lecture1casgs-納米科學(xué)概論(存儲(chǔ)版)
【正文】 trode gate to adjust QD potential independently Another version of SET VG = V0 + V1 cos(2?ft) I = ef, SET can be used as a current standard Application example of SET: 參考文獻(xiàn) 1. P. Moriarty, Nanostructured materials, Rep. Prog. Phys. 64, 297 (2021). 2. G. Timp (ed), Nanotechnology (Springer, New York, 1999). 3. Hari Singh Nalwa (ed), Nanostructured materials and nanotechnology (Academic Press, London, 2021). 4. For 2021 International Technology Roadmap for Semiconductors (ITRS), see website 5. The Royal Society, Nanoscience and nanotechnologies: opportunities and uncertainties, (July 2021). 6. . Griffiths, Introduction to quantum mechanics (Prentice Hall, New Jersey, 1995). 7. . Davis, The physics of lowdimensional semiconductors: an introduction (Cambridge University Press, New York, 1998). 8. A. Shik, Quantum wells: physics and electronics of twodimensional systems (World Scientific, Singapore, 1997). 9. K. Barnham, D. Vvedensky (eds.), Lowdimensional semiconductor structures: Fundamentals and device applications (Cambridge University Press, New York, 2021). 10. . Ferry, . Goodnick, Transport in nanostructures (Cambridge University Press, New York, 1997). 11. T. Ando et al., Mesoscopic physics and electronics (Springer, Berlin, 1998). 12. S. Datta, . McLennan, Quantum transport in ultrasmall devices, Rep. Prog. Phys. 53, 1003 (1990). 13. . Thornton, Mesoscopic devices, Rep. Prog. Phys. 57, 311 (1994). 14. . Smith, Lowdimensional quantum devices, Rep. Prog. Phys. 59, 235 (1996). 15. D. Ferry, . Barker, C. Jacaboni (eds.), Granular Nanoelectronics (Plenum, New York, 1990). 16. H. Grabert, . Devoret (eds.), Single charge tunneling: Coulomb blockade phenomena in nanostructures (Plenum, New York, 1992). 17. H. Koch, H. L252。納米結(jié)構(gòu)物理學(xué) 課程內(nèi)容 1. 納米科學(xué)概論 , 低維體系量子力學(xué) 2. 固體物理 , 表面 /界面科學(xué)及材料生長(zhǎng)簡(jiǎn)介 3. 納米結(jié)構(gòu)常用分析與制備方法 4. 納米線 (管 ,帶 ,桿 ) 5. 團(tuán)簇與晶粒 6. 磁性納米結(jié)構(gòu)及自旋電子學(xué) 1 nm = 109 m = 103 ?m = 10 197。 b are classical turning points) Coherent quantum transport in 1D channel When phase coherence is maintained, electrons should be treated as pure waves 1D electron transportation between two regions separated by an arbitrary potential barrier: ?/)(21 IUEmk ???/)(22 IIUEmk ?? A exp(ik1z) B exp(ik1z) C exp(ik2z) Region I Barrier
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