|
[1] https://mic.iii.org.tw/IndustryObservations-PressRelease02.aspxsqno=491. [2] http:// www.indusoft.com/ blog/ 2016/01/29/ history-of-automation-thetriode- vacuum-tube-the-evolution-into-automation-industrial-and-machinecontrol/. [3] https://www.computerhope.com/issues/ch000984.htm. [4] http://www.cedmagic.com/history/transistor-1947.html. [5] https://en.wikipedia.org/wiki/Integrated-circuit. [6] https:// www.bit-tech.net/ others/ tech/ intel-claims-moore-s-law-isn-t-deadbut-ali/1/. [7] https://www.cnet.com/news/moores-law-to-roll-on-for-another-decade/. [8] http:// semiconductordevice.net/ SemiconductorEquipment/ semiconductorroadmap. [9] K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, Y. Zhang, S. V. Dubonos, I. V. Grigorieva, and A. A. Firsov, “Electric field effect in atomically thin carbon films,” Science, vol. 306, p. 666, Oct. 2004. [10] G. Fiori, F. Bonaccorso, G. Iannaccone, T. Palacios, D. Neumaier,A. Seabaugh, S. K. Banerjee, and L. Colombo, “Electronics based on twodimensional materials,” Nature Nanotechnology, vol. 9, p. 768, Oct. 2014. [11] F. Zhang and J. Appenzeller, “Tunability of short-channel effects in MoS2 field-effect devices,” Nano Lett., vol. 15, pp. 301–306, Jan. 2015. [12] K. Xu, D. Chen, F. Yang, Z. Wang, L. Yin, F. Wang, R. Cheng, K. Liu, J. Xiong, Q. Liu, and J. He, “Sub-10 nm nanopattern architecture for 2D material field-effect transistors,” Nano Lett., vol. 17, pp. 1065–1070, Feb. 2017. [13] A. D. Franklin, M. Luisier, S.-J. Han, G. Tulevski, C. M. Breslin, L. Gignac, M. S. Lundstrom, and W. Haensch, “Sub-10 nm carbon nanotube transistor,”Nano Lett., vol. 12, pp. 758–762, Feb. 2012. [14] A. D. Franklin and Z. Chen, “Length scaling of carbon nanotube transistors,” Nature Nanotechnology, vol. 5, p. 858, Nov. 2010. [15] V. Vitale, A. Curioni, and W. Andreoni, “Metal−carbon nanotube contacts:The link between schottky barrier and chemical bonding,” J. Am. Chem. Soc.,vol. 130, pp. 5848–5849, May 2008. [16] Q. Cao, S.-J. Han, J. Tersoff, A. D. Franklin, Y. Zhu, Z. Zhang, G. S. Tulevski,J. Tang, and W. Haensch, “End-bonded contacts for carbon nanotube transistors with low, size-independent resistance,” Science, vol. 350, p. 68, Oct.2015. [17] J. Tang, Q. Cao, D. B. Farmer, G. Tulevski, and S. J. Han, “High-performance carbon nanotube complementary logic with end-bonded contacts,” IEEE Transactions on Electron Devices, vol. 64, no. 6, pp. 2744–2750, June. [18] H. Liu, M. Si, Y. Deng, A. T. Neal, Y. Du, S. Najmaei, P. M. Ajayan, J. Lou, and P. D. Ye, “Switching mechanism in single-layer molybdenum disulfide transistors: An insight into current flow across schottky barriers,” ACS Nano,vol. 8, pp. 1031–1038, Jan. 2014. [19] C. D. English, G. Shine, V. E. Dorgan, K. C. Saraswat, and E. Pop, “Improved contacts to MoS2 transistors by ultra-high vacuum metal deposition,” Nano Lett., vol. 16, pp. 3824–3830, June 2016. [20] Y. Xu, C. Cheng, S. Du, J. Yang, B. Yu, J. Luo, W. Yin, E. Li, S. Dong, P. Ye, and X. Duan, “Contacts between two- and three-dimensional materials: Ohmic, schottky, and p-n heterojunctions,” ACS Nano, vol. 10, pp. 4895–4919, May 2016. [21] L. Wang, I. Meric, P. Y. Huang, Q. Gao, Y. Gao, H. Tran, T. Taniguchi, K. Watanabe, L. M. Campos, D. A. Muller, J. Guo, P. Kim, J. Hone, K. L. Shepard, and C. R. Dean, “One-dimensional electrical contact to a twodimensional material,” Science, vol. 342, p. 614, Nov. 2013. [22] M. Chhowalla, H. S. Shin, G. Eda, L.-J. Li, K. P. Loh, and H. Zhang,“The chemistry of two-dimensional layered transition metal dichalcogenide nanosheets,” Nature Chemistry, vol. 5, p. 263, Mar. 2013. [23] R. Kappera, D. Voiry, S. E. Yalcin, B. Branch, G. Gupta, A. D. Mohite, and M. Chhowalla, “Phase-engineered low-resistance contacts for ultrathin MoS2 transistors,” Nature Materials, vol. 13, p. 1128, Aug. 2014. [24] Y. Ma, B. Liu, A. Zhang, L. Chen, M. Fathi, C. Shen, A. N. Abbas, M. Ge, M. Mecklenburg, and C. Zhou, “Reversible semiconducting-to-metallic phase transition in chemical vapor deposition grown monolayer WSe2 and applications for devices,” ACS Nano, vol. 9, pp. 7383–7391, July 2015. [25] Q. H. Wang, K. Kalantar-Zadeh, A. Kis, J. N. Coleman, and M. S. Strano, “Electronics and optoelectronics of two-dimensional transition metal dichalcogenides,” Nature Nanotechnology, vol. 7, p. 699, Nov. 2012. [26] H. Yuan, H. Wang, and Y. Cui, “Two-dimensional layered chalcogenides: From rational synthesis to property control via orbital occupation and electron filling,” Acc. Chem. Res., vol. 48, pp. 81–90, Jan. 2015. [27] W. S. Yun, S. W. Han, S. C. Hong, I. G. Kim, and J. D. Lee, “Thickness and strain effects on electronic structures of transition metal dichalcogenides: 2HMX2 semiconductors (M = Mo, W; X = S, Se, Te),” PRB, vol. 85, p. 033305,Jan. 2012. [28] M. Ahmad, E. Müller, C. Habenicht, R. Schuster, M. Knupfer, and B. Büchner,“Semiconductor-to-metal transition in the bulk of WSe2 upon potassium intercalation,” Journal of Physics: Condensed Matter, vol. 29, no. 16,p. 165502, 2017. [29] A. Kuc, N. Zibouche, and T. Heine, “Influence of quantum confinement on the electronic structure of the transition metal sulfide TS2,” PRB, vol. 83, p. 245213, June 2011. [30] K. S. Novoselov, D. Jiang, F. Schedin, T. J. Booth, V. V. Khotkevich, S. V. Morozov, and A. K. Geim, “Two-dimensional atomic crystals,” Proc Natl Acad Sci U S A, vol. 102, p. 10451, July 2005. [31] P. B. G. James D. Plummer, Michael D. Deal, Silicon VLSI Technology. 2000. [32] J.-K. Huang, J. Pu, C.-L. Hsu, M.-H. Chiu, Z.-Y. Juang, Y.-H. Chang, W.-H. Chang, Y. Iwasa, T. Takenobu, and L.-J. Li, “Large-area synthesis of highly crystalline WSe2 monolayers and device applications,” ACS Nano, vol. 8,pp. 923–930, Jan. 2014. [33] Y. Feng, K. Zhang, F. Wang, Z. Liu, M. Fang, R. Cao, Y. Miao, Z. Yang, W. Mi, Y. Han, Z. Song, and H. S. P. Wong, “Synthesis of large-area highly crystalline monolayer molybdenum disulfide with tunable grain size in a H2 atmosphere,” ACS Appl. Mater. Interfaces, vol. 7, pp. 22587–22593, Oct. 2015. [34] Y.-C. Lin, W. Zhang, J.-K. Huang, K.-K. Liu, Y.-H. Lee, C.-T. Liang, C.-W. Chu, and L.-J. Li, “Wafer-scale MoS2 thin layers prepared by MoO3 sulfurization,” Nanoscale, vol. 4, no. 20, pp. 6637–6641, 2012. [35] Y.-H. Lee, X.-Q. Zhang, W. Zhang, M.-T. Chang, C.-T. Lin, K.-D. Chang, Y.-C. Yu, J. T.-W. Wang, C.-S. Chang, L.-J. Li, and T.-W. Lin, “Synthesis of large-area MoS2 atomic layers with chemical vapor deposition,” Adv. Mater., vol. 24, pp. 2320–2325, Aug. 2012. [36] L. Yu, D. El-Damak, U. Radhakrishna, X. Ling, A. Zubair, Y. Lin, Y. Zhang, M.-H. Chuang, Y.-H. Lee, D. Antoniadis, J. Kong, A. Chandrakasan, and T. Palacios, “Design, modeling, and fabrication of chemical vapor deposition grown MoS2 circuits with e-mode FETs for large-area electronics,” Nano Lett., vol. 16, pp. 6349–6356, Oct. 2016. [37] K. K. H. Smithe, C. D. English, S. V. Suryavanshi, and E. Pop, “Intrinsic electrical transport and performance projections of synthetic monolayer MoS2 devices,” 2D Materials, vol. 4, no. 1, p. 011009, 2017. [38] K.-K. Liu, W. Zhang, Y.-H. Lee, Y.-C. Lin, M.-T. Chang, C.-Y. Su, C.-S. Chang, H. Li, Y. Shi, H. Zhang, C.-S. Lai, and L.-J. Li, “Growth of large-area and highly crystalline MoS2 thin layers on insulating substrates,” Nano Lett., vol. 12, pp. 1538–1544, Mar. 2012. [39] X. Luo, Y. Zhao, J. Zhang, M. Toh, C. Kloc, Q. Xiong, and S. Y. Quek, “Effects of lower symmetry and dimensionality on raman spectra in twodimensional WSe2,” PRB, vol. 88, p. 195313, Nov. 2013. [40] W. Zhao, Z. Ghorannevis, K. K. Amara, J. R. Pang, M. Toh, X. Zhang, C. Kloc, P. H. Tan, and G. Eda, “Lattice dynamics in mono- and few-layer sheets of WS2 and WSe2,” Nanoscale, vol. 5, no. 20, pp. 9677–9683, 2013. [41] C. A. Mead and W. G. Spitzer, “Fermi level position at metal-semiconductor interfaces,” PR, vol. 134, pp. A713–A716, May 1964. [42] J. Tersoff, “Schottky barrier heights and the continuum of gap states,” PRL, vol. 52, pp. 465–468, Feb. 1984. [43] H. Hasegawa and T. Sawada, “On the electrical properties of compound semiconductor interfaces in metal/insulator/ semiconductor structures and the possible origin of interface states,” Thin Solid Films, vol. 103, pp. 119–140, Jan. 1983. [44] 施敏、伍國, 半導體元件物理學. 國立交通大學出版社, 2008. [45] J. M. Larson and J. P. Snyder, “Overview and status of metal S/D schottkybarrier MOSFET technology,” IEEE Transactions on Electron Devices, vol. 53, no. 5, pp. 1048–1058, May. [46] R. Islam, G. Shine, and K. C. Saraswat, “Schottky barrier height reduction for holes by fermi level depinning using metal/nickel oxide/silicon contacts,” Appl. Phys. Lett., vol. 105, p. 182103, Aug. 2014. [47] A. Agrawal, J. Lin, M. Barth, R. White, B. Zheng, S. Chopra, S. Gupta, K. Wang, J. Gelatos, S. E. Mohney, and S. Datta, “Fermi level depinning and contact resistivity reduction using a reduced titania interlayer in n-silicon metal-insulator-semiconductor ohmic contacts,” Appl. Phys. Lett., vol. 104, p. 112101, Aug. 2018. [48] C. Kim, I. Moon, D. Lee, M. S. Choi, F. Ahmed, S. Nam, Y. Cho, H.-J. Shin, S. Park, and W. J. Yoo, “Fermi level pinning at electrical metal contacts of monolayer molybdenum dichalcogenides,” ACS Nano, vol. 11, pp. 1588– 1596, Feb. 2017. [49] C. Gong, L. Colombo, R. M. Wallace, and K. Cho, “The unusual mechanism of partial fermi level pinning at metal-MoS2 interfaces,” Nano Lett., vol. 14, pp. 1714–1720, Apr. 2014. [50] Y. Wang, R. X. Yang, R. Quhe, H. Zhong, L. Cong, M. Ye, Z. Ni, Z. Song, J. Yang, J. Shi, J. Li, and J. Lu, “Does p-type ohmic contact exist in WSe2-metal interfaces?,” Nanoscale, vol. 8, no. 2, pp. 1179–1191, 2016. [51] P. Bampoulis, R. van Bremen, Q. Yao, B. Poelsema, H. J. W. Zandvliet, and K. Sotthewes, “Defect dominated charge transport and fermi level pinning in MoS2/metal contacts,” ACS Appl. Mater. Interfaces, vol. 9, pp. 19278–19286, June 2017. [52] W. M. Parkin, A. Balan, L. Liang, P. M. Das, M. Lamparski, C. H. Naylor, J. A. Rodríguez-Manzo, A. T. C. Johnson, V. Meunier, and M. Drndić, “Raman shifts in electron-irradiated monolayer MoS2,” ACS Nano, vol. 10, pp. 4134– 4142, Apr. 2016. [53] Y. Liu, J. Guo, E. Zhu, L. Liao, S.-J. Lee, M. Ding, I. Shakir, V. Gambin, Y. Huang, and X. Duan, “Approaching the schottky-mott limit in van der waals metal-semiconductor junctions,” Nature, vol. 557, pp. 696–700, May 2018. [54] J. Kang, W. Liu, D. Sarkar, D. Jena, and K. Banerjee, “Computational study of metal contacts to monolayer transition-metal dichalcogenide semiconductors,” PRX, vol. 4, p. 031005, July 2014. [55] H. Fang, S. Chuang, T. C. Chang, K. Takei, T. Takahashi, and A. Javey, “Highperformance single layered WSe2 p-FETs with chemically doped contacts,” Nano Lett., vol. 12, pp. 3788–3792, July 2012. [56] L. Yu, A. Zubair, E. J. G. Santos, X. Zhang, Y. Lin, Y. Zhang, and T. Palacios, “High-performance WSe2 complementary metal oxide semiconductor technology and integrated circuits,” Nano Lett., vol. 15, pp. 4928–4934, Aug. 2015. [57] Y. Liu, H. Wu, H.-C. Cheng, S. Yang, E. Zhu, Q. He, M. Ding, D. Li, J. Guo, N. O. Weiss, Y. Huang, and X. Duan, “Toward barrier free contact to molybdenum disulfide using graphene electrodes,” Nano Lett., vol. 15, pp. 3030–3034, May 2015. [58] H.-J. Chuang, B. Chamlagain, M. Koehler, M. M. Perera, J. Yan, D. Mandrus, D. Tománek, and Z. Zhou, “Low-resistance 2D/2D ohmic contacts: A universal approach to high-performance WSe2, MoS2, and MoSe2 transistors,” Nano Lett., vol. 16, pp. 1896–1902, Mar. 2016. [59] T. Chu and Z. Chen, “Understanding the electrical impact of edge contacts in few-layer graphene,” ACS Nano, vol. 8, pp. 3584–3589, Apr. 2014. [60] B. H. Moon, G. H. Han, H. Kim, H. Choi, J. J. Bae, J. Kim, Y. Jin, H. Y. Jeong, M.-K. Joo, Y. H. Lee, and S. C. Lim, “Junction-structure-dependent schottky barrier inhomogeneity and device ideality of monolayer MoS2 fieldeffect transistors,” ACS Appl. Mater. Interfaces, vol. 9, pp. 11240–11246, Mar. 2017. [61] H.-L. Tang, M.-H. Chiu, C.-C. Tseng, S.-H. Yang, K.-J. Hou, S.-Y. Wei, J.- K. Huang, Y.-F. Lin, C.-H. Lien, and L.-J. Li, “Multilayer graphene-WSe2 heterostructures for WSe2 transistors,” ACS Nano, vol. 11, pp. 12817–12823, Dec. 2017. [62] M. H. D. Guimarães, H. Gao, Y. Han, K. Kang, S. Xie, C.-J. Kim, D. A. Muller, D. C. Ralph, and J. Park, “Atomically thin ohmic edge contacts between two-dimensional materials,” ACS Nano, vol. 10, pp. 6392–6399, June 2016. [63] H. Okamoto, “The Pd-Se (palladium-selenium) system,” Journal of Phase Equilibria, vol. 13, pp. 69–72, Feb. 1992. [64] T. Fujimoto and K. Awaga, “Electric-double-layer field-effect transistors with ionic liquids,” Phys. Chem. Chem. Phys., vol. 15, no. 23, pp. 8983–9006, 2013. [65] P. Zhao, D. Kiriya, A. Azcatl, C. Zhang, M. Tosun, Y.-S. Liu, M. Hettick, J. S. Kang, S. McDonnell, K. C. Santosh, J. Guo, K. Cho, R. M. Wallace, and A. Javey, “Air stable p-doping of WSe2 by covalent functionalization,” ACS Nano, vol. 8, pp. 10808–10814, Oct. 2014. [66] M. Tosun, S. Chuang, H. Fang, A. B. Sachid, M. Hettick, Y. Lin, Y. Zeng, and A. Javey, “High-gain inverters based on WSe2 complementary field-effect transistors,” ACS Nano, vol. 8, pp. 4948–4953, May 2014. [67] A. Dathbun, Y. Kim, S. Kim, Y. Yoo, M. S. Kang, C. Lee, and J. H. Cho, “Large-area CVD-grown sub-2 v ReS2 transistors and logic gates,” Nano Lett., vol. 17, pp. 2999–3005, May 2017. [68] P. J. Jeon, J. S. Kim, J. Y. Lim, Y. Cho, A. Pezeshki, H. S. Lee, S. Yu, S.-W. Min, and S. Im, “Low power consumption complementary inverters with n-MoS2 and p-WSe2 dichalcogenide nanosheets on glass for logic and light-emitting diode circuits,” ACS Appl. Mater. Interfaces, vol. 7, pp. 22333– 22340, Oct. 2015.
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