logo
CONTENT TYPES

Figure 1Loading Img

Bent-Shaped p-Type Small-Molecule Organic Semiconductors: A Molecular Design Strategy for Next-Generation Practical Applications

  • Toshihiro Okamoto*
    Toshihiro Okamoto
    Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    University of Tokyo Advanced Operando-Measurement Technology Open Innovation Laboratory (OPERANDO-OIL), National Institute of Advanced Industrial Science and Technology (AIST), 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    PRESTO, JST, 4-1-8 Honcho, Kawaguchi, Saitama 332-0012, Japan
    *[email protected]
  • Craig P. Yu
    Craig P. Yu
    Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    More by Craig P. Yu
  • Chikahiko Mitsui
    Chikahiko Mitsui
    Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
  • Masakazu Yamagishi
    Masakazu Yamagishi
    Department of Applied Chemistry and Chemical Engineering, National Institute of Technology, Toyama College, 13 Hongo-machi, Toyama City, Toyama 939-8630, Japan
  • Hiroyuki Ishii
    Hiroyuki Ishii
    Department of Applied Physics, Faculty of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573, Japan
  • , and 
  • Jun Takeya
    Jun Takeya
    Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    University of Tokyo Advanced Operando-Measurement Technology Open Innovation Laboratory (OPERANDO-OIL), National Institute of Advanced Industrial Science and Technology (AIST), 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    MANA, National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba 205-0044, Japan
    More by Jun Takeya
Cite this: J. Am. Chem. Soc. 2020, 142, 20, 9083–9096
Publication Date (Web):April 15, 2020
https://doi.org/10.1021/jacs.9b10450
Copyright © 2020 American Chemical Society
ACS AuthorChoiceACS AuthorChoice
Article Views
6291
Altmetric
-
Citations
LEARN ABOUT THESE METRICS

Article Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.

Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.

The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated.

PDF (4 MB)
Supporting Info (1)»

Abstract

Significant progress has been made in both molecular design and fundamental scientific understanding of organic semiconductors (OSCs) in recent years. Suitable charge-carrier mobilities (μ) have been obtained by many high-performance OSCs (μ > 10 cm2 V–1 s–1), but drawbacks remain, including low solution processability and poor thermal durability. In addition, since aggregation of OSCs involves weak intermolecular interactions, the molecules are perpetually in thermal motion, even in the solid state, which disrupts charge-carrier transport. These issues limit potential applications of OSCs. The present work examines a molecular design for hole-transporting (p-type) OSCs based on the “bent-shaped” geometry with specific molecular orbital configurations, which aims to enhance effective intermolecular orbital overlaps, stabilize crystal phases, suppress detrimental molecular motions in the solid state, and improve solution processability. The results indicated that such OSCs have high μ and suitable solution processability, and are resistant to ambient and thermal conditions, making them suitable for practical applications.

Introduction

ARTICLE SECTIONS
Jump To

Organic semiconductors (OSCs) are of intense scientific and technological interest due to their potential incorporation in printable and flexible electronics, such as organic field-effect transistors (OFETs),(1−4) organic light-emitting diodes (OLEDs),(5,6) organic photovoltaics (OPVs),(7−11) and organic thermoelectrics (OTE).(12−15) In contrast to their inorganic semiconductor counterparts,(16) the functions of OSCs are governed by intermolecular charge transport between adjacent π-conjugated molecules, molecular geometry, and electronic characteristics.(17−26) Thus, rational, versatile molecular design could lead to the development of high-performance, printable OSCs that are suitable for large-scale industrial production.
The general requirements for printable, flexible electronic devices include (1) high chemical stability under ambient conditions without the need for special precautions, (2) high charge-carrier mobility (μ) that exceeds the performance of conventional amorphous silicon (e.g., 0.5–1.0 cm2 V–1 s–1)(27) and is competitive with that of metal-oxide semiconductors, (3) sufficient solubility in common organic solvents that allows low-cost solution processing for device fabrication, (4) high thermal durability (highly stable crystal phase above 150 °C to withstand fabrication processes),(28) and (5) facile synthetic routes for large-scale production.
To date, various molecular designs based on π-conjugated materials have been reported, with the aim of achieving the high performance required for the aforementioned applications.(29−40) Representative molecular designs in the literature have utilized linear or quasi-linear π-electron cores (π-cores) such as pentacene,(41) [1]benzothieno[3,2-b][1]benzothiophene (BTBT),(42) and dinaphtho[2,3-b:2′,3′-f]thieno[3,2-b]thiophene (DNTT)(43) as a means of obtaining effective intermolecular π-orbital overlaps necessary for charge transport in the solid state (Figure 1).(4,44) These π-cores aggregate through multiple intermolecular C–H···π, S···S, and S···π interactions and form two-dimensional (2D) herringbone (HB)-type packing structures that favor 2D charge carrier transport.(45) Various studies have also focused on side-chain engineering with bulky alkylsilyl,(46,47) linear alkyl,(48−52) and unsymmetrical substituents(53−57) in order to improve the solubility and tune the aggregated structures of these π-cores (Figure 1). As a result, high-performance and solution-processable OSCs with these substituted π-cores having excellent μ (>10 cm2 V–1 s–1) have been reported.(58−60) However, both linear and quasi-linear alkyl-substituted π-cores have exhibited phase transitions from crystalline to liquid crystalline or other crystal phases at temperatures around 90–130 °C,(42,61−63) leading to degradation of transistor performance at elevated temperatures during device fabrication. It has also been recently reported that unsymmetrical substituted BTBT analogues aggregate to form a highly crystalline liquid crystal phase.(53) These challenges associated with various representative OSCs illustrate that it is still difficult to simultaneously achieve sufficient solubility, thermal durability, and high μ with conventional molecular design strategies based on OSC π-cores.

Figure 1

Figure 1. Molecular structures of representative organic semiconductors.

Recently, several fascinating studies have been reported concerning the detrimental effects of large-amplitude molecular motions on the performance of high-mobility OSCs such as pentacene and BTBT derivatives.(64−67) Sirringhaus and co-workers also suggested that the dynamic disorder of OSCs in the solid state might be the parameter having the most harmful effect on charge transport.(67) Hence, it is apparent that future rational molecular design not only should be guided by intramolecular characteristics or intermolecular orbital overlaps, but also must aim to reduce unfavorable molecular motions via unique π-core structures and effective side-chain engineering.
To meet all the aforementioned requirements for promising next-generation OSCs, our group has proposed a series of conceptually new bent-shaped π-cores.(68−73) The traditional linear and quasi-linear molecules have small radii of rotation and translation, which lead to low thermal durability as a result of constant molecular motions. In contrast, bent-shaped molecular geometries possess increased radii of rotation and translation, which suppress detrimental molecular motions in the solid state and simultaneously confer high μ and thermal durability (Figure 2).(74) Another feature of the bent-shaped geometry compared to conventional linear and quasi-linear geometries is an enhanced internal dipole moment resulting from reduced molecular symmetry. On this basis, we attempted to develop highly soluble π-cores that can be solution-processed to fabricate OFETs and that permit fine-tuning of molecular packing structures with further side-chain engineering. Our group has thus far synthesized a series of bent-shaped molecules, including first- and second-generation OSCs, as well as extended analogues. Sulfur atoms were incorporated into these compounds to allow tuning of the electronic structures (specifically, the highest occupied molecular orbital (HOMO) energy level) to achieve efficient hole injections during OFET operations under ambient conditions. In addition, the large HOMO coefficient of the sulfur atom produces favorable intermolecular short-range interactions with adjacent π-cores. These lead to large intermolecular orbital overlaps (increased transfer integral (t) values) and also suppress molecular motions in the solid state.

Figure 2

Figure 2. Molecular designs of first- and second-generation bent-shaped OSCs.

Herein, we summarize our recent work regarding the molecular design of bent-shaped OSCs by providing a detailed analysis of the synthesis, aggregated structures (complemented by theoretical calculations), ionization potentials, thermal stabilities, and solubilities of these compounds. The OFET performances of these bent-shaped OSCs are also presented to demonstrate the effectiveness of the molecular designs. We hope that this work will assist future molecular design of OSCs toward the development of high-performance next-generation electronics materials.

Molecular Design

ARTICLE SECTIONS
Jump To

First-Generation OSCs Based on V- and N-Shaped π-Cores

DNT-V

The V-shaped dinaphtho[2,3-b:2′,3′-d]thiophene (DNT-V) π-core was developed for p-channel OFET applications.(68)DNT-V features a thiophene in the center position that is fused by two naphthalene units on each side. The V-shaped molecular geometry and reduced molecular symmetry of this molecule produce an internal dipole moment that is not present in linear molecules, along with a stabilized crystalline phase (which suppresses molecular motions) and high solubility(75) in common organic solvents. Density functional theory (DFT) calculations revealed a delocalized distribution of HOMO coefficients across the backbone and a large HOMO coefficient of the sulfur atom (Figure 3a). The HOMO level of DNT-V was calculated to be −5.62 eV, which is higher than that of BTBT (−5.79 eV)(42) at the B3LYP/6-311G(d) level. In terms of reorganization energies for hole transport (λh), our calculations estimate a λh of 138 meV for DNT-V, which is significantly smaller than that for BTBT (226 meV) and almost equal to that of DNTT (130 meV).(76) The large HOMO coefficient for the sulfur atom suggests that the central sulfur-based heterocycle is different from thiophene. From the nucleus-independent chemical shift (NICS),(77,78) we hope to gain fundamental understanding on the molecular properties of such fused heterocyclic systems, as well as predict their molecular assemblies and charge transports. Indeed, NICS calculations showed that the central ring is more similar to the less aromatic compound 2,3,4,5-tetramethylenetetrahydrothiophene (thiophenoradialene)(79) (NICS(0) = −2.6 ppm) than to 2,3,4,5-tetramethylthiophene (NICS(0) = −11.6 ppm). Owing to this molecular feature, the large HOMO coefficient for sulfur can potentially contribute to significant intermolecular orbital overlaps that promote hole transports.

Figure 3

Figure 3. Molecular structures, NICS values (calculated at the HF/6-31+G(d)//B3LYP/6-31G(d) level), HOMO coefficients and energy levels, and dipole moments (calculated at the B3LYP/6-311G(d)//B3LYP/6-31G(d) level) of the (a) DNT-V, (b) DAT-V, (c) DNBDT-N, and (d) TBBT-V OSCs.

DAT-V

The recent molecular design of dianthra[2,3-b:2′,3′]thiophene (DAT-V)(71) (Figure 3b) involves the expansion of π-conjugation from the dinaphthalene moiety of DNT-V to a dianthracene group while preserving the overall V-shaped geometry. DFT calculations demonstrate a highly delocalized distribution of HOMO coefficients across the backbone and a sizable HOMO coefficient for the sulfur atom that is similar to that of DNT-V. Extending the π-conjugation increases the calculated HOMO energy level of DAT-V to −5.32 eV, compared to −5.62 eV for DNT-V, which is expected to lower the injection barrier and threshold voltage in OFET operation. NICS calculations showed that the central sulfur-based heterocycle exhibits a much lower degree of aromaticity (NICS(0) = −2.1 ppm). Another attractive feature of the DAT-V π-core is the reduced λh value (99 meV), which is significantly smaller than those for DNT-V (138 meV) and DNTT (130 meV).(76)

DNBDT-N

The N-shaped (dinaphtho[2,3-d:2′,3′-d′]benzo[1,2-b:4,5-b′]dithiophene (DNBDT-N)(70) π-core (Figure 3c) is also considered as an extended V-shaped DNT-V π-core. DNBDT-N adopts a bent-shaped molecular geometry at two terminals that further suppresses molecular motions and stabilizes the crystal phase. The HOMO distribution of DNBDT-N is spread across the entire π-core, including a large coefficient of sulfur atoms. This scenario results in effective intermolecular orbital overlaps. The HOMO level calculated for DNBDT-N is −5.51 eV. This value is significantly higher than that for DNT-V and is attributed to the extended π-electron system of DNBDT-N. NICS calculations showed that the two heterocycle rings exhibit aromatic characteristics intermediate between those of thiophene and thiophenoradialene (NICS(0) = −4.9 ppm). In addition, the increased molecular weight of DNBDT-N compared to the smaller DNT-V molecule would also impart improved thermal durability to thin-film devices.

TBBT-V

The V-shaped thieno[3,2-f:4,5-f′]bis[1]benzothiophene (TBBT-V) molecule (Figure 3d) has electronic and geometric characteristics similar to those of DNT-V, although the outer aromatic units are changed from benzene to thiophene rings. One of the obvious advantages associated with this modification is the ease of functionalizing the more reactive thiophene units, whereas the terminal benzene groups of the DNT-V π-core cannot be selectively functionalized. The HOMO level of the TBBT-V π-core was determined to be −5.64 eV, which is the same as that of DNT-V. However, the terminal thiophene units of the parent TBBT-V can be readily functionalized. As an example, the HOMO level of methyl-substituted TBBT-V (Me-TBBT-V) is increased to −5.50 eV, and further fine-tuning of the HOMO levels can be achieved depending on the choice of substitution. NICS calculations for TBBT-V revealed that the central heterocycle ring exhibits higher aromaticity than the other V- and N-shaped π-cores (NICS(0) = −5.7 ppm). With the incorporation of thiophene in TBBT-V, a high internal dipole moment of 2.14 D is obtained, indicating the potential for device fabrication based on solution processing.

Second-Generation OSCs Based on W- and Zigzag-Shaped π-Cores

DNT-W

The molecular design of W-shaped dinaphtho[1,2-b:2′,1′-d]thiophene (DNT-W) (Figure 4) was inspired by the well-known picene backbone. Picene has been reported as a hole-transporting p-type OSC, although the performance of picene-based OFETs has been shown to be unstable under ambient conditions.(80−82) Moreover, the crystal structure of this compound suggests a relatively large displacement along the long axis, indicating the potential for significant variations in intermolecular orbital overlaps. Thus, we envisioned that a DNT-W π-core incorporating sulfur would provide effective and consistent intermolecular orbital overlaps as well as suppressed molecular motions. In fact, the HOMO and next HOMO (NHOMO) coefficients determined for DNT-W (EHOMO = −5.83 eV, ENHOMO = −5.86 eV) were determined to be almost degenerate. The calculation results show delocalized distributions of the HOMO and NHOMO and also a unique continuous NHOMO having a single phase over the entire π-core. Furthermore, NICS calculations for DNT-W determined that the central heterocycle ring has an almost aromatic character (NICS(0) = −7.3 ppm). These unique characteristics of DNT-W suggest that it will provide the required degree of orbital overlap and also give a well-anchored molecular assembly, leading to high μ.

Figure 4

Figure 4. Molecular structures, NICS(0) values (calculated at the HF/6-31+G(d)//B3LYP/6-31G(d) level), HOMO and NHOMO coefficients and their energy levels, and dipole moments (calculated at the B3LYP/6-311G(d)//B3LYP/6-31G(d) level) of V-, W-, and zigzag-shaped π-cores.

ChDT

Our most recent zigzag-shaped π-core, chryseno[2,1-b:8,7-b′]dithiophene (ChDT), can be considered to be an extended version of DNT-W (Figure 4). In the case of ChDT, HOMO coefficients indicating the same phase (EHOMO = −5.68 eV) extend across the entire π-core, including the terminal thiophene sulfur atoms, which is the same as the NHOMO in DNT-W. NICS calculations for ChDT showed that the terminal heterocycle ring and other aromatic rings have the same aromatic character as benzene (NICS(0) = −9.2 ppm). The incorporation of two terminal thiophene units lowered the HOMO energy levels of ChDT derivatives, which is expected to promote hole injection and provide lower threshold voltages. These terminal thiophene groups also allow facile derivatizations due to the highly reactive α-positions.

Synthesis

ARTICLE SECTIONS
Jump To

The synthetic route to DNT-V and its derivatives is illustrated in Scheme 1. Previously, the synthesis of a similar sulfur-bridged π-core was reported via a 10-step process, but gave only a 12% total yield.(83) In the present work, we developed a facile four-step synthesis to obtain the target compounds using the readily available compound 1 as a starting material. The first step features a selective ortho-lithiation with n-BuLi followed by a Fe(acac)3-catalyzed oxidative homocoupling to afford the dimerized 2 in good yield. After a demethylation reaction using BBr3, the sulfur atom is installed on the naphthalene dimer using thiocarbamoyl, followed by a solventless annulation via Newman–Kwart rearrangement(84) at 320 °C, to generate the target compound DNT-V in 42% total yield over four steps. Various alkyl-substituted DNT-V derivatives can be obtained by means of the same synthetic route using alkylated versions of 1 as starting materials.

Scheme 1

Scheme 1. Synthesis of DNT-V Derivativesa

aReagents and conditions: (a) n-BuLi, Fe(acac)3, 0 °C to rt, 73% (R = C10H21); (b) BBr3, 0 °C to rt, 94% (R = H), 97% (R = C10H21); (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 78% (R = H), 75% (R = C10H21); (d) 300–320 °C, 81% (R = H), 77% (R = C10H21).

Recently, our group developed a simple alternative synthetic route that provides the DNT-V core in only three steps (Scheme 2). This process employs a modification of a previously reported strategy using compound 5 as the starting material to afford the key precursor 6 in excellent yield.(85) A subsequent reduction of the tetraone compound 7 with aqueous hydroiodic acid in acetic acid affords DNT-V in 97% yield, with a total yield of 77% over three steps. Thus, this represents an improvement compared to our previous route. Our current synthetic scheme also avoids the high-temperature Newman–Kwart rearrangement featured in the previous strategy. In addition, expensive transition metal catalysts such as palladium are not required, and the synthesis is well-suited to large-scale production.

Scheme 2

Scheme 2. Modified DNT-V Synthesisa

aReagents and conditions: (a) (1) dithiooxamide, DMF, 55 °C, (2) Et3N, rt, 89%; (b) m-CPBA, CH2Cl2, 30 °C, 88%; (c) HI, AcOH, reflux, 97%.

Although a synthesis of DAT-V was previously reported,(86) we synthesized DAT-V via a process similar to that used to obtain DNT-V (Scheme 3). We employed the anthracene-based precursor 8 as the starting material and conducted a Fe(acac)3-catalyzed homocoupling to afford the dimer, followed by a demethylation with BBr3 to give compound 10 in excellent yield. From 11, we carried out a Newman–Kwart rearrangement to generate DAT-V in satisfactory yield.

Scheme 3

Scheme 3. Synthesis of DAT-Va

aReagents and conditions: (a) n-BuLi, Fe(acac)3, 0 °C to rt, 52%; (b) BBr3, 0 °C to rt, 96%; (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 61%; (d) 300 °C, 68%.

DNBDT-N and decyl-substituted DNBDT-NW (C10-DNBDT-NW) were synthesized in a manner similar to that used for DNT-V and its derivatives (Scheme 4). From 1, selective lithiation with n-BuLi followed by transmetalation afforded the arylzinc intermediate, which was further reacted with 1,4-dibromo-2,5-dimethoxybenzene via Negishi cross-coupling to provide 12 in good yield. Subsequently, demethylation with BBr3 generated the tetra-hydroxyl intermediate 13 with subsequent installation of thiocarbamate groups. The target DNBDT-N derivatives were realized by the Newman–Kwart rearrangement under solventless conditions in 64–67% yield.

Scheme 4

Scheme 4. Synthesis of DNBDT-N Derivativesa

aReagents and conditions: (a) (1) n-BuLi, ZnCl2, 0 °C to rt, (2) 1,4-dibromo-2,5-dimethoxybenzene, PdCl2(dppp), 50 °C, 87% (R = H), 85% (R = C10H21); (b) BBr3, 0 °C to rt, 81% (R = H), 92% (R = C10H21); (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 53% (R = H), 72% (R = C10H21); (d) 310–320 °C, 67% (R = H), 64% (R = C10H21).

The TBBT-V π-core was synthesized according to a procedure previously reported in the literature.(87) This parent π-core was then used to produce three derivatives: C10-TBBT-V, α-C10-Th-TBBT-V, and β-C10-Th-TBBT-V (Scheme 5). TBBT-V was brominated by sequential treatment with lithium 2,2,6,6-tetramethylpiperidide (to deprotonate the α-positions of the thiophene) and 1,2-dibromo-1,1,2,2-tetrachloroethane, to afford Br-TBBT-V. C10-TBBT-V was synthesized in 64% yield, whereas α-C10-Th-TBBT-V and β-C10-Th-TBBT-V were furnished in 86% and 92% yields, respectively. The facile reactions at the α-positions demonstrate the ease of functionalization of TBBT-V and the ready tuning of its molecular properties.

Scheme 5

Scheme 5. Synthesis of TBBT-V Derivativesa

aReagents and conditions: (a) C10H21ZnCl2, PdCl2(dppf)·CH2Cl2, toluene, 70 °C, 64%; (b) (5-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 86%; (c) (4-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 92%.

DNT-W was furnished in a one-pot reaction according to a previously reported procedure.(88) The synthesis of ChDT (Scheme 6) started from compound 15, which was readily synthesized according to a literature procedure.(89) From 15, a halogen–lithium exchange and a transmetalation with zinc chloride were performed, followed by a Negishi cross-coupling to install the thiophene moieties, giving an overall yield of 79%. Facile removal of the trimethylsilyl protecting groups was carried out under basic conditions to give compound 17 in excellent yield. Subsequently, we used PtCl2 to catalyze the 6-exo-dig double cyclizations in DMF to furnish the ChDT π-core in satisfactory yield.(90) The α-positions of the thiophene were readily brominated by sequential treatments with lithium tetramethylpiperidide and 1,1,2,2-tetrachloro-1,2-dibromoethane to afford the key precursor Br-ChDT in 88% yield. Two ChDT derivatives, C10-ChDT and C10-Th-ChDT, were prepared using Negishi and Stille cross-coupling reactions, respectively, in excellent yields.

Scheme 6

Scheme 6. Synthesis of ChDT Derivativesa

aReagents and conditions: (a) (1) n-BuLi, THF, −78 °C, (2) ZnCl2, THF, 0 °C, (3) 3-bromothiophene, Pd2(dba)3·CHCl3, THF, 50 °C, 79%; (b) K2CO3, MeOH, CH2Cl2, rt, 99%; (c) PtCl2, DMF, 80 °C, 58%; (d) (1) LiTMP, THF, −78 °C to −50 °C, (2) 1,2-dibromo-1,1,2,2-tetrachloroethane, −78 °C to rt, 88%; (e) C10H21ZnCl, PdCl2(dppf)·CH2Cl2, THF, 70 °C, 80%; (f) (4-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 81%.

Aggregated Structures, Theoretical Calculations, Thermal Stabilities, Ionization Potentials, and Solubilities

ARTICLE SECTIONS
Jump To

Aggregated Structures and Theoretical Calculations

To understand the aggregated structures and charge-carrier transports of the current bent-shaped OSCs, we examined single crystals of the bent-shaped parent π-cores and their derivatives, grown by either physical vapor transport (PVT)(91,92) or solution techniques, using X-ray diffraction (XRD). A common feature observed in single crystals of V-shaped OSCs was their slightly bent geometries (Figure 5 and Table 1), which differ from the planar conformations suggested by DFT studies. The bent angles increased when substituents were added to the π-cores, as a result of increased attractive intermolecular interactions. N-shaped and second-generation zigzag-shaped OSCs were also observed. The bent geometry in these derivatives potentially allowed for C–H···π and S···π interactions between the prominent central sulfur atom and the adjacent backbone. As a result, higher degrees of intermolecular HOMO overlaps and greater suppression of molecular motions were realized, both of which improve charge-carrier transport and thermal durability.

Figure 5

Figure 5. Representative slightly bent geometries of C10-DNT-VW and C10-DNBDT-NW (front and side views) in single crystals.

Table 1. Packing Modes and Twist Angles for V-, N-, and W-Shaped Derivatives
compoundpacking modebent angle (deg)
DNT-VHB13.9
C10-DNT-VWHB13.3
C10-DNT-VVHB18.0
DAT-VHB17.2
TBBT-VHB10.0
C10-TBBT-VHB11.3
DNBDT-Nπ–π stacking (π–π), slipped HB0.0
C10-DNBDT-NWHB9.7
DNT-WHB9.1
The parent DNT-V, DAT-V, and TBBT-V π-cores were found to adopt 2D HB packing structures, whereas the DNBDT-N demonstrated a less attractive one-dimensional (1D) π–π stacking motif that does not favor charge transport (Table 1). Following the incorporation of various substituents, the packing structures of the V-shaped OSCs were effectively modified to give high degrees of intermolecular orbital overlap, as indicated by the increased absolute t values (Table 2). As for the sign of t, the negative and positive intermolecular orbital overlaps result in positive and negative transfer integrals, respectively (Figure 6).

Figure 6

Figure 6. Relation between sign of transfer integral and intermolecular orbital overlap.

Table 2. Summary of Transfer Integrals for V-Shaped Derivatives
  transfer integral, t (meV)b
compoundpacking mode and HB angle (deg)atHT|tHH||tTT|
DNT-VHB, 45.8°+374613
C10-DNT-VWHB, 45.3°+18c14c32c
+45d61d37d
C6-DNT-VWHB, 46.4°+44c63c36c
+19d10d17d
C10-DNT-VVHB, 36.0°+354215
DAT-VHB, 38.9°+41206.4
C10-TBBT-VHB, 43.6°+526710
a

Herringbone (HB) angles between two mean planes of the π-cores were 56.4° (at 293 K),(93) 52.5° (at 293 K),(43) and 51.1° (at 200 K)(52) for C8-BTBT, DNTT, and C10-DNTT as references.

b

Transfer integrals were calculated at the PBEPBE/6-31G(d) level.

c

Transfer integrals between HOMOs.

d

Transfer integrals between NHOMOs.

Both C10-DNT-VW and C6-DNT-VW had larger absolute t values than the DNT-V π-core, whereas C10-DNT-VV exhibited lower t values (Figure 7). Since C10- and C6-DNT-VW exhibit almost the same HOMO and NHOMO energy levels, the t values between these levels are estimated, and are listed in Table 2. The packing structures of the DNT-V series suggest that more effective intermolecular orbital overlaps were achieved by installing the alkyl chains in the VW fashion. As a consequence, the charge transport capabilities were significantly affected by the alkyl chain positions. Owing to the intrinsic disorder of the α-C10-Th-TBBT-V and β-C10-Th-TBBT-V, only C10-TBBT-V single crystals could be obtained from the TBBT-V series. The HB packing structure of the C10-TBBT-V showed a significantly larger t value in the head-to-tail (tHT) direction than in the head-to-head (tHH) and tail-to-tail (tTT) directions, suggesting anisotropic 2D charge-transport properties.

Figure 7

Figure 7. Representative packing structures and transfer integrals for (a) C10-DNT-VW and (b) C10-DNT-VV for their HOMOs (and NHOMO).

Different from the 1D π–π stacking structure of DNDBT-N, C10-DNBDT-NW formed an HB motif with a layer-by-layer structure (Figure 8). The 2D cofacial molecular arrangement through strong π–π and C–H···π interactions resulted in equal t in the column and transverse directions (tc = +52 meV, tt = +51 meV), demonstrating favorable 2D charge-transport properties (Table 3).

Figure 8

Figure 8. Representative packing structures and transfer integrals for (a) DNBDT-N and (b) C10-DNBDT-NW.

Table 3. Summary of Transfer Integrals for N-Shaped Derivatives
  transfer integral, t (meV)b
compoundpacking mode and HB angle (deg)atcolumn (tc)|ttrans| (|tt|)
DNBDT-Nπ–π and slipped HB, 126.5°+3.27.3
C10-DNBDT-NWHB, 46.7°+5251
a

Herringbone (HB) angles between two mean planes of the π-cores.

b

Transfer integrals were calculated at the PBEPBE/6-31Gd level.

The second-generation zigzag-shaped OSCs all exhibited HB packing structures in the crystalline state (Table 4). DNT-W showed reasonable positive t values in the head-to-tail (tHT) and tail-to-tail (tTT) directions, but larger absolute t values in the transverse head-to-head (tHH) direction (Figure 9). The ChDT derivatives showed strong intermolecular C–H···π and S···π interactions in the HB motif. The parent ChDT demonstrated large absolute t values in both the column (tc) and transverse (tt) directions, but adding C10-alkyl chains on both sides dramatically lowered the absolute t value in the transverse direction. Consequently, the C10-ChDT shows 1D charge transport. Although the tc and tt values for C10-Th-ChDT are well-balanced, these values are relatively small compared to other ChDT derivatives. Thus, the primary reason for the smaller absolute t values for C10-Th-ChDT is the much longer π–π stacking distance (6.90 Å) compared to ChDT (5.97 Å), due to the steric hindrance of the decylthienyl groups.

Figure 9

Figure 9. Representative packing structures and transfer integrals for (a) DNT-W, (b) C10-ChDT, and (c) C10-Th-ChDT.

Table 4. Summary of (Top) Transfer Integrals of DNT-W and (Bottom) Transfer Integrals, Lattice Constants in the Column Direction, and Effective Masses for C10-ChDT, C10-Th-ChDT, and C10-DNBDT-NW
  transfer integral, t (meV)a
compoundpacking mode and HB angle (deg)atHT|tHH||tTT|
DNT-WHB, 41.6°+416240
 
  transfer integral, t (meV)b  
compoundpacking mode and HB angle (deg)atcolumn (tc)c|ttrans| (|tt|)lattice constant in the column direction, dc (Å)effective mass,cm||*/m0,dm*/m0e
C10-ChDTHB, 89.2°–66224.8612.55, 17.2
C10-Th-ChDTHB, 39.2°+31246.8991.86, 5.85
C10-DNBDT-NWHB, 46.7°+52516.1271.31, 2.52
a

Herringbone (HB) angles between two mean planes of the π-core.

b

t values were calculated at the PBEPBE/6-31G(d) level.

c

m0 is the electron rest mass.

d

m* in the column direction.

e

m* in the transverse direction.

Experimental studies have revealed that OSCs having high μ show band transport characteristics,(59,70,74,94,95) with delocalized wave-like carriers over multiple molecules. Based on the band theory, the mobility μ of carrier with charge q is inversely proportional to the effective mass (m*) according to the following equation:where τ is the relaxation time. HOMO band structures, E(k), are obtained by the tight-binding approximation using t values. Effective masses of holes are calculated as the following equation along the respective directions:In the case of the HB-type packing structure studied herein, the top of the HOMO band is located on the Γ (k = 0) point, and the column direction exhibits the highest mobility, except for C10-ChDT. Therefore, we investigate 1/m* at the Γ point along the column direction, given by the following equation:Here, tcolumn (tc or tHT) and ttrans (tt or tHH, tTT) (see Figures 79) refer to the transfer integrals in the column (H-to-T) and transverse (H-to-H and T-to-T) directions of HB packing motif, respectively, and d refers to the lattice constant in the column direction. That is, the reciprocal of the effective mass is proportional to the transfer integral and the square of the lattice constant. In particular, tc is twice as effective as tt, and its sign (whether they are either positive or negative) is also important, as described in Figure 6.
Notably, the effective mass in the column and transverse directions (m||* and m*) for C10-Th-ChDT (1.86 m0 and 5.85 m0) was found to be much smaller and more isotropic than for C10-ChDT (m||* = 2.55 m0 and 17.2 m0) and nearly comparable to that of C10-DNBDT-NW (m||* = 1.31 m0 and 2.52 m0) (see Figure 10). These data indicate that increasing the lattice constant of C10-Th-ChDT in the column direction compensates for the reduction of the transfer integral, resulting in a small effective mass.

Figure 10

Figure 10. HOMO band structures and effective masses of (a) C10-DNBDT-NW and (b) C10-ChDT. The origin of energy axis is set to HOMO level of the molecule. Insets show the first Brillouin zone with symmetry points of Γ(0,0,0), Y(0,π/b,0), Z(0,0,π/c), and S(0,π/b,π/c), where b and c are the lattice constants shown in Figures 8b and 9b. The column directions correspond to Γ–Z (C10-DNBDT-NW) and Γ–Y (C10-ChDT) directions in the reciprocal lattice.

Motivated by the intriguing HOMO configuration of ChDT, we investigated the variance in tt) values. It should be noted that the out-of-plane motion was the most prominent direction of molecular vibrations in the HB packing (Figure 11).(67) A smaller Δt of 5 meV was determined for ChDT, compared to those for DNTT (13 meV) and pentacene (29 meV) over the range of 0.13–0.18 Å. The small Δt for ChDT is a good indication of consistent intermolecular orbital overlaps in the solid state.

Figure 11

Figure 11. Values of t and Δt for ChDT, DNTT, and pentacene.

Thermal Stability

One crucial benefit of the bent-shaped molecular design is the prevention of phase transitions at low temperatures by the suppression of molecular motions. Analysis of the DNT-V derivatives by thermogravimetry (TG) did not show any thermal decomposition before 500 °C. Differential scanning calorimetry (DSC) studies also demonstrated high phase transition temperatures of 202 and 151 °C for C6- and C10-DNT-VW, respectively, but a value of only 90 °C in the case of C10-DNT-VV. This lower temperature is attributed to the large displacements between adjacent molecules in the crystal packing structure of this compound, which result in reduced structural stability. The C10-DNBDT-NW showed higher phase transition and decomposition temperatures than the V-shaped C10-DNT-VW, resulting from the multiple intermolecular interactions and higher molecular weight of the former. C10-DNBDT-NW in a thin film device demonstrated no phase transition up to 200 °C. More importantly, C10-DNBDT-NW is a double V-shaped molecule, and thus should exhibit more effective suppression of molecular motions and stabilization of the crystalline phase compared to the DNT-V series. Both C10-TBBT-V and β-C10-Th-TBBT-V showed multiple phase transition peaks during differential thermal analyses, potentially due to their lower structural rigidity and intrinsic disordering. In contrast, α-C10-Th-TBBT-V showed a phase transition peak above 200 °C. The zigzag-shaped C10-ChDT and C10-Th-ChDT exhibited no phase transitions until above 250 °C. The excellent thermal stability of the current bent-shaped OSCs confirm their physical and chemical robustness, which would permit common purification techniques such as sublimation and PVT. These materials would also be expected to be thermally durable in the solid state.

Ionization Potentials

The electronic properties of these OSCs were further examined using photoelectron yield spectroscopy (PYS) to evaluate the ionization potential (IP) values. The resulting IP values were generally in good agreement with the HOMO energy levels calculated based on DFT. The DNT-V π-core was found to have a somewhat high IP of 5.72 eV, while extending the π-conjugation gave a considerably smaller IP of 5.21 eV for DAT-V. TBBT-V demonstrated an IP of 5.61 eV, similar to that for DNT-V. However, C10-TBBT-V, α-C10-Th-TBBT-V, and β-C10-Th-TBBT-V demonstrated effective tuning of the IP due to the synthetic versatility of the TBBT-V π-core, with values of 5.26, 5.10, and 5.01 eV, respectively. The IP value for the extended N-shaped C10-DNBDT-NW was 5.24 eV, which also indicates an improvement relative to the DNT-V series. The zigzag-shaped DNT-W showed a large IP of 5.87 eV as a result of its relatively short π-conjugation, while the extended analogues C10-ChDT and C10-Th-ChDT had values of 5.56 and 5.53 eV, respectively. Overall, these data confirm fine-tuning of the IP values of the current bent-shaped OSCs by modifying the π-conjugation length and varying the functional groups. Such modifications achieved air-stable p-type performance, and also would be expected to reduce the injection barrier and threshold voltage associated with OFET operations.

Solubility

In contrast to the poor solubility of unsubstituted linear and quasi-linear π-cores (e.g., <0.001 wt% in toluene for DNTT), DNT-V demonstrated superior solubility of up to 0.30 wt% in common organic solvents such as chloroform and toluene at room temperature. Alkyl-substituted DNT-V derivatives showed improved solubility, ranging from 0.38 to 1.53 wt% in the case of the DNT-VW series. In addition, extremely high solubilities in the range of 9.23–15.6 wt% were achieved with the DNT-VV derivative. The unsubstituted TBBT-V showed high solubility on the order of 0.1 wt% due to its large internal dipole moment, while C10-TBBT-V possessed the highest solubility of up to 1.1 wt%. Owing to the increased π-conjugation and molecular weight of DNBDT-N, the parent π-core exhibited limited solubility. However, the incorporation of C10-alkyl chains resulted in adequate solubility for C10-DNBDT-NW of up to 0.043 wt% in common organic solvents at a slightly elevated temperature. Having an equally extended π-conjugated system, C10-ChDT and C10-Th-ChDT showed higher solubilities of 0.068 and 0.13 wt% in toluene, respectively, than C10-DNBDT-NW. The high solubility and thermally stable crystal phases of the bent-shaped OSCs suggest that they show promises with regard to applications in thin-film OFET fabrication via solution-processing methods.

Summary of Properties

The bent-shaped OSCs presented herein exhibit unique NICS values, which suggest that the fused sulfur-containing heterocycles behave more like thiophenoradialene, rather than thiophene. The consequence of such behaviors is that the sulfur atom possesses protruding HOMO that are likely to reinforce the molecular assembly and charge transports. The aggregated structures of bent-shaped OSCs all exhibit some degree of nonplanarity, or bentness, which lead to enhancement of their intermolecular interactions in the favorable herringbone packing structures. Theoretical calculations of transfer integrals and effective masses suggest favorable charge transport properties that are promising for achieving high μ. Thermal studies suggest that the bent-shaped OSCs are thermally stable, and their crystal phases are thermally durable for sustaining elevated-temperature fabrication processes. Compared to the conventional linear and quasi-linear OSCs, the bent-shaped OSCs have their unique advantages to achieve high-performance and robust OSCs for future practical applications.

OFET Performance

ARTICLE SECTIONS
Jump To

To evaluate the device performance of bent-shaped OSCs, single-crystalline-based bottom-gate/top-contact OFETs were fabricated using either manual lamination (ML) or the solution-processed edge-casting (EC) technique that our group previously developed(48−51) (Figure 12 and Supporting Information). These p-channel OFETs were produced by adding the strong electron acceptor F4-TCNQ between the OSC layer and the gold electrodes to reduce contact resistance. The transistors employed SiO2/Si substrates treated with heptadecafluorodecyltrimethoxysilane (F-DTS) in conjunction with the ML technique and either decyltrimethoxysilane (DTS) or β-phenylethyltrimethoxysilane (β-PTS) for the EC technique. All devices incorporating bent-shaped derivatives demonstrated air-stable p-channel OFET characteristics.

Figure 12

Figure 12. Schematic diagrams of (a) the manual lamination and (b) edge-casting techniques.

The parent DNT-V single-crystalline thin-film OFET achieved a satisfactory μh of 1.5 cm2 V–1 s–1, which is similar to the value obtained for a vacuum-deposited polycrystalline thin-film OFET (1.1 cm2 V–1 s–1). [All reported μ values are summarized in Table 5.] The highest μh of 9.5 cm2 V–1 s–1 was demonstrated by single-crystalline C6-DNT-VW grown using the EC technique. This result was expected based on our transfer integral calculations, because this derivative possessed the largest absolute t values in all directions. The other C10-DNT-VW derivative exhibited a comparable maximum μh of 6.5 cm2 V–1 s–1, whereas C10-DNT-VV showed a μh of 1.0 cm2 V–1 s–1. Transmission XRD analyses confirmed that thin-film diffractions of the DNT-V series match with their single-crystal packing structures and that their crystal growth direction was along the b-axis (column) direction (Figure 7). Polycrystalline thin-film OFETs incorporating C6-DNT-VW and C10-DNT-VW fabricated by vacuum deposition also demonstrated decent μh values of 4.0 and 3.7 cm2 V–1 s–1, respectively. The trend of μh observed for the DNT-V derivatives was in perfect agreement with their t values. Moreover, C6-DNT-VW-based transistors demonstrated thermal resistance up to 150 °C.(68)
Table 5. Characteristics of Field-Effect Transistors with Bent-Shape π-Cores
compoundprocess,a SAM, and SiO2 thickness (nm)μmax (cm2/(V·s))μavg (cm2/(V·s))b
DNT-VVD,c DTS, 5001.10.91
DNT-VML, F-DTS, 5001.51.0
C6-DNT-VWVD,d DTS, 5003.73.6
C6-DNT-VWEC, β-PTS, 5009.56.2
C10-DNT-VVVD,d DTS, 5000.450.39
C10-DNT-VVEC, DTS, 5001.00.76
C10-DNT-VWVD,d DTS, 5004.03.6
C10-DNT-VWEC, DTS, 5006.54.0
DAT-VML, F-DTS, 5002.0n.a.e
C10-TBBT-VVD,d DTS, 2001.11.0
C10-TBBT-VDC, β-PTS, 2004.02.0
C10-TBBT-VEC, β-PTS, 2006.24.6
α-C10-Th-TBBT-VEC, β-PTS, 2000.550.53
β-C10-Th-TBBT-VEC, β-PTS, 2002.31.6
DNBDT-NML, F-DTS, 5000.06n.a.c
C10-DNBDT-NWEC, β-PTS, 1001612.1
DNT-WML, F-DTS, 5001.6n.a.e
ChDTML, F-DTS, 5003.1n.a.e
C10-ChDTEC, β-PTS, 5002.6n.a.e
C10-Th-ChDTEC, β-PTS, 50010n.a.e
C8-BTBTEC, DTS, 5005.0n.a.e
C10-DNTTGC, DTS, 500117.0
a

ML, manual lamination process; VD, vacuum deposition process; EC, edge-casting process; DC, drop-casting process; GC, gap-casting process.

b

μavg is the average of mobilities for more than 10 devices.

c

Data at substrate temperature (Tsub) of room temperature.

d

Data at Tsub of 100 °C.

e

μavg was not available because a sufficient number of devices was not evaluated.

PVT-grown single crystals of DAT-V were manually laminated on the OFET substrates. In view of the packing motif and charge transport direction of DAT-V, the OFET channel was constructed along the b-axis to maximize μh, with the assistance of in-plane XRD analysis. The highest μh of 2.0 cm2 V–1 s–1 was obtained with DAT-V. When OFET channels were constructed along the a axis, a lower μh of 1.1 cm2 V–1 s–1 was obtained.(71)
The highest μh of 6.2 cm2 V–1 s–1 was exhibited by the C10-TBBT-V single-crystalline OFET, while α-C10-Th-TBBT-V and β-C10-Th-TBBT-V produced mediocre μh values of 0.55 and 2.3 cm2 V–1 s–1, respectively. Although the C10-TBBT-V device demonstrated a slightly lower μh than C10-DNT-VW (6.5 cm2 V–1 s–1), it showed a lower threshold voltage of −20 to −15 V compared to C10-DNT-VW (−30 to −25 V). In addition, C10-TBBT-V demonstrated excellent solution-processability, and the resulting drop-cast thin-film transistor achieved a μh of 4.0 cm2 V–1 s–1. Owing to the extended π-conjugation of α-C10-Th-TBBT-V and β-C10-Th-TBBT-V, their transistor devices showed significantly lower threshold voltages of 0 to −10 V, albeit with relatively low μh. From the transmission XRD data, we confirmed that the solution-processed single-crystalline C10-TBBT-V thin film regained its single-crystal packing structure, and that the crystal growth direction was along the b-axis, as was also the case for the DNT-V series (column direction, Figure 7).
C10-DNBDT-NW formed excellent single-crystalline thin films using either the EC technique or the continuous EC technique over large areas.(48−51) Optical microscopic and atomic force microscopy images indicated a smooth crystal surface with steps having a height of one C10-DNBDT-NW molecule, indicating well-oriented crystalline films. (Figure 13a,b). Air-stable p-channel OFET performance was obtained using C10-DNBDT-NW with a maximum μh of 16 cm2 V–1 s–1 (Figure 13c,d). A large on/off ratio of 106 to 107 and a small threshold voltage of −10 to 0 V were also determined for the C10-DNBDT-NW device. The small threshold voltage for this material can be attributed to its low IP value (5.24 eV) resulting from the extended π-conjugated core. Moreover, C10-DNBDT-NW-based transistors demonstrated higher thermal resistance up to 200 °C. In addition, Hall effect measurements suggested significant hole diffusion. Thus, the C10-DNBDT-NW-based OSC exhibited a band transport mechanism with delocalized charge-carriers over the OSC layer.(94,95) Furthermore, we have recently reported that bending a flexible device incorporating a C10-DNBDT-NW single-crystalline film caused uniaxial lattice compression and led to a mobility increase of 70% under 3% strain. An in-depth analysis showed that this compression suppresses molecular motion.(96)

Figure 13

Figure 13. (a) Bottom-gate–top-contact device structure and packing structure of C10-DNBDT-NW on the substrate and (b) optical microscopy image. (c) Transfer and (d) output characteristics of the OFET based on a C10-DNBDT-NW single-crystalline film.

DNT-W afforded flat platelet crystals when employing PVT, which could be simply laminated on substrates for OFET evaluation. The resulting DNT-W-based OFETs exhibited typical p-channel transfer and output characteristics with negligible hysteresis and an air-stable μh of 1.6 cm2 V–1 s–1. Despite the encouraging results obtained from our first second-generation zigzag-shaped DNT-W, the associated OFET suffered from a substantial threshold voltage (−50 V), a high injection barrier between the gold electrode and the semiconductor layer (due to the large IP value of 5.87 eV), and a μh insufficient for high-performance electronics. Recently, Yasuda and co-workers developed an original synthetic route for C8-substituted dinaphtho[1,2-b:2′,1-d]chalcogenophenes (DNE), including dinaphtho[1,2-b:2′,1-d]thiophene (DNT), dinaphtho[1,2-b:2′,1-d]selenophene (DNS), and dinaphtho[1,2-b:2′,1-d]tellurophene (DNTe).(97) Incorporation of the alkyl chain increased the solubility of these DNE derivatives such that solution-processing for device fabrication was viable. The introduction of tellurium in DNTe also effectively lowered its IP value to 5.24 eV. However, the threshold voltages of the C8-DNE series remained high.
In the case of the extended zigzag-shaped ChDT π-core, a decent μh of 3.1 cm2 V–1 s–1 was obtained from a single-crystalline thin film by the ML technique. It is worth noting that the threshold voltage for ChDT (−25 V) was found to be significantly improved compared to that for DNT-W due to its extended π-conjugation. C10-ChDT and C10-Th-ChDT both formed well-oriented single-crystalline thin films with smooth surfaces when applying the EC technique and showed maximum μh values of 2.6 and 10 cm2 V–1 s–1, respectively. The high μh exhibited by these ChDT derivatives may be correlated with their low Δt values, that the π-core is insensitive to detrimental molecular motions and shows consistent intermolecular orbital overlaps.
Thermal stress test of high-mobility C10-DNBDT-NW OSCs using solution-processed single-crystalline films on silicon substrates at 200 °C, were performed in transistors. To evaluate the thermal durability of C10-DNBDT-NW accurately, the transistors were prepared as follows: (1) The solution-processed single-crystalline films prepared by the edge-casting method were annealed at 200 °C for 10 min under nitrogen conditions. (2) After the film cooled to room temperature, the F4-TCNQ and gold electrodes were deposited. Notably, it was found that the mobility was unchanged, while the threshold voltage showed a slight positive shift. This might be due to the decrement of channel traps such as water and oxygen by annealing at high temperature. As a comparison, the other transistor was annealed at the same temperature after the F4-TCNQ and gold electrodes were deposited. In this case, the mobility was slightly decreased. This result might be attributed to the morphology change at the interface between OSC and F4-TCNQ. Therefore, the solution-processed single-crystalline film of C10-DNBDT-NW possesses thermal durability over 200 °C.

Conclusions and Future Perspectives

ARTICLE SECTIONS
Jump To

In this Perspective, we have summarized recent advances in the development of bent-shaped OSCs for OFET applications. The bent-shaped molecules presented herein all demonstrated an excellent distribution of HOMO coefficients, leading to effective intermolecular orbital overlaps as well as electronic structures suitable for air-stable p-type OFET operation and charge injection. The incorporation of sulfur leads to a large HOMO coefficient for the sulfur atom that induces various heteroatom interactions and contributes to the reinforcement of the favorable HB packing structure in the solid state. It is apparent that the bent-shaped geometry contributes to the stabilization of the crystal phases of the OSCs, resulting in high thermal durability. Our work with V-shaped OSCs having bent-shaped geometries has mitigated various challenges associated with these compounds, such as low IP values, high OFET threshold voltages, poor thermal durability, and moderate charge mobilities. This was accomplished by extending the length of π-conjugation and alternating the type of bent shape. These endeavors provided a p-channel OFET mobility of 16 cm2 V–1 s–1 in conjunction with N-shaped OSCs, which is adequate for the development of applications such as radio frequency identifier tags. However, the performance of OSCs in transistors is still far inferior to that of inorganic semiconductors, such that OSCs remain best suited to applications in relatively low-end electronics. In addition, the range of high-performance electron-transporting n-type OSCs is still limited, and so there is an urgent need for the development of all-organic complementary logic circuits. To improve the carrier mobility for both p- and n-type OSCs, it is necessary to form a clearer understanding of molecular motion by studying OSCs that exhibit band-transport characteristics using techniques such as Raman spectroscopy, infrared spectroscopy, and neutron scattering. It is our hope that the bent-shaped OSCs described herein will provide insights into the design of molecular geometries and orbital configurations that are suitable for the advancement of the air-stable, thermally durable, high-performance n-type OSCs required for next-generation electronic materials.

Supporting Information

ARTICLE SECTIONS
Jump To

The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/jacs.9b10450.

  • Video demonstrating the edge-casting technique (AVI)

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.

Author Information

ARTICLE SECTIONS
Jump To

  • Corresponding Author
    • Toshihiro Okamoto - Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, JapanUniversity of Tokyo Advanced Operando-Measurement Technology Open Innovation Laboratory (OPERANDO-OIL), National Institute of Advanced Industrial Science and Technology (AIST), 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, JapanPRESTO, JST, 4-1-8 Honcho, Kawaguchi, Saitama 332-0012, JapanOrcidhttp://orcid.org/0000-0002-4783-0621 Email: [email protected]
  • Authors
    • Craig P. Yu - Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, JapanOrcidhttp://orcid.org/0000-0002-1423-5244
    • Chikahiko Mitsui - Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan
    • Masakazu Yamagishi - Department of Applied Chemistry and Chemical Engineering, National Institute of Technology, Toyama College, 13 Hongo-machi, Toyama City, Toyama 939-8630, Japan
    • Hiroyuki Ishii - Department of Applied Physics, Faculty of Pure and Applied Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8573, JapanOrcidhttp://orcid.org/0000-0003-0644-1424
    • Jun Takeya - Material Innovation Research Center (MIRC) and Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, JapanUniversity of Tokyo Advanced Operando-Measurement Technology Open Innovation Laboratory (OPERANDO-OIL), National Institute of Advanced Industrial Science and Technology (AIST), 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, JapanMANA, National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba 205-0044, Japan
  • Notes

    The authors declare no competing financial interest.

Acknowledgments

ARTICLE SECTIONS
Jump To

This work was supported by the Japan Science and Technology Agency (JST) PRESTO programs “Molecular Technology and Creation of New Functions” (grant JPMJPR13K5 and JPMJPR12K2) and “Scientific Innovation for Energy Harvesting Technology” (grant JPMJPR17R2) as well as a Japan Society for the Promotion of Science (JSPS) KAKENHI grant-in-aid for Scientific Research B (no. 17H03104). C.P.Y. would also like to acknowledge support for his graduate work through a Todai Fellowship at the University of Tokyo. Finally, the authors thank R. Wang for performing additional DFT calculations.

References

ARTICLE SECTIONS
Jump To

This article references 97 other publications.

  1. 1
    Bao, Z.; Locklin, J. Organic Field-Effect Transistors, 1st ed.; CRC Press: Boca Raton, FL, 2007.
  2. 2
    Wang, C.; Dong, H.; Hu, W.; Liu, Y.; Zhu, D. Semiconducting π-Conjugated Systems in Field-Effect Transistors: A Material Odyssey of Organic Electronics. Chem. Rev. 2012, 112, 22082267,  DOI: 10.1021/cr100380z
  3. 3
    Root, S. E.; Savagatrup, S.; Printz, A. D.; Rodriquez, D.; Lipomi, D. J. Mechanical Properties of Organic Semiconductors for Stretchable, Highly Flexible, and Mechanically Robust Electronics. Chem. Rev. 2017, 117, 64676499,  DOI: 10.1021/acs.chemrev.7b00003
  4. 4
    Mei, J.; Diao, Y.; Appleton, A. L.; Fang, L.; Bao, Z. Integrated Materials Design of Organic Semiconductors for Field-Effect Transistors. J. Am. Chem. Soc. 2013, 135, 67246746,  DOI: 10.1021/ja400881n
  5. 5
    Müllen, K.; Scherf, U. Organic Light-Emitting Devices: Synthesis, Properties and Applications; Wiley-VCH, 2006.
  6. 6
    Burn, P. L.; Lo, S.-C.; Samuel, I. D. W. The Development of Light-Emitting Dendrimers for Displays. Adv. Mater. 2007, 19, 16751688,  DOI: 10.1002/adma.200601592
  7. 7
    Ostroverkhova, O. Organic Optoelectronic Materials: Mechanisms and Applications. Chem. Rev. 2016, 116, 1327913412,  DOI: 10.1021/acs.chemrev.6b00127
  8. 8
    Thompson, B. C.; Fréchet, J. M. J. Polymer-Fullerene Composite Solar Cells. Angew. Chem., Int. Ed. 2008, 47, 5877,  DOI: 10.1002/anie.200702506
  9. 9
    Günes, S.; Neugebauer, H.; Sariciftci, N. S. Conjugated Polymer-Based Organic Solar Cells. Chem. Rev. 2007, 107, 13241338,  DOI: 10.1021/cr050149z
  10. 10
    Son, H. J.; He, F.; Carsten, B.; Yu, L. Are we there yet? Design of better conjugated polymers for polymer solar cells. J. Mater. Chem. 2011, 21, 1893418945,  DOI: 10.1039/c1jm12388b
  11. 11
    Cheng, Y.-J.; Yang, S.-H.; Hsu, C.-S. Synthesis of Conjugated Polymers for Organic Solar Cell Applications. Chem. Rev. 2009, 109, 58685923,  DOI: 10.1021/cr900182s
  12. 12
    Chen, Y.; Zhao, Y.; Liang, Z. Solution processed organic thermoelectrics: towards flexible thermoelectric modules. Energy Environ. Sci. 2015, 8, 401422,  DOI: 10.1039/C4EE03297G
  13. 13
    Park, T.; Park, C.; Kim, B.; Shin, H.; Kim, E. Flexible PEDOT electrodes with large thermoelectric power factors to generate electricity by the touch of fingertips. Energy Environ. Sci. 2013, 6, 788792,  DOI: 10.1039/c3ee23729j
  14. 14
    Shi, K.; Zhang, F.; Di, C.-A.; Yan, T.-W.; Zou, Y.; Zhou, X.; Zhu, D.; Wang, J.-Y.; Pei, J. Toward High Performance n-Type Thermoelectric Materials by Rational Modification of BDPPV Backbones. J. Am. Chem. Soc. 2015, 137, 69796982,  DOI: 10.1021/jacs.5b00945
  15. 15
    Schlitz, R. A.; Brunetti, F. G.; Glaudell, A. M.; Miller, P. L.; Brady, M. A.; Takacs, C. J.; Hawker, C. J.; Chabinyc, M. L. Solubility-Limited Extrinsic n-Type Doping of a High Electron Mobility Polymer for Thermoelectric Applications. Adv. Mater. 2014, 26, 28252830,  DOI: 10.1002/adma.201304866
  16. 16
    Lavieville, R.; Zhang, Y.; Casu, A.; Genovese, A.; Manna, L.; Di Fabrizio, E.; Krahne, R. Charge Transport in Nanoscale “All-Inorganic” Networks of Semiconductor Nanorods Linked by Metal Domains. ACS Nano 2012, 6, 29402947,  DOI: 10.1021/nn3006625
  17. 17
    Anthony, J. E. Functionalized Acenes and Heteroacenes for Organic Electronics. Chem. Rev. 2006, 106, 50285048,  DOI: 10.1021/cr050966z
  18. 18
    Coropceanu, V.; Cornil, J.; da Silva Filho, D. A.; Olivier, Y.; Silbey, R.; Brédas, J.-L. Charge Transport in Organic Semiconductors. Chem. Rev. 2007, 107, 926952,  DOI: 10.1021/cr050140x
  19. 19
    Takimiya, K.; Shinamura, S.; Osaka, I.; Miyazaki, E. Thienoacene-Based Organic Semiconductors. Adv. Mater. 2011, 23, 43474370,  DOI: 10.1002/adma.201102007
  20. 20
    Liu, C.; Huang, K.; Park, W.-T.; Li, M.; Yang, T.; Liu, X.; Liang, L.; Minari, T.; Noh, Y.-Y. A unified understanding of charge transport in organic semiconductors: the importance of attenuated delocalization for the carriers. Mater. Horiz. 2017, 4, 608618,  DOI: 10.1039/C7MH00091J
  21. 21
    Ji, L.-F.; Fan, J.-X.; Qin, G.-Y.; Zhang, N.-X.; Lin, P.-P.; Ren, A.-M. Theoretical Study on the Electronic Structures and Charge Transport Properties of a Series of Rubrene Derivatives. J. Phys. Chem. C 2018, 122, 2122621238,  DOI: 10.1021/acs.jpcc.8b07018
  22. 22
    Wang, Y.; Sun, L.; Wang, C.; Yang, F.; Ren, X.; Zhang, X.; Dong, H.; Hu, W. Organic crystalline materials in flexible electronics. Chem. Soc. Rev. 2019, 48, 14921530,  DOI: 10.1039/C8CS00406D
  23. 23
    Gryn’ova, G.; Lin, K.-H.; Corminboeuf, C. Read between the Molecules: Computational Insights into Organic Semiconductors. J. Am. Chem. Soc. 2018, 140, 1637016386,  DOI: 10.1021/jacs.8b07985
  24. 24
    McGarry, K. A.; Xie, W.; Sutton, C.; Risko, C.; Wu, Y.; Young, V. G.; Brédas, J.-L.; Frisbie, C. D.; Douglas, C. J. Rubrene-Based Single-Crystal Organic Semiconductors: Synthesis, Electronic Structure, and Charge-Transport Properties. Chem. Mater. 2013, 25, 22542263,  DOI: 10.1021/cm400736s
  25. 25
    Giri, G.; Verploegen, E.; Mannsfeld, S. C. B.; Atahan-Evrenk, S.; Kim, D. H.; Lee, S. Y.; Becerril, H. A.; Aspuru-Guzik, A.; Toney, M. F.; Bao, Z. Tuning charge transport in solution-sheared organic semiconductors using lattice strain. Nature 2011, 480, 504,  DOI: 10.1038/nature10683
  26. 26
    Rühle, V.; Lukyanov, A.; May, F.; Schrader, M.; Vehoff, T.; Kirkpatrick, J.; Baumeier, B.; Andrienko, D. Microscopic Simulations of Charge Transport in Disordered Organic Semiconductors. J. Chem. Theory Comput. 2011, 7, 33353345,  DOI: 10.1021/ct200388s
  27. 27
    Nomura, K.; Ohta, H.; Takagi, A.; Kamiya, T.; Hirano, M.; Hosono, H. Room-temperature fabrication of transparent flexible thin-film transistors using amorphous oxide semiconductors. Nature 2004, 432, 488492,  DOI: 10.1038/nature03090
  28. 28
    Kuribara, K.; Wang, H.; Uchiyama, N.; Fukuda, K.; Yokota, T.; Zschieschang, U.; Jaye, C.; Fischer, D.; Klauk, H.; Yamamoto, T.; Takimiya, K.; Ikeda, M.; Kuwabara, H.; Sekitani, T.; Loo, Y.-L.; Someya, T. Organic transistors with high thermal stability for medical applications. Nat. Commun. 2012, 3, 723,  DOI: 10.1038/ncomms1721
  29. 29
    Payne, M. M.; Parkin, S. R.; Anthony, J. E. Functionalized Higher Acenes: Hexacene and Heptacene. J. Am. Chem. Soc. 2005, 127, 80288029,  DOI: 10.1021/ja051798v
  30. 30
    Tang, M. L.; Okamoto, T.; Bao, Z. High-Performance Organic Semiconductors: Asymmetric Linear Acenes Containing Sulphur. J. Am. Chem. Soc. 2006, 128, 1600216003,  DOI: 10.1021/ja066824j
  31. 31
    Wong, M. Y.; Hedley, G. J.; Xie, G.; Kölln, L. S.; Samuel, I. D. W.; Pertegás, A.; Bolink, H. J.; Zysman-Colman, E. Light-Emitting Electrochemical Cells and Solution-Processed Organic Light-Emitting Diodes Using Small Molecule Organic Thermally Activated Delayed Fluorescence Emitters. Chem. Mater. 2015, 27, 65356542,  DOI: 10.1021/acs.chemmater.5b03245
  32. 32
    Bin, H.; Yang, Y.; Zhang, Z.-G.; Ye, L.; Ghasemi, M.; Chen, S.; Zhang, Y.; Zhang, C.; Sun, C.; Xue, L.; Yang, C.; Ade, H.; Li, Y. 9.73% Efficiency Nonfullerene All Organic Small Molecule Solar Cells with Absorption-Complementary Donor and Acceptor. J. Am. Chem. Soc. 2017, 139, 50855094,  DOI: 10.1021/jacs.6b12826
  33. 33
    Lin, L.-Y.; Chen, Y.-H.; Huang, Z.-Y.; Lin, H.-W.; Chou, S.-H.; Lin, F.; Chen, C.-W.; Liu, Y.-H.; Wong, K.-T. A Low-Energy-Gap Organic Dye for High-Performance Small-Molecule Organic Solar Cells. J. Am. Chem. Soc. 2011, 133, 1582215825,  DOI: 10.1021/ja205126t
  34. 34
    Sun, Y.; Welch, G. C.; Leong, W. L.; Takacs, C. J.; Bazan, G. C.; Heeger, A. J. Solution-processed small-molecule solar cells with 6.7% efficiency. Nat. Mater. 2012, 11, 44,  DOI: 10.1038/nmat3160
  35. 35
    Maliakal, A.; Raghavachari, K.; Katz, H.; Chandross, E.; Siegrist, T. Photochemical Stability of Pentacene and a Substituted Pentacene in Solution and in Thin Films. Chem. Mater. 2004, 16, 49804986,  DOI: 10.1021/cm049060k
  36. 36
    Laquindanum, J. G.; Katz, H. E.; Lovinger, A. J. Synthesis, Morphology, and Field-Effect Mobility of Anthradithiophenes. J. Am. Chem. Soc. 1998, 120, 664672,  DOI: 10.1021/ja9728381
  37. 37
    Mishra, A.; Bäuerle, P. Small Molecule Organic Semiconductors on the Move: Promises for Future Solar Energy Technology. Angew. Chem., Int. Ed. 2012, 51, 20202067,  DOI: 10.1002/anie.201102326
  38. 38
    Leung, L. M.; Lo, W. Y.; So, S. K.; Lee, K. M.; Choi, W. K. A High-Efficiency Blue Emitter for Small Molecule-Based Organic Light-Emitting Diode. J. Am. Chem. Soc. 2000, 122, 56405641,  DOI: 10.1021/ja000927z
  39. 39
    Kulkarni, A. P.; Tonzola, C. J.; Babel, A.; Jenekhe, S. A. Electron Transport Materials for Organic Light-Emitting Diodes. Chem. Mater. 2004, 16, 45564573,  DOI: 10.1021/cm049473l
  40. 40
    Liu, Y.; Li, C.; Ren, Z.; Yan, S.; Bryce, M. R. All-organic thermally activated delayed fluorescence materials for organic light-emitting diodes. Nat. Rev. Mater. 2018, 3, 18020,  DOI: 10.1038/natrevmats.2018.20
  41. 41
    Klauk, H.; Halik, M.; Zschieschang, U.; Schmid, G.; Radlik, W.; Weber, W. High-mobility polymer gate dielectric pentacene thin film transistors. J. Appl. Phys. 2002, 92, 52595263,  DOI: 10.1063/1.1511826
  42. 42
    Ebata, H.; Izawa, T.; Miyazaki, E.; Takimiya, K.; Ikeda, M.; Kuwabara, H.; Yui, T. Highly Soluble [1]Benzothieno[3,2-b]benzothiophene (BTBT) Derivatives for High-Performance, Solution-Processed Organic Field-Effect Transistors. J. Am. Chem. Soc. 2007, 129, 1573215733,  DOI: 10.1021/ja074841i
  43. 43
    Yamamoto, T.; Takimiya, K. Facile Synthesis of Highly π-Extended Heteroarenes, Dinaphtho[2,3-b:2‘,3′-f]chalcogenopheno[3,2-b]chalcogenophenes, and Their Application to Field-Effect Transistors. J. Am. Chem. Soc. 2007, 129, 22242225,  DOI: 10.1021/ja068429z
  44. 44
    Wang, C.; Dong, H.; Hu, W.; Liu, Y.; Zhu, D. Semiconducting π-Conjugated Systems in Field-Effect Transistors: A Material Odyssey of Organic Electronics. Chem. Rev. 2012, 112, 22082267,  DOI: 10.1021/cr100380z
  45. 45
    Curtis, M. D.; Cao, J.; Kampf, J. W. Solid-State Packing of Conjugated Oligomers: From π-Stacks to the Herringbone Structure. J. Am. Chem. Soc. 2004, 126, 43184328,  DOI: 10.1021/ja0397916
  46. 46
    Purushothaman, B.; Bruzek, M.; Parkin, S. R.; Miller, A.-F.; Anthony, J. E. Synthesis and Structural Characterization of Crystalline Nonacenes. Angew. Chem., Int. Ed. 2011, 50, 70137017,  DOI: 10.1002/anie.201102671
  47. 47
    Anthony, J. E. The Larger Acenes: Versatile Organic Semiconductors. Angew. Chem., Int. Ed. 2008, 47, 452483,  DOI: 10.1002/anie.200604045
  48. 48
    Uemura, T.; Hirose, Y.; Uno, M.; Takimiya, K.; Takeya, J. Very High Mobility in Solution-Processed Organic Thin-Film Transistors of Highly Ordered [1]Benzothieno[3,2-b]benzothiophene Derivatives. Appl. Phys. Express 2009, 2, 111501,  DOI: 10.1143/APEX.2.111501
  49. 49
    Soeda, J.; Uemura, T.; Okamoto, T.; Mitsui, C.; Yamagishi, M.; Takeya, J. Inch-Size Solution-Processed Single-Crystalline Films of High-Mobility Organic Semiconductors. Appl. Phys. Express 2013, 6, 076503,  DOI: 10.7567/APEX.6.076503
  50. 50
    Yamamura, A.; Watanabe, S.; Uno, M.; Mitani, M.; Mitsui, C.; Tsurumi, J.; Isahaya, N.; Kanaoka, Y.; Okamoto, T.; Takeya, J. Wafer-scale, layer-controlled organic single crystals for high-speed circuit operation. Sci. Adv. 2018, 4, eaao5758  DOI: 10.1126/sciadv.aao5758
  51. 51
    Yamamura, A.; Matsui, H.; Uno, M.; Isahaya, N.; Tanaka, Y.; Kudo, M.; Ito, M.; Mitsui, C.; Okamoto, T.; Takeya, J. Painting Integrated Complementary Logic Circuits for Single-Crystal Organic Transistors: A Demonstration of a Digital Wireless Communication Sensing Tag. Adv. Electron. Mater. 2017, 3, 1600456,  DOI: 10.1002/aelm.201600456
  52. 52
    Kang, M. J.; Doi, I.; Mori, H.; Miyazaki, E.; Takimiya, K.; Ikeda, M.; Kuwabara, H. Alkylated Dinaphtho[2,3-b:2′,3′-f]Thieno[3,2-b]Thiophenes (Cn-DNTTs): Organic Semiconductors for High-Performance Thin-Film Transistors. Adv. Mater. 2011, 23, 12221225,  DOI: 10.1002/adma.201001283
  53. 53
    Iino, H.; Usui, T.; Hanna, J.-i. Liquid crystals for organic thin-film transistors. Nat. Commun. 2015, 6, 6828,  DOI: 10.1038/ncomms7828
  54. 54
    Inoue, S.; Minemawari, H.; Tsutsumi, J. y.; Chikamatsu, M.; Yamada, T.; Horiuchi, S.; Tanaka, M.; Kumai, R.; Yoneya, M.; Hasegawa, T. Effects of Substituted Alkyl Chain Length on Solution-Processable Layered Organic Semiconductor Crystals. Chem. Mater. 2015, 27, 38093812,  DOI: 10.1021/acs.chemmater.5b00810
  55. 55
    He, K.; Li, W.; Tian, H.; Zhang, J.; Yan, D.; Geng, Y.; Wang, F. Asymmetric Conjugated Molecules Based on [1]Benzothieno[3,2-b][1]benzothiophene for High-Mobility Organic Thin-Film Transistors: Influence of Alkyl Chain Length. ACS Appl. Mater. Interfaces 2017, 9, 3542735436,  DOI: 10.1021/acsami.7b10675
  56. 56
    Grigoriadis, C.; Niebel, C.; Ruzié, C.; Geerts, Y. H.; Floudas, G. Order, Viscoelastic, and Dielectric Properties of Symmetric and Asymmetric Alkyl[1]benzothieno[3,2-b][1]benzothiophenes. J. Phys. Chem. B 2014, 118, 14431451,  DOI: 10.1021/jp412422e
  57. 57
    Inoue, S.; Shinamura, S.; Sadamitsu, Y.; Arai, S.; Horiuchi, S.; Yoneya, M.; Takimiya, K.; Hasegawa, T. Extended and Modulated Thienothiophenes for Thermally Durable and Solution-Processable Organic Semiconductors. Chem. Mater. 2018, 30, 50505060,  DOI: 10.1021/acs.chemmater.8b01339
  58. 58
    Diao, Y.; Tee, B. C. K.; Giri, G.; Xu, J.; Kim, D. H.; Becerril, H. A.; Stoltenberg, R. M.; Lee, T. H.; Xue, G.; Mannsfeld, S. C. B.; Bao, Z. Solution coating of large-area organic semiconductor thin films with aligned single-crystalline domains. Nat. Mater. 2013, 12, 665,  DOI: 10.1038/nmat3650
  59. 59
    Nakayama, K.; Hirose, Y.; Soeda, J.; Yoshizumi, M.; Uemura, T.; Uno, M.; Li, W.; Kang, M. J.; Yamagishi, M.; Okada, Y.; Miyazaki, E.; Nakazawa, Y.; Nakao, A.; Takimiya, K.; Takeya, J. Patternable Solution-Crystallized Organic Transistors with High Charge Carrier Mobility. Adv. Mater. 2011, 23, 16261629,  DOI: 10.1002/adma.201004387
  60. 60
    Yuan, Y.; Giri, G.; Ayzner, A. L.; Zoombelt, A. P.; Mannsfeld, S. C. B.; Chen, J.; Nordlund, D.; Toney, M. F.; Huang, J.; Bao, Z. Ultra-high mobility transparent organic thin film transistors grown by an off-centre spin-coating method. Nat. Commun. 2014, 5, 3005,  DOI: 10.1038/ncomms4005
  61. 61
    Iino, H.; Kobori, T.; Hanna, J.-i. Improved thermal stability in organic FET fabricated with a soluble BTBT derivative. J. Non-Cryst. Solids 2012, 358, 25162519,  DOI: 10.1016/j.jnoncrysol.2012.03.021
  62. 62
    Okamoto, K.; Kawamura, T.; Sone, M.; Ogino, K. Study on liquid crystallinity in 2,9-dialkylpentacenes. Liq. Cryst. 2007, 34, 10011007,  DOI: 10.1080/02678290701478970
  63. 63
    Kuwabara, H.; Ikeda, M.; Takimiya, K. U.S. Patent 2011/0303910 A1, 2010.
  64. 64
    Fratini, S.; Ciuchi, S.; Mayou, D.; de Laissardière, G. T.; Troisi, A. A map of high-mobility molecular semiconductors. Nat. Mater. 2017, 16, 998,  DOI: 10.1038/nmat4970
  65. 65
    Troisi, A.; Orlandi, G.; Anthony, J. E. Electronic Interactions and Thermal Disorder in Molecular Crystals Containing Cofacial Pentacene Units. Chem. Mater. 2005, 17, 50245031,  DOI: 10.1021/cm051150h
  66. 66
    Ciuchi, S.; Fratini, S. Electronic transport and quantum localization effects in organic semiconductors. Phys. Rev. B: Condens. Matter Mater. Phys. 2012, 86, 245201,  DOI: 10.1103/PhysRevB.86.245201
  67. 67
    Illig, S.; Eggeman, A. S.; Troisi, A.; Jiang, L.; Warwick, C.; Nikolka, M.; Schweicher, G.; Yeates, S. G.; Henri Geerts, Y.; Anthony, J. E.; Sirringhaus, H. Reducing dynamic disorder in small-molecule organic semiconductors by suppressing large-amplitude thermal motions. Nat. Commun. 2016, 7, 10736,  DOI: 10.1038/ncomms10736
  68. 68
    Okamoto, T.; Mitsui, C.; Yamagishi, M.; Nakahara, K.; Soeda, J.; Hirose, Y.; Miwa, K.; Sato, H.; Yamano, A.; Matsushita, T.; Uemura, T.; Takeya, J. V-shaped organic semiconductors with solution processability, high mobility, and high thermal durability. Adv. Mater. 2013, 25, 63926397,  DOI: 10.1002/adma.201302086
  69. 69
    Mitsui, C.; Okamoto, T.; Matsui, H.; Yamagishi, M.; Matsushita, T.; Soeda, J.; Miwa, K.; Sato, H.; Yamano, A.; Uemura, T.; Takeya, J. Dinaphtho[1,2b:2′,1’d]chalcogenophenes: Comprehensive Investigation of the Effect of the Chalcogen Atoms in the Phenacene-Type π Electronic Cores. Chem. Mater. 2013, 25, 39523956,  DOI: 10.1021/cm303376g
  70. 70
    Mitsui, C.; Okamoto, T.; Yamagishi, M.; Tsurumi, J.; Yoshimoto, K.; Nakahara, K.; Soeda, J.; Hirose, Y.; Sato, H.; Yamano, A.; Uemura, T.; Takeya, J. High-performance solution-processable N-shaped organic semiconducting materials with stabilized crystal phase. Adv. Mater. 2014, 26, 45464551,  DOI: 10.1002/adma.201400289
  71. 71
    Mitsui, C.; Yamagishi, M.; Shikata, R.; Ishii, H.; Matsushita, T.; Nakahara, K.; Yano, M.; Sato, H.; Yamano, A.; Takeya, J.; Okamoto, T. Oxygen- and sulfur-bridged bianthracene V-shaped organic semiconductors. Bull. Chem. Soc. Jpn. 2017, 90, 931938,  DOI: 10.1246/bcsj.20170030
  72. 72
    Mitsui, C.; Tsuyama, H.; Shikata, R.; Murata, Y.; Kuniyasu, H.; Yamagishi, M.; Ishii, H.; Yamamoto, A.; Hirose, Y.; Yano, M.; Takehara, T.; Suzuki, T.; Sato, H.; Yamano, A.; Fukuzaki, E.; Watanabe, T.; Usami, Y.; Takeya, J.; Okamoto, T. High performance solution-crystallized thin-film transistors based on V-shaped thieno[3,2-f:4,5-f’]bis[1]benzothiophene semiconductors. J. Mater. Chem. C 2017, 5, 19031909,  DOI: 10.1039/C6TC04721A
  73. 73
    Yamamoto, A.; Murata, Y.; Mitsui, C.; Ishii, H.; Yamagishi, M.; Yano, M.; Sato, H.; Yamano, A.; Takeya, J.; Okamoto, T. Zigzag-Elongated Fused pi-Electronic Core: A Molecular Design Strategy to Maximize Charge-Carrier Mobility. Adv. Sci. 2018, 5, 1700317,  DOI: 10.1002/advs.201700317
  74. 74
    Tsurumi, J.; Matsui, H.; Kubo, T.; Hausermann, R.; Mitsui, C.; Okamoto, T.; Watanabe, S.; Takeya, J. Coexistence of ultra-long spin relaxation time and coherent charge transport in organic single-crystal semiconductors. Nat. Phys. 2017, 13, 994998,  DOI: 10.1038/nphys4217
  75. 75
    Solubility Parameter. Bulletin of the American Group; International Institute for Conservation of Historic and Artistic Works, 1968; Vol. 8, pp 2024.
  76. 76

    The reorganization energy was calculated based on the optimized structure by DFT at the B3LYP/6-31G(d) level.

  77. 77
    Schleyer, P. v. R.; Maerker, C.; Dransfeld, A.; Jiao, H.; van Eikema Hommes, N. J. R. Nucleus-Independent Chemical Shifts: A Simple and Efficient Aromaticity Probe. J. Am. Chem. Soc. 1996, 118, 63176318,  DOI: 10.1021/ja960582d
  78. 78
    Chen, Z.; Wannere, C. S.; Corminboeuf, C.; Puchta, R.; Schleyer, P. v. R. Nucleus-Independent Chemical Shifts (NICS) as an Aromaticity Criterion. Chem. Rev. 2005, 105, 38423888,  DOI: 10.1021/cr030088+
  79. 79
    Münzel, N.; Kesper, K.; Schweig, A.; Specht, H. Detection of 2,5-dimethylene-2,5-dihydrothiophene and thiophenoradialene. Tetrahedron Lett. 1988, 29, 62396242,  DOI: 10.1016/S0040-4039(00)82314-X
  80. 80
    Okamoto, H.; Kawasaki, N.; Kaji, Y.; Kubozono, Y.; Fujiwara, A.; Yamaji, M. Air-assisted High-performance Field-effect Transistor with Thin Films of Picene. J. Am. Chem. Soc. 2008, 130, 1047010471,  DOI: 10.1021/ja803291a
  81. 81
    Kawai, N.; Eguchi, R.; Goto, H.; Akaike, K.; Kaji, Y.; Kambe, T.; Fujiwara, A.; Kubozono, Y. Characteristics of Single Crystal Field-Effect Transistors with a New Type of Aromatic Hydrocarbon, Picene. J. Phys. Chem. C 2012, 116, 79837988,  DOI: 10.1021/jp300052p
  82. 82
    De, A.; Ghosh, R.; Roychowdhury, S.; Roychowdhury, P. Structural analysis of picene, C22H14. Acta Crystallogr., Sect. C: Cryst. Struct. Commun. 1985, 41, 907909,  DOI: 10.1107/S0108270185005959
  83. 83
    Tedjamulia, M. L.; Tominaga, Y.; Castle, R. N.; Lee, M. L. The synthesis of dinaphthothiophenes. J. Heterocyclic Chem. 1983, 20, 11431148,  DOI: 10.1002/jhet.5570200502
  84. 84
    Lloyd-Jones, G. C.; Moseley, J. D.; Renny, J. S. Mechanism and Application of the Newman-Kwart O→S Rearrangement of O-Aryl Thiocarbamates. Synthesis 2008, 2008, 661689,  DOI: 10.1055/s-2008-1032179
  85. 85
    Matsuoka, M.; Iwamoto, A.; Kitao, T. Reaction of 2, 3-dichloro-1, 4-naphthoquinone with dithiooxamide. Synthesis of dibenzo[b, i]thianthrene-5, 7, 12, 14-tetrone. J. Heterocycl. Chem. 1991, 28, 14451447,  DOI: 10.1002/jhet.5570280543
  86. 86
    De, P. K.; Neckers, D. C. Sulfur Containing Stable Unsubstituted Heptacene Analogs. Org. Lett. 2012, 14, 7881,  DOI: 10.1021/ol2028724
  87. 87
    Wex, B.; Kaafarani, B. R.; Kirschbaum, K.; Neckers, D. C. Synthesis of the anti and syn Isomers of Thieno[f, f‘]bis[1]benzothiophene. Comparison of the Optical and Electrochemical Properties of the anti and syn Isomers1. J. Org. Chem. 2005, 70, 45024505,  DOI: 10.1021/jo048010w
  88. 88
    Armarego, W. L. F. The synthesis of two dinaphthothiophens. J. Chem. Soc. 1960, 433436,  DOI: 10.1039/jr9600000433
  89. 89
    Shinamura, S.; Osaka, I.; Miyazaki, E.; Nakao, A.; Yamagishi, M.; Takeya, J.; Takimiya, K. Linear- and Angular-Shaped Naphthodithiophenes: Selective Synthesis, Properties, and Application to Organic Field-Effect Transistors. J. Am. Chem. Soc. 2011, 133, 50245035,  DOI: 10.1021/ja110973m
  90. 90
    Mamane, V.; Hannen, P.; Fürstner, A. Synthesis of Phenanthrenes and Polycyclic Heteroarenes by Transition-Metal Catalyzed Cycloisomerization Reactions. Chem. - Eur. J. 2004, 10, 45564575,  DOI: 10.1002/chem.200400220
  91. 91
    Laudise, R. A.; Kloc, C.; Simpkins, P. G.; Siegrist, T. Physical vapor growth of organic semiconductors. J. Cryst. Growth 1998, 187, 449454,  DOI: 10.1016/S0022-0248(98)00034-7
  92. 92
    Kloc, C.; Simpkins, P. G.; Siegrist, T.; Laudise, R. A. Physical vapor growth of centimeter-sized crystals of α-hexathiophene. J. Cryst. Growth 1997, 182, 416427,  DOI: 10.1016/S0022-0248(97)00370-9
  93. 93
    Izawa, T.; Miyazaki, E.; Takimiya, K. Molecular Ordering of High-Performance Soluble Molecular Semiconductors and Re-evaluation of Their Field-Effect Transistor Characteristics. Adv. Mater. 2008, 20, 33883392,  DOI: 10.1002/adma.200800799
  94. 94
    Takeya, J.; Tsukagoshi, K.; Aoyagi, Y.; Takenobu, T.; Iwasa, Y. Hall Effect of Quasi-Hole Gas in Organic Single-Crystal Transistors. Jpn. J. Appl. Phys. 2005, 44, L1393L1396,  DOI: 10.1143/JJAP.44.L1393
  95. 95
    Podzorov, V.; Menard, E.; Rogers, J. A.; Gershenson, M. E. Hall Effect in the Accumulation Layers on the Surface of Organic Semiconductors. Phys. Rev. Lett. 2005, 95, 226601,  DOI: 10.1103/PhysRevLett.95.226601
  96. 96
    Kubo, T.; Haeusermann, R.; Tsurumi, J.; Soeda, J.; Okada, Y.; Yamashita, Y.; Akamatsu, N.; Shishido, A.; Mitsui, C.; Okamoto, T.; Yanagisawa, S.; Matsui, H.; Takeya, J. Suppressing molecular vibrations in organic semiconductors by inducing strain. Nat. Commun. 2016, 7, 11156,  DOI: 10.1038/ncomms11156
  97. 97
    Oyama, T.; Yang, Y. S.; Matsuo, K.; Yasuda, T. Effects of chalcogen atom substitution on the optoelectronic and charge-transport properties in picene-type π-systems. Chem. Commun. 2017, 53, 38143817,  DOI: 10.1039/C7CC01292F

Cited By


This article is cited by 14 publications.

  1. Shohei Kumagai, Hiroyuki Ishii, Go Watanabe, Tatsuro Annaka, Eiji Fukuzaki, Yukio Tani, Hiroki Sugiura, Tetsuya Watanabe, Tadanori Kurosawa, Jun Takeya, Toshihiro Okamoto. Cooperative Aggregations of Nitrogen-Containing Perylene Diimides Driven by Rigid and Flexible Functional Groups. Chemistry of Materials 2020, 32 (21) , 9115-9125. https://doi.org/10.1021/acs.chemmater.0c01888
  2. Kyosuke Isoda, Harufumi Haga, Hajime Kamebuchi, Makoto Tadokoro. Crystallization-Induced Planar Chirality by Asymmetric Ferrocene-Appended Tetraazanaphthacene. Crystal Growth & Design 2020, 20 (11) , 7081-7086. https://doi.org/10.1021/acs.cgd.0c00934
  3. Douglas B. Paixão, Daniel S. Rampon, Helena D. Salles, Eduardo G. O. Soares, Filipe N. Bilheri, Paulo H. Schneider. Trithiocarbonate Anion as a Sulfur Source for the Synthesis of 2,5-Disubstituted Thiophenes and 2-Substituted Benzo[b]thiophenes. The Journal of Organic Chemistry 2020, 85 (20) , 12922-12934. https://doi.org/10.1021/acs.joc.0c01516
  4. Sung Joon Cho, Min Je Kim, Ziang Wu, Jae Hoon Son, Sang Young Jeong, Sungjoo Lee, Jeong Ho Cho, Han Young Woo. A-D-A Type Semiconducting Small Molecules with Bis(alkylsulfanyl)methylene Substituents and Control of Charge Polarity for Organic Field-Effect Transistors. ACS Applied Materials & Interfaces 2020, 12 (37) , 41842-41851. https://doi.org/10.1021/acsami.0c11561
  5. Toshihiro Okamoto, Masato Mitani, Craig P. Yu, Chikahiko Mitsui, Masakazu Yamagishi, Hiroyuki Ishii, Go Watanabe, Shohei Kumagai, Daisuke Hashizume, Shota Tanaka, Masafumi Yano, Tomokatsu Kushida, Hiroyasu Sato, Kunihisa Sugimoto, Takashi Kato, Jun Takeya. Alkyl-Substituted Selenium-Bridged V-Shaped Organic Semiconductors Exhibiting High Hole Mobility and Unusual Aggregation Behavior. Journal of the American Chemical Society 2020, 142 (35) , 14974-14984. https://doi.org/10.1021/jacs.0c05522
  6. Craig P. Yu, Masato Mitani, Hiroyuki Ishii, Masakazu Yamagishi, Hiroki Kitamura, Masafumi Yano, Jun Takeya, Toshihiro Okamoto. Effect of Electronically Distinct Aromatic Substituents on the Molecular Assembly and Hole Transport of V-Shaped Organic Semiconductors. The Journal of Physical Chemistry C 2020, 124 (32) , 17503-17511. https://doi.org/10.1021/acs.jpcc.0c04088
  7. Shakil N. Afraj, Guan‐Yu He, Chih‐Yu Lin, Arulmozhi Velusamy, Chu‐Yun Huang, Po‐Shen Lin, Sureshraju Vegiraju, Ping‐Yu Huang, Jen‐Shyang Ni, Shueh‐Lin Yau, Shih‐Huang Tung, Takeo Minari, Cheng‐Liang Liu, Ming‐Chou Chen. Solution‐Processable Multifused Thiophene Small Molecules and Conjugated Polymer Semiconducting Blend for Organic Field Effect Transistor Application. Advanced Materials Technologies 2021, 142 , 2001028. https://doi.org/10.1002/admt.202001028
  8. Tatsuya Mori, Takuma Yasuda. U‐Shaped Heteroacenes Embedded with Heavy Chalcogen Atoms: Unique Bilayer Self‐Organization of Crooked π‐Cores Enabling Efficient Charge Transport. Advanced Electronic Materials 2021, 135 , 2001052. https://doi.org/10.1002/aelm.202001052
  9. Keiichi Ishida, Tomohiro Higashino, Yoshimasa Wada, Hironori Kaji, Akinori Saeki, Hiroshi Imahori. Thiophene‐Fused Naphthodiphospholes: Modulation of the Structural and Electronic Properties of Polycyclic Aromatics by Precise Fusion of Heteroles. ChemPlusChem 2021, 86 (1) , 130-136. https://doi.org/10.1002/cplu.202000800
  10. Satoru Inoue, Toshiki Higashino, Shunto Arai, Reiji Kumai, Hiroyuki Matsui, Seiji Tsuzuki, Sachio Horiuchi, Tatsuo Hasegawa. Regioisomeric control of layered crystallinity in solution-processable organic semiconductors. Chemical Science 2020, 11 (46) , 12493-12505. https://doi.org/10.1039/D0SC04461J
  11. Chizuru Sawabe, Shohei Kumagai, Masato Mitani, Hiroyuki Ishii, Masakazu Yamagishi, Hajime Sagayama, Reiji Kumai, Hiroyasu Sato, Jun Takeya, Toshihiro Okamoto. Band-like transporting and thermally durable V-shaped organic semiconductors with a phenyl key block. Journal of Materials Chemistry C 2020, 8 (40) , 14172-14179. https://doi.org/10.1039/D0TC03318A
  12. Tatsuyuki Makita, Ryohei Nakamura, Mari Sasaki, Shohei Kumagai, Toshihiro Okamoto, Shun Watanabe, Jun Takeya. Electroless‐Plated Gold Contacts for High‐Performance, Low Contact Resistance Organic Thin Film Transistors. Advanced Functional Materials 2020, 30 (39) , 2003977. https://doi.org/10.1002/adfm.202003977
  13. Jingwen Song, Xiaofang Jia, Katsuhiko Ariga. Interfacial nanoarchitectonics for responsive cellular biosystems. Materials Today Bio 2020, 8 , 100075. https://doi.org/10.1016/j.mtbio.2020.100075
  14. Yuxin Guo, Kaito Yoshioka, Shino Hamao, Yoshihiro Kubozono, Fumito Tani, Kenta Goto, Hideki Okamoto. Facile synthesis of picenes incorporating imide moieties at both edges of the molecule and their application to n -channel field-effect transistors. RSC Advances 2020, 10 (52) , 31547-31552. https://doi.org/10.1039/D0RA06629J
  • Abstract

    Figure 1

    Figure 1. Molecular structures of representative organic semiconductors.

    Figure 2

    Figure 2. Molecular designs of first- and second-generation bent-shaped OSCs.

    Figure 3

    Figure 3. Molecular structures, NICS values (calculated at the HF/6-31+G(d)//B3LYP/6-31G(d) level), HOMO coefficients and energy levels, and dipole moments (calculated at the B3LYP/6-311G(d)//B3LYP/6-31G(d) level) of the (a) DNT-V, (b) DAT-V, (c) DNBDT-N, and (d) TBBT-V OSCs.

    Figure 4

    Figure 4. Molecular structures, NICS(0) values (calculated at the HF/6-31+G(d)//B3LYP/6-31G(d) level), HOMO and NHOMO coefficients and their energy levels, and dipole moments (calculated at the B3LYP/6-311G(d)//B3LYP/6-31G(d) level) of V-, W-, and zigzag-shaped π-cores.

    Scheme 1

    Scheme 1. Synthesis of DNT-V Derivativesa

    aReagents and conditions: (a) n-BuLi, Fe(acac)3, 0 °C to rt, 73% (R = C10H21); (b) BBr3, 0 °C to rt, 94% (R = H), 97% (R = C10H21); (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 78% (R = H), 75% (R = C10H21); (d) 300–320 °C, 81% (R = H), 77% (R = C10H21).

    Scheme 2

    Scheme 2. Modified DNT-V Synthesisa

    aReagents and conditions: (a) (1) dithiooxamide, DMF, 55 °C, (2) Et3N, rt, 89%; (b) m-CPBA, CH2Cl2, 30 °C, 88%; (c) HI, AcOH, reflux, 97%.

    Scheme 3

    Scheme 3. Synthesis of DAT-Va

    aReagents and conditions: (a) n-BuLi, Fe(acac)3, 0 °C to rt, 52%; (b) BBr3, 0 °C to rt, 96%; (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 61%; (d) 300 °C, 68%.

    Scheme 4

    Scheme 4. Synthesis of DNBDT-N Derivativesa

    aReagents and conditions: (a) (1) n-BuLi, ZnCl2, 0 °C to rt, (2) 1,4-dibromo-2,5-dimethoxybenzene, PdCl2(dppp), 50 °C, 87% (R = H), 85% (R = C10H21); (b) BBr3, 0 °C to rt, 81% (R = H), 92% (R = C10H21); (c) dimethylcarbamyl chloride, Et3N, pyridine, THF, 65 °C, 53% (R = H), 72% (R = C10H21); (d) 310–320 °C, 67% (R = H), 64% (R = C10H21).

    Scheme 5

    Scheme 5. Synthesis of TBBT-V Derivativesa

    aReagents and conditions: (a) C10H21ZnCl2, PdCl2(dppf)·CH2Cl2, toluene, 70 °C, 64%; (b) (5-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 86%; (c) (4-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 92%.

    Scheme 6

    Scheme 6. Synthesis of ChDT Derivativesa

    aReagents and conditions: (a) (1) n-BuLi, THF, −78 °C, (2) ZnCl2, THF, 0 °C, (3) 3-bromothiophene, Pd2(dba)3·CHCl3, THF, 50 °C, 79%; (b) K2CO3, MeOH, CH2Cl2, rt, 99%; (c) PtCl2, DMF, 80 °C, 58%; (d) (1) LiTMP, THF, −78 °C to −50 °C, (2) 1,2-dibromo-1,1,2,2-tetrachloroethane, −78 °C to rt, 88%; (e) C10H21ZnCl, PdCl2(dppf)·CH2Cl2, THF, 70 °C, 80%; (f) (4-decylthiophen-2-yl)trimethylstannane, Pd(PPh3)4, LiCl, DMF, 100 °C, 81%.

    Figure 5

    Figure 5. Representative slightly bent geometries of C10-DNT-VW and C10-DNBDT-NW (front and side views) in single crystals.

    Figure 6

    Figure 6. Relation between sign of transfer integral and intermolecular orbital overlap.

    Figure 7

    Figure 7. Representative packing structures and transfer integrals for (a) C10-DNT-VW and (b) C10-DNT-VV for their HOMOs (and NHOMO).

    Figure 8

    Figure 8. Representative packing structures and transfer integrals for (a) DNBDT-N and (b) C10-DNBDT-NW.

    Figure 9

    Figure 9. Representative packing structures and transfer integrals for (a) DNT-W, (b) C10-ChDT, and (c) C10-Th-ChDT.

    Figure 10

    Figure 10. HOMO band structures and effective masses of (a) C10-DNBDT-NW and (b) C10-ChDT. The origin of energy axis is set to HOMO level of the molecule. Insets show the first Brillouin zone with symmetry points of Γ(0,0,0), Y(0,π/b,0), Z(0,0,π/c), and S(0,π/b,π/c), where b and c are the lattice constants shown in Figures 8b and 9b. The column directions correspond to Γ–Z (C10-DNBDT-NW) and Γ–Y (C10-ChDT) directions in the reciprocal lattice.

    Figure 11

    Figure 11. Values of t and Δt for ChDT, DNTT, and pentacene.

    Figure 12

    Figure 12. Schematic diagrams of (a) the manual lamination and (b) edge-casting techniques.

    Figure 13

    Figure 13. (a) Bottom-gate–top-contact device structure and packing structure of C10-DNBDT-NW on the substrate and (b) optical microscopy image. (c) Transfer and (d) output characteristics of the OFET based on a C10-DNBDT-NW single-crystalline film.

  • References

    ARTICLE SECTIONS
    Jump To

    This article references 97 other publications.

    1. 1
      Bao, Z.; Locklin, J. Organic Field-Effect Transistors, 1st ed.; CRC Press: Boca Raton, FL, 2007.
    2. 2
      Wang, C.; Dong, H.; Hu, W.; Liu, Y.; Zhu, D. Semiconducting π-Conjugated Systems in Field-Effect Transistors: A Material Odyssey of Organic Electronics. Chem. Rev. 2012, 112, 22082267,  DOI: 10.1021/cr100380z
    3. 3
      Root, S. E.; Savagatrup, S.; Printz, A. D.; Rodriquez, D.; Lipomi, D. J. Mechanical Properties of Organic Semiconductors for Stretchable, Highly Flexible, and Mechanically Robust Electronics. Chem. Rev. 2017, 117, 64676499,  DOI: 10.1021/acs.chemrev.7b00003
    4. 4
      Mei, J.; Diao, Y.; Appleton, A. L.; Fang, L.; Bao, Z. Integrated Materials Design of Organic Semiconductors for Field-Effect Transistors. J. Am. Chem. Soc. 2013, 135, 67246746,  DOI: 10.1021/ja400881n
    5. 5
      Müllen, K.; Scherf, U. Organic Light-Emitting Devices: Synthesis, Properties and Applications; Wiley-VCH, 2006.
    6. 6
      Burn, P. L.; Lo, S.-C.; Samuel, I. D. W. The Development of Light-Emitting Dendrimers for Displays. Adv. Mater. 2007, 19, 16751688,  DOI: 10.1002/adma.200601592
    7. 7
      Ostroverkhova, O. Organic Optoelectronic Materials: Mechanisms and Applications. Chem. Rev. 2016, 116, 1327913412,  DOI: 10.1021/acs.chemrev.6b00127
    8. 8
      Thompson, B. C.; Fréchet, J. M. J. Polymer-Fullerene Composite Solar Cells. Angew. Chem., Int. Ed. 2008, 47, 5877,  DOI: 10.1002/anie.200702506
    9. 9
      Günes, S.; Neugebauer, H.; Sariciftci, N. S. Conjugated Polymer-Based Organic Solar Cells. Chem. Rev. 2007, 107, 13241338,  DOI: 10.1021/cr050149z
    10. 10
      Son, H. J.; He, F.; Carsten, B.; Yu, L. Are we there yet? Design of better conjugated polymers for polymer solar cells. J. Mater. Chem. 2011, 21, 1893418945,  DOI: 10.1039/c1jm12388b
    11. 11
      Cheng, Y.-J.; Yang, S.-H.; Hsu, C.-S. Synthesis of Conjugated Polymers for Organic Solar Cell Applications. Chem. Rev. 2009, 109, 58685923,  DOI: 10.1021/cr900182s
    12. 12
      Chen, Y.; Zhao, Y.; Liang, Z. Solution processed organic thermoelectrics: towards flexible thermoelectric modules. Energy Environ. Sci. 2015, 8, 401422,  DOI: 10.1039/C4EE03297G
    13. 13
      Park, T.; Park, C.; Kim, B.; Shin, H.; Kim, E. Flexible PEDOT electrodes with large thermoelectric power factors to generate electricity by the touch of fingertips. Energy Environ. Sci. 2013, 6, 788792,  DOI: 10.1039/c3ee23729j
    14. 14
      Shi, K.; Zhang, F.; Di, C.-A.; Yan, T.-W.; Zou, Y.; Zhou, X.; Zhu, D.; Wang, J.-Y.; Pei, J. Toward High Performance n-Type Thermoelectric Materials by Rational Modification of BDPPV Backbones. J. Am. Chem. Soc. 2015, 137, 69796982,  DOI: 10.1021/jacs.5b00945
    15. 15
      Schlitz, R. A.; Brunetti, F. G.; Glaudell, A. M.; Miller, P. L.; Brady, M. A.; Takacs, C. J.; Hawker, C. J.; Chabinyc, M. L. Solubility-Limited Extrinsic n-Type Doping of a High Electron Mobility Polymer for Thermoelectric Applications. Adv. Mater. 2014, 26, 28252830,  DOI: 10.1002/adma.201304866
    16. 16
      Lavieville, R.; Zhang, Y.; Casu, A.; Genovese, A.; Manna, L.; Di Fabrizio, E.; Krahne, R. Charge Transport in Nanoscale “All-Inorganic” Networks of Semiconductor Nanorods Linked by Metal Domains. ACS Nano 2012, 6, 29402947,  DOI: 10.1021/nn3006625
    17. 17
      Anthony, J. E. Functionalized Acenes and Heteroacenes for Organic Electronics. Chem. Rev. 2006, 106, 50285048,  DOI: 10.1021/cr050966z
    18. 18
      Coropceanu, V.; Cornil, J.; da Silva Filho, D. A.; Olivier, Y.; Silbey, R.; Brédas, J.-L. Charge Transport in Organic Semiconductors. Chem. Rev. 2007, 107, 926952,  DOI: 10.1021/cr050140x
    19. 19
      Takimiya, K.; Shinamura, S.; Osaka, I.; Miyazaki, E. Thienoacene-Based Organic Semiconductors. Adv. Mater. 2011, 23, 43474370,  DOI: 10.1002/adma.201102007
    20. 20
      Liu, C.; Huang, K.; Park, W.-T.; Li, M.; Yang, T.; Liu, X.; Liang, L.; Minari, T.; Noh, Y.-Y. A unified understanding of charge transport in organic semiconductors: the importance of attenuated delocalization for the carriers. Mater. Horiz. 2017, 4, 608618,  DOI: 10.1039/C7MH00091J
    21. 21
      Ji, L.-F.; Fan, J.-X.; Qin, G.-Y.; Zhang, N.-X.; Lin, P.-P.; Ren, A.-M. Theoretical Study on the Electronic Structures and Charge Transport Properties of a Series of Rubrene Derivatives. J. Phys. Chem. C 2018, 122, 2122621238,  DOI: 10.1021/acs.jpcc.8b07018
    22. 22
      Wang, Y.; Sun, L.; Wang, C.; Yang, F.; Ren, X.; Zhang, X.; Dong, H.; Hu, W. Organic crystalline materials in flexible electronics. Chem. Soc. Rev. 2019, 48, 14921530,  DOI: 10.1039/C8CS00406D
    23. 23
      Gryn’ova, G.; Lin, K.-H.; Corminboeuf, C. Read between the Molecules: Computational Insights into Organic Semiconductors. J. Am. Chem. Soc. 2018, 140, 1637016386,  DOI: 10.1021/jacs.8b07985
    24. 24
      McGarry, K. A.; Xie, W.; Sutton, C.; Risko, C.; Wu, Y.; Young, V. G.; Brédas, J.-L.; Frisbie, C. D.; Douglas, C. J. Rubrene-Based Single-Crystal Organic Semiconductors: Synthesis, Electronic Structure, and Charge-Transport Properties. Chem. Mater. 2013, 25, 22542263,  DOI: 10.1021/cm400736s
    25. 25
      Giri, G.; Verploegen, E.; Mannsfeld, S. C. B.; Atahan-Evrenk, S.; Kim, D. H.; Lee, S. Y.; Becerril, H. A.; Aspuru-Guzik, A.; Toney, M. F.; Bao, Z. Tuning charge transport in solution-sheared organic semiconductors using lattice strain. Nature 2011, 480, 504,  DOI: 10.1038/nature10683
    26. 26
      Rühle, V.; Lukyanov, A.; May, F.; Schrader, M.; Vehoff, T.; Kirkpatrick, J.; Baumeier, B.; Andrienko, D. Microscopic Simulations of Charge Transport in Disordered Organic Semiconductors. J. Chem. Theory Comput. 2011, 7, 33353345,  DOI: 10.1021/ct200388s
    27. 27
      Nomura, K.; Ohta, H.; Takagi, A.; Kamiya, T.; Hirano, M.; Hosono, H. Room-temperature fabrication of transparent flexible thin-film transistors using amorphous oxide semiconductors. Nature 2004, 432, 488492,  DOI: 10.1038/nature03090
    28. 28
      Kuribara, K.; Wang, H.; Uchiyama, N.; Fukuda, K.; Yokota, T.; Zschieschang, U.; Jaye, C.; Fischer, D.; Klauk, H.; Yamamoto, T.; Takimiya, K.; Ikeda, M.; Kuwabara, H.; Sekitani, T.; Loo, Y.-L.; Someya, T. Organic transistors with high thermal stability for medical applications. Nat. Commun. 2012, 3, 723,  DOI: 10.1038/ncomms1721
    29. 29
      Payne, M. M.; Parkin, S. R.; Anthony, J. E. Functionalized Higher Acenes: Hexacene and Heptacene. J. Am. Chem. Soc. 2005, 127, 80288029,  DOI: 10.1021/ja051798v
    30. 30
      Tang, M. L.; Okamoto, T.; Bao, Z. High-Performance Organic Semiconductors: Asymmetric Linear Acenes Containing Sulphur. J. Am. Chem. Soc. 2006, 128, 1600216003,  DOI: 10.1021/ja066824j
    31. 31
      Wong, M. Y.; Hedley, G. J.; Xie, G.; Kölln, L. S.; Samuel, I. D. W.; Pertegás, A.; Bolink, H. J.; Zysman-Colman, E. Light-Emitting Electrochemical Cells and Solution-Processed Organic Light-Emitting Diodes Using Small Molecule Organic Thermally Activated Delayed Fluorescence Emitters. Chem. Mater. 2015, 27, 65356542,  DOI: 10.1021/acs.chemmater.5b03245
    32. 32
      Bin, H.; Yang, Y.; Zhang, Z.-G.; Ye, L.; Ghasemi, M.; Chen, S.; Zhang, Y.; Zhang, C.; Sun, C.; Xue, L.; Yang, C.; Ade, H.; Li, Y. 9.73% Efficiency Nonfullerene All Organic Small Molecule Solar Cells with Absorption-Complementary Donor and Acceptor. J. Am. Chem. Soc. 2017, 139, 50855094,  DOI: 10.1021/jacs.6b12826
    33. 33
      Lin, L.-Y.; Chen, Y.-H.; Huang, Z.-Y.; Lin, H.-W.; Chou, S.-H.; Lin, F.; Chen, C.-W.; Liu, Y.-H.; Wong, K.-T. A Low-Energy-Gap Organic Dye for High-Performance Small-Molecule Organic Solar Cells. J. Am. Chem. Soc. 2011, 133, 1582215825,  DOI: 10.1021/ja205126t
    34. 34
      Sun, Y.; Welch, G. C.; Leong, W. L.; Takacs, C. J.; Bazan, G. C.; Heeger, A. J. Solution-processed small-molecule solar cells with 6.7% efficiency. Nat. Mater. 2012, 11, 44,  DOI: 10.1038/nmat3160
    35. 35
      Maliakal, A.; Raghavachari, K.; Katz, H.; Chandross, E.; Siegrist, T. Photochemical Stability of Pentacene and a Substituted Pentacene in Solution and in Thin Films. Chem. Mater. 2004, 16, 49804986,  DOI: 10.1021/cm049060k
    36. 36
      Laquindanum, J. G.; Katz, H. E.; Lovinger, A. J. Synthesis, Morphology, and Field-Effect Mobility of Anthradithiophenes. J. Am. Chem. Soc. 1998, 120, 664672,  DOI: 10.1021/ja9728381
    37. 37
      Mishra, A.; Bäuerle, P. Small Molecule Organic Semiconductors on the Move: Promises for Future Solar Energy Technology. Angew. Chem., Int. Ed. 2012, 51, 20202067,  DOI: 10.1002/anie.201102326
    38. 38
      Leung, L. M.; Lo, W. Y.; So, S. K.; Lee, K. M.; Choi, W. K. A High-Efficiency Blue Emitter for Small Molecule-Based Organic Light-Emitting Diode. J. Am. Chem. Soc. 2000, 122, 56405641,  DOI: 10.1021/ja000927z
    39. 39
      Kulkarni, A. P.; Tonzola, C. J.; Babel, A.; Jenekhe, S. A. Electron Transport Materials for Organic Light-Emitting Diodes. Chem. Mater. 2004, 16, 45564573,  DOI: 10.1021/cm049473l
    40. 40
      Liu, Y.; Li, C.; Ren, Z.; Yan, S.; Bryce, M. R. All-organic thermally activated delayed fluorescence materials for organic light-emitting diodes. Nat. Rev. Mater. 2018, 3, 18020,  DOI: 10.1038/natrevmats.2018.20
    41. 41
      Klauk, H.; Halik, M.; Zschieschang, U.; Schmid, G.; Radlik, W.; Weber, W. High-mobility polymer gate dielectric pentacene thin film transistors. J. Appl. Phys. 2002, 92, 52595263,  DOI: 10.1063/1.1511826
    42. 42
      Ebata, H.; Izawa, T.; Miyazaki, E.; Takimiya, K.; Ikeda, M.; Kuwabara, H.; Yui, T. Highly Soluble [1]Benzothieno[3,2-b]benzothiophene (BTBT) Derivatives for High-Performance, Solution-Processed Organic Field-Effect Transistors. J. Am. Chem. Soc. 2007, 129, 1573215733,  DOI: 10.1021/ja074841i
    43. 43
      Yamamoto, T.; Takimiya, K. Facile Synthesis of Highly π-Extended Heteroarenes, Dinaphtho[2,3-b:2‘,3′-f]chalcogenopheno[3,2-b]chalcogenophenes, and Their Application to Field-Effect Transistors. J. Am. Chem. Soc. 2007, 129, 22242225,  DOI: 10.1021/ja068429z
    44. 44
      Wang, C.; Dong, H.; Hu, W.; Liu, Y.; Zhu, D. Semiconducting π-Conjugated Systems in Field-Effect Transistors: A Material Odyssey of Organic Electronics. Chem. Rev. 2012, 112, 22082267,  DOI: 10.1021/cr100380z
    45. 45
      Curtis, M. D.; Cao, J.; Kampf, J. W. Solid-State Packing of Conjugated Oligomers: From π-Stacks to the Herringbone Structure. J. Am. Chem. Soc. 2004, 126, 43184328,  DOI: 10.1021/ja0397916
    46. 46
      Purushothaman, B.; Bruzek, M.; Parkin, S. R.; Miller, A.-F.; Anthony, J. E. Synthesis and Structural Characterization of Crystalline Nonacenes. Angew. Chem., Int. Ed. 2011, 50, 70137017,  DOI: 10.1002/anie.201102671
    47. 47
      Anthony, J. E. The Larger Acenes: Versatile Organic Semiconductors. Angew. Chem., Int. Ed. 2008, 47, 452483,  DOI: 10.1002/anie.200604045
    48. 48
      Uemura, T.; Hirose, Y.; Uno, M.; Takimiya, K.; Takeya, J. Very High Mobility in Solution-Processed Organic Thin-Film Transistors of Highly Ordered [1]Benzothieno[3,2-b]benzothiophene Derivatives. Appl. Phys. Express 2009, 2, 111501,  DOI: 10.1143/APEX.2.111501
    49. 49
      Soeda, J.; Uemura, T.; Okamoto, T.; Mitsui, C.; Yamagishi, M.; Takeya, J. Inch-Size Solution-Processed Single-Crystalline Films of High-Mobility Organic Semiconductors. Appl. Phys. Express 2013, 6, 076503,  DOI: 10.7567/APEX.6.076503
    50. 50
      Yamamura, A.; Watanabe, S.; Uno, M.; Mitani, M.; Mitsui, C.; Tsurumi, J.; Isahaya, N.; Kanaoka, Y.; Okamoto, T.; Takeya, J. Wafer-scale, layer-controlled organic single crystals for high-speed circuit operation. Sci. Adv. 2018, 4, eaao5758  DOI: 10.1126/sciadv.aao5758
    51. 51
      Yamamura, A.; Matsui, H.; Uno, M.; Isahaya, N.; Tanaka, Y.; Kudo, M.; Ito, M.; Mitsui, C.; Okamoto, T.; Takeya, J. Painting Integrated Complementary Logic Circuits for Single-Crystal Organic Transistors: A Demonstration of a Digital Wireless Communication Sensing Tag. Adv. Electron. Mater. 2017, 3, 1600456,  DOI: 10.1002/aelm.201600456
    52. 52
      Kang, M. J.; Doi, I.; Mori, H.; Miyazaki, E.; Takimiya, K.; Ikeda, M.; Kuwabara, H. Alkylated Dinaphtho[2,3-b:2′,3′-f]Thieno[3,2-b]Thiophenes (Cn-DNTTs): Organic Semiconductors for High-Performance Thin-Film Transistors. Adv. Mater. 2011, 23, 12221225,  DOI: 10.1002/adma.201001283
    53. 53
      Iino, H.; Usui, T.; Hanna, J.-i. Liquid crystals for organic thin-film transistors. Nat. Commun. 2015, 6, 6828,  DOI: 10.1038/ncomms7828
    54. 54
      Inoue, S.; Minemawari, H.; Tsutsumi, J. y.; Chikamatsu, M.; Yamada, T.; Horiuchi, S.; Tanaka, M.; Kumai, R.; Yoneya, M.; Hasegawa, T. Effects of Substituted Alkyl Chain Length on Solution-Processable Layered Organic Semiconductor Crystals. Chem. Mater. 2015, 27, 38093812,  DOI: 10.1021/acs.chemmater.5b00810
    55. 55
      He, K.; Li, W.; Tian, H.; Zhang, J.; Yan, D.; Geng, Y.; Wang, F. Asymmetric Conjugated Molecules Based on [1]Benzothieno[3,2-b][1]benzothiophene for High-Mobility Organic Thin-Film Transistors: Influence of Alkyl Chain Length. ACS Appl. Mater. Interfaces 2017, 9, 3542735436,  DOI: 10.1021/acsami.7b10675
    56. 56
      Grigoriadis, C.; Niebel, C.; Ruzié, C.; Geerts, Y. H.; Floudas, G. Order, Viscoelastic, and Dielectric Properties of Symmetric and Asymmetric Alkyl[1]benzothieno[3,2-b][1]benzothiophenes. J. Phys. Chem. B 2014, 118, 14431451,  DOI: 10.1021/jp412422e
    57. 57
      Inoue, S.; Shinamura, S.; Sadamitsu, Y.; Arai, S.; Horiuchi, S.; Yoneya, M.; Takimiya, K.; Hasegawa, T. Extended and Modulated Thienothiophenes for Thermally Durable and Solution-Processable Organic Semiconductors. Chem. Mater. 2018, 30, 50505060,  DOI: 10.1021/acs.chemmater.8b01339
    58. 58
      Diao, Y.; Tee, B. C. K.; Giri, G.; Xu, J.; Kim, D. H.; Becerril, H. A.; Stoltenberg, R. M.; Lee, T. H.; Xue, G.; Mannsfeld, S. C. B.; Bao, Z. Solution coating of large-area organic semiconductor thin films with aligned single-crystalline domains. Nat. Mater. 2013, 12, 665,  DOI: 10.1038/nmat3650
    59. 59
      Nakayama, K.; Hirose, Y.; Soeda, J.; Yoshizumi, M.; Uemura, T.; Uno, M.; Li, W.; Kang, M. J.; Yamagishi, M.; Okada, Y.; Miyazaki, E.; Nakazawa, Y.; Nakao, A.; Takimiya, K.; Takeya, J. Patternable Solution-Crystallized Organic Transistors with High Charge Carrier Mobility. Adv. Mater. 2011, 23, 16261629,  DOI: 10.1002/adma.201004387
    60. 60
      Yuan, Y.; Giri, G.; Ayzner, A. L.; Zoombelt, A. P.; Mannsfeld, S. C. B.; Chen, J.; Nordlund, D.; Toney, M. F.; Huang, J.; Bao, Z. Ultra-high mobility transparent organic thin film transistors grown by an off-centre spin-coating method. Nat. Commun. 2014, 5, 3005,  DOI: 10.1038/ncomms4005
    61. 61
      Iino, H.; Kobori, T.; Hanna, J.-i. Improved thermal stability in organic FET fabricated with a soluble BTBT derivative. J. Non-Cryst. Solids 2012, 358, 25162519,  DOI: 10.1016/j.jnoncrysol.2012.03.021
    62. 62
      Okamoto, K.; Kawamura, T.; Sone, M.; Ogino, K. Study on liquid crystallinity in 2,9-dialkylpentacenes. Liq. Cryst. 2007, 34, 10011007,  DOI: 10.1080/02678290701478970
    63. 63
      Kuwabara, H.; Ikeda, M.; Takimiya, K. U.S. Patent 2011/0303910 A1, 2010.
    64. 64
      Fratini, S.; Ciuchi, S.; Mayou, D.; de Laissardière, G. T.; Troisi, A. A map of high-mobility molecular semiconductors. Nat. Mater. 2017, 16, 998,  DOI: 10.1038/nmat4970
    65. 65
      Troisi, A.; Orlandi, G.; Anthony, J. E. Electronic Interactions and Thermal Disorder in Molecular Crystals Containing Cofacial Pentacene Units. Chem. Mater. 2005, 17, 50245031,  DOI: 10.1021/cm051150h
    66. 66
      Ciuchi, S.; Fratini, S. Electronic transport and quantum localization effects in organic semiconductors. Phys. Rev. B: Condens. Matter Mater. Phys. 2012, 86, 245201,  DOI: 10.1103/PhysRevB.86.245201
    67. 67
      Illig, S.; Eggeman, A. S.; Troisi, A.; Jiang, L.; Warwick, C.; Nikolka, M.; Schweicher, G.; Yeates, S. G.; Henri Geerts, Y.; Anthony, J. E.; Sirringhaus, H. Reducing dynamic disorder in small-molecule organic semiconductors by suppressing large-amplitude thermal motions. Nat. Commun. 2016, 7, 10736,  DOI: 10.1038/ncomms10736
    68. 68
      Okamoto, T.; Mitsui, C.; Yamagishi, M.; Nakahara, K.; Soeda, J.; Hirose, Y.; Miwa, K.; Sato, H.; Yamano, A.; Matsushita, T.; Uemura, T.; Takeya, J. V-shaped organic semiconductors with solution processability, high mobility, and high thermal durability. Adv. Mater. 2013, 25, 63926397,  DOI: 10.1002/adma.201302086
    69. 69
      Mitsui, C.; Okamoto, T.; Matsui, H.; Yamagishi, M.; Matsushita, T.; Soeda, J.; Miwa, K.; Sato, H.; Yamano, A.; Uemura, T.; Takeya, J. Dinaphtho[1,2b:2′,1’d]chalcogenophenes: Comprehensive Investigation of the Effect of the Chalcogen Atoms in the Phenacene-Type π Electronic Cores. Chem. Mater. 2013, 25, 39523956,  DOI: 10.1021/cm303376g
    70. 70
      Mitsui, C.; Okamoto, T.; Yamagishi, M.; Tsurumi, J.; Yoshimoto, K.; Nakahara, K.; Soeda, J.; Hirose, Y.; Sato, H.; Yamano, A.; Uemura, T.; Takeya, J. High-performance solution-processable N-shaped organic semiconducting materials with stabilized crystal phase. Adv. Mater. 2014, 26, 45464551,  DOI: 10.1002/adma.201400289
    71. 71
      Mitsui, C.; Yamagishi, M.; Shikata, R.; Ishii, H.; Matsushita, T.; Nakahara, K.; Yano, M.; Sato, H.; Yamano, A.; Takeya, J.; Okamoto, T. Oxygen- and sulfur-bridged bianthracene V-shaped organic semiconductors. Bull. Chem. Soc. Jpn. 2017, 90, 931938,  DOI: 10.1246/bcsj.20170030
    72. 72
      Mitsui, C.; Tsuyama, H.; Shikata, R.; Murata, Y.; Kuniyasu, H.; Yamagishi, M.; Ishii, H.; Yamamoto, A.; Hirose, Y.; Yano, M.; Takehara, T.; Suzuki, T.; Sato, H.; Yamano, A.; Fukuzaki, E.; Watanabe, T.; Usami, Y.; Takeya, J.; Okamoto, T. High performance solution-crystallized thin-film transistors based on V-shaped thieno[3,2-f:4,5-f’]bis[1]benzothiophene semiconductors. J. Mater. Chem. C 2017, 5, 19031909,  DOI: 10.1039/C6TC04721A
    73. 73
      Yamamoto, A.; Murata, Y.; Mitsui, C.; Ishii, H.; Yamagishi, M.; Yano, M.; Sato, H.; Yamano, A.; Takeya, J.; Okamoto, T. Zigzag-Elongated Fused pi-Electronic Core: A Molecular Design Strategy to Maximize Charge-Carrier Mobility. Adv. Sci. 2018, 5, 1700317,  DOI: 10.1002/advs.201700317
    74. 74
      Tsurumi, J.; Matsui, H.; Kubo, T.; Hausermann, R.; Mitsui, C.; Okamoto, T.; Watanabe, S.; Takeya, J. Coexistence of ultra-long spin relaxation time and coherent charge transport in organic single-crystal semiconductors. Nat. Phys. 2017, 13, 994998,  DOI: 10.1038/nphys4217
    75. 75
      Solubility Parameter. Bulletin of the American Group; International Institute for Conservation of Historic and Artistic Works, 1968; Vol. 8, pp 2024.
    76. 76

      The reorganization energy was calculated based on the optimized structure by DFT at the B3LYP/6-31G(d) level.

    77. 77
      Schleyer, P. v. R.; Maerker, C.; Dransfeld, A.; Jiao, H.; van Eikema Hommes, N. J. R. Nucleus-Independent Chemical Shifts: A Simple and Efficient Aromaticity Probe. J. Am. Chem. Soc. 1996, 118, 63176318,  DOI: 10.1021/ja960582d
    78. 78
      Chen, Z.; Wannere, C. S.; Corminboeuf, C.; Puchta, R.; Schleyer, P. v. R. Nucleus-Independent Chemical Shifts (NICS) as an Aromaticity Criterion. Chem. Rev. 2005, 105, 38423888,  DOI: 10.1021/cr030088+
    79. 79
      Münzel, N.; Kesper, K.; Schweig, A.; Specht, H. Detection of 2,5-dimethylene-2,5-dihydrothiophene and thiophenoradialene. Tetrahedron Lett. 1988, 29, 62396242,  DOI: 10.1016/S0040-4039(00)82314-X
    80. 80
      Okamoto, H.; Kawasaki, N.; Kaji, Y.; Kubozono, Y.; Fujiwara, A.; Yamaji, M. Air-assisted High-performance Field-effect Transistor with Thin Films of Picene. J. Am. Chem. Soc. 2008, 130, 1047010471,  DOI: 10.1021/ja803291a
    81. 81
      Kawai, N.; Eguchi, R.; Goto, H.; Akaike, K.; Kaji, Y.; Kambe, T.; Fujiwara, A.; Kubozono, Y. Characteristics of Single Crystal Field-Effect Transistors with a New Type of Aromatic Hydrocarbon, Picene. J. Phys. Chem. C 2012, 116, 79837988,  DOI: 10.1021/jp300052p
    82. 82
      De, A.; Ghosh, R.; Roychowdhury, S.; Roychowdhury, P. Structural analysis of picene, C22H14. Acta Crystallogr., Sect. C: Cryst. Struct. Commun. 1985, 41, 907909,  DOI: 10.1107/S0108270185005959
    83. 83
      Tedjamulia, M. L.; Tominaga, Y.; Castle, R. N.; Lee, M. L. The synthesis of dinaphthothiophenes. J. Heterocyclic Chem. 1983, 20, 11431148,  DOI: 10.1002/jhet.5570200502
    84. 84
      Lloyd-Jones, G. C.; Moseley, J. D.; Renny, J. S. Mechanism and Application of the Newman-Kwart O→S Rearrangement of O-Aryl Thiocarbamates. Synthesis 2008, 2008, 661689,  DOI: 10.1055/s-2008-1032179
    85. 85
      Matsuoka, M.; Iwamoto, A.; Kitao, T. Reaction of 2, 3-dichloro-1, 4-naphthoquinone with dithiooxamide. Synthesis of dibenzo[b, i]thianthrene-5, 7, 12, 14-tetrone. J. Heterocycl. Chem. 1991, 28, 14451447,  DOI: 10.1002/jhet.5570280543
    86. 86
      De, P. K.; Neckers, D. C. Sulfur Containing Stable Unsubstituted Heptacene Analogs. Org. Lett. 2012, 14, 7881,  DOI: 10.1021/ol2028724
    87. 87
      Wex, B.; Kaafarani, B. R.; Kirschbaum, K.; Neckers, D. C. Synthesis of the anti and syn Isomers of Thieno[f, f‘]bis[1]benzothiophene. Comparison of the Optical and Electrochemical Properties of the anti and syn Isomers1. J. Org. Chem. 2005, 70, 45024505,  DOI: 10.1021/jo048010w
    88. 88
      Armarego, W. L. F. The synthesis of two dinaphthothiophens. J. Chem. Soc. 1960, 433436,  DOI: 10.1039/jr9600000433
    89. 89
      Shinamura, S.; Osaka, I.; Miyazaki, E.; Nakao, A.; Yamagishi, M.; Takeya, J.; Takimiya, K. Linear- and Angular-Shaped Naphthodithiophenes: Selective Synthesis, Properties, and Application to Organic Field-Effect Transistors. J. Am. Chem. Soc. 2011, 133, 50245035,  DOI: 10.1021/ja110973m
    90. 90
      Mamane, V.; Hannen, P.; Fürstner, A. Synthesis of Phenanthrenes and Polycyclic Heteroarenes by Transition-Metal Catalyzed Cycloisomerization Reactions. Chem. - Eur. J. 2004, 10, 45564575,  DOI: 10.1002/chem.200400220
    91. 91
      Laudise, R. A.; Kloc, C.; Simpkins, P. G.; Siegrist, T. Physical vapor growth of organic semiconductors. J. Cryst. Growth 1998, 187, 449454,  DOI: 10.1016/S0022-0248(98)00034-7
    92. 92
      Kloc, C.; Simpkins, P. G.; Siegrist, T.; Laudise, R. A. Physical vapor growth of centimeter-sized crystals of α-hexathiophene. J. Cryst. Growth 1997, 182, 416427,  DOI: 10.1016/S0022-0248(97)00370-9
    93. 93
      Izawa, T.; Miyazaki, E.; Takimiya, K. Molecular Ordering of High-Performance Soluble Molecular Semiconductors and Re-evaluation of Their Field-Effect Transistor Characteristics. Adv. Mater. 2008, 20, 33883392,  DOI: 10.1002/adma.200800799
    94. 94
      Takeya, J.; Tsukagoshi, K.; Aoyagi, Y.; Takenobu, T.; Iwasa, Y. Hall Effect of Quasi-Hole Gas in Organic Single-Crystal Transistors. Jpn. J. Appl. Phys. 2005, 44, L1393L1396,  DOI: 10.1143/JJAP.44.L1393
    95. 95
      Podzorov, V.; Menard, E.; Rogers, J. A.; Gershenson, M. E. Hall Effect in the Accumulation Layers on the Surface of Organic Semiconductors. Phys. Rev. Lett. 2005, 95, 226601,  DOI: 10.1103/PhysRevLett.95.226601
    96. 96
      Kubo, T.; Haeusermann, R.; Tsurumi, J.; Soeda, J.; Okada, Y.; Yamashita, Y.; Akamatsu, N.; Shishido, A.; Mitsui, C.; Okamoto, T.; Yanagisawa, S.; Matsui, H.; Takeya, J. Suppressing molecular vibrations in organic semiconductors by inducing strain. Nat. Commun. 2016, 7, 11156,  DOI: 10.1038/ncomms11156
    97. 97
      Oyama, T.; Yang, Y. S.; Matsuo, K.; Yasuda, T. Effects of chalcogen atom substitution on the optoelectronic and charge-transport properties in picene-type π-systems. Chem. Commun. 2017, 53, 38143817,  DOI: 10.1039/C7CC01292F
  • Supporting Information

    Supporting Information

    ARTICLE SECTIONS
    Jump To

    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/jacs.9b10450.

    • Video demonstrating the edge-casting technique (AVI)


    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.

Pair your accounts.

Export articles to Mendeley

Get article recommendations from ACS based on references in your Mendeley library.

Pair your accounts.

Export articles to Mendeley

Get article recommendations from ACS based on references in your Mendeley library.

You’ve supercharged your research process with ACS and Mendeley!

STEP 1:
Click to create an ACS ID

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

Please note: If you switch to a different device, you may be asked to login again with only your ACS ID.

OOPS

You have to login with your ACS ID befor you can login with your Mendeley account.

MENDELEY PAIRING EXPIRED
Your Mendeley pairing has expired. Please reconnect

This website uses cookies to improve your user experience. By continuing to use the site, you are accepting our use of cookies. Read the ACS privacy policy.

CONTINUE