Long-Term Stable Organic Solar Cells through Amphiphilic AdditivesClick to copy article linkArticle link copied!
- Yisak Tsegazab GeraseYisak Tsegazab GeraseLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyInstitute of Physical Chemistry, Friedrich Schiller University Jena, Helmholtzweg 4, 07743 Jena, GermanyMore by Yisak Tsegazab Gerase
- Javier Garcia LopezJavier Garcia LopezInstitute of Organic Chemistry and Macromolecular Chemistry, Friedrich Schiller University Jena, Lessing Str. 8, 07743 Jena, GermanyMore by Javier Garcia Lopez
- Jose Prince MadalaimuthuJose Prince MadalaimuthuInstitute of Organic Chemistry and Macromolecular Chemistry, Friedrich Schiller University Jena, Lessing Str. 8, 07743 Jena, GermanyCenter for Energy and Environmental Chemistry Jena (CEEC Jena) Friedrich-Schiller University Jena, Philosophenweg 7a, 07743 Jena, GermanyMore by Jose Prince Madalaimuthu
- Anna ElmanovaAnna ElmanovaLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyInstitute of Physical Chemistry, Friedrich Schiller University Jena, Helmholtzweg 4, 07743 Jena, GermanySciclus GmbH & Co. KG, Moritz-von-Rohr-Str. 1a, 07745 Jena, GermanyMore by Anna Elmanova
- Sarah Jasmin FinkelmeyerSarah Jasmin FinkelmeyerLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyInstitute of Physical Chemistry, Friedrich Schiller University Jena, Helmholtzweg 4, 07743 Jena, GermanyMore by Sarah Jasmin Finkelmeyer
- Andrea DellithAndrea DellithLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyMore by Andrea Dellith
- Daniel BlaschkeDaniel BlaschkeLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyMore by Daniel Blaschke
- Heidemarie SchmidtHeidemarie SchmidtLeibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyMore by Heidemarie Schmidt
- Kalina PenevaKalina PenevaInstitute of Organic Chemistry and Macromolecular Chemistry, Friedrich Schiller University Jena, Lessing Str. 8, 07743 Jena, GermanyCenter for Energy and Environmental Chemistry Jena (CEEC Jena) Friedrich-Schiller University Jena, Philosophenweg 7a, 07743 Jena, GermanyJena Center of Soft Matter, Friedrich Schiller University Jena, Philosophenweg 7, 07743 Jena, GermanyMore by Kalina Peneva
- Harald HoppeHarald HoppeInstitute of Organic Chemistry and Macromolecular Chemistry, Friedrich Schiller University Jena, Lessing Str. 8, 07743 Jena, GermanyCenter for Energy and Environmental Chemistry Jena (CEEC Jena) Friedrich-Schiller University Jena, Philosophenweg 7a, 07743 Jena, GermanyMore by Harald Hoppe
- Martin Presselt*Martin Presselt*Email: [email protected]Leibniz Institute of Photonic Technology (IPHT), Albert-Einstein-Str. 9, 07745 Jena, GermanyCenter for Energy and Environmental Chemistry Jena (CEEC Jena) Friedrich-Schiller University Jena, Philosophenweg 7a, 07743 Jena, GermanySciclus GmbH & Co. KG, Moritz-von-Rohr-Str. 1a, 07745 Jena, GermanyMore by Martin Presselt
Abstract
Organic solar cells have recently experienced tremendous efficiency improvements, but their longevity is still limited by morphological degradation, among other factors. We demonstrate in this work that small amounts of amphiphilic small molecules such as perylene monoimide-diamine (PMIDA-C12) admixed to the active layer can dramatically improve the longevity of classical polymer solar cells (P3HT:PC60BM). While fill factors and efficiencies of classical reference solar cells without amphiphile dropped to 35 and 4% of their original values after 588 h of artificial aging (at 80 °C), respectively, these values are stable at 80% of their initial values for the solar cells containing 0.01 wt % PMIDA-C12. Spectroscopic and atomic force microscopy studies indicate that the amphiphiles stabilize the morphology of the active layers. Hence, the presented approach of doping the active layer with an amphiphilic molecule appears to be promising for improving the long-term stability of organic solar cells.
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Attribution (BY): Credit must be given to the creator.
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Introduction
Figure 1
Figure 1. Panel (A) Lewis structure and solvent-accessible surfaces (with solvent radius 1.4 Å, corresponding to water molecule radius) with electrostatic potentials of active layer materials (P3HT:PC60BM) and additive (PMIDA-C12). Panel (B) HOMO (highest occupied molecular orbital) and LUMO (lowest unoccupied molecular orbital) or rather valence and conduction band energies (eV) vs vacuum energy of the materials used for this study; references: (a) Bishnoi et al. (3) Adv. Mater. Interfaces 2022, (b) derived from square wave voltammetry investigation as detailed in the Supporting Information, and (c) Mumyatov et al. (39) J. Mater. Chem. C 2015. Panel (C) Schematic of a classical BHJ solar cell. Interfaces that are potentially stabilized via the amphiphiles are shown in sections CI–CIII, and color codes are in accordance with panel (B).
Results and Discussion
Solar Cell Performance
Figure 2
Figure 2. Current density–voltage (J–V) curves of PMIDA-C12 doped and undoped P3HT:PC60BM (3:2) solar cells, annealed at 80 °C for 10 min. Panel (A) illuminated with AM 1.5; panel (B) dark.
wt % PMIDA-C12 | JSC (mA/cm2) | VOC (mV) | FF | RS (Ω) | RP (Ω) | PCE (%) | ||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
best | Ø + SD | best | Ø + SD | best | Ø + SD | best | Ø + SD | best | Ø + SD | best | Ø + SD | |
0.000 | 8.1 | 7.1 ± 1.2 | 432 | 435.6 ± 3.2 | 39 | 39.0 ± 1.2 | 36 | 42.6 ± 6.5 | 420 | 445 ± 30 | 1.35 | 1.35 ± 0.05 |
0.010 | 8.9 | 9.0 ± 0.2 | 440 | 431.9 ± 8.9 | 42 | 40.5 ± 1.9 | 38 | 33.3 ± 2.3 | 601 | 488 ± 96 | 1.67 | 1.6 (±0.1) |
0.015 | 8.6 | 8.8 ± 0.3 | 422 | 431.8 ± 16 | 47 | 42.3 ± 2.3 | 24 | 33.9 ± 7.0 | 774 | 531 ± 115 | 1.69 | 1.6 (±0.1) |
0.020 | 8.3 | 8.5 ± 0.3 | 443 | 430.8 ± 10 | 47 | 44.8 ± 1.5 | 30 | 37.9 ± 7.9 | 664 | 563 ± 90 | 1.75 | 1.6 (±0.1) |
0.025 | 8.8 | 8.5 ± 0.3 | 435 | 430.0 ± 22 | 45 | 43.3 ± 3.3 | 45 | 42.6 ± 12.0 | 625 | 600 ± 160 | 1.71 | 1.6 (±0.2) |
Annealed at 80 °C for 10 min. The values of the best performing cells and the averages of 8 cells including standard deviation are given.
Figure 3
Figure 3. J–V plot of P3HT:PC60BM (30 mg/mL (3:2) blend) conventional solar cell with and without the PMIDA-C12 additive, post annealing at 160 °C for 5 min. Panel (A) under illumination (AM 1.5) and panel (B) in the dark.
wt % PMIDA-C12 | JSC (mA/cm2) | VOC (mV) | FF | RS (Ω) | RP (Ω) | PCE (%) | ||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
best | Ø ± SD | best | Ø ± SD | best | Ø ± SD | best | Ø ± SD | best | Ø ± SD | best | Ø ± SD | |
0.000 | 9.77 | 9.64 ± 0.12 | 560 | 560 ± 10 | 49 | 48.3 ± 0.47 | 12 | 12.6 ± 0.57 | 992 | 1012 ± 166 | 2.65 | 2.60 ± 0.05 |
0.005 | 9.66 | 9.38 ± 0.21 | 540 | 530 ± 10 | 51 | 49.3 ± 1.7 | 10 | 10 ± 0.82 | 915 | 644 ± 432 | 2.65 | 2.44 ± 0.22 |
0.010 | 10.0 | 9.56 ± 0.28 | 550 | 550 ± 10 | 48 | 49.8 ± 1.1 | 9 | 10 ± 0.82 | 870 | 950 ± 94 | 2.67 | 2.61 ± 0.05 |
The values of the best performing cell and the averages of eight cells including standard deviation are given.
Thermal Stability under Continuous Annealing at 80 °C
Figure 4
Figure 4. Thermal stability of the photovoltaic parameters of a P3HT:PC60BM blend with and without the PMIDA-C12 additive during thermal aging (80 °C) in a nitrogen-filled glovebox. Averages and uncertainties are calculated from four cells. Panel (A) short-circuit current density, panel (B) open-circuit voltage, panel (C) fill factor, and panel (D) power conversion efficiency.
UV–Vis Absorption Analysis
Figure 5
Figure 5. Normalized absorption spectra of the P3HT:PC60BM films with and without the PMIDA-C12 additive as fabricated. Panel (A) 0 h and panel (B) 588 h of thermal aging (80 °C).
Figure 6
Figure 6. Panel (A) shows the vibrational progression in the UV–vis absorption spectrum of a P3HT:PC60BM film is modeled via Huang–Rhys coupled Gaussian functions. For details, see the Supporting Information. The model is fitted to the experimental data from 1.74 to 2.29 eV, while the area under the fitted curve (crystalline P3HT) and the difference from the experimental spectrum (amorphous P3HT) are evaluated in the range from 1.8 to 3.0 eV. The spectrum of a PC60BM film is shown for comparison. Panel (B) shows the ratio of crystalline to amorphous P3HT (areas under the respective curves) versus amphiphile concentration at different thermal aging times.
Photoluminescence Analysis
Figure 7
Figure 7. PL spectra of P3HT:PC60BM (3:2 BHJ) film with and without the PMIDA-C12 additive at different thermal aging (80 °C) times; panel (A) 0 h, panel (B) 450 h, and panel (C) 588 h. PL data are normalized to the maximum of 0.010 wt % of additive which is relatively constant.
Atomic Force Microscopy Analysis
Figure 8
Figure 8. AFM topography and phase images (2.5 μm × 2.5 μm) of P3HT:PC60BM (3:2 BHJ) films and respective height histograms of the different topographies. Row (A) 0.000 wt % PMIDA-C12; row (B) 0.005 wt % PMIDA-C12; row (C) 0.010 wt % PMIDA-C12. Thermal aging was carried out at 80 °C for 0, 450, and 588 h.
Conclusions
Experimental Details
Materials
Solar Cell Fabrication
IV Measurement
UV–Vis Absorption and Fluorescence Spectroscopy
Atomic Force Microscopy
Electrochemical Measurements
Quantum Chemical Calculations
Supporting Information
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acsaelm.3c01722.
Comparison of J–V plots for different concentrations of PMIDA-C12 additive, details of vibrational progression fittings of UV–vis absorption spectra, UV–vis and PL spectra of pristine P3HT and PC60BM films, comparison of photothermal deflection spectra of fresh and thermally aged films, and SWV analysis of PMIDA-C12 additive and details of the synthesis procedure of PMIDA-C12 additive molecule (PDF)
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
Yisak T. Gerase acknowledges the funding from DAAD (Deutscher Akademischer Austauschdienst), funding program/-ID: 5750787. The German Research Foundation (DFG, Deutsche Forschungsgemeinschaft) is gratefully acknowledged for the support of this work in the Collaborative Research Center (CRC) “CataLight” (Transregio SFB TRR 234, Project number 364549901, projects A3, B9). K.P. also acknowledges the financial support of the DFG for the support of this work (Project number 455748945). The authors further acknowledge the DFG for funding in the framework of FOR5301 “FuncHeal” (projects P3 and P4). We would like to acknowledge the NMR platform at the Friedrich Schiller University Jena for support in NMR spectroscopy.
References
This article references 69 other publications.
- 1Berger, P. R.; Kim, M. Polymer Solar Cells: P3ht:Pcbm and Beyond. J. Renewable Sustainable Energy 2018, 10 (1), 013508, DOI: 10.1063/1.5012992Google Scholar1Polymer solar cells: P3HT:PCBM and beyondBerger, P. R.; Kim, M.Journal of Renewable and Sustainable Energy (2018), 10 (1), 013508/1-013508/26CODEN: JRSEBH; ISSN:1941-7012. (American Institute of Physics)A review. For the last two decades, polymer solar cells (PSCs) have been a cynosure of the photovoltaic community, as evidenced by the growing no. of patent applications and scientific publications. Efforts to achieve high power conversion efficiency in PSC, propelled by advances in device architecture, material combination, and nanomorphol. control, evolved into poly(3-hexylthiophene-2,5-diyl) (P3HT):phenyl-C61-Butyric-Acid-Me Ester (PCBM) bulk heterojunction PSCs, which had been the best seller in PSC research for a decade. Subsequently, PSC research was redirected towards the synthesis of low bandgap materials and optimization of tandem cells, which led to a power conversion efficiency of ∼13%. Even though this efficiency may not be sufficient enough to compete with that of inorg. solar cells, unique properties of PSCs, such as mass roll-to-roll prodn. capability, as well as flexibility and lightness, suggest their niche market opportunities. In this review, an overview of developments in PSCs is presented during the last three decades encompassing pre- and post-P3HT:PCBM era. Emphasis is given on evolution in device architecture, coupled with material selection for pre-P3HT:PCBM era, and synthesis of low-bandgap materials, coupled with a tandem structure for post-P3HT:PCBM era. Last but not least, efforts toward the longer operational lifetime of PSCs by encapsulation are reviewed. (c) 2018 American Institute of Physics.
- 2Cheng, P.; Yang, Y. Narrowing the Band Gap: The Key to High-Performance Organic Photovoltaics. Acc. Chem. Res. 2020, 53 (6), 1218– 1228, DOI: 10.1021/acs.accounts.0c00157Google Scholar2Narrowing the Band Gap: The Key to High-Performance Organic PhotovoltaicsCheng, Pei; Yang, YangAccounts of Chemical Research (2020), 53 (6), 1218-1228CODEN: ACHRE4; ISSN:0001-4842. (American Chemical Society)A review. Conspectus: Org. photovoltaics (OPVs) have attracted considerable attention in the last two decades to overcome the terawatt energy challenge and serious environmental problems. During their early development, only wide-band-gap org. semiconductors were synthesized and employed as the active layer, mainly utilizing photons in the UV-visible region and yielding power conversion efficiencies (PCEs) lower than 5%. Afterward, considerable efforts were made to narrow the polymer donor band gap in order to utilize the IR photons, which led to the enhancement of the PCE from 5% to 12% in about a decade. Since 2017, the study of narrow-band-gap non-fullerene acceptors helped usher in a new era in OPV research and boosted the achievable the PCE to 17% in only 3 years. In essence, the history of OPV development in the last 15 years can be summarized as an attempt to narrow the band gap of org. semiconductors and better position the energy levels. There are multiple benefits of a narrower band gap: (1) considerable IR photons can be utilized, and as a result, the short-circuit c.d. can increase significantly; (2) the energy offset of the LUMO energy levels or HOMO energy levels between the donor and acceptor can be reduced, which will reduce the open-circuit voltage loss by minimizing the loss caused by the donor/acceptor charge transfer state; (3) because of the unique MOs of org. semiconductors, the red-shifted absorption will induce high transmittance in the visible region, which is ideal for the rear subcells in tandem-junction OPVs and transparent OPVs. In this Account, we first summarize our work beginning in 2008 on the design and synthesis of narrow-band-gap polymer donors/non-fullerene acceptors. Several strategies for constructing these materials, including enhancing the intramol. charge transfer effect and steric hindrance/energy level engineering are discussed. In this part, in addn. to systematic analyses of the design of narrow-band-gap polymer donors based on BDT/TT or BDT/DPP, donors/acceptors based on the new donor moieties DTP or BZPT are discussed as well. Esp., we highlight our work on the first report on the narrow-band-gap acceptor Y1 (based on the new donor moiety BZPT), which pioneered the future development and usage of acceptors belonging to the Y1 family (or series). Subsequently, we analyze several reported certified world record single-junction or tandem-junction OPVs that use these narrow-band-gap donors or acceptors. We share our experiences and insights from a device perspective in terms of donor/acceptor selection, energy level alignment management, film morphol. control, current matching of subcells, interconnecting layer construction, interface engineering, and device geometry selection. In this part, the construction of high-performance ternary-blend OPVs and transparent OPVs based on these narrow-band-gap donors/acceptors is also discussed. Finally, in order to push the field into the 20-25% high-efficiency era in the next few years, some suggestions to further develop narrow-band-gap donors/acceptors and related device technologies are proposed.
- 3Bishnoi, S.; Datt, R.; Arya, S.; Gupta, S.; Gupta, R.; Tsoi, W. C.; Sharma, S. N.; Patole, S. P.; Gupta, V. Engineered Cathode Buffer Layers for Highly Efficient Organic Solar Cells: A Review. Adv. Mater. Interfaces 2022, 9 (19), 2101693, DOI: 10.1002/admi.202101693Google ScholarThere is no corresponding record for this reference.
- 4Nrel - Best Research-Cell Efficiency Chart. https://www.nrel.gov/pv/cell-efficiency.html (accessed on May 3, 2023).Google ScholarThere is no corresponding record for this reference.
- 5Cheng, P.; Zhan, X. Stability of Organic Solar Cells: Challenges and Strategies. Chem. Soc. Rev. 2016, 45 (9), 2544– 2582, DOI: 10.1039/C5CS00593KGoogle Scholar5Stability of organic solar cells: challenges and strategiesCheng, Pei; Zhan, XiaoweiChemical Society Reviews (2016), 45 (9), 2544-2582CODEN: CSRVBR; ISSN:0306-0012. (Royal Society of Chemistry)Org. solar cells (OSCs) present some advantages, such as simple prepn., light wt., low cost and large-area flexible fabrication, and have attracted much attention in recent years. Although the power conversion efficiencies have exceeded 10%, the inferior device stability still remains a great challenge. In this review, we summarize the factors limiting the stability of OSCs, such as metastable morphol., diffusion of electrodes and buffer layers, oxygen and water, irradn., heating and mech. stress, and survey recent progress in strategies to increase the stability of OSCs, such as material design, device engineering of active layers, employing inverted geometry, optimizing buffer layers, using stable electrodes and encapsulation. Some research areas of device stability that may deserve further attention are also discussed to help readers understand the challenges and opportunities in achieving high efficiency and high stability of OSCs towards future industrial manuf.
- 6Hoppe, H.; Niggemann, M.; Winder, C.; Kraut, J.; Hiesgen, R.; Hinsch, A.; Meissner, D.; Sariciftci, N. S. Nanoscale Morphology of Conjugated Polymer/Fullerene-Based Bulk-Heterojunction Solar Cells. Adv. Funct. Mater. 2004, 14 (10), 1005– 1011, DOI: 10.1002/adfm.200305026Google Scholar6Nanoscale morphology of conjugated polymer/fullerene-based bulk-heterojunction solar cellsHoppe, Harald; Niggemann, Michael; Winder, Christoph; Kraut, Juergen; Hiesgen, Renate; Hinsch, Andreas; Meissner, Dieter; Sariciftci, Niyazi SerdarAdvanced Functional Materials (2004), 14 (10), 1005-1011CODEN: AFMDC6; ISSN:1616-301X. (Wiley-VCH Verlag GmbH & Co. KGaA)The relation between the nanoscale morphol. and device properties for conjugated polymer/fullerene bulk-heterojunction plastic solar cells, was studied. Complementary measurements on solid-state blends of poly[2-methoxy-5-(3,7-dimethyloctyloxy)]-1,4-phenylenevinylene (MDMO-PPV) and the sol. fullerene C60 deriv. 1-(3-methoxycarbonyl) propyl-1-Ph [6,6]C61 (PCBM), spin-cast from toluene or chlorobenzene solns., were made. The characterization of the nanomorphol. was carried out by SEM and AFM, while solar-cell devices were characterized by I-V and spectral photocurrent measurements. The morphol. was manipulated by annealing to increase the extent of phase sepn. in the thin-film blends and to identify the distribution of materials. Photoluminescence measurements confirm the demixing of the materials by the thermal treatment. The photoluminescence of PCBM clusters with sizes of up to a few hundred nanometers indicates a photocurrent loss in films of the coarser phase-sepd. blends cast from toluene. For toluene-cast films the scale of phase sepn. depends strongly on the ratio of MDMO-PPV to PCBM, as well as on the total concn. of the casting soln. Small beads of 20-30 nm diam. were obsd. in blend films cast from both toluene and chlorobenzene and these are attributed to MDMO-PPV.
- 7Bronstein, H.; Nielsen, C. B.; Schroeder, B. C.; McCulloch, I. The Role of Chemical Design in the Performance of Organic Semiconductors. Nat. Rev. Chem 2020, 4 (2), 66– 77, DOI: 10.1038/s41570-019-0152-9Google Scholar7The role of chemical design in the performance of organic semiconductorsBronstein, Hugo; Nielsen, Christian B.; Schroeder, Bob C.; McCulloch, IainNature Reviews Chemistry (2020), 4 (2), 66-77CODEN: NRCAF7; ISSN:2397-3358. (Nature Research)A review. Org. semiconductors are soln.-processable, lightwt. and flexible and are increasingly being used as the active layer in a wide range of new technologies. The versatility of synthetic org. chem. enables the materials to be tuned such that they can be incorporated into biol. sensors, wearable electronics, photovoltaics and flexible displays. These devices can be improved by improving their material components, not only by developing the synthetic chem. but also by improving the anal. and computational techniques that enable us to understand the factors that govern material properties. Judicious mol. design provides control of the semiconductor frontier MO energy distribution and guides the hierarchical assembly of org. semiconductors into functional films where we can manipulate the properties and motion of charges and excited states. This Review describes how mol. design plays an integral role in developing org. semiconductors for electronic devices in present and emerging technologies.
- 8Cui, C.; Li, Y. Morphology Optimization of Photoactive Layers in Organic Solar Cells. Aggregate 2021, 2 (2), e31 DOI: 10.1002/agt2.31Google ScholarThere is no corresponding record for this reference.
- 9Huang, Y.-C.; Liu, W.-S.; Tsao, C.-S.; Wang, L. Mechanistic Insights into the Effect of Polymer Regioregularity on the Thermal Stability of Polymer Solar Cells. ACS Appl. Mater. Interfaces 2019, 11 (43), 40310– 40319, DOI: 10.1021/acsami.9b12482Google Scholar9Mechanistic Insights into the Effect of Polymer Regioregularity on the Thermal Stability of Polymer Solar CellsHuang, Yu-Ching; Liu, Wei-Shin; Tsao, Cheng-Si; Wang, LeeyihACS Applied Materials & Interfaces (2019), 11 (43), 40310-40319CODEN: AAMICK; ISSN:1944-8244. (American Chemical Society)Thermal stability is a bottleneck toward commercialization of polymer solar cells (PSCs). The effect of PCBM aggregation on a multilength scale on the bulk-heterojunction (BHJ) structure, performance, and thermal stability of PSCs is studied here by grazing-incidence small- and wide-angle x-ray scattering. The evolution of hierarchical BHJ structures of a blend film tuned by regioregularity of polymers from the as-cast state to the thermally unstable state is systematically studied. The thermal stability of PSCs with high polymer regioregularity values can be improved because of the good mutual interaction between polymer crystallites and fullerene aggregates. The insights obtained from this study provide an approach to manipulate the film structure on a multilength scale and to enhance the thermal stability of P3HT-based PSCs.
- 10Urquhart, S. G.; Martinson, M.; Eger, S.; Murcia, V.; Ade, H.; Collins, B. A. Connecting Molecular Conformation to Aggregation in P3ht Using near Edge X-Ray Absorption Fine Structure Spectroscopy. J. Phys. Chem. C 2017, 121 (39), 21720– 21728, DOI: 10.1021/acs.jpcc.7b07143Google Scholar10Connecting Molecular Conformation to Aggregation in P3HT Using Near Edge X-ray Absorption Fine Structure SpectroscopyUrquhart, Stephen G.; Martinson, Mercedes; Eger, Shaylin; Murcia, Victor; Ade, Harald; Collins, Brian A.Journal of Physical Chemistry C (2017), 121 (39), 21720-21728CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)C 1s near edge x-ray absorption fine structure (NEXAFS) and UV-visible spectroscopy are used to examine differences between highly aggregated and poorly aggregated forms of the polymer poly(3-hexylthiophene) (P3HT), based on as-cast and annealed regiorandom and regioregular P3HT samples. UV-visible spectra show characteristic signatures of unaggregated P3HT in regiorandom P3HT, and of H-aggregation in regioregular P3HT samples. Distinct spectroscopic differences, including energy shifts, are obsd. in the NEXAFS spectra of aggregated P3HT relative to the unaggregated forms. These differences are reproduced with transition-potential d. functional theory (TP-DFT) calcns. which explore aggregation and mol. conformation. Differences in the NEXAFS spectra of P3HT are assigned to thiophene backbone twisting in the unaggregated forms of P3HT, and to various degrees of chain planarization in aggregated forms of P3HT that also correlate to the exciton bandwidth. These results open up the prospect of characterizing conformation and related difficult to assess structural details through NEXAFS spectroscopy and correlative theory and electronic structure anal.
- 11Steyrleuthner, R.; Di Pietro, R.; Collins, B. A.; Polzer, F.; Himmelberger, S.; Schubert, M.; Chen, Z. H.; Zhang, S. M.; Salleo, A.; Ade, H.; Facchetti, A.; Neher, D. The Role of Regioregularity, Crystallinity, and Chain Orientation on Electron Transport in a High-Mobility N-Type Copolymer. J. Am. Chem. Soc. 2014, 136 (11), 4245– 4256, DOI: 10.1021/ja4118736Google Scholar11The Role of Regioregularity, Crystallinity, and Chain Orientation on Electron Transport in a High-Mobility n-Type CopolymerSteyrleuthner, Robert; Di Pietro, Riccardo; Collins, Brian A.; Polzer, Frank; Himmelberger, Scott; Schubert, Marcel; Chen, Zhihua; Zhang, Shiming; Salleo, Alberto; Ade, Harald; Facchetti, Antonio; Neher, DieterJournal of the American Chemical Society (2014), 136 (11), 4245-4256CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)We investigated the correlation between the polymer backbone structural regularity and the charge transport properties of poly{[N,N'-bis(2-octyldodecyl)-1,4,5,8-naphthalenediimide-2,6-diyl]-alt-5,5'-(2,2'-bithiophene)} [P(NDI2OD-T2)], a widely studied semiconducting polymer exhibiting high electron mobility and an unconventional micromorphol. To understand the influence of the chem. structure and crystal packing of conventional regioregular P(NDI2OD-T2) [RR-P(NDI2OD-T2)] on the charge transport, the corresponding regioirregular polymer RI-P(NDI2OD-T2) was synthesized. By combining optical, x-ray, and TEM data, we quant. characterized the aggregation, crystn., and backbone orientation of all of the polymer films, which were then correlated to the electron mobilities in electron-only diodes. By carefully selecting the prepn. conditions, we were able to obtain RR-P(NDI2OD-T2) films with similar cryst. structure along the three crystallog. axes but with different orientations of the polymer chains with respect to the substrate surface. RI-P(NDI2OD-T2), though exhibiting a rather similar LUMO structure and energy compared with the regioregular counterpart, displayed a very different packing structure characterized by the formation of ordered stacks along the lamellar direction without detectable π-stacking. Vertical electron mobilities were extd. from the space-charge-limited currents in unipolar devices. We demonstrate the anisotropy of the charge transport along the different crystallog. directions and how the mobility depends on π-stacking but is insensitive to the degree or coherence of lamellar stacking. The comparison between the regioregular and regioirregular polymers also shows how the use of large planar functional groups leads to improved charge transport, with mobilities that are less affected by chem. and structural disorder with respect to classic semicryst. polymers such as poly(3-hexylthiophene).
- 12Wang, S.; Fabiano, S.; Himmelberger, S.; Puzinas, S.; Crispin, X.; Salleo, A.; Berggren, M. Experimental Evidence That Short-Range Intermolecular Aggregation Is Sufficient for Efficient Charge Transport in Conjugated Polymers. Proc. Natl. Acad. Sci. U.S.A. 2015, 112 (34), 10599– 10604, DOI: 10.1073/pnas.1501381112Google Scholar12Experimental evidence that short-range intermolecular aggregation is sufficient for efficient charge transport in conjugated polymersWang, Suhao; Fabiano, Simone; Himmelberger, Scott; Puzinas, Skomantas; Crispin, Xavier; Salleo, Alberto; Berggren, MagnusProceedings of the National Academy of Sciences of the United States of America (2015), 112 (34), 10599-10604CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Efficiency, current throughput, and speed of electronic devices are to a great extent dictated by charge carrier mobility. The classic approach to impart high carrier mobility to polymeric semiconductors has often relied on the assumption that extensive order and crystallinity are needed. Recently, however, this assumption has been challenged, because high mobility has been reported for semiconducting polymers that exhibit a surprisingly low degree of order. Here, we show that semiconducting polymers can be confined into weakly ordered fibers within an inert polymer matrix without affecting their charge transport properties. In these conditions, the semiconducting polymer chains are inhibited from attaining long-range order in the π-stacking or alkyl-stacking directions, as demonstrated from the absence of significant X-ray diffraction intensity corresponding to these crystallog. directions, yet still remain extended along the backbone direction and aggregate on a local length scale. As a result, the polymer films maintain high mobility even at very low concns. Our findings provide a simple picture that clarifies the role of local order and connectivity of domains.
- 13Wang, Y.; Guo, M.; Yang, L.; Li, L.; Qin, W.; Yin, S. Toward Morphological Stabilization in Polymer Bulk Heterojunction Solar Cells by Crosslinking Using an Additive. IEEE J. Photovoltaics 2016, 6 (3), 710– 718, DOI: 10.1109/JPHOTOV.2016.2545342Google ScholarThere is no corresponding record for this reference.
- 14Landerer, D.; Sprau, C.; Baumann, D.; Pingel, P.; Leonhard, T.; Zimmermann, D.; Chochos, C. L.; Krüger, H.; Janietz, S.; Colsmann, A. Thermal Stabilization of the Bulk-Heterojunction Morphology in Polymer: Fullerene Solar Cells Using a Bisazide Cross-Linker. Solar RRL 2019, 3 (2), 1800266, DOI: 10.1002/solr.201800266Google ScholarThere is no corresponding record for this reference.
- 15Wang, S.; Qu, Y.; Li, S.; Ye, F.; Chen, Z.; Yang, X. Improved Thermal Stability of Polymer Solar Cells by Incorporating Porphyrins. Adv. Funct. Mater. 2015, 25 (5), 748– 757, DOI: 10.1002/adfm.201403018Google ScholarThere is no corresponding record for this reference.
- 16Jia, Z.; Xia, X.; Wang, X.; Wang, T.; Xu, G.; Liu, B.; Zhou, J.; Li, F. All-Conjugated Amphiphilic Diblock Copolymers for Improving Morphology and Thermal Stability of Polymer/Nanocrystals Hybrid Solar Cells. Front. Mater. Sci. 2018, 12 (3), 225– 238, DOI: 10.1007/s11706-018-0428-xGoogle ScholarThere is no corresponding record for this reference.
- 17Herrmann, F.; Muhsin, B.; Singh, C. R.; Shokhovets, S.; Gobsch, G.; Hoppe, H.; Presselt, M. Influence of Interface Doping on Charge-Carrier Mobilities and Sub-Bandgap Absorption in Organic Solar Cells. J. Phys. Chem. C 2015, 119 (17), 9036– 9040, DOI: 10.1021/acs.jpcc.5b00124Google ScholarThere is no corresponding record for this reference.
- 18Moustafa, E.; Torimtubun, A. A. A.; Pallares, J.; Marsal, L. F. Effect of Additives and Annealing on the Performance of Nonfullerene-Based Binary and Ternary Organic Photovoltaics. Sol. RRL 2022, 6 (5), 2100480, DOI: 10.1002/solr.202100480Google ScholarThere is no corresponding record for this reference.
- 19Nam, M.; Yoo, J.; Park, Y.; Noh, H. Y.; Park, Y.; Cho, J.; Kim, J.-A.; Kim, J.; Lee, H. H.; Chang, R. Ternary Blend Organic Solar Cells with Improved Morphological Stability. J. Mater. Chem. A 2019, 7 (16), 9698– 9707, DOI: 10.1039/c9ta00382gGoogle ScholarThere is no corresponding record for this reference.
- 20Xu, X.; Li, Y.; Peng, Q. Ternary Blend Organic Solar Cells: Understanding the Morphology from Recent Progress. Adv. Mater. 2022, 34 (46), 2107476, DOI: 10.1002/adma.202107476Google Scholar20Ternary Blend Organic Solar Cells: Understanding the Morphology from Recent ProgressXu, Xiaopeng; Li, Ying; Peng, QiangAdvanced Materials (Weinheim, Germany) (2022), 34 (46), 2107476CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)A review. Ternary blend org. solar cells (TB-OSCs) incorporating multiple donor and/or acceptor materials into the active layer have emerged as a promising strategy to simultaneously improve the overall device parameters for realizing higher performances than binary devices. Whereas introducing multiple materials also results in a more complicated morphol. than their binary blend counterparts. Understanding the morphol. is crucially important for further improving the device performance of TB-OSC. This review introduces the soly. and miscibility parameters that affect the morphol. of ternary blends. Then, this review summarizes the recent processes of morphol. study on ternary blends from the aspects of mol. crystallinity, mol. packing orientation, domain size and purity, directly observation of morphol., vertical phase sepn. as well as morphol. stability. Finally, summary and prospects of TB-OSCs are concluded.
- 21Liao, H.-C.; Chen, P.-H.; Chang, R. P.; Su, W.-F. Morphological Control Agent in Ternary Blend Bulk Heterojunction Solar Cells. Polymers 2014, 6 (11), 2784– 2802, DOI: 10.3390/polym6112784Google ScholarThere is no corresponding record for this reference.
- 22Park, S. A.; Kim, D. H.; Chung, D.; Kim, J.; Park, T.; Cho, S.; Kim, M. Asymmetric Polymer Additive for Morphological Regulation and Thermally Stable Organic Solar Cells. ACS Appl. Mater. Interfaces 2023, 15 (22), 27026– 27033, DOI: 10.1021/acsami.3c04804Google ScholarThere is no corresponding record for this reference.
- 23Habenicht, S. H.; Schramm, S.; Fischer, S.; Sachse, T.; Herrmann-Westendorf, F.; Bellmann, A.; Dietzek, B.; Presselt, M.; Weiß, D.; Beckert, R.; Gorls, H. Tuning the Polarity and Surface Activity of Hydroxythiazoles - Extending the Applicability of Highly Fluorescent Self-Assembling Chromophores to Supra-Molecular Photonic Structures. J. Mater. Chem. C 2016, 4 (5), 958– 971, DOI: 10.1039/C5TC03632AGoogle Scholar23Tuning the polarity and surface activity of hydroxythiazoles - extending the applicability of highly fluorescent self-assembling chromophores to supra-molecular photonic structuresHabenicht, S. H.; Schramm, S.; Fischer, S.; Sachse, T.; Herrmann-Westendorf, F.; Bellmann, A.; Dietzek, B.; Presselt, M.; Weiss, D.; Beckert, R.; Goerls, H.Journal of Materials Chemistry C: Materials for Optical and Electronic Devices (2016), 4 (5), 958-971CODEN: JMCCCX; ISSN:2050-7534. (Royal Society of Chemistry)A small library of N,N-diethyl- and -diethanolsulfonamides of differently substituted 2-(2-pyridyl)- and 2-pyrazinyl-4-alkoxythiazoles was synthesized and studied in terms of their photophys. properties, electronic structure (quantum chem. calcns. at the CAM-B3LYP/6-31+G(d,p) level of theory) and thin film morphol. (Langmuir-Blodgett- and spin-cast films). By using the Langmuir-Blodgett technique to exert direct control over the degree of aggregation in thin films made from different thiazole type dyes. In combination with spectroscopic studies, the authors gained an in-depth understanding of the influence of aggregation on the electrooptical properties of thin films made of the here-studied substances.
- 24Hupfer, M. L.; Kaufmann, M.; Herrmann-Westendorf, F.; Sachse, T.; Roussille, L.; Feller, K. H.; Weiß, D.; Deckert, V.; Beckert, R.; Dietzek, B.; Presselt, M. On the Control of Chromophore Orientation, Supramolecular Structure, and Thermodynamic Stability of an Amphiphilic Pyridyl-Thiazol Upon Lateral Compression and Spacer Length Variation. ACS Appl. Mater. Interfaces 2017, 9 (50), 44181– 44191, DOI: 10.1021/acsami.7b13042Google ScholarThere is no corresponding record for this reference.
- 25Hupfer, M. L.; Kaufmann, M.; May, S.; Preiß, J.; Weiß, D.; Dietzek, B.; Beckert, R.; Presselt, M. Enhancing the Supramolecular Stability of Monolayers by Combining Dipolar with Amphiphilic Motifs: A Case of Amphiphilic Push-Pull-Thiazole. Phys. Chem. Chem. Phys. 2019, 21 (24), 13241– 13247, DOI: 10.1039/C9CP02013FGoogle ScholarThere is no corresponding record for this reference.
- 26Hupfer, M. L.; Kaufmann, M.; Roussille, L.; Preiß, J.; Weiß, D.; Hinrichs, K.; Deckert, V.; Dietzek, B.; Beckert, R.; Presselt, M. Arylic Versus Alkylic-Hydrophobic Linkers Determine the Supramolecular Structure and Optoelectronic Properties of Tripodal Amphiphilic Push-Pull Thiazoles. Langmuir 2019, 35 (7), 2561– 2570, DOI: 10.1021/acs.langmuir.8b03893Google ScholarThere is no corresponding record for this reference.
- 27Hupfer, M. L.; Meyer, R.; Deckert-Gaudig, T.; Ghosh, S.; Skabeev, A.; Peneva, K.; Deckert, V.; Dietzek, B.; Presselt, M. Supramolecular Reorientation During Deposition onto Metal Surfaces of Quasi-Two-Dimensional Langmuir Monolayers Composed of Bifunctional Amphiphilic, Twisted Perylenes. Langmuir 2021, 37 (37), 11018– 11026, DOI: 10.1021/acs.langmuir.1c01525Google ScholarThere is no corresponding record for this reference.
- 28Lin, Y.; Nugraha, M. I.; Firdaus, Y.; Scaccabarozzi, A. D.; Aniés, F.; Emwas, A.-H.; Yengel, E.; Zheng, X.; Liu, J.; Wahyudi, W. A Simple N-Dopant Derived from Diquat Boosts the Efficiency of Organic Solar Cells to 18.3%. ACS Energy Lett. 2020, 5 (12), 3663– 3671, DOI: 10.1021/acsenergylett.0c01949Google Scholar28A Simple n-Dopant Derived from Diquat Boosts the Efficiency of Organic Solar Cells to 18.3%Lin, Yuanbao; Nugraha, Mohamad Insan; Firdaus, Yuliar; Scaccabarozzi, Alberto D.; Anies, Filip; Emwas, Abdul-Hamid; Yengel, Emre; Zheng, Xiaopeng; Liu, Jiakai; Wahyudi, Wandi; Yarali, Emre; Faber, Hendrik; Bakr, Osman M.; Tsetseris, Leonidas; Heeney, Martin; Anthopoulos, Thomas D.ACS Energy Letters (2020), 5 (12), 3663-3671CODEN: AELCCP; ISSN:2380-8195. (American Chemical Society)Mol. doping has recently been shown to improve the operating characteristics of org. photovoltaics (OPVs). Here, we prep. neutral Diquat (DQ) and use it as n-dopant to improve the performance of state-of-the-art OPVs. Adding DQ in ternary bulk-heterojunction (BHJ) cells based of PM6:Y6:PC71BM is found to consistently increase their power conversion efficiency (PCE) from 16.7 to 17.4%. Analyses of materials and devices reveal that DQ acts as n-type dopant and morphol. modifier for the BHJ leading to observable changes in its surface topog. The resulting n-doped BHJs exhibit higher optical absorption coeffs., balanced ambipolar transport, longer carrier lifetimes and suppressed bimol. recombination, which are ultimately responsible for the increased PCE. The use of DQ was successfully extended to OPVs based on PM6:BTP-eC9:PC71BM for which a max. PCE of 18.3% (uncertified) was achieved. Our study highlights DQ as a promising dopant for application in next generation org. solar cells.
- 29Jeong, S.; Woo, S.-H.; Lyu, H.-K.; Kim, C.; Kim, H.; Han, Y. S. Improvement of Photovoltaic Properties by Addition of a Perylene Compound in P3ht: Pcbm Bhj System. J. Nanosci. Nanotechnol. 2012, 12 (5), 4147– 4153, DOI: 10.1166/jnn.2012.5898Google ScholarThere is no corresponding record for this reference.
- 30Vivo, P.; Dubey, R.; Lehtonen, E.; Kivistö, H.; Vuorinen, T.; Lemmetyinen, H. Dipyrrolidinyl-Substituted Perylene Diimide as Additive for Poly (3-Hexylthiophene):[6, 6]-Phenyl C61 Butyric Acid Methylester Bulk-Heterojunction Blends. Thin Solid Films 2013, 548, 398– 405, DOI: 10.1016/j.tsf.2013.08.106Google ScholarThere is no corresponding record for this reference.
- 31Li, F.; Werner, A.; Pfeiffer, M.; Leo, K.; Liu, X. Leuco Crystal Violet as a Dopant for N-Doping of Organic Thin Films of Fullerene C60. J. Phys. Chem. B 2004, 108 (44), 17076– 17082, DOI: 10.1021/jp0478615Google Scholar31Leuco Crystal Violet as a Dopant for n-Doping of Organic Thin Films of Fullerene C60Li, Fenghong; Werner, Ansgar; Pfeiffer, Martin; Leo, Karl; Liu, XianjieJournal of Physical Chemistry B (2004), 108 (44), 17076-17082CODEN: JPCBFK; ISSN:1520-6106. (American Chemical Society)The triphenylmethane dye crystal violet (CV) and its leuco base, leucocrystal violet (LCV), are investigated as dopants for n-type doping of fullerene C60. Conductivities up to 8 × 10-3 S/cm at 30° are achieved when C60 is doped with CV. Mass spectroscopy and optical spectroscopy (UV/VIS/NIR absorption and Fourier transform IR transmission) confirm that the leuco base LCV is formed during sublimation of the cationic CV dye. When the com. available LCV was directly used as a dopant in C60, a max. cond. of 1.3 × 10-2 S/cm was obtained at 30°. We found that in both cases, the leuco base became reoxidized to the cationic form by electron transfer to electron-accepting matrixes, leading to the doping effect. The donor properties of LCV in a charge-transfer complex with 7,7,8,8-tetracyanoquinodimethane (TCNQ) were confirmed by UV/VIS/NIR absorption and Fourier transform IR (FTIR) spectroscopy. C60 anions were obsd. in the FTIR or NIR absorption spectra of the mixed films of C60 and LCV. Photoinduced charge transfer between LCV and C60 provides free electrons, which increase the n-type cond. The electron transfer becomes irreversible by hydride abstraction.
- 32Vivo, P.; Kaunisto, K.; Alekseev, A. S.; Pekkola, O.; Tolkki, A.; Chukharev, V.; Lemmetyinen, H. Vectorial Photoinduced Electron Transfer in Multicomponent Film Systems of Poly (3-Hexylthiophene), Porphyrin-Fullerene Dyad, and Perylenetetracarboxidiimide. Photochem. Photobiol. Sci. 2010, 9 (9), 1212– 1217, DOI: 10.1039/c0pp00180eGoogle ScholarThere is no corresponding record for this reference.
- 33Vivo, P.; Vuorinen, T.; Chukharev, V.; Tolkki, A.; Kaunisto, K.; Ihalainen, P.; Peltonen, J.; Lemmetyinen, H. Multicomponent Molecularly Controlled Langmuir- Blodgett Systems for Organic Photovoltaic Applications. J. Phys. Chem. C 2010, 114 (18), 8559– 8567, DOI: 10.1021/jp1009862Google Scholar33Multicomponent Molecularly Controlled Langmuir-Blodgett Systems for Organic Photovoltaic ApplicationsVivo, Paola; Vuorinen, Tommi; Chukharev, Vladimir; Tolkki, Antti; Kaunisto, Kimmo; Ihalainen, Petri; Peltonen, Jouko; Lemmetyinen, HelgeJournal of Physical Chemistry C (2010), 114 (18), 8559-8567CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)The capability of Violanthrone-79 (V-79) and N,N'-bis(2,5-di-tert-butylphenyl)-3,4:9,10-perylenebis(dicarboximide) (PDI) to act as electron acceptors, with respect to poly(3-hexylthiophene) (PHT) and to the photoinduced fullerene anion of porphyrin-fullerene (P-F) dyad, was demonstrated in Langmuir-Blodgett films by the time-resolved Maxwell displacement charge method. The introduction of V-79 and PDI in oriented multilayered films led to improved light harvesting and increased lifetime of the charge sepn., enhancing the photocurrent generation measured using a three-electrode photoelectrochem. cell. The best solar cell performance was achieved for the multifunctional film structure where efficient PHT-phthalocyanine heterojunction (PHT|ZnPH4) was combined with the P-F|V-79 system.
- 34Kaloyanova, S.; Zagranyarski, Y.; Ritz, S.; Hanulová, M.; Koynov, K.; Vonderheit, A.; Müllen, K.; Peneva, K. Water-Soluble Nir-Absorbing Rylene Chromophores for Selective Staining of Cellular Organelles. J. Am. Chem. Soc. 2016, 138 (9), 2881– 2884, DOI: 10.1021/jacs.5b10425Google Scholar34Water-Soluble NIR-Absorbing Rylene Chromophores for Selective Staining of Cellular OrganellesKaloyanova, Stefka; Zagranyarski, Yulian; Ritz, Sandra; Hanulova, Maria; Koynov, Kaloian; Vonderheit, Andreas; Muellen, Klaus; Peneva, KalinaJournal of the American Chemical Society (2016), 138 (9), 2881-2884CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Biocompatible org. dyes emitting in the near-IR are highly desirable in fluorescence imaging techniques. Herein we report a synthetic approach for building novel small peri-guanidine-fused naphthalene monoimide and perylene monoimide chromophores. The presented structures possess near-IR absorption and emission, high photostability, and good water soly. After a fast cellular uptake, they selectively stain mitochondria with a low background in live and fixed cells. They can be addnl. modified in a one-step reaction with functional groups for covalent labeling of proteins. The low cytotoxicity allows a long time exposure of live cells to the dyes without the necessity of washing. Successful application in localization super-resoln. microscopy was demonstrated in phosphate-buffered saline without any reducing or oxidizing additives.
- 35Fujimoto, K.; Takahashi, M.; Izawa, S.; Hiramoto, M. Development of Perylene-Based Non-Fullerene Acceptors through Bay-Functionalization Strategy. Materials 2020, 13 (9), 2148, DOI: 10.3390/ma13092148Google ScholarThere is no corresponding record for this reference.
- 36Hupfer, M. L.; Ghosh, S.; Wang, Y.; Opsomer, T.; Mayerhöfer, T. G.; Dehaen, W.; Presselt, M. Dichroic Dipole Antenna Membranes from Aligned Linear Bophy Dyes. Adv. Mater. Interfaces 2021, 9 (1), 2101490, DOI: 10.1002/admi.202101490Google ScholarThere is no corresponding record for this reference.
- 37Hupfer, M. L.; Koszarna, B.; Ghosh, S.; Gryko, D. T.; Presselt, M. Langmuir-Blodgett Films of Diketopyrrolopyrroles with Tunable Amphiphilicity. Langmuir 2021, 37 (34), 10272– 10278, DOI: 10.1021/acs.langmuir.1c01113Google ScholarThere is no corresponding record for this reference.
- 38Presselt, M.; Dehaen, W.; Maes, W.; Klamt, A.; Martínez, T.; Beenken, W. J. D.; Kruk, M. Quantum Chemical Insights into the Dependence of Porphyrin Basicity on the Meso-Aryl Substituents: Thermodynamics, Buckling, Reaction Sites and Molecular Flexibility. Phys. Chem. Chem. Phys. 2015, 17 (21), 14096– 14106, DOI: 10.1039/C5CP01808KGoogle ScholarThere is no corresponding record for this reference.
- 39Mumyatov, A.; Prudnov, F.; Inasaridze, L.; Mukhacheva, O.; Troshin, P. High Lumo Energy Pyrrolidinofullerenes as Promising Electron-Acceptor Materials for Organic Solar Cells. J. Mater. Chem. C 2015, 3 (44), 11612– 11617, DOI: 10.1039/C5TC02509EGoogle ScholarThere is no corresponding record for this reference.
- 40Hupfer, M. L.; Kaufmann, M.; Preiß, J.; Weiß, D.; Beckert, R.; Dietzek, B.; Presselt, M. Assembly of T-Shaped Amphiphilic Thiazoles on the Air-Water Interface: Impact of Polar Chromophore Moieties, as Well as Dipolarity and Pi-Extension of the Chromophore on the Supramolecular Structure. Langmuir 2019, 35 (7), 2587– 2600, DOI: 10.1021/acs.langmuir.8b04063Google ScholarThere is no corresponding record for this reference.
- 41Hupfer, M. L.; Blaschke, D.; Schmidt, H.; Presselt, M. Embedding an Amphiphilic 4-Hydroxy Thiazole Dye in Langmuir Matrices: Studying Miscibilities with Arylic and Alkylic Matrix Amphiphiles Via Langmuir Isotherms and Photo-Induced Force Microscopy. Langmuir 2021, 37 (45), 13255– 13264, DOI: 10.1021/acs.langmuir.1c01772Google ScholarThere is no corresponding record for this reference.
- 42Finkelmeyer, S. J.; Askins, E. J.; Eichhorn, J.; Ghosh, S.; Siegmund, C.; Tauscher, E.; Dellith, A.; Hupfer, M. L.; Dellith, J.; Ritter, U.; Strzalka, J.; Glusac, K.; Schacher, F. H.; Presselt, M. Tailoring the Weight of Surface and Intralayer Edge States to Control Lumo Energies. Adv. Mater. 2023, 35 (40), e2305006 DOI: 10.1002/adma.202305006Google ScholarThere is no corresponding record for this reference.
- 43Hupfer, M. L.; Dellith, J.; Seyring, M.; Diegel, M.; Dellith, A.; Ghosh, S.; Rettenmayr, M.; Dietzek-Ivanšić, B.; Presselt, M. Bifacial Dye Membranes: Ultrathin and Free-Standing Although Not Being Covalently Bound. Adv. Mater. 2023, 35 (1), 2204874, DOI: 10.1002/adma.202204874Google ScholarThere is no corresponding record for this reference.
- 44Bertho, S.; Janssen, G.; Cleij, T. J.; Conings, B.; Moons, W.; Gadisa, A.; D’Haen, J.; Goovaerts, E.; Lutsen, L.; Manca, J. Effect of Temperature on the Morphological and Photovoltaic Stability of Bulk Heterojunction Polymer: Fullerene Solar Cells. Sol. Energy Mater. Sol. Cells 2008, 92 (7), 753– 760, DOI: 10.1016/j.solmat.2008.01.006Google Scholar44Effect of temperature on the morphological and photovoltaic stability of bulk heterojunction polymer:fullerene solar cellsBertho, Sabine; Janssen, Griet; Cleij, Thomas J.; Conings, Bert; Moons, Wouter; Gadisa, Abay; D'Haen, Jan; Goovaerts, Etienne; Lutsen, Laurence; Manca, Jean; Vanderzande, DirkSolar Energy Materials & Solar Cells (2008), 92 (7), 753-760CODEN: SEMCEQ; ISSN:0927-0248. (Elsevier B.V.)In high performance polymer:fullerene bulk heterojunction solar cells the nanoscale morphol. of interpenetrating acceptor:donor materials is optimized through appropriate prepn. conditions such as annealing and choice of solvent, but this initial state-of-the-art morphol. will not remain stable during long-term operation. We report the effects of prolonged storage at elevated temps. on both the morphol. and the photovoltaic performance for the model systems MDMO-PPV:PCBM and poly(3-hexylthiophene):PCBM as compared to high Tg PPV:PCBM based solar cells, where the high Tg PPV is characterized by its high glass transition temp. (138°). In situ monitoring of the photocurrent-voltage characteristics at elevated temps., in combination with a systematic transmission electron microscopy study and complementary optical spectroscopy, reveals distinct degrdn. kinetics and morphol. changes that indicate the occurrence of different underlying physicochem. mechanisms.
- 45Chao, Y.-C.; Chuang, C.-H.; Hsu, H.-L.; Wang, H.-J.; Hsu, Y.-C.; Chen, C.-P.; Jeng, R.-J. Enhanced Thermal Stability of Organic Photovoltaics Via Incorporating Triphenylamine Derivatives as Additives. Sol. Energy Mater. Sol. Cells 2016, 157, 666– 675, DOI: 10.1016/j.solmat.2016.07.041Google Scholar45Enhanced thermal stability of organic photovoltaics via incorporating triphenylamine derivatives as additivesChao, Ying-Chieh; Chuang, Chia-Hsin; Hsu, Hsiang-Lin; Wang, Hsing-Ju; Hsu, Yu-Chi; Chen, Chih-Ping; Jeng, Ru-JongSolar Energy Materials & Solar Cells (2016), 157 (), 666-675CODEN: SEMCEQ; ISSN:0927-0248. (Elsevier B.V.)In this work, we prepd. four star-shaped conjugated small mols., the triphenylamine dithiophene (TBT) derivs., namely TBT-H, TBT-Br, TBT-OH, and TBT-N3 presenting hydride, bromide, hydroxyl, and azide terminal functional groups, resp. These TBT derivs. were used as additives in the active layers of org. photovoltaics to investigate the effect of intermol. interactions (TBT-H, TBT-OH) or crosslinking (TBT-N3, TBT-Br) on the long-term thermal stability of the devices. From analyses of blend film morphologies, and optoelectronic and device performance, we obsd. significant enhancements in thermal stability during accelerated heating tests at 150 °C for the devices incorporated with the additives TBT-N3 and TBT-Br. These two additives functioned as crosslinkers, and constructed local borders that effectively impeded heat-promoted fullerene aggregation, thereby leading to highly stable morphologies. When compared with corresponding normal devices, the TBT-N3-derived devices based on poly(3-hexylthiophene) exhibited greater stability, with the power conversion efficiency (PCE) remaining as high as 2.5% after 144h at 150 °C. Because of this enhancement, a device based on an amorphous low-bandgap polymer, namely poly(thieno[3,4-b]thiophene-alt-benzodithiophene), with the addn. of TBT-N3 was fabricated. We obsd. a significant improvement in device stability, retaining approx. 60% (from 5.0 to 3.3%) of its initial PCE under accelerated heating (150 °C). In contrast, the PCE of the corresponding normal device decayed to 0.01% of its initial value.
- 46Reinspach, J. A.; Diao, Y.; Giri, G.; Sachse, T.; England, K.; Zhou, Y.; Tassone, C.; Worfolk, B. J.; Presselt, M.; Toney, M. F.; Mannsfeld, S.; Bao, Z. Tuning the Morphology of Solution-Sheared P3ht:Pcbm Films. ACS Appl. Mater. Interfaces 2016, 8 (3), 1742– 1751, DOI: 10.1021/acsami.5b09349Google ScholarThere is no corresponding record for this reference.
- 47Presselt, M.; Herrmann, F.; Shokhovets, S.; Hoppe, H.; Runge, E.; Gobsch, G. Sub-Bandgap Absorption in Polymer-Fullerene Solar Cells Studied by Temperature-Dependent External Quantum Efficiency and Absorption Spectroscopy. Chem. Phys. Lett. 2012, 542, 70– 73, DOI: 10.1016/j.cplett.2012.05.063Google Scholar47Sub-bandgap absorption in polymer-fullerene solar cells studied by temperature-dependent external quantum efficiency and absorption spectroscopyPresselt, Martin; Herrmann, Felix; Shokhovets, Sviatoslav; Hoppe, Harald; Runge, Erich; Gobsch, GerhardChemical Physics Letters (2012), 542 (), 70-73CODEN: CHPLBC; ISSN:0009-2614. (Elsevier B.V.)We study the sub-bandgap absorption in solar cells made of poly(3-hexylthiophene-2,5-diyl) and [6,6]-Ph C61 butyric acid Me ester (PCBM) by photothermal deflection absorption spectroscopy and measurement of temp.-dependent external quantum efficiency spectra. Several models for sub-bandgap absorption are critically reviewed in view of the external quantum efficiency results. The latter suggest polaron-related transitions as origin of the Gaussian sub-bandgap peak near 1.6 eV. Intermol. charge transfer excitations as an explanation cannot completely be ruled out. However, the assumption of charge transfer excitons with large binding energies is difficult to reconcile with the rapid loss of wt. of the Gaussian sub-bandgap peak seen in external quantum efficiency above room temp.
- 48Presselt, M.; Bärenklau, M.; Rösch, R.; Beenken, W. J. D.; Runge, E.; Shokhovets, S.; Hoppe, H.; Gobsch, G. Sub-Bandgap Absorption in Polymer-Fullerene Solar Cells. Appl. Phys. Lett. 2010, 97 (25), 253302, DOI: 10.1063/1.3527077Google ScholarThere is no corresponding record for this reference.
- 49Presselt, M.; Herrmann, F.; Hoppe, H.; Shokhovets, S.; Runge, E.; Gobsch, G. Influence of Phonon Scattering on Exciton and Charge Diffusion in Polymer-Fullerene Solar Cells. Adv. Energy Mater. 2012, 2 (8), 999– 1003, DOI: 10.1002/aenm.201100793Google Scholar49Influence of phonon scattering on exciton and charge diffusion in polymer-fullerene solar cellsPresselt, Martin; Herrmann, Felix; Hoppe, Harald; Shokhovets, Sviatoslav; Runge, Erich; Gobsch, GerhardAdvanced Energy Materials (2012), 2 (8), 999-1003CODEN: ADEMBC; ISSN:1614-6840. (Wiley-Blackwell)Thermally activated transport and phonon scattering in P3HT:PCBM (poly(3-hexylthiophene-2,5-diyl):[6,6]-phenylC61-butyric acid Me ester) bulk heterojunction (BHJ) org. solar cells is studied via temp.-dependent external-quantum-efficiency (EQE) spectroscopy. The hopping barriers for combined exciton and charge transport are balanced for the individual blended materials in a sample, which possesses a blending ratio and a morphol. that give rise to a maximal power-conversion efficiency. Increasing the PCBM wt. fraction leads to a redn. of exciton hopping barriers in PCBM, while for P3HT exciton hopping barriers remain const. This redn. of PCBM exciton hopping barriers is attributed to a higher PCBM crystallinity in the PCBM-rich solar cell as compared to the BHJ with the optimized blending ratio. The morphol.-dependent difference in exciton hopping activation energies between P3HT and PCBM is attributed to a higher impact of phonon scattering in P3HT than in PCBM, as concluded from the much stronger decrease of P3HT-related temp.-dependent external quantum efficiencies above room temp. in the PCBM-rich BHJ solar cell. All EQE data of P3HT:PCBM-based BHJ solar cells is modeled consistently over a broad temp. range by a simple anal. expression involving temp. activation and phonon scattering, without the need to distinguish two sep. hopping regimes.
- 50Hupfer, M. L.; Herrmann-Westendorf, F.; Kaufmann, M.; Weiß, D.; Beckert, R.; Dietzek, B.; Presselt, M. Autonomous Supramolecular Interface Self-Healing Monitored by Restoration of Uv/Vis Absorption Spectra of Self-Assembled Thiazole Layers. Chem.─Eur. J. 2019, 25 (36), 8630– 8634, DOI: 10.1002/chem.201901549Google ScholarThere is no corresponding record for this reference.
- 51Hupfer, M.; Herrmann-Westendorf, F.; Dietzek, B.; Presselt, M. In Situ Photothermal Deflection Spectroscopy Revealing Intermolecular Interactions Upon Self-Assembly of Dye Monolayers. Analyst 2021, 146 (16), 5033– 5036, DOI: 10.1039/D1AN00582KGoogle ScholarThere is no corresponding record for this reference.
- 52Das, S.; Presselt, M. Progress and Development in Structural and Optoelectronic Tunability of Supramolecular Nonbonded Fullerene Assemblies. J. Mater. Chem. C 2019, 7 (21), 6194– 6216, DOI: 10.1039/C9TC00889FGoogle Scholar52Progress and development in structural and optoelectronic tunability of supramolecular nonbonded fullerene assembliesDas, Saunak; Presselt, MartinJournal of Materials Chemistry C: Materials for Optical and Electronic Devices (2019), 7 (21), 6194-6216CODEN: JMCCCX; ISSN:2050-7534. (Royal Society of Chemistry)A review. Assembly of fullerenes utilizing self-organization at solvent/non-solvent interfaces or by introducing hydrophobic(philic) end-groups have yielded diverse molecularly-ordered structures. Taking advantage of the multiple π-π interaction between adjacent C60-moieties, structurally elegant and functionally promising fullerene assemblies were synthesized by several groups over the last 20 yr. Considerable improvement of device parameters is witnessed if non-covalent fullerene layers assembled using interfacial self assembly are used as electron extn. layer, for example in hybrid solar cells. Thus a pre-detd. choice of C60-nanostructures for photovoltaic application stems from an understanding of fullerene-fullerene interaction, a priori from the mol. level. Could we eventually define the outcomes of the last 3 decades of fullerene aggregation chem.. This review summarizes the course of understanding of optoelectronic properties of fullerene-morphologies, bridging the gap between single mol. and device scale which shall be significant for their judicious implementation in mol. electronics.
- 53Das, S.; Herrmann-Westendorf, F.; Schacher, F. H.; Tauscher, E.; Ritter, U.; Dietzek, B.; Presselt, M. Controlling Electronic Transitions in Fullerene Van Der Waals Aggregates Via Supramolecular Assembly. ACS Appl. Mater. Interfaces 2016, 8 (33), 21512– 21521, DOI: 10.1021/acsami.6b06800Google ScholarThere is no corresponding record for this reference.
- 54Ghosh, R.; Spano, F. C. Excitons and Polarons in Organic Materials. Acc. Chem. Res. 2020, 53 (10), 2201– 2211, DOI: 10.1021/acs.accounts.0c00349Google Scholar54Excitons and Polarons in Organic MaterialsGhosh, Raja; Spano, Frank C.Accounts of Chemical Research (2020), 53 (10), 2201-2211CODEN: ACHRE4; ISSN:0001-4842. (American Chemical Society)Conspectus: Excitons and polarons play a central role in the electronic and optical properties of org. semiconducting polymers and mol. aggregates, and are of fundamental importance in understanding the operation of org. optoelectronic devices such as solar cells and light-emitting diodes. For many conjugated org. mols. and polymers, the creation of neutral electronic excitations or ionic radicals is assocd. with significant nuclear relaxation, the bulk of which occurs along the vinyl-stretching mode or the arom.-quinoidal stretching mode when conjugated rings are present. Within a polymer chain or mol. aggregate, nuclear relaxation competes with energy- and charge-transfer, mediated by electronic interactions between the constituent units (repeat units for polymers and individual chromophores for a mol. aggregate); for neutral electronic excitations, such inter-unit interactions lead to extended excited states or excitons, while for pos. (or neg.) charges, interactions lead to delocalized hole (or electron) polarons. The electronic coupling as well as the local coupling between electronic and nuclear degrees of freedom in both excitons and polarons can be described with a Holstein Hamiltonian. However, although excitons and polarons derive from similarly structured Hamiltonians, their optical signatures are quite distinct, largely due to differing ground states and optical selection rules. In this Account, we explore the similarities and differences in the spectral response of excitons and polarons in org. polymers and mol. aggregates. We limit our anal. to the subspace of excitons and hole polarons contg. at most one excitation; hence, we omit the influence of bipolarons, biexcitons, and higher multiparticle excitations. Using a generic linear array of coupled units as a model host for both excitons and polarons, we compare and contrast the optical responses of both quasiparticles, with a particular emphasis on the spatial coherence length, the length over which an exciton or polaron possesses wave-like properties important for more efficient transport. For excitons, the UV-vis absorption spectrum is generally represented by a distorted vibronic progression with H-like or J-like signatures depending on the sign of the electronic coupling, Jex. The spectrum broadens with increasing site disorder, with the spectral area preserved due to an oscillator strength sum rule. For (hole) polarons, the generally stronger electronic coupling results in a mid-IR spectrum consisting of a narrow, low-energy peak (A) with energy near a vibrational quantum of the vinyl stretching mode, and a broader, higher-energy feature (B). In contrast to the UV-vis spectrum, the mid-IR spectrum is invariant to the sign of the electronic coupling, th, and completely resistant to long-range disorder, where it remains entirely homogeneously broadened. Even in the presence of short-range disorder, the width of peak A remains surprisingly narrow as long as |th| remains sufficiently large, a property that can be understood in terms of Herzberg-Teller coupling. Unlike for excitons, for polarons, the absorption spectral area decreases with increasing short-range disorder σ (i.e., there is no oscillator sum rule) reflective of a decreasing polaron coherence length. The intensity of the low-energy peak A in relation to B is an important signature of polaron coherence. By contrast, for excitons, the absorption spectrum contains no unambiguous signs of exciton coherence. One must instead resort to the shape of the steady-state photoluminescence spectrum. The Holstein-based model has been highly successful in accounting for the spectral properties of mol. aggregates as well as conjugated polymers like poly(3-hexylthiophene) (P3HT) in the mid-IR and UV-vis spectral regions.
- 55Clark, J.; Silva, C.; Friend, R. H.; Spano, F. C. Role of Intermolecular Coupling in the Photophysics of Disordered Organic Semiconductors: Aggregate Emission in Regioregular Polythiophene. Phys. Rev. Lett. 2007, 98 (20), 206406, DOI: 10.1103/PhysRevLett.98.206406Google Scholar55Role of Intermolecular Coupling in the Photophysics of Disordered Organic Semiconductors: Aggregate Emission in Regioregular PolythiopheneClark, Jenny; Silva, Carlos; Friend, Richard H.; Spano, Frank C.Physical Review Letters (2007), 98 (20), 206406/1-206406/4CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)The authors address the role of excitonic coupling on the nature of photoexcitations in the conjugated polymer regioregular poly(3-hexylthiophene). By temp.-dependent absorption and photoluminescence spectroscopy, optical emission is overwhelmingly dominated by weakly coupled H aggregates. The relative absorbance of the 0-0 and 0-1 vibronic peaks provides a powerfully simple means to ext. the magnitude of the intermol. coupling energy, of ∼5 and 30 meV for films spun from isodurene and CHCl3 solns., resp.
- 56Alam, S.; Anand, A.; Islam, M. M.; Meitzner, R.; Djoumessi, A. S.; Slowik, J.; Teklu, Z.; Fischer, P.; Kästner, C.; Khan, J. I. P3ht: Pcbm Polymer Solar Cells from a Didactic Perspective. J. Photonics Energy 2022, 12 (3), 035501, DOI: 10.1117/1.jpe.12.035501Google ScholarThere is no corresponding record for this reference.
- 57Cardona, C. M.; Li, W.; Kaifer, A. E.; Stockdale, D.; Bazan, G. C. Electrochemical Considerations for Determining Absolute Frontier Orbital Energy Levels of Conjugated Polymers for Solar Cell Applications. Adv. Mater. 2011, 23 (20), 2367– 2371, DOI: 10.1002/adma.201004554Google Scholar57Electrochemical Considerations for Determining Absolute Frontier Orbital Energy Levels of Conjugated Polymers for Solar Cell ApplicationsCardona, Claudia M.; Li, Wei; Kaifer, Angel E.; Stockdale, David; Bazan, Guillermo C.Advanced Materials (Weinheim, Germany) (2011), 23 (20), 2367-2371CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)Narrow bandgap conjugated polymers in combination with fullerene acceptors are under intense investigation in the field of org. photovoltaics (OPVs). The open circuit voltage, and thereby the power conversion efficiency, of the devices is related to the offset of the frontier orbital energy levels of the donor and acceptor components which are widely detd. by cyclic voltammetry. Inconsistencies have appeared in the use of the ferrocenium/ferrocene (Fc+/Fc) redox couple, as well as the values used for the abs. potentials of std. electrodes, which can complicate the comparison of materials properties and detn. of structure/property relationships.
- 58Titov, A. V.; Ufimtsev, I. S.; Luehr, N.; Martinez, T. J. Generating Efficient Quantum Chemistry Codes for Novel Architectures. J. Chem. Theory Comput. 2013, 9 (1), 213– 221, DOI: 10.1021/ct300321aGoogle Scholar58Generating Efficient Quantum Chemistry Codes for Novel ArchitecturesTitov, Alexey V.; Ufimtsev, Ivan S.; Luehr, Nathan; Martinez, Todd J.Journal of Chemical Theory and Computation (2013), 9 (1), 213-221CODEN: JCTCCE; ISSN:1549-9618. (American Chemical Society)We describe an extension of our graphics processing unit (GPU) electronic structure program TeraChem to include atom-centered Gaussian basis sets with d angular momentum functions. This was made possible by a "meta-programming" strategy that leverages computer algebra systems for the derivation of equations and their transformation to correct code. We generate a multitude of code fragments that are formally math. equiv., but differ in their memory and floating-point operation footprints. We then select between different code fragments using empirical testing to find the highest performing code variant. This leads to an optimal balance of floating-point operations and memory bandwidth for a given target architecture without laborious manual tuning. We show that this approach is capable of similar performance compared to our hand-tuned GPU kernels for basis sets with s and p angular momenta. We also demonstrate that mixed precision schemes (using both single and double precision) remain stable and accurate for mols. with d functions. We provide benchmarks of the execution time of entire SCF calcns. using our GPU code and compare to mature CPU based codes, showing the benefits of the GPU architecture for electronic structure theory with appropriately redesigned algorithms. We suggest that the meta-programming and empirical performance optimization approach may be important in future computational chem. applications, esp. in the face of quickly evolving computer architectures.
- 59Beenken, W. J. D.; Sun, M.; Zhao, G.; Pullerits, T. Excited State Properties of Neutral and Charged Ter-Fluorene with and without a Keto-Defect. Phys. Status Solidi B 2008, 245 (5), 849– 853, DOI: 10.1002/pssb.200743442Google ScholarThere is no corresponding record for this reference.
- 60Song, C.; Wang, L.-P.; Sachse, T.; Preiß, J.; Presselt, M.; Martínez, T. J. Efficient Implementation of Effective Core Potential Integrals and Gradients on Graphical Processing Units. J. Chem. Phys. 2015, 143 (1), 014114, DOI: 10.1063/1.4922844Google ScholarThere is no corresponding record for this reference.
- 61Presselt, M.; Dietzek, B.; Schmitt, M.; Rau, S.; Winter, A.; Jäger, M.; Schubert, U. S.; Popp, J. A Concept to Tailor Electron Delocalization: Applying Qtaim Analysis to Phenyl-Terpyridine Compounds. J. Phys. Chem. A 2010, 114 (50), 13163– 13174, DOI: 10.1021/jp107007aGoogle Scholar61A Concept to Tailor Electron Delocalization: Applying QTAIM Analysis to Phenyl-Terpyridine CompoundsPresselt, Martin; Dietzek, Benjamin; Schmitt, Michael; Rau, Sven; Winter, Andreas; Jager, Michael; Schubert, Ulrich S.; Popp, JurgenJournal of Physical Chemistry A (2010), 114 (50), 13163-13174CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)To gain a deeper understanding of how structural modifications may influence photochem. properties of 4'-phenyl-2,2':6',2''-terpyridines, the investigations presented here focus on electron delocalization in 4'-phenyl-2,2':6',2''-terpyridine derivs. and their Ru(II) and Zn(II) complexes. In those systems of neighboring arom. rings the considerable torsion between the rings is commonly regarded to be the limiting factor for a well pronounced π-conjugation between the rings. A common approach to improve the π-conjugation is to lower the steric hindrance, thus achieving a more planar geometry. Here, we present a fundamentally different approach towards enhanced π-conjugation by manipulation of the electronic properties of the pyridine-Ph (py-ph) bond. This is accomplished by introducing various substituents at the phenylene moiety or coordinating the terpyridine moiety to transition metal ions. The electron delocalization was quantified via the DFT-calcd. ellipticity in the bond-crit. point (BCP) of the py-ph bond. This ellipticity can be modified due to substituents in the para position of phenylene and via the transition metals coordinated to the terpyridine moiety. Changes in electron d. distribution induced by the substituents and the metal ions are further studied by means of intermol. electron d. difference plots. It was shown that a NH2 group in the para position of the Ph ring as well as the coordination to Ru(II) or Zn(II) ions significantly enhances the π-character of the py-ph bond. Surprisingly, an even higher π-character of the py-ph bond is achieved by introducing addnl. NH2 groups in ortho position to the py-ph bond, despite the increased torsion between pyridine and phenylene. The introduction of other substituents (-NO2, -Br, -CN, -vinyl, -ethynyl) studied within the presented work enables an actuation of the electron delocalization between terpyridine and phenylene. In doing so, the ellipticity is a concise quantity to characterize electron delocalization in the studied systems. Furthermore, the ellipticity in the BCP of the py-ph bond is related to the corresponding geometrical properties (e.g., bond length and dihedral angle) and to the DFT-calcd. HOMO and LUMO energies.
- 62Presselt, M.; Schnedermann, C.; Muller, M.; Schmitt, M.; Popp, J. Derivation of Correlation Functions to Predict Bond Properties of Phenyl–CH Bonds Based on Vibrational and 1H NMR Spectroscopic Quantities. J. Phys. Chem. A 2010, 114 (37), 10287– 10296, DOI: 10.1021/jp105348dGoogle Scholar62Derivation of Correlation Functions to Predict Bond Properties of Phenyl-CH Bonds Based on Vibrational and 1H NMR Spectroscopic QuantitiesPresselt, Martin; Schnedermann, Christoph; Mueller, Michael; Schmitt, Michael; Popp, JuergenJournal of Physical Chemistry A (2010), 114 (37), 10287-10296CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)The study of electron d. properties significantly contributes to the detn. of important chem. relations. The exptl. detn. of the electron d. distribution is limited to single crystals. However, equiv. information is often desired for mols., which do not crystallize in a sufficient manner. Furthermore, it is of high impact to study changes in the electron d. distribution (i.e., related reactivities) upon environmental variations. Consequently, here we investigate methods to derive electron d. properties from spectroscopic data. In particular correlation functions are introduced, which are able to predict electron d. properties in all five CH-bonds of monosubstituted benzene derivs. at once. The prediction performance for electron densities and the corresponding Laplacians is lower as compared to previously introduced local functions, but far less spectroscopic input data are needed. However, for ellipticities a higher prediction performance than this obtained for the previously derived local functions could be obtained despite the fact that less spectroscopic data were used. Thus, ellipticities are best predicted using 1H NMR data for the para position of monosubstituted benzene derivs.
- 63Beenken, W.; Presselt, M.; Ngo, T. H.; Dehaen, W.; Maes, W.; Kruk, M. Molecular Structures and Absorption Spectra Assignment of Corrole Nh Tautomers. J. Phys. Chem. A 2014, 118 (5), 862– 871, DOI: 10.1021/jp411033hGoogle Scholar63Molecular Structures and Absorption Spectra Assignment of Corrole NH TautomersBeenken, Wichard; Presselt, Martin; Ngo, Thien H.; Dehaen, Wim; Maes, Wouter; Kruk, MikalaiJournal of Physical Chemistry A (2014), 118 (5), 862-871CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)The individual absorption spectra of the two NH tautomers of 10-(4,6-dichloropyrimidin-5-yl)-5,15-dimesitylcorrole are assigned on the basis of the Gouterman four-orbital model and a quantum chem. TD-DFT study. The assignment indicates that the red-shifted T1 tautomer is the one with protonated pyrrole nitrogen atoms N(21), N(22) and N(23), whereas the blue-shifted T2 tautomer has pyrrole nitrogen atoms N(21), N(22) and N(24) protonated. A wave-like nonplanar distortion of the macrocycle in the ground state is found for both NH tautomers, with the wave axis going through the pyrroles contg. N(22) and N(24). The 7C plane detd. by the least-squares distances to the carbon atoms C1, C4, C5, C6, C9, C16, and C19 is suggested as a mean corrole macrocycle plane for the anal. of out-of-plane distortions. The magnitude of these distortions is distinctly different for the two NH tautomers, leading to substantial perturbations of their acid-base properties, which are rationalized by the interplay of the degree of out-of-plane distortion of the macrocycle as a whole and the tendency of the pyrrole nitrogen atoms toward pyramidalization, with the former leading to a basicity increase whereas the latter enhances the acidity.
- 64Presselt, M.; Wojdyr, M.; Beenken, W. J. D.; Kruk, M.; Martinez, T. J. Steric and Electronic Contributions to the Core Reactivity of Monoprotonated 5-Phenylporphyrin: A Dft Study. Chem. Phys. Lett. 2014, 603 (0), 21– 27, DOI: 10.1016/j.cplett.2014.04.011Google ScholarThere is no corresponding record for this reference.
- 65Preiß, J.; Jäger, M.; Rau, S.; Dietzek, B.; Popp, J.; Martínez, T.; Presselt, M. How Does Peripheral Functionalization of Ruthenium(Ii)-Terpyridine Complexes Affect Spatial Charge Redistribution after Photoexcitation at the Franck-Condon Point?. ChemPhysChem 2015, 16 (7), 1395– 1404, DOI: 10.1002/cphc.201500223Google ScholarThere is no corresponding record for this reference.
- 66Fischer, S.; Vestfrid, J.; Mahammed, A.; Herrmann-Westendorf, F.; Schulz, M.; Muller, J.; Kiesewetter, O.; Dietzek, B.; Gross, Z.; Presselt, M. Photometric Detection of Nitric Oxide Using a Dissolved Iron(Iii) Corrole as a Sensitizer. ChemPlusChem 2016, 81 (7), 594– 603, DOI: 10.1002/cplu.201500553Google ScholarThere is no corresponding record for this reference.
- 67Preiß, J.; Herrmann-Westendorf, F.; Ngo, T. H.; Martínez, T.; Dietzek, B.; Hill, J. P.; Ariga, K.; Kruk, M. M.; Maes, W.; Presselt, M. Absorption and Fluorescence Features of an Amphiphilic Meso-Pyrimidinylcorrole: Experimental Study and Quantum Chemical Calculations. J. Phys. Chem. A 2017, 121 (45), 8614– 8624, DOI: 10.1021/acs.jpca.7b08910Google ScholarThere is no corresponding record for this reference.
- 68Sachse, T.; Martinez, T. J.; Presselt, M. On Combining the Conductor-Like Screening Model and Optimally Tuned Range-Separated Hybrid Density Functionals. J. Chem. Phys. 2019, 150 (17), 174117, DOI: 10.1063/1.5064730Google Scholar68On combining the conductor-like screening model and optimally tuned range-separated hybrid density functionalsSachse, Torsten; Martinez, Todd J.; Presselt, MartinJournal of Chemical Physics (2019), 150 (17), 174117/1-174117/8CODEN: JCPSA6; ISSN:0021-9606. (American Institute of Physics)Range-sepd. hybrid functionals whose range-sepn. parameter γ has been nonempirically tuned to a particular mol. have been shown to yield frontier orbital energies and other properties in very good agreement with expts. However, many cases, such as org. optoelectronic devices, require the description of mols. embedded in an environment. This can be done by combining the γ-tuning procedure with polarizable continuum models in general and the very versatile conductor-like screening model in particular. There are at least two different ways of performing this combination. The partially vertical γ-tuning employs equil. solvation throughout. The strictly vertical γ-tuning, on the other hand, employs nonequil. solvation to obtain ionization energies. In this article, we compare ground-state and excited-state properties of several different mols. relevant to org. optoelectronics that were obtained using both of the two different tuning procedures. While there are significant differences in the ground-state properties, we see virtually no difference in the excited-state properties. Given these results, we conclude that both tuning procedures have to be used in conjunction for the correct description of both ground-state and excited-state properties. (c) 2019 American Institute of Physics.
- 69Kozlíková, B.; Krone, M.; Falk, M.; Lindow, N.; Baaden, M.; Baum, D.; Viola, I.; Parulek, J.; Hege, H.-C. Visualization of Biomolecular Structures: State of the Art Revisited. Computer Graphics Forum 2017, 36 (8), 178– 204, DOI: 10.1111/cgf.13072Google ScholarThere is no corresponding record for this reference.
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Abstract
Figure 1
Figure 1. Panel (A) Lewis structure and solvent-accessible surfaces (with solvent radius 1.4 Å, corresponding to water molecule radius) with electrostatic potentials of active layer materials (P3HT:PC60BM) and additive (PMIDA-C12). Panel (B) HOMO (highest occupied molecular orbital) and LUMO (lowest unoccupied molecular orbital) or rather valence and conduction band energies (eV) vs vacuum energy of the materials used for this study; references: (a) Bishnoi et al. (3) Adv. Mater. Interfaces 2022, (b) derived from square wave voltammetry investigation as detailed in the Supporting Information, and (c) Mumyatov et al. (39) J. Mater. Chem. C 2015. Panel (C) Schematic of a classical BHJ solar cell. Interfaces that are potentially stabilized via the amphiphiles are shown in sections CI–CIII, and color codes are in accordance with panel (B).
Figure 2
Figure 2. Current density–voltage (J–V) curves of PMIDA-C12 doped and undoped P3HT:PC60BM (3:2) solar cells, annealed at 80 °C for 10 min. Panel (A) illuminated with AM 1.5; panel (B) dark.
Figure 3
Figure 3. J–V plot of P3HT:PC60BM (30 mg/mL (3:2) blend) conventional solar cell with and without the PMIDA-C12 additive, post annealing at 160 °C for 5 min. Panel (A) under illumination (AM 1.5) and panel (B) in the dark.
Figure 4
Figure 4. Thermal stability of the photovoltaic parameters of a P3HT:PC60BM blend with and without the PMIDA-C12 additive during thermal aging (80 °C) in a nitrogen-filled glovebox. Averages and uncertainties are calculated from four cells. Panel (A) short-circuit current density, panel (B) open-circuit voltage, panel (C) fill factor, and panel (D) power conversion efficiency.
Figure 5
Figure 5. Normalized absorption spectra of the P3HT:PC60BM films with and without the PMIDA-C12 additive as fabricated. Panel (A) 0 h and panel (B) 588 h of thermal aging (80 °C).
Figure 6
Figure 6. Panel (A) shows the vibrational progression in the UV–vis absorption spectrum of a P3HT:PC60BM film is modeled via Huang–Rhys coupled Gaussian functions. For details, see the Supporting Information. The model is fitted to the experimental data from 1.74 to 2.29 eV, while the area under the fitted curve (crystalline P3HT) and the difference from the experimental spectrum (amorphous P3HT) are evaluated in the range from 1.8 to 3.0 eV. The spectrum of a PC60BM film is shown for comparison. Panel (B) shows the ratio of crystalline to amorphous P3HT (areas under the respective curves) versus amphiphile concentration at different thermal aging times.
Figure 7
Figure 7. PL spectra of P3HT:PC60BM (3:2 BHJ) film with and without the PMIDA-C12 additive at different thermal aging (80 °C) times; panel (A) 0 h, panel (B) 450 h, and panel (C) 588 h. PL data are normalized to the maximum of 0.010 wt % of additive which is relatively constant.
Figure 8
Figure 8. AFM topography and phase images (2.5 μm × 2.5 μm) of P3HT:PC60BM (3:2 BHJ) films and respective height histograms of the different topographies. Row (A) 0.000 wt % PMIDA-C12; row (B) 0.005 wt % PMIDA-C12; row (C) 0.010 wt % PMIDA-C12. Thermal aging was carried out at 80 °C for 0, 450, and 588 h.
References
This article references 69 other publications.
- 1Berger, P. R.; Kim, M. Polymer Solar Cells: P3ht:Pcbm and Beyond. J. Renewable Sustainable Energy 2018, 10 (1), 013508, DOI: 10.1063/1.50129921Polymer solar cells: P3HT:PCBM and beyondBerger, P. R.; Kim, M.Journal of Renewable and Sustainable Energy (2018), 10 (1), 013508/1-013508/26CODEN: JRSEBH; ISSN:1941-7012. (American Institute of Physics)A review. For the last two decades, polymer solar cells (PSCs) have been a cynosure of the photovoltaic community, as evidenced by the growing no. of patent applications and scientific publications. Efforts to achieve high power conversion efficiency in PSC, propelled by advances in device architecture, material combination, and nanomorphol. control, evolved into poly(3-hexylthiophene-2,5-diyl) (P3HT):phenyl-C61-Butyric-Acid-Me Ester (PCBM) bulk heterojunction PSCs, which had been the best seller in PSC research for a decade. Subsequently, PSC research was redirected towards the synthesis of low bandgap materials and optimization of tandem cells, which led to a power conversion efficiency of ∼13%. Even though this efficiency may not be sufficient enough to compete with that of inorg. solar cells, unique properties of PSCs, such as mass roll-to-roll prodn. capability, as well as flexibility and lightness, suggest their niche market opportunities. In this review, an overview of developments in PSCs is presented during the last three decades encompassing pre- and post-P3HT:PCBM era. Emphasis is given on evolution in device architecture, coupled with material selection for pre-P3HT:PCBM era, and synthesis of low-bandgap materials, coupled with a tandem structure for post-P3HT:PCBM era. Last but not least, efforts toward the longer operational lifetime of PSCs by encapsulation are reviewed. (c) 2018 American Institute of Physics.
- 2Cheng, P.; Yang, Y. Narrowing the Band Gap: The Key to High-Performance Organic Photovoltaics. Acc. Chem. Res. 2020, 53 (6), 1218– 1228, DOI: 10.1021/acs.accounts.0c001572Narrowing the Band Gap: The Key to High-Performance Organic PhotovoltaicsCheng, Pei; Yang, YangAccounts of Chemical Research (2020), 53 (6), 1218-1228CODEN: ACHRE4; ISSN:0001-4842. (American Chemical Society)A review. Conspectus: Org. photovoltaics (OPVs) have attracted considerable attention in the last two decades to overcome the terawatt energy challenge and serious environmental problems. During their early development, only wide-band-gap org. semiconductors were synthesized and employed as the active layer, mainly utilizing photons in the UV-visible region and yielding power conversion efficiencies (PCEs) lower than 5%. Afterward, considerable efforts were made to narrow the polymer donor band gap in order to utilize the IR photons, which led to the enhancement of the PCE from 5% to 12% in about a decade. Since 2017, the study of narrow-band-gap non-fullerene acceptors helped usher in a new era in OPV research and boosted the achievable the PCE to 17% in only 3 years. In essence, the history of OPV development in the last 15 years can be summarized as an attempt to narrow the band gap of org. semiconductors and better position the energy levels. There are multiple benefits of a narrower band gap: (1) considerable IR photons can be utilized, and as a result, the short-circuit c.d. can increase significantly; (2) the energy offset of the LUMO energy levels or HOMO energy levels between the donor and acceptor can be reduced, which will reduce the open-circuit voltage loss by minimizing the loss caused by the donor/acceptor charge transfer state; (3) because of the unique MOs of org. semiconductors, the red-shifted absorption will induce high transmittance in the visible region, which is ideal for the rear subcells in tandem-junction OPVs and transparent OPVs. In this Account, we first summarize our work beginning in 2008 on the design and synthesis of narrow-band-gap polymer donors/non-fullerene acceptors. Several strategies for constructing these materials, including enhancing the intramol. charge transfer effect and steric hindrance/energy level engineering are discussed. In this part, in addn. to systematic analyses of the design of narrow-band-gap polymer donors based on BDT/TT or BDT/DPP, donors/acceptors based on the new donor moieties DTP or BZPT are discussed as well. Esp., we highlight our work on the first report on the narrow-band-gap acceptor Y1 (based on the new donor moiety BZPT), which pioneered the future development and usage of acceptors belonging to the Y1 family (or series). Subsequently, we analyze several reported certified world record single-junction or tandem-junction OPVs that use these narrow-band-gap donors or acceptors. We share our experiences and insights from a device perspective in terms of donor/acceptor selection, energy level alignment management, film morphol. control, current matching of subcells, interconnecting layer construction, interface engineering, and device geometry selection. In this part, the construction of high-performance ternary-blend OPVs and transparent OPVs based on these narrow-band-gap donors/acceptors is also discussed. Finally, in order to push the field into the 20-25% high-efficiency era in the next few years, some suggestions to further develop narrow-band-gap donors/acceptors and related device technologies are proposed.
- 3Bishnoi, S.; Datt, R.; Arya, S.; Gupta, S.; Gupta, R.; Tsoi, W. C.; Sharma, S. N.; Patole, S. P.; Gupta, V. Engineered Cathode Buffer Layers for Highly Efficient Organic Solar Cells: A Review. Adv. Mater. Interfaces 2022, 9 (19), 2101693, DOI: 10.1002/admi.202101693There is no corresponding record for this reference.
- 4Nrel - Best Research-Cell Efficiency Chart. https://www.nrel.gov/pv/cell-efficiency.html (accessed on May 3, 2023).There is no corresponding record for this reference.
- 5Cheng, P.; Zhan, X. Stability of Organic Solar Cells: Challenges and Strategies. Chem. Soc. Rev. 2016, 45 (9), 2544– 2582, DOI: 10.1039/C5CS00593K5Stability of organic solar cells: challenges and strategiesCheng, Pei; Zhan, XiaoweiChemical Society Reviews (2016), 45 (9), 2544-2582CODEN: CSRVBR; ISSN:0306-0012. (Royal Society of Chemistry)Org. solar cells (OSCs) present some advantages, such as simple prepn., light wt., low cost and large-area flexible fabrication, and have attracted much attention in recent years. Although the power conversion efficiencies have exceeded 10%, the inferior device stability still remains a great challenge. In this review, we summarize the factors limiting the stability of OSCs, such as metastable morphol., diffusion of electrodes and buffer layers, oxygen and water, irradn., heating and mech. stress, and survey recent progress in strategies to increase the stability of OSCs, such as material design, device engineering of active layers, employing inverted geometry, optimizing buffer layers, using stable electrodes and encapsulation. Some research areas of device stability that may deserve further attention are also discussed to help readers understand the challenges and opportunities in achieving high efficiency and high stability of OSCs towards future industrial manuf.
- 6Hoppe, H.; Niggemann, M.; Winder, C.; Kraut, J.; Hiesgen, R.; Hinsch, A.; Meissner, D.; Sariciftci, N. S. Nanoscale Morphology of Conjugated Polymer/Fullerene-Based Bulk-Heterojunction Solar Cells. Adv. Funct. Mater. 2004, 14 (10), 1005– 1011, DOI: 10.1002/adfm.2003050266Nanoscale morphology of conjugated polymer/fullerene-based bulk-heterojunction solar cellsHoppe, Harald; Niggemann, Michael; Winder, Christoph; Kraut, Juergen; Hiesgen, Renate; Hinsch, Andreas; Meissner, Dieter; Sariciftci, Niyazi SerdarAdvanced Functional Materials (2004), 14 (10), 1005-1011CODEN: AFMDC6; ISSN:1616-301X. (Wiley-VCH Verlag GmbH & Co. KGaA)The relation between the nanoscale morphol. and device properties for conjugated polymer/fullerene bulk-heterojunction plastic solar cells, was studied. Complementary measurements on solid-state blends of poly[2-methoxy-5-(3,7-dimethyloctyloxy)]-1,4-phenylenevinylene (MDMO-PPV) and the sol. fullerene C60 deriv. 1-(3-methoxycarbonyl) propyl-1-Ph [6,6]C61 (PCBM), spin-cast from toluene or chlorobenzene solns., were made. The characterization of the nanomorphol. was carried out by SEM and AFM, while solar-cell devices were characterized by I-V and spectral photocurrent measurements. The morphol. was manipulated by annealing to increase the extent of phase sepn. in the thin-film blends and to identify the distribution of materials. Photoluminescence measurements confirm the demixing of the materials by the thermal treatment. The photoluminescence of PCBM clusters with sizes of up to a few hundred nanometers indicates a photocurrent loss in films of the coarser phase-sepd. blends cast from toluene. For toluene-cast films the scale of phase sepn. depends strongly on the ratio of MDMO-PPV to PCBM, as well as on the total concn. of the casting soln. Small beads of 20-30 nm diam. were obsd. in blend films cast from both toluene and chlorobenzene and these are attributed to MDMO-PPV.
- 7Bronstein, H.; Nielsen, C. B.; Schroeder, B. C.; McCulloch, I. The Role of Chemical Design in the Performance of Organic Semiconductors. Nat. Rev. Chem 2020, 4 (2), 66– 77, DOI: 10.1038/s41570-019-0152-97The role of chemical design in the performance of organic semiconductorsBronstein, Hugo; Nielsen, Christian B.; Schroeder, Bob C.; McCulloch, IainNature Reviews Chemistry (2020), 4 (2), 66-77CODEN: NRCAF7; ISSN:2397-3358. (Nature Research)A review. Org. semiconductors are soln.-processable, lightwt. and flexible and are increasingly being used as the active layer in a wide range of new technologies. The versatility of synthetic org. chem. enables the materials to be tuned such that they can be incorporated into biol. sensors, wearable electronics, photovoltaics and flexible displays. These devices can be improved by improving their material components, not only by developing the synthetic chem. but also by improving the anal. and computational techniques that enable us to understand the factors that govern material properties. Judicious mol. design provides control of the semiconductor frontier MO energy distribution and guides the hierarchical assembly of org. semiconductors into functional films where we can manipulate the properties and motion of charges and excited states. This Review describes how mol. design plays an integral role in developing org. semiconductors for electronic devices in present and emerging technologies.
- 8Cui, C.; Li, Y. Morphology Optimization of Photoactive Layers in Organic Solar Cells. Aggregate 2021, 2 (2), e31 DOI: 10.1002/agt2.31There is no corresponding record for this reference.
- 9Huang, Y.-C.; Liu, W.-S.; Tsao, C.-S.; Wang, L. Mechanistic Insights into the Effect of Polymer Regioregularity on the Thermal Stability of Polymer Solar Cells. ACS Appl. Mater. Interfaces 2019, 11 (43), 40310– 40319, DOI: 10.1021/acsami.9b124829Mechanistic Insights into the Effect of Polymer Regioregularity on the Thermal Stability of Polymer Solar CellsHuang, Yu-Ching; Liu, Wei-Shin; Tsao, Cheng-Si; Wang, LeeyihACS Applied Materials & Interfaces (2019), 11 (43), 40310-40319CODEN: AAMICK; ISSN:1944-8244. (American Chemical Society)Thermal stability is a bottleneck toward commercialization of polymer solar cells (PSCs). The effect of PCBM aggregation on a multilength scale on the bulk-heterojunction (BHJ) structure, performance, and thermal stability of PSCs is studied here by grazing-incidence small- and wide-angle x-ray scattering. The evolution of hierarchical BHJ structures of a blend film tuned by regioregularity of polymers from the as-cast state to the thermally unstable state is systematically studied. The thermal stability of PSCs with high polymer regioregularity values can be improved because of the good mutual interaction between polymer crystallites and fullerene aggregates. The insights obtained from this study provide an approach to manipulate the film structure on a multilength scale and to enhance the thermal stability of P3HT-based PSCs.
- 10Urquhart, S. G.; Martinson, M.; Eger, S.; Murcia, V.; Ade, H.; Collins, B. A. Connecting Molecular Conformation to Aggregation in P3ht Using near Edge X-Ray Absorption Fine Structure Spectroscopy. J. Phys. Chem. C 2017, 121 (39), 21720– 21728, DOI: 10.1021/acs.jpcc.7b0714310Connecting Molecular Conformation to Aggregation in P3HT Using Near Edge X-ray Absorption Fine Structure SpectroscopyUrquhart, Stephen G.; Martinson, Mercedes; Eger, Shaylin; Murcia, Victor; Ade, Harald; Collins, Brian A.Journal of Physical Chemistry C (2017), 121 (39), 21720-21728CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)C 1s near edge x-ray absorption fine structure (NEXAFS) and UV-visible spectroscopy are used to examine differences between highly aggregated and poorly aggregated forms of the polymer poly(3-hexylthiophene) (P3HT), based on as-cast and annealed regiorandom and regioregular P3HT samples. UV-visible spectra show characteristic signatures of unaggregated P3HT in regiorandom P3HT, and of H-aggregation in regioregular P3HT samples. Distinct spectroscopic differences, including energy shifts, are obsd. in the NEXAFS spectra of aggregated P3HT relative to the unaggregated forms. These differences are reproduced with transition-potential d. functional theory (TP-DFT) calcns. which explore aggregation and mol. conformation. Differences in the NEXAFS spectra of P3HT are assigned to thiophene backbone twisting in the unaggregated forms of P3HT, and to various degrees of chain planarization in aggregated forms of P3HT that also correlate to the exciton bandwidth. These results open up the prospect of characterizing conformation and related difficult to assess structural details through NEXAFS spectroscopy and correlative theory and electronic structure anal.
- 11Steyrleuthner, R.; Di Pietro, R.; Collins, B. A.; Polzer, F.; Himmelberger, S.; Schubert, M.; Chen, Z. H.; Zhang, S. M.; Salleo, A.; Ade, H.; Facchetti, A.; Neher, D. The Role of Regioregularity, Crystallinity, and Chain Orientation on Electron Transport in a High-Mobility N-Type Copolymer. J. Am. Chem. Soc. 2014, 136 (11), 4245– 4256, DOI: 10.1021/ja411873611The Role of Regioregularity, Crystallinity, and Chain Orientation on Electron Transport in a High-Mobility n-Type CopolymerSteyrleuthner, Robert; Di Pietro, Riccardo; Collins, Brian A.; Polzer, Frank; Himmelberger, Scott; Schubert, Marcel; Chen, Zhihua; Zhang, Shiming; Salleo, Alberto; Ade, Harald; Facchetti, Antonio; Neher, DieterJournal of the American Chemical Society (2014), 136 (11), 4245-4256CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)We investigated the correlation between the polymer backbone structural regularity and the charge transport properties of poly{[N,N'-bis(2-octyldodecyl)-1,4,5,8-naphthalenediimide-2,6-diyl]-alt-5,5'-(2,2'-bithiophene)} [P(NDI2OD-T2)], a widely studied semiconducting polymer exhibiting high electron mobility and an unconventional micromorphol. To understand the influence of the chem. structure and crystal packing of conventional regioregular P(NDI2OD-T2) [RR-P(NDI2OD-T2)] on the charge transport, the corresponding regioirregular polymer RI-P(NDI2OD-T2) was synthesized. By combining optical, x-ray, and TEM data, we quant. characterized the aggregation, crystn., and backbone orientation of all of the polymer films, which were then correlated to the electron mobilities in electron-only diodes. By carefully selecting the prepn. conditions, we were able to obtain RR-P(NDI2OD-T2) films with similar cryst. structure along the three crystallog. axes but with different orientations of the polymer chains with respect to the substrate surface. RI-P(NDI2OD-T2), though exhibiting a rather similar LUMO structure and energy compared with the regioregular counterpart, displayed a very different packing structure characterized by the formation of ordered stacks along the lamellar direction without detectable π-stacking. Vertical electron mobilities were extd. from the space-charge-limited currents in unipolar devices. We demonstrate the anisotropy of the charge transport along the different crystallog. directions and how the mobility depends on π-stacking but is insensitive to the degree or coherence of lamellar stacking. The comparison between the regioregular and regioirregular polymers also shows how the use of large planar functional groups leads to improved charge transport, with mobilities that are less affected by chem. and structural disorder with respect to classic semicryst. polymers such as poly(3-hexylthiophene).
- 12Wang, S.; Fabiano, S.; Himmelberger, S.; Puzinas, S.; Crispin, X.; Salleo, A.; Berggren, M. Experimental Evidence That Short-Range Intermolecular Aggregation Is Sufficient for Efficient Charge Transport in Conjugated Polymers. Proc. Natl. Acad. Sci. U.S.A. 2015, 112 (34), 10599– 10604, DOI: 10.1073/pnas.150138111212Experimental evidence that short-range intermolecular aggregation is sufficient for efficient charge transport in conjugated polymersWang, Suhao; Fabiano, Simone; Himmelberger, Scott; Puzinas, Skomantas; Crispin, Xavier; Salleo, Alberto; Berggren, MagnusProceedings of the National Academy of Sciences of the United States of America (2015), 112 (34), 10599-10604CODEN: PNASA6; ISSN:0027-8424. (National Academy of Sciences)Efficiency, current throughput, and speed of electronic devices are to a great extent dictated by charge carrier mobility. The classic approach to impart high carrier mobility to polymeric semiconductors has often relied on the assumption that extensive order and crystallinity are needed. Recently, however, this assumption has been challenged, because high mobility has been reported for semiconducting polymers that exhibit a surprisingly low degree of order. Here, we show that semiconducting polymers can be confined into weakly ordered fibers within an inert polymer matrix without affecting their charge transport properties. In these conditions, the semiconducting polymer chains are inhibited from attaining long-range order in the π-stacking or alkyl-stacking directions, as demonstrated from the absence of significant X-ray diffraction intensity corresponding to these crystallog. directions, yet still remain extended along the backbone direction and aggregate on a local length scale. As a result, the polymer films maintain high mobility even at very low concns. Our findings provide a simple picture that clarifies the role of local order and connectivity of domains.
- 13Wang, Y.; Guo, M.; Yang, L.; Li, L.; Qin, W.; Yin, S. Toward Morphological Stabilization in Polymer Bulk Heterojunction Solar Cells by Crosslinking Using an Additive. IEEE J. Photovoltaics 2016, 6 (3), 710– 718, DOI: 10.1109/JPHOTOV.2016.2545342There is no corresponding record for this reference.
- 14Landerer, D.; Sprau, C.; Baumann, D.; Pingel, P.; Leonhard, T.; Zimmermann, D.; Chochos, C. L.; Krüger, H.; Janietz, S.; Colsmann, A. Thermal Stabilization of the Bulk-Heterojunction Morphology in Polymer: Fullerene Solar Cells Using a Bisazide Cross-Linker. Solar RRL 2019, 3 (2), 1800266, DOI: 10.1002/solr.201800266There is no corresponding record for this reference.
- 15Wang, S.; Qu, Y.; Li, S.; Ye, F.; Chen, Z.; Yang, X. Improved Thermal Stability of Polymer Solar Cells by Incorporating Porphyrins. Adv. Funct. Mater. 2015, 25 (5), 748– 757, DOI: 10.1002/adfm.201403018There is no corresponding record for this reference.
- 16Jia, Z.; Xia, X.; Wang, X.; Wang, T.; Xu, G.; Liu, B.; Zhou, J.; Li, F. All-Conjugated Amphiphilic Diblock Copolymers for Improving Morphology and Thermal Stability of Polymer/Nanocrystals Hybrid Solar Cells. Front. Mater. Sci. 2018, 12 (3), 225– 238, DOI: 10.1007/s11706-018-0428-xThere is no corresponding record for this reference.
- 17Herrmann, F.; Muhsin, B.; Singh, C. R.; Shokhovets, S.; Gobsch, G.; Hoppe, H.; Presselt, M. Influence of Interface Doping on Charge-Carrier Mobilities and Sub-Bandgap Absorption in Organic Solar Cells. J. Phys. Chem. C 2015, 119 (17), 9036– 9040, DOI: 10.1021/acs.jpcc.5b00124There is no corresponding record for this reference.
- 18Moustafa, E.; Torimtubun, A. A. A.; Pallares, J.; Marsal, L. F. Effect of Additives and Annealing on the Performance of Nonfullerene-Based Binary and Ternary Organic Photovoltaics. Sol. RRL 2022, 6 (5), 2100480, DOI: 10.1002/solr.202100480There is no corresponding record for this reference.
- 19Nam, M.; Yoo, J.; Park, Y.; Noh, H. Y.; Park, Y.; Cho, J.; Kim, J.-A.; Kim, J.; Lee, H. H.; Chang, R. Ternary Blend Organic Solar Cells with Improved Morphological Stability. J. Mater. Chem. A 2019, 7 (16), 9698– 9707, DOI: 10.1039/c9ta00382gThere is no corresponding record for this reference.
- 20Xu, X.; Li, Y.; Peng, Q. Ternary Blend Organic Solar Cells: Understanding the Morphology from Recent Progress. Adv. Mater. 2022, 34 (46), 2107476, DOI: 10.1002/adma.20210747620Ternary Blend Organic Solar Cells: Understanding the Morphology from Recent ProgressXu, Xiaopeng; Li, Ying; Peng, QiangAdvanced Materials (Weinheim, Germany) (2022), 34 (46), 2107476CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)A review. Ternary blend org. solar cells (TB-OSCs) incorporating multiple donor and/or acceptor materials into the active layer have emerged as a promising strategy to simultaneously improve the overall device parameters for realizing higher performances than binary devices. Whereas introducing multiple materials also results in a more complicated morphol. than their binary blend counterparts. Understanding the morphol. is crucially important for further improving the device performance of TB-OSC. This review introduces the soly. and miscibility parameters that affect the morphol. of ternary blends. Then, this review summarizes the recent processes of morphol. study on ternary blends from the aspects of mol. crystallinity, mol. packing orientation, domain size and purity, directly observation of morphol., vertical phase sepn. as well as morphol. stability. Finally, summary and prospects of TB-OSCs are concluded.
- 21Liao, H.-C.; Chen, P.-H.; Chang, R. P.; Su, W.-F. Morphological Control Agent in Ternary Blend Bulk Heterojunction Solar Cells. Polymers 2014, 6 (11), 2784– 2802, DOI: 10.3390/polym6112784There is no corresponding record for this reference.
- 22Park, S. A.; Kim, D. H.; Chung, D.; Kim, J.; Park, T.; Cho, S.; Kim, M. Asymmetric Polymer Additive for Morphological Regulation and Thermally Stable Organic Solar Cells. ACS Appl. Mater. Interfaces 2023, 15 (22), 27026– 27033, DOI: 10.1021/acsami.3c04804There is no corresponding record for this reference.
- 23Habenicht, S. H.; Schramm, S.; Fischer, S.; Sachse, T.; Herrmann-Westendorf, F.; Bellmann, A.; Dietzek, B.; Presselt, M.; Weiß, D.; Beckert, R.; Gorls, H. Tuning the Polarity and Surface Activity of Hydroxythiazoles - Extending the Applicability of Highly Fluorescent Self-Assembling Chromophores to Supra-Molecular Photonic Structures. J. Mater. Chem. C 2016, 4 (5), 958– 971, DOI: 10.1039/C5TC03632A23Tuning the polarity and surface activity of hydroxythiazoles - extending the applicability of highly fluorescent self-assembling chromophores to supra-molecular photonic structuresHabenicht, S. H.; Schramm, S.; Fischer, S.; Sachse, T.; Herrmann-Westendorf, F.; Bellmann, A.; Dietzek, B.; Presselt, M.; Weiss, D.; Beckert, R.; Goerls, H.Journal of Materials Chemistry C: Materials for Optical and Electronic Devices (2016), 4 (5), 958-971CODEN: JMCCCX; ISSN:2050-7534. (Royal Society of Chemistry)A small library of N,N-diethyl- and -diethanolsulfonamides of differently substituted 2-(2-pyridyl)- and 2-pyrazinyl-4-alkoxythiazoles was synthesized and studied in terms of their photophys. properties, electronic structure (quantum chem. calcns. at the CAM-B3LYP/6-31+G(d,p) level of theory) and thin film morphol. (Langmuir-Blodgett- and spin-cast films). By using the Langmuir-Blodgett technique to exert direct control over the degree of aggregation in thin films made from different thiazole type dyes. In combination with spectroscopic studies, the authors gained an in-depth understanding of the influence of aggregation on the electrooptical properties of thin films made of the here-studied substances.
- 24Hupfer, M. L.; Kaufmann, M.; Herrmann-Westendorf, F.; Sachse, T.; Roussille, L.; Feller, K. H.; Weiß, D.; Deckert, V.; Beckert, R.; Dietzek, B.; Presselt, M. On the Control of Chromophore Orientation, Supramolecular Structure, and Thermodynamic Stability of an Amphiphilic Pyridyl-Thiazol Upon Lateral Compression and Spacer Length Variation. ACS Appl. Mater. Interfaces 2017, 9 (50), 44181– 44191, DOI: 10.1021/acsami.7b13042There is no corresponding record for this reference.
- 25Hupfer, M. L.; Kaufmann, M.; May, S.; Preiß, J.; Weiß, D.; Dietzek, B.; Beckert, R.; Presselt, M. Enhancing the Supramolecular Stability of Monolayers by Combining Dipolar with Amphiphilic Motifs: A Case of Amphiphilic Push-Pull-Thiazole. Phys. Chem. Chem. Phys. 2019, 21 (24), 13241– 13247, DOI: 10.1039/C9CP02013FThere is no corresponding record for this reference.
- 26Hupfer, M. L.; Kaufmann, M.; Roussille, L.; Preiß, J.; Weiß, D.; Hinrichs, K.; Deckert, V.; Dietzek, B.; Beckert, R.; Presselt, M. Arylic Versus Alkylic-Hydrophobic Linkers Determine the Supramolecular Structure and Optoelectronic Properties of Tripodal Amphiphilic Push-Pull Thiazoles. Langmuir 2019, 35 (7), 2561– 2570, DOI: 10.1021/acs.langmuir.8b03893There is no corresponding record for this reference.
- 27Hupfer, M. L.; Meyer, R.; Deckert-Gaudig, T.; Ghosh, S.; Skabeev, A.; Peneva, K.; Deckert, V.; Dietzek, B.; Presselt, M. Supramolecular Reorientation During Deposition onto Metal Surfaces of Quasi-Two-Dimensional Langmuir Monolayers Composed of Bifunctional Amphiphilic, Twisted Perylenes. Langmuir 2021, 37 (37), 11018– 11026, DOI: 10.1021/acs.langmuir.1c01525There is no corresponding record for this reference.
- 28Lin, Y.; Nugraha, M. I.; Firdaus, Y.; Scaccabarozzi, A. D.; Aniés, F.; Emwas, A.-H.; Yengel, E.; Zheng, X.; Liu, J.; Wahyudi, W. A Simple N-Dopant Derived from Diquat Boosts the Efficiency of Organic Solar Cells to 18.3%. ACS Energy Lett. 2020, 5 (12), 3663– 3671, DOI: 10.1021/acsenergylett.0c0194928A Simple n-Dopant Derived from Diquat Boosts the Efficiency of Organic Solar Cells to 18.3%Lin, Yuanbao; Nugraha, Mohamad Insan; Firdaus, Yuliar; Scaccabarozzi, Alberto D.; Anies, Filip; Emwas, Abdul-Hamid; Yengel, Emre; Zheng, Xiaopeng; Liu, Jiakai; Wahyudi, Wandi; Yarali, Emre; Faber, Hendrik; Bakr, Osman M.; Tsetseris, Leonidas; Heeney, Martin; Anthopoulos, Thomas D.ACS Energy Letters (2020), 5 (12), 3663-3671CODEN: AELCCP; ISSN:2380-8195. (American Chemical Society)Mol. doping has recently been shown to improve the operating characteristics of org. photovoltaics (OPVs). Here, we prep. neutral Diquat (DQ) and use it as n-dopant to improve the performance of state-of-the-art OPVs. Adding DQ in ternary bulk-heterojunction (BHJ) cells based of PM6:Y6:PC71BM is found to consistently increase their power conversion efficiency (PCE) from 16.7 to 17.4%. Analyses of materials and devices reveal that DQ acts as n-type dopant and morphol. modifier for the BHJ leading to observable changes in its surface topog. The resulting n-doped BHJs exhibit higher optical absorption coeffs., balanced ambipolar transport, longer carrier lifetimes and suppressed bimol. recombination, which are ultimately responsible for the increased PCE. The use of DQ was successfully extended to OPVs based on PM6:BTP-eC9:PC71BM for which a max. PCE of 18.3% (uncertified) was achieved. Our study highlights DQ as a promising dopant for application in next generation org. solar cells.
- 29Jeong, S.; Woo, S.-H.; Lyu, H.-K.; Kim, C.; Kim, H.; Han, Y. S. Improvement of Photovoltaic Properties by Addition of a Perylene Compound in P3ht: Pcbm Bhj System. J. Nanosci. Nanotechnol. 2012, 12 (5), 4147– 4153, DOI: 10.1166/jnn.2012.5898There is no corresponding record for this reference.
- 30Vivo, P.; Dubey, R.; Lehtonen, E.; Kivistö, H.; Vuorinen, T.; Lemmetyinen, H. Dipyrrolidinyl-Substituted Perylene Diimide as Additive for Poly (3-Hexylthiophene):[6, 6]-Phenyl C61 Butyric Acid Methylester Bulk-Heterojunction Blends. Thin Solid Films 2013, 548, 398– 405, DOI: 10.1016/j.tsf.2013.08.106There is no corresponding record for this reference.
- 31Li, F.; Werner, A.; Pfeiffer, M.; Leo, K.; Liu, X. Leuco Crystal Violet as a Dopant for N-Doping of Organic Thin Films of Fullerene C60. J. Phys. Chem. B 2004, 108 (44), 17076– 17082, DOI: 10.1021/jp047861531Leuco Crystal Violet as a Dopant for n-Doping of Organic Thin Films of Fullerene C60Li, Fenghong; Werner, Ansgar; Pfeiffer, Martin; Leo, Karl; Liu, XianjieJournal of Physical Chemistry B (2004), 108 (44), 17076-17082CODEN: JPCBFK; ISSN:1520-6106. (American Chemical Society)The triphenylmethane dye crystal violet (CV) and its leuco base, leucocrystal violet (LCV), are investigated as dopants for n-type doping of fullerene C60. Conductivities up to 8 × 10-3 S/cm at 30° are achieved when C60 is doped with CV. Mass spectroscopy and optical spectroscopy (UV/VIS/NIR absorption and Fourier transform IR transmission) confirm that the leuco base LCV is formed during sublimation of the cationic CV dye. When the com. available LCV was directly used as a dopant in C60, a max. cond. of 1.3 × 10-2 S/cm was obtained at 30°. We found that in both cases, the leuco base became reoxidized to the cationic form by electron transfer to electron-accepting matrixes, leading to the doping effect. The donor properties of LCV in a charge-transfer complex with 7,7,8,8-tetracyanoquinodimethane (TCNQ) were confirmed by UV/VIS/NIR absorption and Fourier transform IR (FTIR) spectroscopy. C60 anions were obsd. in the FTIR or NIR absorption spectra of the mixed films of C60 and LCV. Photoinduced charge transfer between LCV and C60 provides free electrons, which increase the n-type cond. The electron transfer becomes irreversible by hydride abstraction.
- 32Vivo, P.; Kaunisto, K.; Alekseev, A. S.; Pekkola, O.; Tolkki, A.; Chukharev, V.; Lemmetyinen, H. Vectorial Photoinduced Electron Transfer in Multicomponent Film Systems of Poly (3-Hexylthiophene), Porphyrin-Fullerene Dyad, and Perylenetetracarboxidiimide. Photochem. Photobiol. Sci. 2010, 9 (9), 1212– 1217, DOI: 10.1039/c0pp00180eThere is no corresponding record for this reference.
- 33Vivo, P.; Vuorinen, T.; Chukharev, V.; Tolkki, A.; Kaunisto, K.; Ihalainen, P.; Peltonen, J.; Lemmetyinen, H. Multicomponent Molecularly Controlled Langmuir- Blodgett Systems for Organic Photovoltaic Applications. J. Phys. Chem. C 2010, 114 (18), 8559– 8567, DOI: 10.1021/jp100986233Multicomponent Molecularly Controlled Langmuir-Blodgett Systems for Organic Photovoltaic ApplicationsVivo, Paola; Vuorinen, Tommi; Chukharev, Vladimir; Tolkki, Antti; Kaunisto, Kimmo; Ihalainen, Petri; Peltonen, Jouko; Lemmetyinen, HelgeJournal of Physical Chemistry C (2010), 114 (18), 8559-8567CODEN: JPCCCK; ISSN:1932-7447. (American Chemical Society)The capability of Violanthrone-79 (V-79) and N,N'-bis(2,5-di-tert-butylphenyl)-3,4:9,10-perylenebis(dicarboximide) (PDI) to act as electron acceptors, with respect to poly(3-hexylthiophene) (PHT) and to the photoinduced fullerene anion of porphyrin-fullerene (P-F) dyad, was demonstrated in Langmuir-Blodgett films by the time-resolved Maxwell displacement charge method. The introduction of V-79 and PDI in oriented multilayered films led to improved light harvesting and increased lifetime of the charge sepn., enhancing the photocurrent generation measured using a three-electrode photoelectrochem. cell. The best solar cell performance was achieved for the multifunctional film structure where efficient PHT-phthalocyanine heterojunction (PHT|ZnPH4) was combined with the P-F|V-79 system.
- 34Kaloyanova, S.; Zagranyarski, Y.; Ritz, S.; Hanulová, M.; Koynov, K.; Vonderheit, A.; Müllen, K.; Peneva, K. Water-Soluble Nir-Absorbing Rylene Chromophores for Selective Staining of Cellular Organelles. J. Am. Chem. Soc. 2016, 138 (9), 2881– 2884, DOI: 10.1021/jacs.5b1042534Water-Soluble NIR-Absorbing Rylene Chromophores for Selective Staining of Cellular OrganellesKaloyanova, Stefka; Zagranyarski, Yulian; Ritz, Sandra; Hanulova, Maria; Koynov, Kaloian; Vonderheit, Andreas; Muellen, Klaus; Peneva, KalinaJournal of the American Chemical Society (2016), 138 (9), 2881-2884CODEN: JACSAT; ISSN:0002-7863. (American Chemical Society)Biocompatible org. dyes emitting in the near-IR are highly desirable in fluorescence imaging techniques. Herein we report a synthetic approach for building novel small peri-guanidine-fused naphthalene monoimide and perylene monoimide chromophores. The presented structures possess near-IR absorption and emission, high photostability, and good water soly. After a fast cellular uptake, they selectively stain mitochondria with a low background in live and fixed cells. They can be addnl. modified in a one-step reaction with functional groups for covalent labeling of proteins. The low cytotoxicity allows a long time exposure of live cells to the dyes without the necessity of washing. Successful application in localization super-resoln. microscopy was demonstrated in phosphate-buffered saline without any reducing or oxidizing additives.
- 35Fujimoto, K.; Takahashi, M.; Izawa, S.; Hiramoto, M. Development of Perylene-Based Non-Fullerene Acceptors through Bay-Functionalization Strategy. Materials 2020, 13 (9), 2148, DOI: 10.3390/ma13092148There is no corresponding record for this reference.
- 36Hupfer, M. L.; Ghosh, S.; Wang, Y.; Opsomer, T.; Mayerhöfer, T. G.; Dehaen, W.; Presselt, M. Dichroic Dipole Antenna Membranes from Aligned Linear Bophy Dyes. Adv. Mater. Interfaces 2021, 9 (1), 2101490, DOI: 10.1002/admi.202101490There is no corresponding record for this reference.
- 37Hupfer, M. L.; Koszarna, B.; Ghosh, S.; Gryko, D. T.; Presselt, M. Langmuir-Blodgett Films of Diketopyrrolopyrroles with Tunable Amphiphilicity. Langmuir 2021, 37 (34), 10272– 10278, DOI: 10.1021/acs.langmuir.1c01113There is no corresponding record for this reference.
- 38Presselt, M.; Dehaen, W.; Maes, W.; Klamt, A.; Martínez, T.; Beenken, W. J. D.; Kruk, M. Quantum Chemical Insights into the Dependence of Porphyrin Basicity on the Meso-Aryl Substituents: Thermodynamics, Buckling, Reaction Sites and Molecular Flexibility. Phys. Chem. Chem. Phys. 2015, 17 (21), 14096– 14106, DOI: 10.1039/C5CP01808KThere is no corresponding record for this reference.
- 39Mumyatov, A.; Prudnov, F.; Inasaridze, L.; Mukhacheva, O.; Troshin, P. High Lumo Energy Pyrrolidinofullerenes as Promising Electron-Acceptor Materials for Organic Solar Cells. J. Mater. Chem. C 2015, 3 (44), 11612– 11617, DOI: 10.1039/C5TC02509EThere is no corresponding record for this reference.
- 40Hupfer, M. L.; Kaufmann, M.; Preiß, J.; Weiß, D.; Beckert, R.; Dietzek, B.; Presselt, M. Assembly of T-Shaped Amphiphilic Thiazoles on the Air-Water Interface: Impact of Polar Chromophore Moieties, as Well as Dipolarity and Pi-Extension of the Chromophore on the Supramolecular Structure. Langmuir 2019, 35 (7), 2587– 2600, DOI: 10.1021/acs.langmuir.8b04063There is no corresponding record for this reference.
- 41Hupfer, M. L.; Blaschke, D.; Schmidt, H.; Presselt, M. Embedding an Amphiphilic 4-Hydroxy Thiazole Dye in Langmuir Matrices: Studying Miscibilities with Arylic and Alkylic Matrix Amphiphiles Via Langmuir Isotherms and Photo-Induced Force Microscopy. Langmuir 2021, 37 (45), 13255– 13264, DOI: 10.1021/acs.langmuir.1c01772There is no corresponding record for this reference.
- 42Finkelmeyer, S. J.; Askins, E. J.; Eichhorn, J.; Ghosh, S.; Siegmund, C.; Tauscher, E.; Dellith, A.; Hupfer, M. L.; Dellith, J.; Ritter, U.; Strzalka, J.; Glusac, K.; Schacher, F. H.; Presselt, M. Tailoring the Weight of Surface and Intralayer Edge States to Control Lumo Energies. Adv. Mater. 2023, 35 (40), e2305006 DOI: 10.1002/adma.202305006There is no corresponding record for this reference.
- 43Hupfer, M. L.; Dellith, J.; Seyring, M.; Diegel, M.; Dellith, A.; Ghosh, S.; Rettenmayr, M.; Dietzek-Ivanšić, B.; Presselt, M. Bifacial Dye Membranes: Ultrathin and Free-Standing Although Not Being Covalently Bound. Adv. Mater. 2023, 35 (1), 2204874, DOI: 10.1002/adma.202204874There is no corresponding record for this reference.
- 44Bertho, S.; Janssen, G.; Cleij, T. J.; Conings, B.; Moons, W.; Gadisa, A.; D’Haen, J.; Goovaerts, E.; Lutsen, L.; Manca, J. Effect of Temperature on the Morphological and Photovoltaic Stability of Bulk Heterojunction Polymer: Fullerene Solar Cells. Sol. Energy Mater. Sol. Cells 2008, 92 (7), 753– 760, DOI: 10.1016/j.solmat.2008.01.00644Effect of temperature on the morphological and photovoltaic stability of bulk heterojunction polymer:fullerene solar cellsBertho, Sabine; Janssen, Griet; Cleij, Thomas J.; Conings, Bert; Moons, Wouter; Gadisa, Abay; D'Haen, Jan; Goovaerts, Etienne; Lutsen, Laurence; Manca, Jean; Vanderzande, DirkSolar Energy Materials & Solar Cells (2008), 92 (7), 753-760CODEN: SEMCEQ; ISSN:0927-0248. (Elsevier B.V.)In high performance polymer:fullerene bulk heterojunction solar cells the nanoscale morphol. of interpenetrating acceptor:donor materials is optimized through appropriate prepn. conditions such as annealing and choice of solvent, but this initial state-of-the-art morphol. will not remain stable during long-term operation. We report the effects of prolonged storage at elevated temps. on both the morphol. and the photovoltaic performance for the model systems MDMO-PPV:PCBM and poly(3-hexylthiophene):PCBM as compared to high Tg PPV:PCBM based solar cells, where the high Tg PPV is characterized by its high glass transition temp. (138°). In situ monitoring of the photocurrent-voltage characteristics at elevated temps., in combination with a systematic transmission electron microscopy study and complementary optical spectroscopy, reveals distinct degrdn. kinetics and morphol. changes that indicate the occurrence of different underlying physicochem. mechanisms.
- 45Chao, Y.-C.; Chuang, C.-H.; Hsu, H.-L.; Wang, H.-J.; Hsu, Y.-C.; Chen, C.-P.; Jeng, R.-J. Enhanced Thermal Stability of Organic Photovoltaics Via Incorporating Triphenylamine Derivatives as Additives. Sol. Energy Mater. Sol. Cells 2016, 157, 666– 675, DOI: 10.1016/j.solmat.2016.07.04145Enhanced thermal stability of organic photovoltaics via incorporating triphenylamine derivatives as additivesChao, Ying-Chieh; Chuang, Chia-Hsin; Hsu, Hsiang-Lin; Wang, Hsing-Ju; Hsu, Yu-Chi; Chen, Chih-Ping; Jeng, Ru-JongSolar Energy Materials & Solar Cells (2016), 157 (), 666-675CODEN: SEMCEQ; ISSN:0927-0248. (Elsevier B.V.)In this work, we prepd. four star-shaped conjugated small mols., the triphenylamine dithiophene (TBT) derivs., namely TBT-H, TBT-Br, TBT-OH, and TBT-N3 presenting hydride, bromide, hydroxyl, and azide terminal functional groups, resp. These TBT derivs. were used as additives in the active layers of org. photovoltaics to investigate the effect of intermol. interactions (TBT-H, TBT-OH) or crosslinking (TBT-N3, TBT-Br) on the long-term thermal stability of the devices. From analyses of blend film morphologies, and optoelectronic and device performance, we obsd. significant enhancements in thermal stability during accelerated heating tests at 150 °C for the devices incorporated with the additives TBT-N3 and TBT-Br. These two additives functioned as crosslinkers, and constructed local borders that effectively impeded heat-promoted fullerene aggregation, thereby leading to highly stable morphologies. When compared with corresponding normal devices, the TBT-N3-derived devices based on poly(3-hexylthiophene) exhibited greater stability, with the power conversion efficiency (PCE) remaining as high as 2.5% after 144h at 150 °C. Because of this enhancement, a device based on an amorphous low-bandgap polymer, namely poly(thieno[3,4-b]thiophene-alt-benzodithiophene), with the addn. of TBT-N3 was fabricated. We obsd. a significant improvement in device stability, retaining approx. 60% (from 5.0 to 3.3%) of its initial PCE under accelerated heating (150 °C). In contrast, the PCE of the corresponding normal device decayed to 0.01% of its initial value.
- 46Reinspach, J. A.; Diao, Y.; Giri, G.; Sachse, T.; England, K.; Zhou, Y.; Tassone, C.; Worfolk, B. J.; Presselt, M.; Toney, M. F.; Mannsfeld, S.; Bao, Z. Tuning the Morphology of Solution-Sheared P3ht:Pcbm Films. ACS Appl. Mater. Interfaces 2016, 8 (3), 1742– 1751, DOI: 10.1021/acsami.5b09349There is no corresponding record for this reference.
- 47Presselt, M.; Herrmann, F.; Shokhovets, S.; Hoppe, H.; Runge, E.; Gobsch, G. Sub-Bandgap Absorption in Polymer-Fullerene Solar Cells Studied by Temperature-Dependent External Quantum Efficiency and Absorption Spectroscopy. Chem. Phys. Lett. 2012, 542, 70– 73, DOI: 10.1016/j.cplett.2012.05.06347Sub-bandgap absorption in polymer-fullerene solar cells studied by temperature-dependent external quantum efficiency and absorption spectroscopyPresselt, Martin; Herrmann, Felix; Shokhovets, Sviatoslav; Hoppe, Harald; Runge, Erich; Gobsch, GerhardChemical Physics Letters (2012), 542 (), 70-73CODEN: CHPLBC; ISSN:0009-2614. (Elsevier B.V.)We study the sub-bandgap absorption in solar cells made of poly(3-hexylthiophene-2,5-diyl) and [6,6]-Ph C61 butyric acid Me ester (PCBM) by photothermal deflection absorption spectroscopy and measurement of temp.-dependent external quantum efficiency spectra. Several models for sub-bandgap absorption are critically reviewed in view of the external quantum efficiency results. The latter suggest polaron-related transitions as origin of the Gaussian sub-bandgap peak near 1.6 eV. Intermol. charge transfer excitations as an explanation cannot completely be ruled out. However, the assumption of charge transfer excitons with large binding energies is difficult to reconcile with the rapid loss of wt. of the Gaussian sub-bandgap peak seen in external quantum efficiency above room temp.
- 48Presselt, M.; Bärenklau, M.; Rösch, R.; Beenken, W. J. D.; Runge, E.; Shokhovets, S.; Hoppe, H.; Gobsch, G. Sub-Bandgap Absorption in Polymer-Fullerene Solar Cells. Appl. Phys. Lett. 2010, 97 (25), 253302, DOI: 10.1063/1.3527077There is no corresponding record for this reference.
- 49Presselt, M.; Herrmann, F.; Hoppe, H.; Shokhovets, S.; Runge, E.; Gobsch, G. Influence of Phonon Scattering on Exciton and Charge Diffusion in Polymer-Fullerene Solar Cells. Adv. Energy Mater. 2012, 2 (8), 999– 1003, DOI: 10.1002/aenm.20110079349Influence of phonon scattering on exciton and charge diffusion in polymer-fullerene solar cellsPresselt, Martin; Herrmann, Felix; Hoppe, Harald; Shokhovets, Sviatoslav; Runge, Erich; Gobsch, GerhardAdvanced Energy Materials (2012), 2 (8), 999-1003CODEN: ADEMBC; ISSN:1614-6840. (Wiley-Blackwell)Thermally activated transport and phonon scattering in P3HT:PCBM (poly(3-hexylthiophene-2,5-diyl):[6,6]-phenylC61-butyric acid Me ester) bulk heterojunction (BHJ) org. solar cells is studied via temp.-dependent external-quantum-efficiency (EQE) spectroscopy. The hopping barriers for combined exciton and charge transport are balanced for the individual blended materials in a sample, which possesses a blending ratio and a morphol. that give rise to a maximal power-conversion efficiency. Increasing the PCBM wt. fraction leads to a redn. of exciton hopping barriers in PCBM, while for P3HT exciton hopping barriers remain const. This redn. of PCBM exciton hopping barriers is attributed to a higher PCBM crystallinity in the PCBM-rich solar cell as compared to the BHJ with the optimized blending ratio. The morphol.-dependent difference in exciton hopping activation energies between P3HT and PCBM is attributed to a higher impact of phonon scattering in P3HT than in PCBM, as concluded from the much stronger decrease of P3HT-related temp.-dependent external quantum efficiencies above room temp. in the PCBM-rich BHJ solar cell. All EQE data of P3HT:PCBM-based BHJ solar cells is modeled consistently over a broad temp. range by a simple anal. expression involving temp. activation and phonon scattering, without the need to distinguish two sep. hopping regimes.
- 50Hupfer, M. L.; Herrmann-Westendorf, F.; Kaufmann, M.; Weiß, D.; Beckert, R.; Dietzek, B.; Presselt, M. Autonomous Supramolecular Interface Self-Healing Monitored by Restoration of Uv/Vis Absorption Spectra of Self-Assembled Thiazole Layers. Chem.─Eur. J. 2019, 25 (36), 8630– 8634, DOI: 10.1002/chem.201901549There is no corresponding record for this reference.
- 51Hupfer, M.; Herrmann-Westendorf, F.; Dietzek, B.; Presselt, M. In Situ Photothermal Deflection Spectroscopy Revealing Intermolecular Interactions Upon Self-Assembly of Dye Monolayers. Analyst 2021, 146 (16), 5033– 5036, DOI: 10.1039/D1AN00582KThere is no corresponding record for this reference.
- 52Das, S.; Presselt, M. Progress and Development in Structural and Optoelectronic Tunability of Supramolecular Nonbonded Fullerene Assemblies. J. Mater. Chem. C 2019, 7 (21), 6194– 6216, DOI: 10.1039/C9TC00889F52Progress and development in structural and optoelectronic tunability of supramolecular nonbonded fullerene assembliesDas, Saunak; Presselt, MartinJournal of Materials Chemistry C: Materials for Optical and Electronic Devices (2019), 7 (21), 6194-6216CODEN: JMCCCX; ISSN:2050-7534. (Royal Society of Chemistry)A review. Assembly of fullerenes utilizing self-organization at solvent/non-solvent interfaces or by introducing hydrophobic(philic) end-groups have yielded diverse molecularly-ordered structures. Taking advantage of the multiple π-π interaction between adjacent C60-moieties, structurally elegant and functionally promising fullerene assemblies were synthesized by several groups over the last 20 yr. Considerable improvement of device parameters is witnessed if non-covalent fullerene layers assembled using interfacial self assembly are used as electron extn. layer, for example in hybrid solar cells. Thus a pre-detd. choice of C60-nanostructures for photovoltaic application stems from an understanding of fullerene-fullerene interaction, a priori from the mol. level. Could we eventually define the outcomes of the last 3 decades of fullerene aggregation chem.. This review summarizes the course of understanding of optoelectronic properties of fullerene-morphologies, bridging the gap between single mol. and device scale which shall be significant for their judicious implementation in mol. electronics.
- 53Das, S.; Herrmann-Westendorf, F.; Schacher, F. H.; Tauscher, E.; Ritter, U.; Dietzek, B.; Presselt, M. Controlling Electronic Transitions in Fullerene Van Der Waals Aggregates Via Supramolecular Assembly. ACS Appl. Mater. Interfaces 2016, 8 (33), 21512– 21521, DOI: 10.1021/acsami.6b06800There is no corresponding record for this reference.
- 54Ghosh, R.; Spano, F. C. Excitons and Polarons in Organic Materials. Acc. Chem. Res. 2020, 53 (10), 2201– 2211, DOI: 10.1021/acs.accounts.0c0034954Excitons and Polarons in Organic MaterialsGhosh, Raja; Spano, Frank C.Accounts of Chemical Research (2020), 53 (10), 2201-2211CODEN: ACHRE4; ISSN:0001-4842. (American Chemical Society)Conspectus: Excitons and polarons play a central role in the electronic and optical properties of org. semiconducting polymers and mol. aggregates, and are of fundamental importance in understanding the operation of org. optoelectronic devices such as solar cells and light-emitting diodes. For many conjugated org. mols. and polymers, the creation of neutral electronic excitations or ionic radicals is assocd. with significant nuclear relaxation, the bulk of which occurs along the vinyl-stretching mode or the arom.-quinoidal stretching mode when conjugated rings are present. Within a polymer chain or mol. aggregate, nuclear relaxation competes with energy- and charge-transfer, mediated by electronic interactions between the constituent units (repeat units for polymers and individual chromophores for a mol. aggregate); for neutral electronic excitations, such inter-unit interactions lead to extended excited states or excitons, while for pos. (or neg.) charges, interactions lead to delocalized hole (or electron) polarons. The electronic coupling as well as the local coupling between electronic and nuclear degrees of freedom in both excitons and polarons can be described with a Holstein Hamiltonian. However, although excitons and polarons derive from similarly structured Hamiltonians, their optical signatures are quite distinct, largely due to differing ground states and optical selection rules. In this Account, we explore the similarities and differences in the spectral response of excitons and polarons in org. polymers and mol. aggregates. We limit our anal. to the subspace of excitons and hole polarons contg. at most one excitation; hence, we omit the influence of bipolarons, biexcitons, and higher multiparticle excitations. Using a generic linear array of coupled units as a model host for both excitons and polarons, we compare and contrast the optical responses of both quasiparticles, with a particular emphasis on the spatial coherence length, the length over which an exciton or polaron possesses wave-like properties important for more efficient transport. For excitons, the UV-vis absorption spectrum is generally represented by a distorted vibronic progression with H-like or J-like signatures depending on the sign of the electronic coupling, Jex. The spectrum broadens with increasing site disorder, with the spectral area preserved due to an oscillator strength sum rule. For (hole) polarons, the generally stronger electronic coupling results in a mid-IR spectrum consisting of a narrow, low-energy peak (A) with energy near a vibrational quantum of the vinyl stretching mode, and a broader, higher-energy feature (B). In contrast to the UV-vis spectrum, the mid-IR spectrum is invariant to the sign of the electronic coupling, th, and completely resistant to long-range disorder, where it remains entirely homogeneously broadened. Even in the presence of short-range disorder, the width of peak A remains surprisingly narrow as long as |th| remains sufficiently large, a property that can be understood in terms of Herzberg-Teller coupling. Unlike for excitons, for polarons, the absorption spectral area decreases with increasing short-range disorder σ (i.e., there is no oscillator sum rule) reflective of a decreasing polaron coherence length. The intensity of the low-energy peak A in relation to B is an important signature of polaron coherence. By contrast, for excitons, the absorption spectrum contains no unambiguous signs of exciton coherence. One must instead resort to the shape of the steady-state photoluminescence spectrum. The Holstein-based model has been highly successful in accounting for the spectral properties of mol. aggregates as well as conjugated polymers like poly(3-hexylthiophene) (P3HT) in the mid-IR and UV-vis spectral regions.
- 55Clark, J.; Silva, C.; Friend, R. H.; Spano, F. C. Role of Intermolecular Coupling in the Photophysics of Disordered Organic Semiconductors: Aggregate Emission in Regioregular Polythiophene. Phys. Rev. Lett. 2007, 98 (20), 206406, DOI: 10.1103/PhysRevLett.98.20640655Role of Intermolecular Coupling in the Photophysics of Disordered Organic Semiconductors: Aggregate Emission in Regioregular PolythiopheneClark, Jenny; Silva, Carlos; Friend, Richard H.; Spano, Frank C.Physical Review Letters (2007), 98 (20), 206406/1-206406/4CODEN: PRLTAO; ISSN:0031-9007. (American Physical Society)The authors address the role of excitonic coupling on the nature of photoexcitations in the conjugated polymer regioregular poly(3-hexylthiophene). By temp.-dependent absorption and photoluminescence spectroscopy, optical emission is overwhelmingly dominated by weakly coupled H aggregates. The relative absorbance of the 0-0 and 0-1 vibronic peaks provides a powerfully simple means to ext. the magnitude of the intermol. coupling energy, of ∼5 and 30 meV for films spun from isodurene and CHCl3 solns., resp.
- 56Alam, S.; Anand, A.; Islam, M. M.; Meitzner, R.; Djoumessi, A. S.; Slowik, J.; Teklu, Z.; Fischer, P.; Kästner, C.; Khan, J. I. P3ht: Pcbm Polymer Solar Cells from a Didactic Perspective. J. Photonics Energy 2022, 12 (3), 035501, DOI: 10.1117/1.jpe.12.035501There is no corresponding record for this reference.
- 57Cardona, C. M.; Li, W.; Kaifer, A. E.; Stockdale, D.; Bazan, G. C. Electrochemical Considerations for Determining Absolute Frontier Orbital Energy Levels of Conjugated Polymers for Solar Cell Applications. Adv. Mater. 2011, 23 (20), 2367– 2371, DOI: 10.1002/adma.20100455457Electrochemical Considerations for Determining Absolute Frontier Orbital Energy Levels of Conjugated Polymers for Solar Cell ApplicationsCardona, Claudia M.; Li, Wei; Kaifer, Angel E.; Stockdale, David; Bazan, Guillermo C.Advanced Materials (Weinheim, Germany) (2011), 23 (20), 2367-2371CODEN: ADVMEW; ISSN:0935-9648. (Wiley-VCH Verlag GmbH & Co. KGaA)Narrow bandgap conjugated polymers in combination with fullerene acceptors are under intense investigation in the field of org. photovoltaics (OPVs). The open circuit voltage, and thereby the power conversion efficiency, of the devices is related to the offset of the frontier orbital energy levels of the donor and acceptor components which are widely detd. by cyclic voltammetry. Inconsistencies have appeared in the use of the ferrocenium/ferrocene (Fc+/Fc) redox couple, as well as the values used for the abs. potentials of std. electrodes, which can complicate the comparison of materials properties and detn. of structure/property relationships.
- 58Titov, A. V.; Ufimtsev, I. S.; Luehr, N.; Martinez, T. J. Generating Efficient Quantum Chemistry Codes for Novel Architectures. J. Chem. Theory Comput. 2013, 9 (1), 213– 221, DOI: 10.1021/ct300321a58Generating Efficient Quantum Chemistry Codes for Novel ArchitecturesTitov, Alexey V.; Ufimtsev, Ivan S.; Luehr, Nathan; Martinez, Todd J.Journal of Chemical Theory and Computation (2013), 9 (1), 213-221CODEN: JCTCCE; ISSN:1549-9618. (American Chemical Society)We describe an extension of our graphics processing unit (GPU) electronic structure program TeraChem to include atom-centered Gaussian basis sets with d angular momentum functions. This was made possible by a "meta-programming" strategy that leverages computer algebra systems for the derivation of equations and their transformation to correct code. We generate a multitude of code fragments that are formally math. equiv., but differ in their memory and floating-point operation footprints. We then select between different code fragments using empirical testing to find the highest performing code variant. This leads to an optimal balance of floating-point operations and memory bandwidth for a given target architecture without laborious manual tuning. We show that this approach is capable of similar performance compared to our hand-tuned GPU kernels for basis sets with s and p angular momenta. We also demonstrate that mixed precision schemes (using both single and double precision) remain stable and accurate for mols. with d functions. We provide benchmarks of the execution time of entire SCF calcns. using our GPU code and compare to mature CPU based codes, showing the benefits of the GPU architecture for electronic structure theory with appropriately redesigned algorithms. We suggest that the meta-programming and empirical performance optimization approach may be important in future computational chem. applications, esp. in the face of quickly evolving computer architectures.
- 59Beenken, W. J. D.; Sun, M.; Zhao, G.; Pullerits, T. Excited State Properties of Neutral and Charged Ter-Fluorene with and without a Keto-Defect. Phys. Status Solidi B 2008, 245 (5), 849– 853, DOI: 10.1002/pssb.200743442There is no corresponding record for this reference.
- 60Song, C.; Wang, L.-P.; Sachse, T.; Preiß, J.; Presselt, M.; Martínez, T. J. Efficient Implementation of Effective Core Potential Integrals and Gradients on Graphical Processing Units. J. Chem. Phys. 2015, 143 (1), 014114, DOI: 10.1063/1.4922844There is no corresponding record for this reference.
- 61Presselt, M.; Dietzek, B.; Schmitt, M.; Rau, S.; Winter, A.; Jäger, M.; Schubert, U. S.; Popp, J. A Concept to Tailor Electron Delocalization: Applying Qtaim Analysis to Phenyl-Terpyridine Compounds. J. Phys. Chem. A 2010, 114 (50), 13163– 13174, DOI: 10.1021/jp107007a61A Concept to Tailor Electron Delocalization: Applying QTAIM Analysis to Phenyl-Terpyridine CompoundsPresselt, Martin; Dietzek, Benjamin; Schmitt, Michael; Rau, Sven; Winter, Andreas; Jager, Michael; Schubert, Ulrich S.; Popp, JurgenJournal of Physical Chemistry A (2010), 114 (50), 13163-13174CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)To gain a deeper understanding of how structural modifications may influence photochem. properties of 4'-phenyl-2,2':6',2''-terpyridines, the investigations presented here focus on electron delocalization in 4'-phenyl-2,2':6',2''-terpyridine derivs. and their Ru(II) and Zn(II) complexes. In those systems of neighboring arom. rings the considerable torsion between the rings is commonly regarded to be the limiting factor for a well pronounced π-conjugation between the rings. A common approach to improve the π-conjugation is to lower the steric hindrance, thus achieving a more planar geometry. Here, we present a fundamentally different approach towards enhanced π-conjugation by manipulation of the electronic properties of the pyridine-Ph (py-ph) bond. This is accomplished by introducing various substituents at the phenylene moiety or coordinating the terpyridine moiety to transition metal ions. The electron delocalization was quantified via the DFT-calcd. ellipticity in the bond-crit. point (BCP) of the py-ph bond. This ellipticity can be modified due to substituents in the para position of phenylene and via the transition metals coordinated to the terpyridine moiety. Changes in electron d. distribution induced by the substituents and the metal ions are further studied by means of intermol. electron d. difference plots. It was shown that a NH2 group in the para position of the Ph ring as well as the coordination to Ru(II) or Zn(II) ions significantly enhances the π-character of the py-ph bond. Surprisingly, an even higher π-character of the py-ph bond is achieved by introducing addnl. NH2 groups in ortho position to the py-ph bond, despite the increased torsion between pyridine and phenylene. The introduction of other substituents (-NO2, -Br, -CN, -vinyl, -ethynyl) studied within the presented work enables an actuation of the electron delocalization between terpyridine and phenylene. In doing so, the ellipticity is a concise quantity to characterize electron delocalization in the studied systems. Furthermore, the ellipticity in the BCP of the py-ph bond is related to the corresponding geometrical properties (e.g., bond length and dihedral angle) and to the DFT-calcd. HOMO and LUMO energies.
- 62Presselt, M.; Schnedermann, C.; Muller, M.; Schmitt, M.; Popp, J. Derivation of Correlation Functions to Predict Bond Properties of Phenyl–CH Bonds Based on Vibrational and 1H NMR Spectroscopic Quantities. J. Phys. Chem. A 2010, 114 (37), 10287– 10296, DOI: 10.1021/jp105348d62Derivation of Correlation Functions to Predict Bond Properties of Phenyl-CH Bonds Based on Vibrational and 1H NMR Spectroscopic QuantitiesPresselt, Martin; Schnedermann, Christoph; Mueller, Michael; Schmitt, Michael; Popp, JuergenJournal of Physical Chemistry A (2010), 114 (37), 10287-10296CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)The study of electron d. properties significantly contributes to the detn. of important chem. relations. The exptl. detn. of the electron d. distribution is limited to single crystals. However, equiv. information is often desired for mols., which do not crystallize in a sufficient manner. Furthermore, it is of high impact to study changes in the electron d. distribution (i.e., related reactivities) upon environmental variations. Consequently, here we investigate methods to derive electron d. properties from spectroscopic data. In particular correlation functions are introduced, which are able to predict electron d. properties in all five CH-bonds of monosubstituted benzene derivs. at once. The prediction performance for electron densities and the corresponding Laplacians is lower as compared to previously introduced local functions, but far less spectroscopic input data are needed. However, for ellipticities a higher prediction performance than this obtained for the previously derived local functions could be obtained despite the fact that less spectroscopic data were used. Thus, ellipticities are best predicted using 1H NMR data for the para position of monosubstituted benzene derivs.
- 63Beenken, W.; Presselt, M.; Ngo, T. H.; Dehaen, W.; Maes, W.; Kruk, M. Molecular Structures and Absorption Spectra Assignment of Corrole Nh Tautomers. J. Phys. Chem. A 2014, 118 (5), 862– 871, DOI: 10.1021/jp411033h63Molecular Structures and Absorption Spectra Assignment of Corrole NH TautomersBeenken, Wichard; Presselt, Martin; Ngo, Thien H.; Dehaen, Wim; Maes, Wouter; Kruk, MikalaiJournal of Physical Chemistry A (2014), 118 (5), 862-871CODEN: JPCAFH; ISSN:1089-5639. (American Chemical Society)The individual absorption spectra of the two NH tautomers of 10-(4,6-dichloropyrimidin-5-yl)-5,15-dimesitylcorrole are assigned on the basis of the Gouterman four-orbital model and a quantum chem. TD-DFT study. The assignment indicates that the red-shifted T1 tautomer is the one with protonated pyrrole nitrogen atoms N(21), N(22) and N(23), whereas the blue-shifted T2 tautomer has pyrrole nitrogen atoms N(21), N(22) and N(24) protonated. A wave-like nonplanar distortion of the macrocycle in the ground state is found for both NH tautomers, with the wave axis going through the pyrroles contg. N(22) and N(24). The 7C plane detd. by the least-squares distances to the carbon atoms C1, C4, C5, C6, C9, C16, and C19 is suggested as a mean corrole macrocycle plane for the anal. of out-of-plane distortions. The magnitude of these distortions is distinctly different for the two NH tautomers, leading to substantial perturbations of their acid-base properties, which are rationalized by the interplay of the degree of out-of-plane distortion of the macrocycle as a whole and the tendency of the pyrrole nitrogen atoms toward pyramidalization, with the former leading to a basicity increase whereas the latter enhances the acidity.
- 64Presselt, M.; Wojdyr, M.; Beenken, W. J. D.; Kruk, M.; Martinez, T. J. Steric and Electronic Contributions to the Core Reactivity of Monoprotonated 5-Phenylporphyrin: A Dft Study. Chem. Phys. Lett. 2014, 603 (0), 21– 27, DOI: 10.1016/j.cplett.2014.04.011There is no corresponding record for this reference.
- 65Preiß, J.; Jäger, M.; Rau, S.; Dietzek, B.; Popp, J.; Martínez, T.; Presselt, M. How Does Peripheral Functionalization of Ruthenium(Ii)-Terpyridine Complexes Affect Spatial Charge Redistribution after Photoexcitation at the Franck-Condon Point?. ChemPhysChem 2015, 16 (7), 1395– 1404, DOI: 10.1002/cphc.201500223There is no corresponding record for this reference.
- 66Fischer, S.; Vestfrid, J.; Mahammed, A.; Herrmann-Westendorf, F.; Schulz, M.; Muller, J.; Kiesewetter, O.; Dietzek, B.; Gross, Z.; Presselt, M. Photometric Detection of Nitric Oxide Using a Dissolved Iron(Iii) Corrole as a Sensitizer. ChemPlusChem 2016, 81 (7), 594– 603, DOI: 10.1002/cplu.201500553There is no corresponding record for this reference.
- 67Preiß, J.; Herrmann-Westendorf, F.; Ngo, T. H.; Martínez, T.; Dietzek, B.; Hill, J. P.; Ariga, K.; Kruk, M. M.; Maes, W.; Presselt, M. Absorption and Fluorescence Features of an Amphiphilic Meso-Pyrimidinylcorrole: Experimental Study and Quantum Chemical Calculations. J. Phys. Chem. A 2017, 121 (45), 8614– 8624, DOI: 10.1021/acs.jpca.7b08910There is no corresponding record for this reference.
- 68Sachse, T.; Martinez, T. J.; Presselt, M. On Combining the Conductor-Like Screening Model and Optimally Tuned Range-Separated Hybrid Density Functionals. J. Chem. Phys. 2019, 150 (17), 174117, DOI: 10.1063/1.506473068On combining the conductor-like screening model and optimally tuned range-separated hybrid density functionalsSachse, Torsten; Martinez, Todd J.; Presselt, MartinJournal of Chemical Physics (2019), 150 (17), 174117/1-174117/8CODEN: JCPSA6; ISSN:0021-9606. (American Institute of Physics)Range-sepd. hybrid functionals whose range-sepn. parameter γ has been nonempirically tuned to a particular mol. have been shown to yield frontier orbital energies and other properties in very good agreement with expts. However, many cases, such as org. optoelectronic devices, require the description of mols. embedded in an environment. This can be done by combining the γ-tuning procedure with polarizable continuum models in general and the very versatile conductor-like screening model in particular. There are at least two different ways of performing this combination. The partially vertical γ-tuning employs equil. solvation throughout. The strictly vertical γ-tuning, on the other hand, employs nonequil. solvation to obtain ionization energies. In this article, we compare ground-state and excited-state properties of several different mols. relevant to org. optoelectronics that were obtained using both of the two different tuning procedures. While there are significant differences in the ground-state properties, we see virtually no difference in the excited-state properties. Given these results, we conclude that both tuning procedures have to be used in conjunction for the correct description of both ground-state and excited-state properties. (c) 2019 American Institute of Physics.
- 69Kozlíková, B.; Krone, M.; Falk, M.; Lindow, N.; Baaden, M.; Baum, D.; Viola, I.; Parulek, J.; Hege, H.-C. Visualization of Biomolecular Structures: State of the Art Revisited. Computer Graphics Forum 2017, 36 (8), 178– 204, DOI: 10.1111/cgf.13072There is no corresponding record for this reference.
Supporting Information
Supporting Information
The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acsaelm.3c01722.
Comparison of J–V plots for different concentrations of PMIDA-C12 additive, details of vibrational progression fittings of UV–vis absorption spectra, UV–vis and PL spectra of pristine P3HT and PC60BM films, comparison of photothermal deflection spectra of fresh and thermally aged films, and SWV analysis of PMIDA-C12 additive and details of the synthesis procedure of PMIDA-C12 additive molecule (PDF)
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