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Volumn 33, Issue 12, 1986, Pages 8345-8359

kp theory of semiconductor superlattice electronic structure. I. Formal results

Author keywords

[No Author keywords available]

Indexed keywords

EID: 33749336446 PISSN: 01631829 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevB.33.8345 Document Type: Article

Times cited : (152)

References (30)

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- Esaki, L.¹

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- 0021392307
- Room temperature excitonic nonlinear absorption and refraction in GaAs/AlGaAs multiple quantum well structures
- (1984) IEEE Journal of Quantum Electronics , vol.20 QE , pp. 265
- Chemla, D.S.¹ Miller, D.A.B.² Smith, P.W.³ Gossard, A.C.⁴ Wiegmann, W.⁵

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- 35949021835
- (1981) Phys. Rev. Lett. , vol.47 , pp. 879
- White, S.R.¹ Sham, L.J.²

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- following paper.
- (1986) Phys. Rev. B , vol.33 – 1 , pp. 8360
- Mailhiot, C.¹ Smith, D.L.²

11
- 36049057570
- (1966) Phys. Rev. , vol.141 , pp. 789
- Cohen, M.L.¹ Bergstresser, T.K.²

15
- 84926606637
- That is, we neglect k dependence of the spin-orbit and stress interactions and terms proportional to Δ VlHs.o.l and Δ VlHstl.

16
- 0000216028
- (1982) Phys. Rev. B , vol.25 , pp. 3975
- Chang, Y.C.¹ Schulman, J.N.²

17
- 84926603690
- Although the dropped terms in H2 are smaller than the retained terms, the justification for neglecting them is primarily the way they enter the calculation.

18
- 84926533280
- One could retain these terms in H0. It improves, slightly, the bands as a function of k vecpara.

19
- 84926570327
- Their coupling to physically significant states at the interfaces is very small.

23
- 0000645471
- (1963) Phys. Rev. , vol.131 , pp. 2529
- Schlosser, H.¹ Marcus, P.M.²

24
- 84926591172
- Residual terms are of order ( Δ dd prime )2; that is, second order in Δ V.

25
- 84926556867
- Residual terms are of order Δ dd prime ; that is, first order in Δ V.

26
- 84926548965
- We use the notation (a,n;b,m) to indicate the interface between material a in the nth superlattice cycle and material b in the mth superlattice cycle.

27
- 84926570438
- For any periodic system described by a Hermitian Hamiltonian, if Q is a wave vector at a given energy, Qstar must also be a wave vector at this energy. A superlattice can be described by a Hermitian Hamiltonian and thus must have this property. Therefore, is important to show that our description of the superlattice, which is not directly based on a superlattice Hamiltonian, correctly describes this feature of the superlattice electronic structure.

28
- 77957047253
- edited by, R. K. Willardson, A. C. Beer, Academic, New York
- (1966) Semiconductors and Semimetals , vol.1 , pp. 75
- Kane, E.O.¹

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