參考文獻
[1] J. F. Kang, H. Y. Yu, C. Ren, N. Sa, H. Yang, M.-F. Li, D. S. H. Chan, X.Y. Liu, R. Q. Han, and D.-L. Kwong, J. Electrochem. Soc. 154(11), H927 (2007).
[2] H. Y. Yu, H. F. Lim, J. H. Chen, M. F. Li, C. X. Zhu, C. H. Tung, A. Y.Du, W. D. Wang, D. Z. Chi, and D. L. Kwong, IEEE Electron Device Lett.24, 230 (2003).
[3] J. F. Kang, H. Y. Yu, C. Ren, M.-F. Li, D. S. H. Chan, X. Y. Liu, and D.-L. Kwong, Electrochem. Solid-State Lett. 8(11), G311 (2005).
[4] C. J. Yim, D.-H. Ko, M. H. Jang, K. B. Chung, M.-H. Cho, and H. T. Jeon,Appl. Phys. Lett. 92, 012922 (2008).
[5] 翁偉智,”氮化鋯之薄膜特性與微觀組織之研究”中山大學,2003
[6] 廖為銅,”反應性濺鍍鋯基二元與三元薄膜在銅金屬化製程的應用”,逢甲大學,95
[7] 劉傳璽,陳進來,”半導體元件物理與製程理論與實務”,五南圖書出版
[8] 蕭宏著、羅正忠、張鼎張譯,” 半導體製程技術導論” ,歐亞書局
[9]施敏著、黃調元譯,”半導體元件物理與製作技術”,交大出版社
[10]M. Lenzlinger and E. H. Snow,” Fowler-Nordheim tunnel into thermally grown SiO2,”J. Appl.Phys. vol. 33,pp.205 1965.
[11] S.M. Sze,”Physics of Semiconductor Device, 2nd ed.,”Wiley,New York, 1981.
[12] D. K.Schroder,”Semiconductor material and sevic characteristics,”Wiley,Arizona,1998.
[13] C. H. Chio,K. H.Oh,J. S.Goo,Z. Yu,and R. W. Dutton,”Direct tunneling current model for circuit simulation”,IEDM Technical Digest.International,735(1999).
[14] The International Technology Roadmap for Semiconductors (ITRS), Semiconductor Industry Association (2005).
[15] Thomas Y. Hoffmann, Imec, Leuven, Belgium,” 高介電係數介電層與金屬閘極的製程選擇:閘極先製還是閘極後製?”,半導體科技,(2010)
[16] Pi-Chun Juan, Fan-Chen Mong, and Jen-Hung Huang,” The role of ZrN capping layer deposited on ultra-thin high-k Zr-doped yttrium oxide for metal-gate metal–insulator–semiconductor applications” JOURNAL OF APPLIED PHYSICS 114, 084110 (2013)
[17] J Robertson and P W Peacock,” Electronic structure and band offsets of high-dielectric-constant gate oxides”,Materials Research Society 27,217(2002).
[18] 吳錦裕、梁文龍、艾啟峰”新鍍膜技術-高功率脈衝磁控濺射之介紹及研發”,真空科技 22 卷‧第 4 期 (24)[19] Maria Palmucci, Nikolay Britun, Stephanos Konstantinidis, and Rony Snyders,” Rarefaction windows in a high-power impulse magnetron sputtering plasma” JOURNAL OF APPLIED PHYSICS 114, 113302 (2013)
[20] A. P. Ehiasarian, A. Vetushka, A. Hecimovic, and S. Konstantinidis,” Ion composition produced by high power impulse magnetron sputtering discharge snear the substrate” JOURNAL OF APPLIED PHYSICS 104, 083305 2008
[21] A. P. Ehiasarian, A. Vetushka, Y. Aranda Gonzalvo, G. Sáfrán, L. Székely, and P. B. Barna,” Influence of high power impulse magnetron sputtering plasma ionization on the
microstructure of TiN thin films” JOURNAL OF APPLIED PHYSICS 109, 104314 (2011)
[22] G. T. West, P. J. Kelly, and J. W. Bradley,” A Comparison of Thin Silver Films Grown Onto Zinc Oxide via Conventional Magnetron Sputtering and HiPIMS Deposition” IEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 38, NO. 11, NOVEMBER 2010
[23] Fridrik Magnus, Arni S. Ingason, Sveinn Olafsson, and Jon T. Gudmundsson,” Nucleation and Resistivity of Ultrathin TiN Films Grown by High-Power Impulse Magnetron Sputtering”, IEEE ELECTRON DEVICE LETTERS, VOL. 33, NO. 7, JULY 2012
[24] A.S. Ingason,F. Magnus,J. S. Agustsson, S.Olafsson, and
J. T. Gudmundsson,“In-situ electrical characterization of ultrathin TiN films grown by reactive dc magnetron sputtering on SiO 2 ,”Thin Solid Films, vol. 517, no. 24, pp. 6731–6736, Oct. 2009.
[25] Grzegorz Greczynski, Jens Jensen, and Lars Hultman,” CrN x Films Prepared by DC Magnetron Sputtering and High-Power Pulsed Magnetron Sputtering: A Comparative Study”, IEEE TRANSACTIONS ON PLASMA SCIENCE, VOL. 38, NO. 11, NOVEMBER 2010
[26] P.C. Juan et al “The effect of ZrN antidiffusion capping layer on the electrical and physical properties of metal-gate/ZrN/Zr-graded Dy 2O3 /Si MIS nanolaminated structures”, Microelectronic Engineering 109(2013)172–176
[27] P. A. Cormier,et al. ” Measuring the energy flux at the substrate position during magnetron sputter deposition processes” JOURNAL OF APPLIED PHYSICS 113, 013305 (2013)
[28] 張瑞慶,” 奈米壓痕技術與應用”, 聖約翰科技大學機械系