- About this Journal ·
- Abstracting and Indexing ·
- Advance Access ·
- Aims and Scope ·
- Article Processing Charges ·
- Articles in Press ·
- Author Guidelines ·
- Bibliographic Information ·
- Citations to this Journal ·
- Contact Information ·
- Editorial Board ·
- Editorial Workflow ·
- Free eTOC Alerts ·
- Publication Ethics ·
- Reviewers Acknowledgment ·
- Submit a Manuscript ·
- Subscription Information ·
- Table of Contents
International Journal of Polymer Science
Volume 2012 (2012), Article ID 852063, 10 pages
Polysilsesquioxanes for Gate-Insulating Materials of Organic Thin-Film Transistors
1Electronic Material Research Division, Osaka Municipal Technical Research Institute, Osaka 536-8553, Japan
2JST Innovation Plaza Osaka, Osaka 594-1131, Japan
3Department of Physics and Electronics, Osaka Prefecture University, Osaka 599-8531, Japan
Received 11 August 2012; Accepted 11 September 2012
Academic Editor: Yoshiro Kaneko
Copyright © 2012 Kimihiro Matsukawa et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Printable organic thin-film transistor (O-TFT) is one of the most recognized technical issues nowadays. Our recent progress on the formation of organic-inorganic hybrid thin films consists of polymethylsilsesquioxane (PMSQ), and its applications for the gate-insulating layer of O-TFTs are introduced in this paper. PMSQ synthesized in toluene solution with formic acid catalyst exhibited the electric resistivity of higher than 1014 Ω cm after thermal treatment at 150°C, and the very low concentration of residual silanol groups in PMSQ was confirmed. The PMSQ film contains no mobile ionic impurities, and this is also important property for the practical use for the gate-insulating materials. In the case of top-contact type TFT using poly(3-hexylthiophene) (P3HT) with PMSQ gate-insulating layer, the device properties were comparable with the TFTs having thermally grown SiO2 gate-insulating layer. The feasibility of PMSQ as a gate-insulating material for O-TFTs, which was fabricated on a flexible plastic substrate, has been demonstrated. Moreover, by the modification of PMSQ, further functionalities, such as surface hydrophobicity, high permittivity that allows low driving voltage, and photocurability that allows photolithography, could be appended to the PMSQ gate-insulating layers.
Organic thin-film transistor (O-TFT) is an indispensable component in the development of large-area, flexible, and low-cost electronic devices, such as paper-like displays, radio frequency identification tags, and high-performance sensors. However, as the conventional method of O-TFT fabrication, which includes multiple steps of vacuum processing, is complicated and costly, the convenient fabrication process for O-TFT is required in the industrial demand. Thus, the solution based method has attracted increasing attention to achieve low-cost fabrication of O-TFTs. Printable organic semiconductors have been widely investigated [1, 2] and the wide technology for printed electronics is progressing rapidly. As a solution processible gate-insulating layer for O-TFT devices, various organic polymers have been examined, including polyvinylphenol (PVP) [3, 4], polymethylmethacrylate , polyimide , and polyvinylalcohol , so far. Since organic polymer based gate-insulating materials exhibited lower electric and chemical resistivity than that of inorganic dielectrics, those organic polymers are not the optimum material for the insulating layer of multilayered electronic devices. On the other hand, organic-inorganic hybrid materials will be the most promising materials that can solve these problems, because organic-inorganic hybrids are expected to have specific properties derived from both organic and inorganic component, that is, solution processibility, flexibility, and high resistivity. In the point of view from organic-inorganic hybrids, we have developed novel organic-inorganic hybrid materials that can make a gate-insulating layer of O-TFT by a simple solution process. In this paper, our recent progresses on the construction of organic-inorganic hybrid thin films consist of polysilsesquioxane, and its applications for the gate-insulating layer of O-TFTs are introduced.
2. Required Properties of Gate-Insulating Layer for O-TFT
As shown in Figure 1, a bottom-gate/top-contact type O-TFT consists of a gate electrode, gate-insulating layer, organic semiconductor layer, and source and drain electrodes, respectively. Furthermore, in order to keep the high durability of O-TFT component, the O-TFT must be covered by a passivation layer, and an upper electrode is formed on the passivation layer. The upper electrode is connected with the drain electrode through a contact hole in the passivation layer, which transfers electric signals from O-TFT to a driving electrode of devices such as liquid crystal or electric paper ink. In those components of O-TFT, electric resistivity and permittivity of the gate-insulating layer are known to largely affect the electric performance of the O-TFT, because charge transfer through the channel, that is, the gap between the source and drain electrodes, is strictly controlled by applied gate-voltage (), which induces electric field through the gate-insulating layer and results in charge accumulation at the interface between the gate-insulating layer and the organic semiconductor layer. In general, the well-known inorganic gate-insulating films, such as silicon nitrate by plasma CVD , aluminum oxide , and tantalum oxide  by sputter process, are prepared by a costly high-temperature vacuum process. There is a requirement of optimized material for gate-insulating layer to manufacture high-performance O-TFTs. In case of fabricating O-TFT onto flexible plastic substrates, the most important requirement is a low-temperature curability, since there is a limitation of process temperature. As a material must form a cross-linked thin film at relatively low temperature, polysilsesquioxane has been recognized as a promising candidate [11–15]. However, previous attempts resulted in low electric resistivity and stability [14, 15], because residual silanol groups in polysilsesquioxane have not condensed completely. It is indispensable for polysilsesquioxane to solve this problem, in order to apply as gate-insulating material of O-TFTs. In addition, gate-insulating materials are also required to be low ionic impurity concentration, high permittivity, high-surface smoothness, low-surface free energy, and so forth. We have developed novel polysilsesquioxanes that accomplished these requirements.
3. Synthesis of Polymethylsilsesquioxane (PMSQ)
Materials for gate-insulating layer of O-TFTs should exhibit high electric resistivity (more than 1013 Ω cm) and high permittivity. As a possible material for such requirements, we investigated polymethylsilsesquioxane (PMSQ) that can be synthesized by sol-gel condensation of methyltrimethoxysilane (Figure 2). In order to develop highly cross-linked PMSQ films with low concentration of residual silanol groups, which have reduced electric resistivity, PMSQ was synthesized under various reaction conditions . 1H-NMR spectra of PMSQ prepared in methanol and toluene are shown in Figure 3. The amounts of silanol Si-OH were estimated based on the amount of silylmethyl group Si-CH3, revealing that silanol content was extremely small when PMSQ was prepared in toluene compared to that in methanol. Also by a measurement of 29Si-NMR, the amount of highly cross-linked T3 structure, which is corresponding to the silicon atom attached to one alkyl group and three siloxane groups, was twice larger in toluene than that in methanol. This observation indicates also low concentration of silanol groups. It is found that these results were caused by the difference of the polarity of solvents. In the case of the sol-gel reaction under hydrophobic condition in toluene, the collision frequency of silanol groups will increase by hydrophilic interaction, so that enhances the condensation reaction rate, leading to a decrease in the silanol concentration. On the other hand, the excessive water or methanol molecules in the reaction mixture will stabilize silanol groups, which interfere with the condensation reaction to PMSQ with less residual silanols. Therefore, the condensation was carried out under reduced pressure, as shown in Figure 2, to remove methanol and water from propylene glycol monomethyl ether acetate (PGMEA) solution. For the practical use of PMSQ as a gate-insulating material, PMSQ solution should be coated onto the gate electrode, and the thin film was baked to complete consumption of residual silanols. Figure 4 shows the FT-IR spectra of spin-coated PMSQ films before and after thermal treatment at 100 and 150°C for 1 h in air. The absorption bands at 902 cm−1, 1030 cm−1, and 1270 cm−1 are attributed to the bonds of Si–OH, Si–O–Si, and Si–CH3, respectively. The absorption peak of the silanol groups (Si–OH) disappeared completely, and the intensity of the siloxane bonds (Si–O–Si) markedly increased on thermal treatment at 150°C . This result clearly indicated that the cross-linking reaction of the silanol groups proceeded effectively even at low-temperature treatment less than 150°C, forming the higher cross-linked siloxane network.
Electric resistivity and permittivity of PMSQ thin films prepared in different solvents were measured using Al/PMSQ/Al cell structures fabricated on glass substrates and summarized in Table 1. It was found that the electrical resistivity of PMSQ thin films significantly changed in the range from 1012 to 1014 Ω cm depending on the organic solvent used in the synthesis. The PMSQ synthesized in toluene exhibited a high resistivity of 1.6 × 1014 Ω cm, which were two orders of magnitude higher than that synthesized in methanol. Current density-electric field characteristics shown in Figure 5(a) also revealed the formation of dense siloxane networks in the PMSQ film which were cured at 150°C. The PMSQ film had a very high breakdown field of over 3.0 MV cm−1 and exhibited an extremely low leakage current, which was much lower than that of PVP and polyimide  and more than two orders of magnitude lower than that of previously reported PMSQ films . Furthermore, since mobile ionic impurities in gate-insulating layer seriously suffer the property of O-TFTs, it is important to confirm their existence by means of impedance spectroscopy, that is, measurement of permittivity as a function of frequency in wide range of temperature . As shown in Figure 5(b), the dielectronic constant (k ~ 3.6) did not significantly change for wide frequency sweeps (10 mHz~100 kHz) and wide temperature sweeps (30~150°C), which indicated extremely low concentration of mobile ionic impurities. The reason of the absence of mobile ionic impurities is probably due to the preparation condition of PMSQ. The novel synthetic process introduced here utilizes formic acid as a volatile acid catalyst for the sol-gel reaction, and after the condensation, it was completely removed under reduced pressure with exchanging the solvent by adding PGMEA of higher boiling point.
The PMSQ thin films, which were made by spin-coating and subsequent thermal treatment at 150°C, were not dissolved in common organic solvents such as chloroform, toluene, and xylene, which allows the next coating of soluble organic semiconductors, such as poly(3-hexylthiophene) (P3HT), onto the PMSQ gate-insulating layer. The PMSQ thin films have the pinhole-less smooth surface with average roughness of 0.24 nm, which came out by AFM measurements. Relatively less volatile nature of PGMEA and fluidity of PMSQ before the thermal treatment will be attributable to this surface smoothness of the thin films. Moreover, PMSQ film had a hydrophobic surface exhibiting the water contact angle of 90.7°, and this also satisfies one of the requirements for the gate-insulating layer of O-TFTs.
4. Characteristics of PMSQ as a Gate-Insulating Material
Top-contact P3HT TFTs with gate-insulating layer of PMSQ were fabricated on a glass substrate with an indium-tin-oxide (ITO) gate electrode. The spin-coated PMSQ thin films were cured at 150°C for 1 h in ambient air, which were 450 nm in thickness. A solution of regioregular P3HT in chloroform was spin-coated onto the gate-insulating layer, and the source and drain electrodes were evaporated onto the P3HT layer through a shadow mask, as shown in Figure 6 for TFT structure. Figure 7 shows the output curves and transfer curves of the P3HT TFT with PMSQ gate-insulating layer (where , and stand for drain current, drain voltage, and gate voltage, resp.). In Figure 7(a), all curves display good linear and saturation behaviors with no leakage current at V. Figure 7(b) shows that the device exhibited no hysteresis with respect to a sweep from +20 to −80 V and then from −80 to +20 V, indicating that P3HT TFT with PMSQ gate-insulating layer has stable TFT characteristics significantly. For comparison, P3HT TFT using a highly doped Si substrate with a thermally grown SiO2 gate-insulating layer (365 nm thickness) were also fabricated. The surfaces of the SiO2 gate-insulating layers were modified with the hydrophobic self-assembled monolayers (SAMs) of alkyltrichlorosilanes with different alkyl lengths (CnH2n+1-SiCl3, , 6, 12, and 18). The field-effect mobility (μ) and induced threshold voltage () shift for the sweep of the devices with different gate-insulating layer surfaces are summarized in Table 2. P3HT TFT with PMSQ gate-insulating layer exhibited fair TFT characteristics with μ = 7.1 × 10−3 cm2 V−1 s−1 and V, whereas the device with untreated SiO2 gate-insulating layer exhibited one order magnitude of small mobility and larger negative shift because of hydrophilic surface. The suppression of hysteresis behavior and smaller negative shift of the device with PMSQ gate-insulating layer also indicates that cured PMSQ films may contain a small number of uncross-linked residual silanol groups. The mobility of SAM-modified SiO2 gate-insulating layer showed a close correlation to the water contact angle; that is, a more hydrophobic surface gives a higher mobility. Such behavior has been observed by a number of authors, indicating that mobility enhancement is caused by the improvement in the structural ordering of the P3HT molecules at low-energy surfaces [20–22]. A large contact angle of the PMSQ surfaces would originate from the high density of the methyl groups and the small amount of the residual Si–OH groups, which are responsible for enhanced mobility.
As described above, the spin-coated thin films of PMSQ can be cured at a low temperature of 150°C, which is suitable for a plastic substrate. Thus, fabrications of O-TFTs on flexible plastic substrates were also investigated. Polycarbonate (PC) substrate coated with an indium zinc oxide (IZO) layer was prepatterned by wet etching and used as a gate electrode, a gate-insulating layer of PMSQ was formed by spin-coating and subsequent thermal treatment, followed by spin-coating of P3HT, and source and drain electrodes were thermally deposited . The P3HT TFT fabricated on PC substrate exhibited field-effect mobility of μ = 5.8 × 10−3 cm2 V−1 s−1, which was comparable to those of the devices fabricated on glass substrates. Also, on a polyethylenenaphtalate (PEN) substrate, P3HT TFT with PMSQ gate-insulating layer has been similarly fabricated . As shown in Figure 8, the transfer characteristic curves of P3HT TFT on a glass substrate and that on a PEN substrate were almost equal each other. The field effect mobility and on/off ratio were also comparable with different substrates as summarized in Table 3. These results demonstrate that low-temperature processible PMSQ is extremely useful gate-insulating material for enhancing electrical stability as well as for a fabrication of printable O-TFTs.
5. Functionalization of PMSQ Gate-Insulating Layer
5.1. Control of Surface Hydrophobicity of PMSQ
As mentioned above, SAM modification on utilizing a thermally grown SiO2 layer as a gate-insulating layer is essential step for the higher performance of O-TFT. Similarly, we studied to improve the TFT properties by the SAM modification of PMSQ surface . PMSQ was spin-coated on the glass substrates and heated at 80°C for 2 min. At this stage, PMSQ thin films were not completely cured and the silanol could clearly be observed by IR measurement, but as the cross-linked films were not dissolved in organic solvents, the SAM modification could be performed with the remaining silanol group on the surface of PMSQ thin film. After PMSQ thin film on the substrate were immersed in the 5 wt.% various alkyltrichlorosilanes of hexane/chloroform (3 : 1) solution and then washed with hexane as shown in Figure 9, which is a stepwise modification. In order to complete the modification and curing of PMSQ, the substrate was heated at 150°C for 1 h.
In the case of SAM modification using octadecyltrichlorosilane (OTS), signals of silanol on IR spectra completely disappeared lower than 150°C of thermal treatment, and the film exhibited higher water contact angle of 100°, whereas the nonmodified PMSQ films show lower water contact angle of 89°. To examine the effect of surface modification of PMSQ for O-TFT performance, O-TFTs were fabricated using the nontreated PMSQ and the OTS-treated PMSQ thin films as gate-insulating layers. Figures 10(a) and 10(b) show the output characteristics of P3HT TFTs with the non-treated PMSQ and OTS-treated PMSQ films, respectively. The O-TFT with the OTS-treated PMSQ thin films showed higher mobility and larger on/off ratio compared to that with the nontreated PMSQ films. It will be noteworthy that the mobility of the O-TFT with OTS-treated PMSQ was 4 times larger than that with nontreated PMSQ.
Instead of the SAM modification of PMSQ surface, copolymethylsilsesquoxanes (co-PMSQs), which were prepared from cocondensation of methyltrimethoxysilane and a small amount of alkyltrimethoxysilanes, were used for the direct formation of hydrophobic surface . And co-PMSQ gate-insulating layers were fabricated by a simple spin-coating and subsequent thermal treatment as shown in Figure 11. The relation between the surface free energy of co-PMSQ layer and field effect mobility was investigated. The surface properties of co-PMSQ with several alkyl groups were summarized in Table 4, and it seems that the surface of co-PMSQ thin films were more hydrophobic than that of normal PMSQ, indicating that hydrophobic functional groups migrated and accumulated on the surface. Especially, co-PMSQ derived from tridecafuluoro-1,1,2,2-tetrahydrooctyltrimethoxysilane exhibited very low surface free energy.
Figure 12 shows the relation between the surface free energy and mobility of the O-TFTs fabricated with the co-PMSQ gate-insulating layer. It could be clearly observed that the mobility increased with lower surface free energy. This result follows the same tendency of SAM-modified thermal grown SiO2, and it was concluded that co-PMSQ prepared from cocondensation is an effective gate-insulating materials with a highly hydrophobic surface.
5.2. Improvement of Permittivity of PMSQ
As driving O-TFTs with low operating voltage is an important function for a high performance device, the gate-insulating layer of high permittivity is required. We have also tried to develop polysilsesquioxane having high permittivity. Some modified PMSQs were synthesized by cocondensation of several alkyltrialkoxysilanes and methyltrimethoxysilane. It revealed that the introduction of polar functional groups, such as epoxy and cyano, leads to the co-PMSQs with high permittivity. Co-PMSQ containing epoxy group (PMSQ-epoxy) showed very high permittivity, although TFT properties with PMSQ-epoxy gate-insulating layer was not superior, because hydroxyl groups generated by ring-opening of epoxy groups affected the charge trapping. On the other hand, co-PMSQ containing cyano group (PMSQ-CN), which is a product from cocondensation with cyanoethyltrimethoxysilane, improved permittivity with the increase of cyano group as shown in Figure 13 . When the feed ratio of cyano group was 1 : 1, the permittivity was 3 times larger than that of PMSQ without cyano group. Although PMSQ-CN had slightly less hydrophobic surface than that of normal PMSQ, field-effect mobility using two gate-insulating layer did not differ much. The field-effect mobility (μ) of O-TFTs with PMSQ and PMSQ-CN are 3.7 × 10−3 cm2 V−1 s−1 and 2.8 × 10−3 cm2 V−1 s−1, respectively. As clearly shown in Figure 13, of the P3HT TFT with gate-insulating layer of PMSQ-CN was ca. 4 times larger than that of PMSQ without cyano groups at V. This result suggested that required to obtain a certain could be lowered by using PMSQ-CN gate-insulating layer, and thus, PMSQ-CN revealed to be a promising gate-insulating material for the high-performance O-TFT of low-operating voltage.
5.3. Photocurable PMSQ
A photolithography is indispensable process for the fabrication of electric devices using photoresists and UV irradiation. Introduction of photocurability to PMSQ is seemed to become applicable not only for O-TFT, but also various electronic devices. Therefore, the photocurable PMSQ was investigated by introducing photofunctional acrylic groups . As shown in Figure 14, a sol-gel cocondensation of methyltrimethoxysilane and acryloxypropyltrimethoxysilane was carried out under the same condition that have already described above. The spin-coated film of thus obtained copolysilsesquioxane (PMSQ-acryl) with Darocure 1173 as a photoradical initiator was exposed to UV light through a photo mask, then the 250 μm line and space negative-patterns were obtained by the development with 2-propanol. As shown in the inset table in Figure 14, the increasing acrylic groups in PMSQ lead to slightly decrease of electric resistivity. However, these values of resistivity are sufficient for gate-insulating materials of O-TFT. Also, it was found that the thin film from PMSQ-acryl exhibited no permittivity change even in higher temperature by the impedance spectroscopy, which was indicating no existence of ionic impurities. The properties of O-TFT with PMSQ-acryl as a gate-insulating layer were comparable to that with normal PMSQ. These results have suggested that the photo-curable PMSQ is not only useful material as a gate-insulating layer of O-TFT but also promising insulating material for other electronic devices.
The term of “printed electronics” refers to electronic devices fabricated by solution processes, which are less energy consumption and cost comparing to vacuum processes. For the sake of achieving printed electronics, there should be close connection between three research steps of material development, process design, and device characterization. We have developed PMSQ derivatives for gate-insulating layer of O-TFT based on three research steps. Possessing the property of both organic and inorganic materials, one of the typical organic-inorganic hybrid materials, polysilsesquioxane, has been revealed to be an important field of materials for printed electronics. The careful investigation of the preparation condition of PMSQs has enabled the development of material suitable for gate-insulating layer of O-TFTs. Recently, we have fabricated flexible O-TFT utilizing PMSQ described above, and succeeded to drive an electric-paper device. The property adjustability of PMSQ, that is, resistivity, surface hydrophobicity, permittivity, and photo-curability, suggests further possibility of applications. We are certainly expecting the polysilsesquioxane derivatives to be one of key materials for new electronic devices.
- H. Sirringhaus, P. J. Brown, R. H. Friend et al., “Two-dimensional charge transport in self-organized, high-mobility conjugated polymers,” Nature, vol. 401, no. 6754, pp. 685–688, 1999.
- A. Afzali, C. D. Dimitrakopoulos, and T. L. Breen, “High-performance, solution-processed organic thin film transistors from a novel pentacene precursor,” Journal of the American Chemical Society, vol. 124, no. 30, pp. 8812–8813, 2002.
- T. Kawase, H. Sirringhaus, R. H. Friend, and T. Shimoda, “Inkjet printed via-hole interconnections and resistors for all-polymer transistor circuits,” Advanced Materials, vol. 13, no. 21, pp. 1601–1605, 2001.
- H. Klauk, M. Halik, U. Zschieschang, G. Schmid, W. Radlik, and W. Weber, “High-mobility polymer gate dielectric pentacene thin film transistors,” Journal of Applied Physics, vol. 92, no. 9, p. 5259, 2002.
- J. A. Rogers, Z. Bao, A. Makhija, and P. Braun, “Printing process suitable for reel-to-reel production of high-performance organic transistors and circuits,” Advanced Materials, vol. 11, no. 9, pp. 741–745, 1999.
- C. D. Sheraw, D. J. Gundlach, and T. N. Jockson, “Spin-on polymer gate dielectric for high performance organic thin film transistors,” Materials Research Society Symposium Proceedings, vol. 558, article 403, 2000.
- T. B. Singh, F. Meghdadi, S. Günes et al., “High-performance ambipolar pentacene organic field-effect transistors on poly(vinyl alcohol) organic gate dielectric,” Advanced Materials, vol. 17, no. 19, pp. 2315–2320, 2005.
- D. Knipp, R. A. Street, A. Vokel, and J. Ho, “Pentacene thin film transistors on inorganic dielectrics: morphology, structural properties, and electronic transport,” Journal of Applied Physics, vol. 93, no. 1, article 347, 9 pages, 2003.
- J. Wang, X. Yan, Y. Xu, J. Zhang, and D. Yan, “Organic thin-film transistors having inorganic/organic double gate insulators,” Applied Physics Letters, vol. 85, no. 22, article 5424, 3 pages, 2004.
- A. Facchetti, M. H. Yoon, and T. J. Marks, “Gate dielectrics for organic field-effect transistors: new opportunities for organic electronics,” Advanced Materials, vol. 17, no. 14, pp. 1705–1725, 2005.
- Z. Bao, V. Kuck, J. A. Rogers, and M. A. Paczkowski, “Silsesquioxane resins as high-performance solution processible dielectric materials for organic transistor applications,” Advanced Functional Materials, vol. 12, no. 8, pp. 526–531, 2002.
- P. Liu, Y. Wu, Y. Li, B. S. Ong, and S. Zhu, “Enabling gate dielectric design for all solution-processed, high-performance, flexible organic thin-film transistors,” Journal of the American Chemical Society, vol. 128, no. 14, pp. 4554–4555, 2006.
- Y. Wu, P. Lin, and B. S. Ong, “Organic thin-film transistors with poly(methyl silsesquioxane) modified dielectric interfaces,” Applied Physics Letters, vol. 89, no. 1, Article ID 013505, 2006.
- S. Jeong, D. Kim, S. Lee, B. K. Park, and J. Moon, Applied PhysicsLetters, vol. 89, Article ID 092101, 2006.
- S. Jeong, D. Kim, S. Lee, B. K. Park, and J. Moon, “Influence of silanol groups on the electrical performance of organic thin-film transistors utilizing organosiloxane-based organic-inorganic hybrid dielectrics,” Nanotechnology, vol. 18, no. 2, Article ID 025204, 2007.
- K. Tomatsu, T. Hamada, T. Nagase et al., “Fabrication and characterization of poly(3-hexylthiophene)-based field-effect transistors with silsesquioxane gate insulators,” Japanese Journal of Applied Physics, vol. 47, no. 4, pp. 3196–3199, 2008.
- T. Nagase, T. Hamada, K. Tomatsu et al., “Low-temperature processable organic-inorganic hybrid gate dielectrics for solution-based organic field-effect transistors,” Advanced Materials, vol. 22, no. 42, pp. 4706–4710, 2010.
- S. Y. Yang, S. H. Kim, K. Shin, H. Jeon, and C. E. Park, “Low-voltage pentacene field-effect transistors with ultrathin polymer gate dielectrics,” Applied Physics Letters, vol. 88, no. 17, Article ID 173507, 3 pages, 2006.
- S. Uemura, “Low-frequency dielectric behavior of poly(vinylidene fluoride),” Journal of Polymer Science, vol. 12, no. 6, pp. 1177–1188, 1974.
- J. Veres, S. Ogier, G. Lloyd, and D. de Leeuw, “Gate insulators in organic field-effect transistors,” Chemistry of Materials, vol. 16, no. 23, pp. 4543–4555, 2004.
- A. Salleo, M. L. Chabinyc, M. S. Yang, and R. A. Street, “Polymer thin-film transistors with chemically modified dielectric interfaces,” Applied Physics Letters, vol. 81, no. 23, pp. 4383–4385, 2002.
- K. P. Pernstich, S. Haas, D. Oberhoff et al., “Threshold voltage shift in organic field effect transistors by dipole monolayers on the gate insulator,” Journal of Applied Physics, vol. 96, no. 11, pp. 6431–6438, 2004.
- S. Yamazaki, T. Hamada, K. Tomatsu et al., “Electrical characteristics of polymer field-effect transistors with poly(methylsilsesquioxane) gate dielectrics on plastic substrates,” Thin Solid Films, vol. 517, no. 4, pp. 1343–1345, 2008.
- T. Hamada, S. Yamazaki, T. Nagase et al., “Chemical design of polysilsesquioxane as a gate insulator for organic thin-film transistors,” in Proceedings of the 15th International Display Workshops (IDW '08), pp. 1665–1668, December 2008.
- T. Hamada, T. Nagase, T. Kobayashi, K. Matsukawa, and H. Naito, “Effective control of surface property on poly(silsesquioxane) films by chemical modification,” Thin Solid Films, vol. 517, no. 4, pp. 1335–1339, 2008.
- M. Watanabe, K. Muro, T. Hamada et al., “Surface modification of organic-inorganic hybrid insulator for printable organic field-effect transistors,” Chemistry Letters, vol. 38, no. 1, pp. 34–35, 2009.
- T. Hamada, T. Nagase, M. Watanabe, S. Watase, H. Naito, and K. Matsukawa, “Preparation and dielectric property of photo-curable polysilsesquioxane hybrids,” Journal of Photopolymer Science and Technology, vol. 21, no. 2, pp. 319–320, 2008.