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2002
DOI: 10.1103/physrevb.65.165328
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Interface electronic states and boundary conditions for envelope functions

Abstract: The envelope-function method with generalized boundary conditions is applied to the description of localized and resonant interface states. A complete set of phenomenological conditions which restrict the form of connection rules for envelope functions is derived using the Hermiticity and symmetry requirements. Empirical coefficients in the connection rules play role of material parameters which characterize an internal structure of every particular heterointerface. As an illustration we present the derivation… Show more

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Cited by 40 publications
(43 citation statements)
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References 42 publications
(78 reference statements)
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“…20 As this theory was originally developed for strained zinc-blende crystals, the equations must be augmented for heterostructures by boundary conditions, which describe how the envelope functions are to be joined at the boundaries of adjacent regions. [31][32][33][34][35][36][37] For QDs, the operator of Eq. ͑13͒ is converted into a differential operator via the replacement…”
Section: Calculation Of Energy Levelsmentioning
confidence: 99%
“…20 As this theory was originally developed for strained zinc-blende crystals, the equations must be augmented for heterostructures by boundary conditions, which describe how the envelope functions are to be joined at the boundaries of adjacent regions. [31][32][33][34][35][36][37] For QDs, the operator of Eq. ͑13͒ is converted into a differential operator via the replacement…”
Section: Calculation Of Energy Levelsmentioning
confidence: 99%
“…When applied to semiconductor quantum structures, it is implicitly assumed that the EFA equations are also valid across an atomically abrupt material interface. The original derivation by Luttinger and Kohn [52] is, however, not strictly applicable to this case and a lot of work has been done to derive a consistent EFA theory [66][67][68][69][70][71][72], with position-dependent material parameters. Burt [73,74] and Foreman [75,76] have developed an alternative formulation of the envelope function theory for semiconductor heterostructures, starting from the single-particle Schrödinger equation.…”
Section: The Envelope Wave Function Theory Of Burt and Foremanmentioning
confidence: 99%
“…There are many studies [2,3,7,[9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25] (see references therein) aimed at choosing matching conditions for the envelope wave functions at the interface and constructing a simplified system of equations valid for the whole heterostructure. However, in this paper, we do not intend to analyze and discuss the results of the studies.…”
Section: Introductionmentioning
confidence: 99%