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authorEugeniy E. Mikhailov <evgmik@gmail.com>2021-01-29 16:23:05 -0500
committerEugeniy E. Mikhailov <evgmik@gmail.com>2021-01-29 16:23:05 -0500
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+% tvdantzig_logbarrier.m
+%
+% Solve the total variation Dantzig program
+%
+% min_x TV(x) subject to ||A'(Ax-b)||_\infty <= epsilon
+%
+% Recast as the SOCP
+% min sum(t) s.t. ||D_{ij}x||_2 <= t, i,j=1,...,n
+% <a_{ij},Ax - b> <= epsilon i,j=1,...,n
+% and use a log barrier algorithm.
+%
+% Usage: xp = tvdantzig_logbarrier(x0, A, At, b, epsilon, lbtol, mu, cgtol, cgmaxiter)
+%
+% x0 - Nx1 vector, initial point.
+%
+% A - Either a handle to a function that takes a N vector and returns a K
+% vector , or a KxN matrix. If A is a function handle, the algorithm
+% operates in "largescale" mode, solving the Newton systems via the
+% Conjugate Gradients algorithm.
+%
+% At - Handle to a function that takes a K vector and returns an N vector.
+% If A is a KxN matrix, At is ignored.
+%
+% b - Kx1 vector of observations.
+%
+% epsilon - scalar, constraint relaxation parameter
+%
+% lbtol - The log barrier algorithm terminates when the duality gap <= lbtol.
+% Also, the number of log barrier iterations is completely
+% determined by lbtol.
+% Default = 1e-3.
+%
+% mu - Factor by which to increase the barrier constant at each iteration.
+% Default = 10.
+%
+% cgtol - Tolerance for Conjugate Gradients; ignored if A is a matrix.
+% Default = 1e-8.
+%
+% cgmaxiter - Maximum number of iterations for Conjugate Gradients; ignored
+% if A is a matrix.
+% Default = 200.
+%
+% Written by: Justin Romberg, Caltech
+% Email: jrom@acm.caltech.edu
+% Created: October 2005
+%
+
+function xp = tvdantzig_logbarrier(x0, A, At, b, epsilon, lbtol, mu, cgtol, cgmaxiter)
+
+largescale = isa(A,'function_handle');
+
+if (nargin < 6), lbtol = 1e-3; end
+if (nargin < 7), mu = 10; end
+if (nargin < 8), cgtol = 1e-8; end
+if (nargin < 9), cgmaxiter = 200; end
+
+newtontol = lbtol;
+newtonmaxiter = 50;
+
+N = length(x0);
+n = round(sqrt(N));
+
+% create (sparse) differencing matrices for TV
+Dv = spdiags([reshape([-ones(n-1,n); zeros(1,n)],N,1) ...
+ reshape([zeros(1,n); ones(n-1,n)],N,1)], [0 1], N, N);
+Dh = spdiags([reshape([-ones(n,n-1) zeros(n,1)],N,1) ...
+ reshape([zeros(n,1) ones(n,n-1)],N,1)], [0 n], N, N);
+
+if (largescale)
+ if (norm(A(x0)-b) > epsilon)
+ disp('Starting point infeasible; using x0 = At*inv(AAt)*y.');
+ AAt = @(z) A(At(z));
+ [w, cgres] = cgsolve(AAt, b, cgtol, cgmaxiter, 0);
+ if (cgres > 1/2)
+ disp('A*At is ill-conditioned: cannot find starting point');
+ xp = x0;
+ return;
+ end
+ x0 = At(w);
+ end
+else
+ if (norm(A*x0-b) > epsilon)
+ disp('Starting point infeasible; using x0 = At*inv(AAt)*y.');
+ opts.POSDEF = true; opts.SYM = true;
+ [w, hcond] = linsolve(A*A', b, opts);
+ if (hcond < 1e-14)
+ disp('A*At is ill-conditioned: cannot find starting point');
+ xp = x0;
+ return;
+ end
+ x0 = A'*w;
+ end
+end
+x = x0;
+Dhx = Dh*x; Dvx = Dv*x;
+t = 1.05*sqrt(Dhx.^2 + Dvx.^2) + .01*max(sqrt(Dhx.^2 + Dvx.^2));
+
+% choose initial value of tau so that the duality gap after the first
+% step will be about the origial TV
+tau = 3*N/sum(sqrt(Dhx.^2+Dvx.^2));
+
+lbiter = ceil((log(3*N)-log(lbtol)-log(tau))/log(mu));
+disp(sprintf('Number of log barrier iterations = %d\n', lbiter));
+totaliter = 0;
+for ii = 1:lbiter
+
+ [xp, tp, ntiter] = tvdantzig_newton(x, t, A, At, b, epsilon, tau, newtontol, newtonmaxiter, cgtol, cgmaxiter);
+ totaliter = totaliter + ntiter;
+ tvxp = sum(sqrt((Dh*xp).^2 + (Dv*xp).^2));
+
+ disp(sprintf('\nLog barrier iter = %d, TV = %.3f, functional = %8.3f, tau = %8.3e, total newton iter = %d\n', ...
+ ii, tvxp, sum(tp), tau, totaliter));
+
+ x = xp;
+ t = tp;
+
+ tau = mu*tau;
+
+end
+ \ No newline at end of file