Finite-element analysis of the miniband structures of semiconductor superlattices with arbitrary periodic potential profiles

The method is based on the Galerkin procedure, and the third-order Hermitian line elements are used for finite elements. The periodic boundary condition is applied to the edges of one period of the periodic potential. A generalized boundary condition at the heterointerface is also introduced by use of the interface matrix. The validity of the method is confirmed by calculating the miniband structures and the envelope functions in rectangular superlattices made of GaAs-AlGaAs and GaSb-InAs. Numerical results for a biperiodic structure, a superlattice with graded interfaces, and a modulation-doped superlattice are presented. >

[1]  L. J. Sham,et al.  Electronic Properties of Flat-Band Semiconductor Heterostructures , 1981 .

[2]  Eigenstate calculation of quantum well structures using finite elements , 1988 .

[3]  J. Lin,et al.  Band structure of superlattice with graded interfaces , 1987 .

[4]  Tsuneya Ando Effective-mass theory of semiconductor heterojunctions and superlattices , 1982 .

[5]  Simulations of the current-voltage characteristics of semiconductor tunnel structures , 1987 .

[6]  Matsuura,et al.  Subbands and excitons in a quantum well in an electric field. , 1986, Physical review. B, Condensed matter.

[7]  H. Saunders Book Reviews : The Finite Element Method (Revised): O.C. Zienkiewicz McGraw-Hill Book Co., New York, New York , 1980 .

[8]  Krishna Thyagarajan,et al.  A novel numerical technique for solving the one-dimensional Schroedinger equation using matrix approach-application to quantum well structures , 1988 .

[9]  F. Peeters,et al.  New method of controlling the gaps between the minibands of a superlattice , 1989 .

[10]  Ian J. Fritz,et al.  Energy levels of finite‐depth quantum wells in an electric field , 1987 .

[11]  W. Lui,et al.  Exact solution of the Schrodinger equation across an arbitrary one‐dimensional piecewise‐linear potential barrier , 1986 .

[12]  M. Rezwan Khan,et al.  Transmission line analogy of resonance tunneling phenomena: the generalized impedance concept , 1988 .

[13]  M. Koshiba,et al.  Finite-element calculation of the transmission probability and the resonant-tunneling lifetime through arbitrary potential barriers , 1991 .

[14]  Well size dependence of Stark shifts for heavy‐hole and light‐hole levels in GaAs/AlGaAs quantum wells , 1986 .

[15]  L. Esaki,et al.  A bird's-eye view on the evolution of semiconductor superlattices and quantum wells , 1986 .

[16]  M. Koshiba,et al.  Finite-element analysis of quantum wells of arbitrary semiconductors with arbitrary potential profiles , 1989 .

[17]  Raphael Tsu,et al.  Superlattice and negative differential conductivity in semiconductors , 1970 .

[18]  Yuji Ando,et al.  Calculation of transmission tunneling current across arbitrary potential barriers , 1987 .

[19]  Karl Woodbridge,et al.  Computer modeling of the electric field dependent absorption spectrum of multiple quantum well material , 1988 .