Code covered by the BSD License
-
H=genmatrix1D(pot,y,mass)
GENMATRIX1D compute matrix for Schroedinger solution in 1D
-
H=genmatrix2D(pot,x,y,massx,m...
GENMATRIX2D compute matrix for Schroedinger solution in 2D
-
[E,psi]=schrsolv1D(pot,x,y,ma...
SCHRSOLV1D solve Schroedinger equation in 1D
-
[E,psi]=schrsolv2D(pot,x,y,ma...
SCHRSOLV2D solve Schroedinger equation in 2D
-
[E,psi]=schrtrack1D(pot,x,y,m...
SCHRTRACK1D refine eigenvalues in 1D
-
[E,psi]=schrtrack2D(pot,x,y,m...
SCHRTRACK2D refine eigenvalues in 2D
-
a=gaasmaterial(x,prop)
GAASMATERIAL material database for GaAs/AlGaAs mertial system
-
add_bias(xyminmax,bias)
ADD_BIAS new biased region
-
add_boundary(varargin)
ADD_BOUNDARY set boundary condition
-
b=extend1D(a,x)
EXTEND1D extrapolate field in 1D
-
b=extend2D(a)
EXTEND2D extrapolate field in 2D
-
buildstructure;
BUILDSTRUCTURE set up structure
-
charge=addqcharge(charge,delt...
ADDQCHARGE add QBOX charge
-
charge=gencharge(phi,tp,varar...
GENCHARGE compute charge density
-
charge=genqcharge(nr,tp,sub,v...
GENQCHARGE compute quantum charge density
-
charge=sumcharge(phi,varargin...
SUMCHARGE collect charge
-
genmatrixpoi
GENMATRIXPOI compute matrix for Poisson solution in 2D and 1D
-
integral=integrate(field,posb...
INTEGRATE integrate a field
-
ret=fermi(order,x);
FERMI complete Fermi integrals
-
rhs=genrhspoi(charge,varargin...
GENRHSPOI form right hand side of Poisson equation
-
runstructure
RUNSTRUCTURE performs computation
-
schrsolve(potential,fl)
SCHRSOLVE solve Schroedinger equation
-
startpotential(startpot)
STARTPOTENTIAL use non-zero startpotential
-
Contents.m
-
bugs.m
-
constants.m
-
howto.m
-
initaquila.m
-
lowdens.m
-
mdsi.m
-
qwrsubst.m
-
readme.m
-
sl.m
-
structures.m
-
wire.m
-
View all files
from
2D Schroedinger Poisson solver AQUILA
by Martin Rother
AQUILA is a 2D Schroedinger Poisson solver for GaAs / AlGaAs semiconductor nanostructures.
|
| bugs.m |
%Known bugs and things that AQUILA 1.0 cannot handle
%
%- The material database might not be completely correct, I just copied some
% values from some papers and code and some values from Landolt-Bornstein/Adachi.
%
%- The Gamma nonparabolicity is taken into account only for classical treated
% electron densities. For quantum densities and for the computation of
% energy levels the parabolic approximation is used. Thus especially higher
% levels and densities in higher subbands may be wrong.
%
%- The algorithm may be failing to converge for certain boundary conditions
% and structures as the iteration gets trapped in a local minimum.
%
%- p-doping is included only as fixed space charge.
%
%- drift and diffusion is not included. Thus diffusion regions can not be handeled properly.
%
%- Sometimes a 'matrix close to singular' warning from routine 'inviter' occurs.
% This may be ignored.
%
%- inverse vectoriteration sometimes loses eigenvalues.
%
%- several other simplifying assumptions. Mail me for the details on whether and how
% something is treated.
%Copyright 1999 Martin Rother
%
%This file is part of AQUILA.
%
%AQUILA is free software; you can redistribute it and/or modify
%it under the terms of the BSD License as published by
%the Open Source Initiative according to the License Policy
%on MATLAB(R)CENTRAL.
%
%AQUILA is distributed in the hope that it will be useful,
%but WITHOUT ANY WARRANTY; without even the implied warranty of
%MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
%BSD License for more details.
|
|
Contact us at files@mathworks.com