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Extraction of interface state density and resistivity of suspended p-type silicon nanobridges 被引量:1

Extraction of interface state density and resistivity of suspended p-type silicon nanobridges
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摘要 The evaluation of the influence of the bending deformation of silicon nanobridges on their electrical properties is crucial for sensing and actuating applications. A combined theory/experimental approach for de- termining the resistivity and the density of interface states of the bending silicon nanobridges is presented. The suspended p-type silicon nanobridge test structures were fabricated from silicon-on-insulator wafers by using a standard CMOS lithography and anisotropic wet etching release process. After that, we measured the resistance of a set of silicon nanobridges versus their length and width under different bias voltages. In conjunction with a theoretical model, we have finally extracted both the interface state density of and resistivity suspended silicon nanobridges under different bending deformations, and found that the resistivity of silicon nanobridges without bending was 9.45 mΩ.cm and the corresponding interface charge density was around 1.7445 × 10^13 cm-2. The bending deformation due to the bias voltage slightly changed the resistivity of the silicon nanobridge, however, it significantly changed the distribution of interface state charges, which strongly depends on the intensity of the stress induced by bending deformation. The evaluation of the influence of the bending deformation of silicon nanobridges on their electrical properties is crucial for sensing and actuating applications. A combined theory/experimental approach for de- termining the resistivity and the density of interface states of the bending silicon nanobridges is presented. The suspended p-type silicon nanobridge test structures were fabricated from silicon-on-insulator wafers by using a standard CMOS lithography and anisotropic wet etching release process. After that, we measured the resistance of a set of silicon nanobridges versus their length and width under different bias voltages. In conjunction with a theoretical model, we have finally extracted both the interface state density of and resistivity suspended silicon nanobridges under different bending deformations, and found that the resistivity of silicon nanobridges without bending was 9.45 mΩ.cm and the corresponding interface charge density was around 1.7445 × 10^13 cm-2. The bending deformation due to the bias voltage slightly changed the resistivity of the silicon nanobridge, however, it significantly changed the distribution of interface state charges, which strongly depends on the intensity of the stress induced by bending deformation.
出处 《Journal of Semiconductors》 EI CAS CSCD 2013年第5期7-12,共6页 半导体学报(英文版)
基金 supported by the National Natural Science Foundation of China(No.41075026) the Natural Science Foundation of Jiangsu Province (No.BK2012460) the Special Fund for Meteorology Research in the Public Interest(No.GYHY200906037) the Universities Natural Science Research Project of Jiangsu Province(No.12KJB510011) the Priority Academic Program Development of Sensor Networks and Modern Meteorological Equipment of Jiangsu Higher Education Institutions
关键词 interface state density RESISTIVITY silicon nanobridges bias voltages interface state density resistivity silicon nanobridges bias voltages
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  • 1Craighead H G 2000 Science 290 1532.
  • 2Feng X L, He R R, Yang P D and Roukes M L 2007 Nano Lett. 7 1953.
  • 3He R R and Yang P D 2006 Nature Nanotechnology 1 42.
  • 4Gil-Santos E, Ramos D, Martlnez J, Fernndez-Regfilez M, Garcia R, Paulo A S, Calleja M and Tamayo J 2010 Nature Nanotechnology 5 641.
  • 5Jin Q H, Li T, Zhou P and Wang Y L 2009 J. Nanomater. 2009 319842.
  • 6Kizuka T, Takatani Y, Asaka K and Yoshizaki R 2005 Phys. Rev. B 72 035333.
  • 7Zhu Y, Xu F, Qin Q, Fung W Y and Lu W 2009 Nano Lett. 9 3934.
  • 8Namazu T, Isono Y and Tanaka T 2000 J. Microelec- tromech. Syst. 9 450.
  • 9Virwani K R, Malshe A P, 2003 Smart. Mater. Struct Schmidt W F and Sood D K 12 1028.
  • 10Paulo A S, Bokor J, Howe R T, He R, Yang P, Gao D, Carraro C and Maboudian R 2005 Appl. Phys. Lett. 87 053111.

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  • 1裴立宅,唐元洪,陈扬文,张勇.掺杂硅纳米线的研究进展[J].功能材料与器件学报,2004,10(4):399-406. 被引量:8
  • 2尤思宇,王燕.表面钝化硅纳米线的能带结构[J].Journal of Semiconductors,2006,27(11):1927-1933. 被引量:2
  • 3Zhao X Y, Wei C M, Chou M Y. Quantum confine-ment and electronic properties of silicon nanowires [J]. Phys. Rev. Lett., 2004, 92(23) : 236805.
  • 4Kobayashi M, Hiramoto T. Experimental study on quantum confinement effects in silicon nanowire metal -oxide - semiconductor field - effect transistors and single - electron transistors [ J 1. J. Appl. Phys. , 2008, 103: 053709.
  • 5Mulazimoglu E, Coskun S, Gunoven M, et al. Silicon nanowire network metal -semiconductor- metal photo- detectors [ J ]. Appl. Phys. Lett. , 2013, 103: 083114.
  • 6Chen Y, Wang X H, Hong M, et al. Surface - modi- fied silicon nano- channel for urea sensing [J]. Sen- sors and Actuators B, 2008, 133 : 593.
  • 7Toiyama T, Funai D, Sugiyama S. Piezoresistance measurement on single crystal silicon nanowires [ J ]. J. Appl. Phys. , 2003, 93: 561.
  • 8Lugstein A, Steinmair M, Steiger A, et al. Anamalous piezoresistive effect in ultrastrained silicon nanowires [J]. Nano Lett. , 2010, 10: 3204.
  • 9Li D Y, Wu Y Y, Kim P, et al. Thermal conductivity of individual silicon nanowires [ J ]. Appl. Phys. Lett., 2003, 83(14): 2934.
  • 10Agarwal A, Buddharaju K, Lao I K, et al. Silicon nanowire sensor array using top - down CMOS technol- ogy [J]. Sensors and Actuators A, 2008, 145 - 146: 207.

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