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Volumn 70, Issue 19, 2004, Pages 1-13

Real-space finite-difference method for conductance calculations

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; BOUNDARY LAYER; CHEMICAL STRUCTURE; CONDUCTANCE; ELECTRODE; ELECTRON TRANSPORT; FINITE ELEMENT ANALYSIS; HAMILTON SCALE; MATHEMATICAL ANALYSIS; MATHEMATICAL COMPUTING; NEUTRON SCATTERING; QUANTUM MECHANICS;

EID: 12344289075     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.70.195402     Document Type: Article
Times cited : (82)

References (61)
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    • note
    • If one uses Green functions, one has to distinguish between retarded and advanced Green functions. This can be done by subtracting or adding a (small) imaginary number to the energy.
  • 39
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    • note
    • The size of the scattering region does not have to be an integer multiple of the size of the cell in the leads. One can choose cells of a different size in the scattering region. One also chooses differently sized cells in the left and right leads in case the leads are different. We have not introduced cells of different size here in order not to complicate the notation, but the strategy for solving the scattering problem as outlined in Appendix A 4 also works in that case.
  • 48
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    • 0, is used as the local potential. Tests using a nonlocal pseudopotential with s and p parts gave a virtually identical electronic structure for bulk sodium, indicating that the use of a local potential is a good approximation for sodium.
    • (1991) Phys. Rev. B , vol.43 , pp. 1993
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    • note
    • z=3456.
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    • note
    • -3 from the highly accurate results.
  • 59
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    • note
    • -5 hartrees yields a potential that can change the conductance by up to 5% and can even suppress the even-odd oscillation almost completely.
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    • note
    • 3S.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.