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📄 pt_nonorm.m

📁 量子信息科学使用的源码以及量子进化算法
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% pt_nonorm    partial transposition of a density matrix%              for a qudit register; the density matrix is not%              normalized%    pt_nonorm(M,list,d) computes the matrix obtained from M%    by partially transposing the qudits given in the list.%    The numbering of the qudits starts with 1.%    Here d is the dimension of the qudits.%    If d is not provided then d is taken to be 2 (qubits).%    M is normalized making the trace 1 before any further%    computation. Unlike for pt, the density matrix is%    not normalized.% Copyright (C) 2007  Geza Toth    E.mail: toth@alumni.nd.edu%% This program 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; see gpl.txt% of this subroutine package.%% This program 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 this program; if not, write to the Free Software% Foundation, Inc., 51 Franklin Street, Fifth Floor, % Boston, MA  02110-1301, USA.function rhoT=pt_nonorm(rho,list,varargin)% There is no normalization% rho=ketbra2(rho);if nargin==2,   d=2;elseif nargin==3,   d=varargin{1};else       error('Wrong number of input arguments.');end %if    for n=1:length(list)      nn=list(n);      nmax=d^(nn-1);      nmax2=d^nn;      [y,x]=size(rho);      rhoT=zeros(y,x);      % Partial transpostion #1      for k=1:nmax      for l=1:nmax          rhoT(k:nmax:end,l:nmax:end)=rho(k:nmax:end,l:nmax:end).';      end %for      end %for      rho=rhoT;      % Partial transpostion #2      for k=1:nmax2      for l=1:nmax2          rhoT(k:nmax2:end,l:nmax2:end)=rho(k:nmax2:end,l:nmax2:end).';      end %for      end %for             rho=rhoT;   end %for   

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