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Volumn 95, Issue 10, 2004, Pages 5545-5582

Analysis of quantum ballistic electron transport in ultrasmall silicon devices including space-charge and geometric effects

Author keywords

[No Author keywords available]

Indexed keywords

BAND STRUCTURE; HEAT CONDUCTION; MATHEMATICAL MODELS; PHASE EQUILIBRIA; QUANTUM THEORY; RESONANT TUNNELING; SILICON; SPECTRUM ANALYSIS; VORTEX FLOW;

EID: 2942571688     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.1695597     Document Type: Review
Times cited : (99)

References (99)
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    • The availability of the 1-D and 3-D versions of NEMO is described at 〈http://hpc.jpl.nasa.gov/PEP/gekco/nemo_avail.html〉
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    • note
    • z* equal to that of the silicon to permit this separation.
  • 41
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    • edited by N. G. Einspruch and W. R. Frensley (Academic, San Diego, LA)
    • W. R. Frensley, in Heterostructures and Quantum Devices, edited by N. G. Einspruch and W. R. Frensley (Academic, San Diego, LA, 1993); VLSI Electron. 24, 273.
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    • Using the "quantum transmitting boundary method" to derive the density-of-states for self-consistent poisson-schrödinger ballistic device simulation
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    • note
    • We term an energy "two-dimensional" to identify it as originating from a solution of a two-dimensional Schrödinger equation, where confusion with one-dimensional solutions might occur.
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    • 2942547831 scopus 로고    scopus 로고
    • note
    • t-2, as discussed following Eq. (A17).
  • 59
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    • note
    • P=0 over most of the device domain.
  • 69
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    • note
    • While the same formula for injection velocity applies, here we are invoking the concept at the source contact, while it was previously invoked at the top of the potential barrier in the FET channel.
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    • One other interesting observation from H. Wu and D. W. L. Sprung, Phys. Rev. A 49, 4305 (1994) is that in three dimensions, a vortex is not formed by an isolated occurrence of Φ = 0. Rather, vortex formation requires a continuous curve of points where Φ = 0. This curve can be either closed on itself or terminate on a device boundary, where Φ = 0 by definition. In our case, this curve is a line normal to and intersecting the simulation plane where Φ = 0.
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    • note
    • 0. We have also discussed an analogous compression operation for the Poisson equation in Appendix B, differing in the important detail that the boundary values applied are not necessarily zero.
  • 94
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    • note
    • 0.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.