X-Git-Url: https://git.creatis.insa-lyon.fr/pubgit/?p=CreaPhase.git;a=blobdiff_plain;f=octave_packages%2Fsecs1d-0.0.8%2FDDG%2FDDGgummelmap.m;fp=octave_packages%2Fsecs1d-0.0.8%2FDDG%2FDDGgummelmap.m;h=eaf6f344448513b9bfb25199bfc68d059bf4c3a1;hp=0000000000000000000000000000000000000000;hb=c880e8788dfc484bf23ce13fa2787f2c6bca4863;hpb=1705066eceaaea976f010f669ce8e972f3734b05

diff --git a/octave_packages/secs1d-0.0.8/DDG/DDGgummelmap.m b/octave_packages/secs1d-0.0.8/DDG/DDGgummelmap.m
new file mode 100644
index 0000000..eaf6f34
--- /dev/null
+++ b/octave_packages/secs1d-0.0.8/DDG/DDGgummelmap.m
@@ -0,0 +1,147 @@
+function [odata,it,res] =...
+      DDGgummelmap (x,idata,toll,maxit,ptoll,pmaxit,verbose)
+
+ 
+%
+% [odata,it,res] =...
+%            DDGgummelmap (x,idata,toll,maxit,ptoll,pmaxit,verbose)
+%
+% Solves the scaled stationary bipolar DD equation system
+%     using Gummel algorithm
+%
+%     input: x          spatial grid
+%            idata.D    doping profile
+%            idata.p    initial guess for hole concentration
+%            idata.n    initial guess for electron concentration
+%            idata.V    initial guess for electrostatic potential
+%            idata.Fn   initial guess for electron Fermi potential
+%            idata.Fp   initial guess for hole Fermi potential
+%            idata.l2   scaled electric permittivity (diffusion coefficient in Poisson equation)
+%            idata.un   scaled electron mobility
+%            idata.up   scaled electron mobility
+%            idata.nis  scaled intrinsic carrier density
+%            idata.tn   scaled electron lifetime
+%            idata.tp   scaled hole lifetime
+%            toll       tolerance for Gummel iterarion convergence test
+%            maxit      maximum number of Gummel iterarions
+%            ptoll      tolerance for Newton iterarion convergence test for non linear Poisson
+%            pmaxit     maximum number of Newton iterarions
+%            verbose    verbosity level: 0,1,2
+%
+%     output: odata.n     electron concentration
+%             odata.p     hole concentration
+%             odata.V     electrostatic potential
+%             odata.Fn    electron Fermi potential
+%             odata.Fp    hole Fermi potential
+%             it          number of Gummel iterations performed
+%             res         total potential increment at each step
+
+## This file is part of 
+##
+## SECS1D - A 1-D Drift--Diffusion Semiconductor Device Simulator
+## -------------------------------------------------------------------
+## Copyright (C) 2004-2007  Carlo de Falco
+##
+##
+##
+##  SECS1D is free software; you can redistribute it and/or modify
+##  it under the terms of the GNU General Public License as published by
+##  the Free Software Foundation; either version 2 of the License, or
+##  (at your option) any later version.
+##
+##  SECS1D 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
+##  GNU General Public License for more details.
+##
+##  You should have received a copy of the GNU General Public License
+##  along with SECS1D; If not, see <http://www.gnu.org/licenses/>.
+
+
+odata = idata;
+
+Nnodes=rows(x);
+
+D         = idata.D;
+vout(:,1) = idata.V;
+hole_density (:,1) = idata.p;
+electron_density (:,1)= idata.n;
+fermin (:,1)=idata.Fn;
+fermip (:,1)=idata.Fp;
+
+for i=1:1:maxit
+	if (verbose>1)
+		fprintf(1,'*****************************************************************\n');  
+		fprintf(1,'****    start of gummel iteration number: %d\n',i);
+		fprintf(1,'*****************************************************************\n');  
+    end
+
+	if (verbose>1)
+		fprintf(1,'solving non linear poisson equation\n\n');
+    end
+	[vout(:,2),electron_density(:,2),hole_density(:,2)] =...
+	DDGnlpoisson (x,[1:Nnodes],vout (:,1),electron_density(:,1),hole_density(:,1),...
+	fermin(:,1),fermip(:,1),D,idata.l2,ptoll,pmaxit,verbose);
+	
+	if (verbose>1)
+		fprintf (1,'\n\nupdating electron qfl\n\n');
+    end
+	electron_density(:,3)=...
+	DDGelectron_driftdiffusion(vout(:,2), x, electron_density(:,2),hole_density(:,2),idata.nis,idata.tn,idata.tp,idata.un);
+    
+    fermin(:,2) = DDGn2phin(vout(:,2),electron_density(:,3));
+    fermin(1,2)   = idata.Fn(1);
+    fermin(end:2) = idata.Fn(end);
+    
+	if (verbose>1)
+		fprintf(1,'updating hole qfl\n\n');
+    end
+
+	hole_density(:,3)=...
+    DDGhole_driftdiffusion(vout(:,2), x, hole_density(:,2),electron_density(:,2),idata.nis,idata.tn,idata.tp,idata.up);
+    fermip(:,2) = DDGp2phip(vout(:,2),hole_density(:,3));
+    fermip(1,2)   = idata.Fp(1);
+    fermip(end,2) = idata.Fp(end);
+    
+    if (verbose>1)
+		fprintf(1,'checking for convergence\n\n');
+    end
+	nrfn= norm(fermin(:,2)-fermin(:,1),inf);
+	nrfp= norm (fermip(:,2)-fermip(:,1),inf);
+	nrv = norm (vout(:,2)-vout(:,1),inf);
+	nrm(i) = max([nrfn;nrfp;nrv]);
+	
+	if (verbose>1)
+		fprintf (1,' max(|phin_(k+1)-phinn_(k)| , |phip_(k+1)-phip_(k)| , |v_(k+1)- v_(k)| )= %d\n',nrm(i));
+    end
+	if (nrm(i)<toll)
+		break
+    end
+
+	vout(:,1) = vout(:,end);
+	hole_density (:,1) = hole_density (:,end) ;
+	electron_density (:,1)= electron_density (:,end);
+	fermin (:,1)= fermin (:,end);
+	fermip (:,1)= fermip (:,end);
+	
+	
+	if(verbose)
+		DDGplotresults(x,electron_density,hole_density,vout,fermin,fermip);		
+    end
+end
+
+it = i;
+res = nrm;
+
+if (verbose>0)
+	fprintf(1,'\n\nInitial guess computed by DD: # of Gummel iterations = %d\n\n',it);
+end
+
+odata.n     = electron_density(:,end);
+odata.p     = hole_density(:,end);
+odata.V     = vout(:,end);
+odata.Fn    = fermin(:,end);
+odata.Fp    = fermip(:,end);
+
+
+