1983
DOI: 10.1103/physrevb.27.3519
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Interface connection rules for effective-mass wave functions at an abrupt heterojunction between two different semiconductors

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Cited by 268 publications
(196 citation statements)
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“…Experimental Signatures.-To explore the experimental signatures of the newly discovered SABSs, we consider a normal metal/superconductor (NS) junction in a doped WSM and calculate the normalized tunneling conductance σ n (eV ) = σ S (eV )/σ N (eV ) using the tight binding model in Eq. (1) with an appropriate boundary condition [51,52]. Here σ S (eV ) is the conductance of the NS junction, and σ N (eV ) is that in the normal state.…”
Section: (B)mentioning
confidence: 99%
“…Experimental Signatures.-To explore the experimental signatures of the newly discovered SABSs, we consider a normal metal/superconductor (NS) junction in a doped WSM and calculate the normalized tunneling conductance σ n (eV ) = σ S (eV )/σ N (eV ) using the tight binding model in Eq. (1) with an appropriate boundary condition [51,52]. Here σ S (eV ) is the conductance of the NS junction, and σ N (eV ) is that in the normal state.…”
Section: (B)mentioning
confidence: 99%
“…However, our approach is different from the very beginning because we propose an ordering for kinetic term based on a specific argument for the matching conditions. This ordering is also used in [24] for studying connection rules for effective-mass wave functions across an abrupt heterojunction.…”
Section: Introductionmentioning
confidence: 99%
“…Em 1969, Gora e Williams [12] estudaram o caso α = −1, β = γ = 0. Zhu e Kroemer [13], em 1983, analisaram sistemas com α = γ = − [14].…”
Section: Solução Da Equação De Schrödinger -Algebra De Heisenberg E Aunclassified