• 沒有找到結果。

In this work, channel material quality and the device structure are not optimized,

and the leakage current is rather high. It has been found that polycrystalline

silicon-germanium film has much more defects than polycrystalline silicon film. To

further improve the device performance, it is important to reduce the defects and

trap-states in silicon-germanium film for the nanowire TFTs. It could be achieved by

using laser annealing, MILC, SPE or other new technologies replacing the SPC step

to enlarge the grain size of the silicon-germanium film, or we can use other plasma

treatment technology to aid NH3 plasma treatment.

Although double-gated nanowire TFTs have been demonstrated to show better

device performance, further improvement in the electrical performance is possible by

adding a back-gate to form a tri-gated nanowire TFTs, or by modifying the structure

to form a surrounding-gate nanowire TFTs. As long as decent performance is achieved,

the new nanowire device can be readily applied to a variety of novel applications in

the future.

References

[1] C. H. Fa and T. T. Jew, “The poly-silicon insulated-gate field-effect transistor,”

IEEE Trans. Electron Devices, vol. 13, no. 2, p. 290, 1966.

[2] S. Morozumi, K. Oguchi, SYazawa, T. Kodaira, H. Ohshima, and T. Mano,

“B/W and color LC video display addressed by poly-Si TFTs,” SID Dig., p. 156,

1983.

[3] R. E. Proano, R. S. Misage, D. Jones, and D. G. Ast, “Guest-Host active matrix

liquid-crystal display using high-voltage polysilicon thin-film transistors,” IEEE

Trans. Electron Devices, vol. 38, p. 1781, 1991.

[4] Y. Hayashi, M. Negishi, T. Matsushita, “A thermal printer head with CMOS

thin-film transistors and heating elements integrated on a chip,” IEEE Int.

Solid-State Circuits Conference, p. 266, 1988.

[5] T. Kaneko, Y. Hosokawa, M. Tadauchi, Y. Kita, and H. Andoh, “400 dpi

integrated contact type linear image with poly-Si TFT’s analog readout circuits

and dynamic shift registers,” IEEE Trans. Electron Devices, vol. 38, no. 5, pp.

1086-1093, 1991.

[6] I. Fujieda, F. Okumura, K. Srea, H. Asada and H. Sekine, “Self-reference poly-Si

TFT amplifier readout for a linear image sensor,” in IEDM Tech. Dig., p.

587,1993.

[7] M. G. Clark, “Current status and feature prospects of poly-Si,” IEE Proc.

Circuits Devices Syst., vol. 141, no. 1, p. 3, 1994.

[8] N. Yamauchi, Y. Ihada, and M. Okamura, “An integrated

photodetector-amplifier using α-Si p-i-n photodiodes and poly-Si thin-film

transistors,” IEEE Photonic Tech. Lett., vol. 5, p. 319, 1993.

[9] S. D. S. Mahli, H. Shichijo, S. K. Banerjee. R. Sundaresan, M.Elahy, G.

P.Pillack, W. F. Richardson, A. H. Shah, L. R. Hite, R. H. Womack, P. K.

Chatterjee, and H. W. Lam, “Characteristics and three-dimensional integration of

MOSFET’s in small-grain LPCVD polycrystalline silicon,” IEEE Trans.

Electron Devices, vol. 32, p. 258, 1985.

[10] S. Batra, “Development of drain-offset {DO} TFT technology for high density

SRAM’s,” Extended Abstracts, vol. 94-2, in Electrochmeical Soc. Fall Mtg.,

Miami Beach, FL, Oct. p. 677, 1994.

[11] T. Yamanaka, T. Hashimoto, N. Hasegawa, T. Tanaka, N. Hashimoto, A.

Shimizu, N. Ohki, K. Ishibashi, K. Sasaki, T. Nishida, T. Mine, E. Takeda, and T.

Nagano, “Advanced TFT SRAM cell technology using a phase-shift

lithography,” IEEE Trans. Electron Devices, vol. 4, no. 7, pp. 1305-1313, 1995.

[12] K. Yoshizaki, H. Takahashi, Y. Kamigaki, T. Yasui. K. Komori, and H. Katto,

ISSCC Digest of Tech. Papers, p. 166, February 1985.

[13] M. Cao, et ad., “A simple EEPROM cell using twin polysilicon thin-film

transistors,” IEEE Photonic Tech. Lett., vol. 15, p. 304, 1994.

[14] N. D. Young, G. Harkin, R. M. Bunn, D. J. McCulloch, and I. D. French, “The

fabrication and characterization of EEPROMarrays on glass using a low

temperature poly-Si TFT process,” IEEE Trans. Electron Devices, vol. 43, no. 11,

pp. 1930-1936, 1995.

[15] S. D. Brotherton, N. D. Young, M. J. Edwards, A. Gill, M. J. Trainor, J. R. Ayres,

I. R. Clarence, R. M. Bunn, and J. P. Gowers, “Low temperature furnace

processed poly-Si TFT AMLCDs,” in IDRC Digest, Santa Ana, CA: SID, pp.

130-133, 1994.

[16] I. W. Wu, “Low temperature poly-Si TFT technology for AMLCD application,”

Tech. Dig. Active Matrix Liquid Crystal Display, p. 7, 1995.

[17] T. Serikawa, S. Shirai, A. Okamoto, and S. Suyama, “Low temperature

fabrication of high mobility poly- Si TFT’s for large-area LCD’s,” IEEE Trans.

Electron Devices, vol. 36, p. 1929, 1989.

[18] R. B. Iverson, and R. Reif, “Recrystallization of amorphized polycrystalline

silicon films on SiO2: temperature dependence of the crystallization parameters,”

J. Appl. Phys., vol. 62, no. 5, pp. 1675-1681, 1987.

[19] F. Emoto, K. Senda, E. Fujii, A. Nakamura, A. Yamamoto, Y. Yamamoto, Y.

Uemoto and Gota Kano, “Solid phase growth technique for high cut-off

frequency polysilicon TFT integrated circuits on a quartz substrate,” IEEE Trans.

Electron Devices, vol. 37, p. 1462, 1990.

[20] T. Sameshima, S. Usui and M. Sekiya, “XeCl excimer laser annealing used in the

fabrication of poly-Si TFT’s” IEEE Trans. Electron Device Lett., vol. 7, no. 5, pp.

276-278, 1986.

[21] D. H. Choi, E Sadayuki, O. Sugiura and M. Matsumra, “Excimer-laser

crystallized poly-Si TFT’s with mobility of more than 600 cm2/V.s,” IEEE Trans.

Electron Devices, vol. 41, no. 11, p. 2129, 1993.

[22] Z. Jin, Kwok, H. S., Man Wong, “Performance of thin-film transistors with

ultrathin Ni-MILC polycrystalline silicon channel layers,” IEEE Trans. Electron

Device Lett., vol. 20, no. 4, pp. 167-169, 1999.

[23] B. Mohadjeri, J. Linnros, B. G. Svensson, and M. Ostling, “Nickel-enhanced

solid-phase epitaxial regrowth of amorphous silicon,” Phys. Rev. Lett., vol. 68,

pp. 1872-1875, 1992.

[24] R. Kakkad, J. Smith, W. S. Lau, and S. J. Fonash, “Crystallized Si films by

low-temperature rapid thermal annealing of amorphous silicon,” J. Appl. Phys.,

vol. 65, no. 5, pp. 2069-2072, 1989.

[25] M. Bonnel, N. Duhamel, T. henrion, B. Loisel, and L. Haji, “Furance and rapid

thermal annealing for polysilicon thin film transistors-influence of channel film

thickness,” J. Electrochem. Soc., vol. 140, pp. 3584-3587, 1993.

[26] S. Batra, K. Park, S. Banerjee, D. Kwong, A. Tasch, M. Rodder and R.

Sundaresan, “Rapid thermal hydrogen passivation of polysilicon MOSFETs,”

IEEE Trans. Electron Device Lett., vol.11, no. 5, p. 194, 1990.

[27] K. Ono, T. Anoyama, N. Konishi, and K. Miyata, “Analysis of current–voltage

characteristics of low-temperature-processed polysilicon thin-film transistors,”

IEEE Trans. Electron Devices, vol. 39, pp. 792–802, 1992.

[28] B. A. Khan and R. Pandya, “Activation-energy of source-drain current in

hydrogenated and unhydrogenated polysilicon thin-films transistors,” IEEE

Trans. Electron Devices, vol. 37, pp. 1727–1734, 1990.

[29] M. J. Tsai, F. S. Wang, K. L. Cheng, S. Y. Wang, M. S. Feng, and H. C. Cheng,

“Characterization of H2/N2 plasma passivation process for poly-Si thin-film

transistors (TFT’s),” Solid State Electron., vol. 38, pp. 1233–1238, 1995.

[30] C. K. Yang, T. F. Lei, and C. L. Lee, “Improved electrical characteristics of

thin-film transistors fabricated on nitrogen-implanted polysilicon films,” in

IEDM Tech. Dig., 1994, pp. 505-508.

[31] H. C. Cheng, F. S. Wang, and C. Y. Huang, “Effects of NH3 plasma passivation on

N-channel polycrystalline silicon thin-film transistors,” IEEE Trans. Electron

Devices, vol. 44, no. 1, pp. 64-68, 1997.

[32] T. J. King and K. C. Saraswat, “A low-temperature ( ≦ 550℃)

silicon-germanium thin-film transistor technology for large-area electronics,” in

Int. Electron Devices Meet., Techn. Dig., pp. 567-570. 1991.

[33] T. J. King. J. R. Pfiester, and K. C. Saraswat, “A variable-workfunction

polycrystalline Sil-xGex, gate material for submicrometer CMOS technologies,”

IEEE Electron Device Left., vol. 12. pp. 533-535, Oct. 1991.

[34] T. J. King and K. C. Saraswat, “Polycrystalline silicon-germanium thin-film

Transistors,” IEEE Trans. Electron Devices, vol. 41, no. 9, pp. 1581-1591, 1994.

[35] M. S. Gudiksen, J. Wang, and C. M. Lieber, “Synthetic control of the diameter

and length of single crystal semiconductor nanowires” J. Phys. Chem. B, pp.

4062 - 4064, 2001.

[36] Y. Wu, J. Xiang, C. Yang, W. Lu and C. M. Lieber, “Single-crystal metallic

nanowires and metal/semiconductor nanowire heterostructures,” Nature, pp.

61-65, 2004.

[37] Y. Huang, X. Duan, Y. Cui, L. J. Lauhon, K. H. Kim, C. M. Lieber, “Logic gates

and computation from assembled nanowire building blocks,” Science, vol. 294,

no. 5545, pp. 1313-1317, 2001.

[38] Z. Zhong, D. Wang, Y. Cui, M. W. Bockrath, C. M. Lieber, “Nanowire crossbar

arrays as address decoders for integrated nanosystems,” Science, vol. 302. no.

5649, pp. 1377-1379, 2003.

[39] M. C. McAlpine, R. S. Friedman, S. Jin, K. H. Lin, W. U. Wang, and C. M.

Lieber, “High-performance nanowire electronics and photonics on glass and

plastic substrates,” Nano Lett, pp 1531-1535, 2003.

[40] J. A. Rogers, Z. Bao, K. Baldwin, A. Dodabalapur, B. Crone, V. R. Raju, V.

Kuck, H. Katz, K. Amundson, J. Ewing, and P. Drzaic, “Paper-like electronic

displays: large-area rubberstamped plastic sheets of electronics and

microencapsulated electrophoretic inks,” PNAS, vol. 98, no. 9, pp. 4835-4840,

2001.

[41] M. S. Gudiksen, L. J. Lauhon, J. Wang, D. C. Smith and C. M. Lieber, “Growth

of nanowire superlattice structures for nanoscale photonics and electronics,”

Nature, pp. 617-620, 2002.

[42] Alfredo M. Morales and Charles M. Lieber, “A laser ablation method for the

synthesis of crystalline semiconductor nanowires”, Science, Vol. 279,

pp.208-211., 1998.

[43] Dunwei Wang, Qian Wang, et al., “Germanium nanowire field-effect transistors

with SiO2 and high-k HfO2 gate dielectrics”, Appl. Phys. Lett., Vol. 83, pp.

2432-2434, 2003.

[44] N. Wang, Y. F. Zhang, Y. H. Tang, et al., “SiO2-enhanced synthesis of Si

nanowires by laser ablation”, Appl. Phys. Lett., Vol. 73, pp. 3902-3904, 1998.

[45] Y. Kaneko, K. Tsutsui, H. Matsumaru, H. Yamamoto, T. Tsukada, “Amorphous

silicon thin film transistor with a buried double-gate structure,” IEDM, pp.

337-340, 1989.

[46] Yuan Taur, D. A. Buchanan, W. Chen, D. J. Frank, K. E. Ismail, S. H. Lo,

Sai-Halasz, G.A., R. G. Viswanathan, H. J. C. Wann, S. J. Wind, H. S. Wong,

“CMOS scaling into the nanometer regime,” Proceedings of the IEEE, Vol.

85, Issue 4, pp. 486-504, 1997.

[47] G. K. Celler, S. Cristoloveanu, “Frontiers of silicon-on-insulator,” J. Appl. Phys.,

pp. 4955-4978, 2003.

[48] W. Daum, H.-J. Krause, U. Reichel, and H. Ibach, “Identification of strained

silicon layers at Si-SiO2 interfaces and clean Si surfaces by nonlinear optical

spectroscopy,” Phys. Rev. Lett., Vol. 71, no. 8, pp. 1234-1237, 1993.

[49] T. Tezuka, N. Sugiyama, T. Mizuno, M. Suzuki and S. Takagi, “A novel

fabrication technique of ultrathin and relaxed SiGe buffer layers with high Ge

fraction for sub-100 nm strained silicon-on-insulator MOSFETs” Jpn. J. Appl.

Phys.,Vol. 40, 2001.

[50] Sander J. Tans, A. M. Verschueren and C. Dekker, “Room-temperature transistor

based on a single carbon nanotube,” Nature, pp. 49-52, 1998.

[51] R. H. Baughman, A. A. Zakhidov, W. A. de Heer, “Carbon nanotubes--the route

toward applications,” Science, Vol. 297. no. 5582, pp. 787-792, 2002.

[52] A. G. Lewis, D. D. Lee, and R. H. Bruce, “Polysilicon TFT circuit design and

performance,” IEEE J. Solid-State Circuits, vol. 27, pp. 1833-1841, 1992.

[53] H. Kuriyama, Y. Ishigaki, Y. Fujii, S. Maegawa, S. Maeda, S. Miyamoto, K.

Tsutsumi, H. Miyoshi, and A. Yasuoka, “A C-switch cell for low voltage and

high-density SRAMs,” IEEE Trans. Electron Devices, vol. 45, pp. 2483-2488,

1998.

[54] K. P. A. Kumar, J. K. O. Sin, C. T. Nguyen, and P. K. Ko, “Kink-free

polycrystalline silicon double-gate elevated-channel thin-film transistors,” IEEE

Trans. Electron Devices, vol. 45, pp. 2514-2510, 1998.

[55] H.C. Lin, M. H. Lee, and C. J. Su, submitted to IEEE Trans. Electron Devices.

[56] G. Fortunato, P. Migliorato, “Field-effect analysis for the determination of

gap-state density and Fermi-level temperature dependence in polycrystalline

silicon,” Phil. Mag. B., vol. 57, pp. 573-586, 1988.

[57] Philips Research Laboratories, Redhill, Surrey, “Analysis of field-effect

conductance measurements on amorphous semiconductors,” Phil. Mag. B. vol.

43, pp. 93-103, 1981.

[58] Weisfield R. L, and Anderson D. A. “Analysis of field effect conductance

measurements on amorphous semiconductor,” Phil. Mag. B. vol. 33, p. 935,

1981.

[59] G. Fortunato, P. Migliorato, “Field-effect analysis for the determination of

gap-state density and Fermi-level temperature dependence in polycrystalline

silicon,” Phil. Mag. B. vol. 57, pp. 573-586, 1988.

Table 2-1 NH3 plasma treatment conditions.

Plasma RF power (watt)

Pressure (pa)

Flow rate (sccm)

Temperature (℃)

NH3 200 50 200 300

Table 3-1 Key parameters of the silicon-germanium nanowire TFTs with different NH3 plasma passivation times.

NH3 plasma passivaiton

time

Threshold Voltage (V) Vth

Subthreshold swing (V/decade)

S.S.

mobility

As-fabricated 12.96 1.36 0.87

30 mins 7.00 0.705 5.62

1 hour 5.75 0.572 11.87

Table 3-2 Summary of key parameters for n-type poly-Si and poly-Sil-xGex nanowire TFTs at VD = 0.5 V.

Table 3-3 Summary of key parameters for p-type poly-Si and poly-Sil-xGex nanowire TFTs at VD = 0.5 V.

SiGe-channel 3.74 0.77 12.03

P-Channel

SiGe-channel -12.3081 0.87 4.40

Table 4-1 Characteristics of nanowire TFT with DG and SG operations.

Table 4-2 Improving DIBL effect by varying sub-gate voltage.\

Threshold voltage

Figure 2-1 Definition of the main gate.

Figure 2-2 Deposition of LPCVD TEOS and channel layer.

Figure 2-3 Ion implantation.

Figure 2-4 Self-aligned formation of nanowire channel.

Figure 2-5 Deposition of passivation oxide layer.

Figure 2-6 Definition of sub-gate.

Figure 2-7 Top view of nanowire TFT with double-gated structure.

Figure 2-8(a) Cross sectional picture of sidewall spacer nanowire channel of poly-Si TFT.

Figure 2-8(b) Cross sectional picture of sidewall spacer nanowire channel of poly-Si TFT.

Figure 2-8(c) Cross sectional picture of sidewall spacer nanowire channel of poly-SiGe TFT.

VD = 0.5 V, L = 1 µm

Figure 3-1 Transfer characteristics of silicon-germanium nanowire TFTs with different NH3 plasma passivation times.

相關文件