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N. Papadakis, G. Peyré, E. Oudet. Optimal Transport with Proximal Splitting. SIAM Journal on Imaging Sciences, 7(1), pp. 212–238, 2014.

Home Page: https://hal.archives-ouvertes.fr/hal-00816211

MATLAB 22.21% TeX 77.79%

2013-siims-ot-splitting's Introduction

This Matlab package contains the source code to reproduce the figure of the article:

N. Papadakis, G. Peyré, E. Oudet. Optimal Transport with Proximal Splitting. SIAM Journal on Imaging Sciences, 7(1), pp. 212–238, 2014.

Example of OT interpolation

Copyright (c) 2009 Gabriel Peyré

============= Description

This archive contains the Douglas-Rachford (DR) and Primal-Dual (PD) solvers applied to the Benamou-Brenier (BB) problem discretized on a staggered grid.

They can be tested with:

  • test_bb_dr.m: DR algorithm.
  • test_bb_pd.m: DR algorithm.

============= Principal options

The principal options are the following:

  1. chose your test case with

test = 'gaussian';

(you can create your own scenario by defining f0 and f1 the initial and final densities)

  1. chose the dimension of the problem:

N=32; P=32; Q=32;

(N and P are the discrete spatial dimensions and Q is the temporal discretization)

  1. Parameterization of the solver:

For DR:

mu = 1.98; % should be in ]0,2[ gamma = 1./230.; % should be >0 niter = 1000;

For PD:

sigma=85; niter = 1000; % (increase the maximum number of iteration to have better results)

  1. Generalized cost functions:

Minimize \sum_k w_k f_k^\alpha |v_k|^2

alpha= 1; % should be in [0;1];

alpha=1 computes the L2-Wasserstein distance, 0 is for the H^-1 one and intermediate values gives interpolations between the norms

obstacle=zeros(N,P,Q);

Define the points of the 3D volume where the mass can not pass. For instance, setting

obstacle(N/2,P/2,:)=1;

will create an obstacle in the middle of the spatial domain.

============= Exemples of settings:

test = 'gaussian'; N=32; P=32; Q=32;
niter = 200;

test = 'obstacle'; niter = 2000;

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