive exploration and data mining. The Materials Project also seeks to create open-source platforms for developing robust, sophisticated materials analyses. Future efforts will enable users to perform rapid-prototyping'' of new materials in silico, and provide researchers with new avenues for cost-effective, data-driven materials design. (c) 2013 American Institute of Physics.
- 65de Jong, M.; Chen, W.; Angsten, T.; Jain, A.; Notestine, R.; Gamst, A.; Sluiter, M.; Krishna Ande, C.; van der Zwaag, S.; Plata, J. J.; Toher, C.; Curtarolo, S.; Ceder, G.; Persson, K. A.; Asta, M. Charting the complete elastic properties of inorganic crystalline compounds. Sci. Data 2015, 2, 150009, DOI: 10.1038/sdata.2015.965https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXoslOku74%253D&md5=0479a0c29355429904fd5fe14ca08cd8Charting the complete elastic properties of inorganic crystalline compoundsde Jong, Maarten; Chen, Wei; Angsten, Thomas; Jain, Anubhav; Notestine, Randy; Gamst, Anthony; Sluiter, Marcel; Krishna Ande, Chaitanya; van der Zwaag, Sybrand; Plata, Jose J.; Toher, Cormac; Curtarolo, Stefano; Ceder, Gerbrand; Persson, Kristin A.; Asta, MarkScientific Data (2015), 2 (), 150009CODEN: SDCABS; ISSN:2052-4463. (Nature Publishing Group)The elastic const. tensor of an inorg. compd. provides a complete description of the response of the material to external stresses in the elastic limit. It thus provides fundamental insight into the nature of the bonding in the material, and it is known to correlate with many mech. properties. Despite the importance of the elastic const. tensor, it has been measured for a very small fraction of all known inorg. compds., a situation that limits the ability of materials scientists to develop new materials with targeted mech. responses. To address this deficiency, we present here the largest database of calcd. elastic properties for inorg. compds. to date. The database currently contains full elastic information for 1,181 inorg. compds., and this no. is growing steadily. The methods used to develop the database are described, as are results of tests that establish the accuracy of the data. In addn., we document the database format and describe the different ways it can be accessed and analyzed in efforts related to materials discovery and design.
- 66Perdew, J. P.; Burke, K.; Ernzerhof, M. Generalized gradient approximation made simple. Phys. Rev. Lett. 1996, 77, 3865, DOI: 10.1103/PhysRevLett.77.386566https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaK28XmsVCgsbs%253D&md5=55943538406ee74f93aabdf882cd4630Generalized gradient approximation made simplePerdew, John P.; Burke, Kieron; Ernzerhof, MatthiasPhysical Review Letters (1996), 77 (18), 3865-3868CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)Generalized gradient approxns. (GGA's) for the exchange-correlation energy improve upon the local spin d. (LSD) description of atoms, mols., and solids. We present a simple derivation of a simple GGA, in which all parameters (other than those in LSD) are fundamental consts. Only general features of the detailed construction underlying the Perdew-Wang 1991 (PW91) GGA are invoked. Improvements over PW91 include an accurate description of the linear response of the uniform electron gas, correct behavior under uniform scaling, and a smoother potential.
- 67Paszke, A.; Gross, S.; Chintala, S.; Chanan, G.; Yang, E.; DeVito, Z.; Lin, Z.; Desmaison, A.; Antiga, L.; Lerer, A. Automatic differentiation in PyTorch , NIPS-W, 2017.There is no corresponding record for this reference.
- 68Tikekar, M. D.; Archer, L. A.; Koch, D. L. Stabilizing electrodeposition in elastic solid electrolytes containing immobilized anions. Sci. Adv. 2016, 2, 1600320, DOI: 10.1126/sciadv.160032068https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC1cXkslKrtLo%253D&md5=63591374b78e8f147b116ede066d3fa7Stabilizing electrodeposition in elastic solid electrolytes containing immobilized anionsTikekar, Mukul D.; Archer, Lynden A.; Koch, Donald L.Science Advances (2016), 2 (7), e1600320/1-e1600320/15CODEN: SACDAF; ISSN:2375-2548. (American Association for the Advancement of Science)Ion transport - driven instabilities in electrodeposition of metals that lead to morphol. instabilities and dendrites are receiving renewed attention because mitigation strategies are needed for improving recharge-ability and safety of lithium batteries. The growth rate of these morphol. instabilities can be slowed by immobilizing a fraction of anions within the electrolyte to reduce the elec. field at the metal electrode. We analyze the role of elastic deformation of the solid electrolyte with immobilized anions and present theory combining the roles of separator elasticity and modified transport to evaluate the factors affecting the stability of planar deposition over a wide range of current densities. We find that stable electrodeposition can be easily achieved even at relatively high current densities in electrolytes/separators with moderate polymer-like mech. moduli, provided a small fraction of anions are immobilized in the separator.
- 69Seino, Y.; Ota, T.; Takada, K.; Hayashi, A.; Tatsumisago, M. A sulphide lithium super ion conductor is superior to liquid ion conductors for use in rechargeable batteries. Energy Environ. Sci. 2014, 7, 627– 631, DOI: 10.1039/C3EE41655K69https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2cXhsFakt7Y%253D&md5=bdd225e1bf4147f70baf646869b2c4f7A sulphide lithium super ion conductor is superior to liquid ion conductors for use in rechargeable batteriesSeino, Yoshikatsu; Ota, Tsuyoshi; Takada, Kazunori; Hayashi, Akitoshi; Tatsumisago, MasahiroEnergy & Environmental Science (2014), 7 (2), 627-631CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)We report that a heat-treated Li2S-P2S5 glass-ceramic conductor has an extremely high ionic cond. of 1.7 × 10-2 S cm-1 and the lowest conduction activation energy of 17 kJ mol-1 at room temp. among lithium-ion conductors reported to date. The optimum conditions of the heat treatment reduce the grain boundary resistance, and the influence of voids, to increase the Li+ ionic cond. of the solid electrolyte so that it is greater than the conductivities of liq. electrolytes, when the transport no. of lithium ions in the inorg. electrolyte is unity.
- 70Li, Y.; Li, Y.; Pei, A.; Yan, K.; Sun, Y.; Wu, C.-L.; Joubert, L.-M.; Chin, R.; Koh, A. L.; Yu, Y.; Perrino, J.; Butz, B.; Chu, S.; Cui, Y. Atomic structure of sensitive battery materials and interfaces revealed by cryo–electron microscopy. Science 2017, 358, 506– 510, DOI: 10.1126/science.aam601470https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhslSgsb7O&md5=313b19162d2034ecf59cdef499b39565Atomic structure of sensitive battery materials and interfaces revealed by cryo-electron microscopyLi, Yuzhang; Li, Yanbin; Pei, Allen; Yan, Kai; Sun, Yongming; Wu, Chun-Lan; Joubert, Lydia-Marie; Chin, Richard; Koh, Ai Leen; Yu, Yi; Perrino, John; Butz, Benjamin; Chu, Steven; Cui, YiScience (Washington, DC, United States) (2017), 358 (6362), 506-510CODEN: SCIEAS; ISSN:0036-8075. (American Association for the Advancement of Science)Whereas std. transmission electron microscopy studies are unable to preserve the native state of chem. reactive and beam-sensitive battery materials after operation, such materials remain pristine at cryogenic conditions. It is then possible to atomically resolve individual Li metal atoms and their interface with the solid electrolyte interphase (SEI). We observe that dendrites in carbonate-based electrolytes grow along the <111> (preferred), <110>, or <211> directions as faceted, single-cryst. nanowires. These growth directions can change at kinks with no observable crystallog. defect. We reveal distinct SEI nanostructures formed in different electrolytes.
- 71Stroh, A. N. Dislocations and Cracks in Anisotropic Elasticity. Philos. Mag. 1958, 3, 625– 646, DOI: 10.1080/1478643580856580471https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaG1MXitV2ltQ%253D%253D&md5=4195bf838814988673bec6632a6b1dc8Dislocations and cracks in anisotropic elasticityStroh, A. N.Philosophical Magazine (1798-1977) (1958), 3 (), 625-46CODEN: PHMAA4; ISSN:0031-8086.The solution of the elastic equations is considered for the case in which the state of the solid is independent of 1 of the 3 Cartesian co.ovrddot.ordinates. The stresses due to a dislocation, a wall of parallel dislocations, and a crack in an arbitrary nonuniform stress field are obtained. The results hold for the most general anisotropy in which no symmetry elements of the crystal are assumed.
- 72Stroh, A. N. Steady State Problems in Anisotropic Elasticity. J. Math. Phys. 1962, 41, 77– 103, DOI: 10.1002/sapm196241177There is no corresponding record for this reference.
- 73Hall, S. R.; Allen, F. H.; Brown, I. D. The crystallographic information file (CIF): a new standard archive file for crystallography. Acta Crystallogr., Sect. A: Found. Crystallogr. 1991, 47, 655– 685, DOI: 10.1107/S010876739101067XThere is no corresponding record for this reference.
- 74Mouhat, F.; Coudert, F. m. c.-X. Necessary and sufficient elastic stability conditions in various crystal systems. Phys. Rev. B: Condens. Matter Mater. Phys. 2014, 90, 224104, DOI: 10.1103/PhysRevB.90.22410474https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXivVGkur0%253D&md5=d8f5d43f831b6e45962e567bee94a008Necessary and sufficient elastic stability conditions in various crystal systemsMouhat, Felix; Coudert, Francois-XavierPhysical Review B: Condensed Matter and Materials Physics (2014), 90 (22), 224104/1-224104/4, 4 pp.CODEN: PRBMDO; ISSN:1098-0121. (American Physical Society)While the Born elastic stability criteria are well known for cubic crystals, there is some confusion in the literature about the form they should take for lower-symmetry crystal classes. Here we present closed form necessary and sufficient conditions for elastic stability in all crystal classes, as a concise and pedagogical ref. to stability criteria in noncubic materials.
- 75Ahmad, Z.; Viswanathan, V. Quantification of uncertainty in first-principles predicted mechanical properties of solids: Application to solid ion conductors. Phys. Rev. B: Condens. Matter Mater. Phys. 2016, 94, 064105, DOI: 10.1103/PhysRevB.94.064105There is no corresponding record for this reference.
- 76Friedman, J. H. Greedy Function Approximation: A Gradient Boosting Machine. Ann. Stat. 2001, 29, 1189– 1232, DOI: 10.1214/aos/1013203451There is no corresponding record for this reference.
- 77Friedman, J. H.; Hastie, T.; Tibshirani, R. The elements of statistical learning; Springer series in statistics: New York, 2001; Vol. 1.There is no corresponding record for this reference.
- 78Freund, Y.; Schapire, R. E. A Decision-Theoretic Generalization of On-Line Learning and an Application to Boosting. J. Comput. Syst. Sci. 1997, 55, 119– 139, DOI: 10.1006/jcss.1997.1504There is no corresponding record for this reference.
- 79Drucker, H. Improving Regressors Using Boosting Techniques , Proceedings of the Fourteenth International Conference on Machine Learning, San Francisco, CA, United States, 1997; pp 107– 115.There is no corresponding record for this reference.
- 80Smola, A. J.; Schülkopf, B. A tutorial on support vector regression. Statistics and Computing 2004, 14, 199– 222, DOI: 10.1023/B:STCO.0000035301.49549.88There is no corresponding record for this reference.
- 81MacKay, D. J. C. Bayesian Interpolation. Neural Comput. 1992, 4, 415– 447, DOI: 10.1162/neco.1992.4.3.415There is no corresponding record for this reference.
- 82Pedregosa, F. Scikit-learn: Machine Learning in Python. J. Mach. Learn. Res. 2011, 12, 2825– 2830There is no corresponding record for this reference.
- 83Deng, Z.; Wang, Z.; Chu, I.-H.; Luo, J.; Ong, S. P. Elastic Properties of Alkali Superionic Conductor Electrolytes from First Principles Calculations. J. Electrochem. Soc. 2016, 163, A67– A74, DOI: 10.1149/2.0061602jes83https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhvFylurvI&md5=b8172c27880503a159ab9fe8a1a7c6c3Elastic Properties of Alkali Superionic Conductor Electrolytes from First Principles CalculationsDeng, Zhi; Wang, Zhenbin; Chu, Iek-Heng; Luo, Jian; Ong, Shyue PingJournal of the Electrochemical Society (2016), 163 (2), A67-A74CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)In this work, we present a comprehensive investigation of the elastic properties (the full elastic tensor, bulk, shear and Young's moduli, and Poisson's ratio) of 23 well-known ceramic alkali superionic conductor electrolytes (SICEs) using first principles calcns. We find that the computed elastic moduli are in good agreement with exptl. data (wherever available) and chem. bonding nature. The anion species and structural framework have a significant influence on the elastic properties, and the relative elastic moduli of the various classes of SICEs follow the order thiophosphate < antiperovskite < phosphate < NASICON < garnet < perovskite. Within the same framework structure, we observe that Na SICEs are softer than their Li analogs. We discuss the implications of these findings in the context of fabrication, battery operation, and enabling a Li metal anode. The data computed in this work will also serve as a useful ref. for future expts. as well as theor. modeling of SICEs for rechargeable alkali-ion batteries.
- 84Ranganathan, S. I.; Ostoja-Starzewski, M. Universal Elastic Anisotropy Index. Phys. Rev. Lett. 2008, 101, 055504, DOI: 10.1103/PhysRevLett.101.05550484https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1cXhtVSju7nN&md5=40a1e4eb5d42153f25575b60665ccab9Universal elastic anisotropy indexRanganathan, Shivakumar I.; Ostoja-Starzewski, MartinPhysical Review Letters (2008), 101 (5), 055504/1-055504/4CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)Practically all elastic single crystals are anisotropic, which calls for an appropriate universal measure to quantify the extent of anisotropy. A review of the existing anisotropy measures in the literature leads to a conclusion that they lack universality in the sense that they are nonunique and ignore contributions from the bulk part of the elastic stiffness (or compliance) tensor. Proceeding from extremal principles of elasticity, the authors introduce a new universal anisotropy index that overcomes the above limitations. Also, the authors establish special relations between the proposed anisotropy index and the existing anisotropy measures for special cases. A new elastic anisotropy diagram is constructed for over 100 different crystals (from cubic through triclinic), demonstrating that the proposed anisotropy measure is applicable to all types of elastic single crystals, and thus fills an important void in the existing literature.
- 85Lu, Z.; Ciucci, F. Metal Borohydrides as Electrolytes for Solid-State Li, Na, Mg, and Ca Batteries: A First-Principles Study. Chem. Mater. 2017, 29, 9308– 9319, DOI: 10.1021/acs.chemmater.7b0328485https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXhs1Sks77I&md5=4f24aceeeec626b708e8a2546488d8c9Metal Borohydrides as Electrolytes for Solid-State Li, Na, Mg, and Ca Batteries: A First-Principles StudyLu, Ziheng; Ciucci, FrancescoChemistry of Materials (2017), 29 (21), 9308-9319CODEN: CMATEX; ISSN:0897-4756. (American Chemical Society)Metal borohydrides are a family of materials that were recently discovered to have extraordinary ionic conductivities, making them promising candidates as electrolytes for solid-state batteries (SSBs). In fact, various groups have measured the ionic conductivities and assembled batteries using specific borohydrides. However, there are no comprehensive studies assessing the thermodn. properties or discussing the suitability of metal borohydrides as electrolytes in SSBs, esp. for beyond-lithium applications. In this work, we investigate the electrochem. stability, interfacial characteristics, mech. properties, and ionic conductivities of Li, Na, Ca, and Mg borohydrides using first-principles calcns. Our results suggest that Li and Na borohydrides are unstable at high voltages. However, the corresponding decompn. products, i.e., B12H122--contg. phases, have wide electrochem. windows which protect the electrolyte, leading to large electrochem. windows as wide as 5 V. In addn., our simulations indicate that metal borohydrides are ductile, suggesting facile processing. However, their low shear moduli may result in metal dendrite formation. For Ca and Mg borohydrides, while they possess reasonably good electrochem. stability, the low cationic diffusivity may impede their practical use. Finally, the anion rotation barrier was shown to correlate with the superionic phase transition temp., suggesting that anion mixing may be a potential approach to achieve room-temp. superionic cond.
- 86Varley, J. B.; Kweon, K.; Mehta, P.; Shea, P.; Heo, T. W.; Udovic, T. J.; Stavila, V.; Wood, B. C. Understanding Ionic Conductivity Trends in Polyborane Solid Electrolytes from Ab Initio Molecular Dynamics. ACS Energy Lett. 2017, 2, 250– 255, DOI: 10.1021/acsenergylett.6b0062086https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28XitFektb3P&md5=10bc784c32c1869968e8c1ae8ab49401Understanding Ionic Conductivity Trends in Polyborane Solid Electrolytes from Ab Initio Molecular DynamicsVarley, Joel B.; Kweon, Kyoung; Mehta, Prateek; Shea, Patrick; Heo, Tae Wook; Udovic, Terrence J.; Stavila, Vitalie; Wood, Brandon C.ACS Energy Letters (2017), 2 (1), 250-255CODEN: AELCCP; ISSN:2380-8195. (American Chemical Society)Polyborane salts based on B12H122-, B10H102-, CB11H12-, and CB9H10- demonstrate high Li and Na superionic cond. that makes them attractive as electrolytes in all-solid-state batteries. Their chem. and structural diversity creates a versatile design space that could be used to optimize materials with higher cond. at lower temps.; however, many mechanistic details remain enigmatic, including reasons why certain known modifications lead to improved performance. We use extensive ab initio mol. dynamics simulations to explore the dependence of ionic cond. on cation/anion pair combinations for Li and Na polyborane salts. Further simulations are used to probe the influence of local modifications to chem., stoichiometry, and compn. Carbon doping, anion alloying, and cation off-stoichiometry are found to favorably introduce intrinsic disorder, facilitating local deviation from the expected cation population. Lattice expansion likewise has a pos. effect by aiding anion reorientations that are crit. for conduction. Implications for engineering polyboranes for improved ionic cond. are discussed.
- 87Tang, W. S.; Matsuo, M.; Wu, H.; Stavila, V.; Zhou, W.; Talin, A. A.; Soloninin, A. V.; Skoryunov, R. V.; Babanova, O. A.; Skripov, A. V.; Unemoto, A.; Orimo, S.; Udovic, T. J. Liquid-Like Ionic Conduction in Solid Lithium and Sodium Monocarba-closo-Decaborates Near or at Room Temperature. Adv. Energy Mater. 2016, 6, 1502237, DOI: 10.1002/aenm.201502237There is no corresponding record for this reference.
- 88Tang, W. S.; Unemoto, A.; Zhou, W.; Stavila, V.; Matsuo, M.; Wu, H.; Orimo, S.-i.; Udovic, T. J. Unparalleled lithium and sodium superionic conduction in solid electrolytes with large monovalent cage-like anions. Energy Environ. Sci. 2015, 8, 3637– 3645, DOI: 10.1039/C5EE02941D88https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2MXhs1amsr%252FL&md5=6ce33938ab3579da7ee531eb41f73964Unparalleled lithium and sodium superionic conduction in solid electrolytes with large monovalent cage-like anionsTang, Wan Si; Unemoto, Atsushi; Zhou, Wei; Stavila, Vitalie; Matsuo, Motoaki; Wu, Hui; Orimo, Shin-ichi; Udovic, Terrence J.Energy & Environmental Science (2015), 8 (12), 3637-3645CODEN: EESNBY; ISSN:1754-5706. (Royal Society of Chemistry)Solid electrolytes with sufficiently high conductivities and stabilities are the elusive answer to the inherent shortcomings of org. liq. electrolytes prevalent in today's rechargeable batteries. We recently revealed a novel fast-ion-conducting sodium salt, Na2B12H12, which contains large, icosahedral, divalent B12H122- anions that enable impressive superionic cond., albeit only above its 529 K phase transition. Its lithium congener, Li2B12H12, possesses an even more technol. prohibitive transition temp. above 600 K. Here we show that the chem. related LiCB11H12 and NaCB11H12 salts, which contain icosahedral, monovalent CB11H12- anions, both exhibit much lower transition temps. near 400 K and 380 K, resp., and truly stellar ionic conductivities (>0.1 S cm-1) unmatched by any other known polycryst. materials at these temps. With proper modifications, we are confident that room-temp.-stabilized superionic salts incorporating such large polyhedral anion building blocks are attainable, thus enhancing their future prospects as practical electrolyte materials in next-generation, all-solid-state batteries.
- 89Malmgren, S.; Ciosek, K.; Lindblad, R.; Plogmaker, S.; Kühn, J.; Rensmo, H.; Edström, K.; Hahlin, M. Consequences of air exposure on the lithiated graphite SEI. Electrochim. Acta 2013, 105, 83– 91, DOI: 10.1016/j.electacta.2013.04.11889https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC3sXhtVehsbvE&md5=6475c40a670e813d2a8de45c21003e64Consequences of air exposure on the lithiated graphite SEIMalmgren, Sara; Ciosek, Katarzyna; Lindblad, Rebecka; Plogmaker, Stefan; Kuhn, Julius; Rensmo, Haakan; Edstroem, Kristina; Hahlin, MariaElectrochimica Acta (2013), 105 (), 83-91CODEN: ELCAAV; ISSN:0013-4686. (Elsevier Ltd.)Consequences of air exposure on the surface compn. of one of the most reactive Li-ion battery components, the lithiated graphite, was studied using 280-835 eV soft XPS (SOXPES) as well as 1486.7 eV XPS (∼2 and ∼10 nm probing depth, resp.). Different depth regions of the solid electrolyte interphase (SEI) of graphite cycled vs. LiFePO4 were thereby examd. Also, the air sensitivity of samples subject to four different combinations of pre-treatments (washed/unwashed and exposed to air before or after vacuum treatment) was explored. The samples showed important changes after exposure to air, which are largely dependent on sample pre-treatment. Changes after exposure of unwashed samples exposed before vacuum treatment were attributed to reactions involving volatile species. On washed, air exposed samples, as well as unwashed samples exposed after vacuum treatment, effects attributed to LiOH formation in the innermost SEI were obsd. and suggested to be assocd. with partial delithiation of the surface region of the lithiated graphite electrode. Also, effects that can be attributed to LiPF6 decompn. were obsd. However, these effects were less pronounced than those attributed to reactions involving solvent species and the lithiated graphite.
- 90Tasaki, K.; Goldberg, A.; Lian, J.-J.; Walker, M.; Timmons, A.; Harris, S. Solubility of Lithium Salts Formed on the Lithium-Ion Battery Negative Electrode Surface in Organic Solvents. J. Electrochem. Soc. 2009, 156, A1019– A1027, DOI: 10.1149/1.323985090https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1MXhtlCmsbzN&md5=433ac8ee99379a475c1e174d35423704Solubility of Lithium Salts Formed on the Lithium-Ion Battery Negative Electrode Surface in Organic SolventsTasaki, Ken; Goldberg, Alex; Lian, Jian-Jie; Walker, Merry; Timmons, Adam; Harris, Stephen J.Journal of the Electrochemical Society (2009), 156 (12), A1019-A1027CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)The soly. of lithium salts in di-Me carbonate (DMC) found in solid electrolyte interface films was detd. The salt-DMC solns. were evapd., and the salts were transferred into water for ion cond. measurements. The salts examd. included Li2CO3, lithium oxalate [(LiCO2)2], LiF, LiOH, lithium Me carbonate (LiOCO2CH3), and lithium Et carbonate (LiOCO2C2H5). The salt molarity in DMC ranged from 9.6 × 10-4 mol/L (LiOCO2CH3) to 9 × 10-5 mol/L (Li2CO3) in the order of LiOCO2CH3 > LiOCO2C2H5 > LiOH > LiF > (LiCO2)2 > Li2CO3. XPS measurements on solid electrolyte interface films on the surface of the anode taken from a com. battery after soaking in DMC for 1 h suggested that the films can dissolve. Sep., the heat of dissoln. of the salts was calcd. from computer simulations for the same salts, including Li2O, lithium methoxide (LiOCH3), and dilithium ethylene glycol dicarbonate [(CH2OCO2Li)2:LiEDC] in both DMC and ethylene carbonate. The results from the computer simulations suggested that the order in which the salt was likely to dissolve in both DMC and ethylene carbonate was LiEDC > LiOCO2CH3 > LiOH > LiOCO2C2H5 > LiOCH3 > LiF > (LiCO2)2 > Li2CO3 > Li2O. This order agreed with the expt. in DMC within the exptl. error. Both expt. and computer simulations showed that the org. salts are more likely to dissolve in DMC than the inorg. salts. The calcns. also predicted that the salts dissolve more likely in ethylene carbonate than in DMC, in general. Moreover, the results from the study were used to discuss the capacity fading mechanism during the storage of lithium-ion batteries.
- 91Matsuo, M.; Nakamori, Y.; ichi Orimo, S.; Maekawa, H.; Takamura, H. Lithium superionic conduction in lithium borohydride accompanied by structural transition. Appl. Phys. Lett. 2007, 91, 224103, DOI: 10.1063/1.281793491https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD2sXhsVequ7zJ&md5=8949f5d9d2da1f61bf6ad230dac90749Lithium superionic conduction in lithium borohydride accompanied by structural transitionMatsuo, Motoaki; Nakamori, Yuko; Orimo, Shin-ichi; Maekawa, Hideki; Takamura, HitoshiApplied Physics Letters (2007), 91 (22), 224103/1-224103/3CODEN: APPLAB; ISSN:0003-6951. (American Institute of Physics)The elec. cond. of LiBH4 measured by a.c. complex impedance increased by 3 orders of magnitude due to structural transition from orthorhombic to hexagonal at ∼390 K. The hexagonal phase exhibited a high elec. cond. of about 10-3 S/cm. The cond. calcd. from the Nernst-Einstein equation using the correlation time obtained from 7Li NMR agreed with the measured elec. cond. The elec. cond. in the hexagonal phase is due to Li superionic conduction.
- 92Johnson, R.; Biefeld, R.; Keck, J. Ionic conductivity in Li5AlO4 and LiOH. Mater. Res. Bull. 1977, 12, 577– 587, DOI: 10.1016/0025-5408(77)90066-692https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADyaE2sXkslKqs7k%253D&md5=49b9b53cd2c56638c6e2539226cf0764Ionic conductivity in lithium aluminum oxide (Li5AlO4) and lithium hydroxideJohnson, R. T., Jr.; Biefeld, R. M.; Keck, J. D.Materials Research Bulletin (1977), 12 (6), 577-87CODEN: MRBUAC; ISSN:0025-5408.The ionic cond. and thermal properties of Li5AlO4 and LiOH were measured in wet and dry environments. An endothehrmic reaction at ∼415°C and an assocd. large increase in cond. were obsd. both in Li5AlO4, in wet environment, and in LiOH. The large cond. increase in Li5AlO4 results from LiOH retained within the material. The reaction(s) for formation of LiOH within Li5AlO4 ad the assocd. elec. changes appear to be reversible as the environment switches from wet to dry at high temps. There is a significant (>1%) electronic contribution to the cond. in these materials.
- 93Maekawa, H.; Matsuo, M.; Takamura, H.; Ando, M.; Noda, Y.; Karahashi, T.; Orimo, S.-i. Halide-Stabilized LiBH4, a Room-Temperature Lithium Fast-Ion Conductor. J. Am. Chem. Soc. 2009, 131, 894– 895, DOI: 10.1021/ja807392k93https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1MXisValtQ%253D%253D&md5=7602a4b2a0f259ac649e6ce4dfe8e53bHalide-Stabilized LiBH4, a Room-Temperature Lithium Fast-Ion ConductorMaekawa, Hideki; Matsuo, Motoaki; Takamura, Hitoshi; Ando, Mariko; Noda, Yasuto; Karahashi, Taiki; Orimo, Shin-ichiJournal of the American Chemical Society (2009), 131 (3), 894-895CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)A review on development of lithium superionic conductors based on LiBH4 and lithium halides. Using these compds., room-temp. high lithium ion cond. was imparted to a hydride system that had not been considered a lithium ion electrolyte. The electrochem. measurements showed a great advantage of this material as an extremely lightwt. lithium electrolyte for high energy d. batteries. Versatile properties of these materials make them suitable for use in all-solid-state batteries.
- 94Das, S.; Ngene, P.; Norby, P.; Vegge, T.; de Jongh, P. E.; Blanchard, D. All-Solid-State Lithium-Sulfur Battery Based on a Nanoconfined LiBH4 Electrolyte. J. Electrochem. Soc. 2016, 163, A2029– A2034, DOI: 10.1149/2.0771609jes94https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC28Xht1Krsr%252FP&md5=ee1106f5cdf799cd3505e1078501696fAll-Solid-State Lithium-Sulfur Battery Based on a Nanoconfined LiBH4 ElectrolyteDas, Supti; Ngene, Peter; Norby, Poul; Vegge, Tejs; de Jongh, Petra E.; Blanchard, DidierJournal of the Electrochemical Society (2016), 163 (9), A2029-A2034CODEN: JESOAN; ISSN:0013-4651. (Electrochemical Society)In this work we characterize all-solid-state lithium-sulfur batteries based on nano-confined LiBH4 in mesoporous silica as solid electrolytes. The nano-confined LiBH4 has fast ionic lithium cond. at room temp., 0.1 mScm-1, negligible electronic cond. and its cationic transport no. (t+ = 0.96), close to unity, demonstrates a purely cationic conductor. The electrolyte has an excellent stability against lithium metal. The behavior of the batteries is studied by cyclic voltammetry and repeated charge/discharge cycles in galvanostatic conditions. The batteries show good performance, delivering high capacities vs. sulfur mass, typically 1220 mAhg-1 after 40 cycles at moderate temp. (55°), 0.03 C rates and working voltage of 2 V.
- 95Morales-García, A.; Valero, R.; Illas, F. An Empirical, yet Practical Way To Predict the Band Gap in Solids by Using Density Functional Band Structure Calculations. J. Phys. Chem. C 2017, 121, 18862– 18866, DOI: 10.1021/acs.jpcc.7b0742195https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXht12mtLnE&md5=b0a676344af3832e6ff75461b9232229An empirical, yet practical way to predict the band gap in solids by using density functional band structure calculationsMorales-Garcia, Angel; Valero, Rosendo; Illas, FrancescJournal of Physical Chemistry C (2017), 121 (34), 18862-18866CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)Band structure calcns. based on d. functional theory (DFT) with local or gradient-cor. exchange-correlation potentials are known to severely underestimate the band gap of semiconducting and insulating materials. Alternative approaches have been proposed: from semiempirical setups, such as the so-called DFT+U, to hybrid d. functionals using a fraction of nonlocal Fock exchange, to modifications of semilocal d. functionals. However, the resulting methods appear to be material dependent and lack theor. rigor. The rigorous many-body perturbation theory based on GW methods provides accurate results but at a very high computational cost. Hereby, we show that a linear correlation between the electronic band gaps obtained from std. DFT and GW approaches exists for most materials and argue that (1) this is a strong indication that the problem of predicting band gaps from std. DFT calcn. arises from the assignment of a phys. meaning to the Kohn-Sham energy levels rather than from intrinsic errors of the DFT methods and (2) it provides a practical way to obtain GW-like quality results from std. DFT calcns. The latter will be esp. useful for systems where the unit cell involves a large no. of atoms as in the case of doped or defect-contg. materials for which GW calcns. become unfeasible.
- 96Towns, J.; Cockerill, T.; Dahan, M.; Foster, I.; Gaither, K.; Grimshaw, A.; Hazlewood, V.; Lathrop, S.; Lifka, D.; Peterson, G. D.; Roskies, R.; Scott, J. R.; Wilkins-Diehr, N. XSEDE: Accelerating Scientific Discovery. Comput. Sci. Eng. 2014, 16, 62– 74, DOI: 10.1109/MCSE.2014.80There is no corresponding record for this reference.
- 97Nystrom, N. A.; Levine, M. J.; Roskies, R. Z.; Scott, J. R. Bridges: A Uniquely Flexible HPC Resource for New Communities and Data Analytics. Proceedings of the 2015 XSEDE Conference: Scientific Achievements Enabled by Enhanced Cyberinfrastructure 2015, 1– 8, DOI: 10.1145/2792745.2792775There is no corresponding record for this reference.
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Details of machine-learning models and additional figures including schematics and visualizations, shear modulus values, and stability parameter values (PDF)
Anisotropic stability parameter for training data (XLSX)
Shear modulus of 60 648 compounds predicted using CGCNN (XLSX)
Anisotropic stability parameter for predicted data (XLSX)
Bulk modulus of 60 648 compounds predicted using CGCNN (XLSX)
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