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authorNicolas Courty <ncourty@irisa.fr>2018-09-07 11:58:42 +0200
committerNicolas Courty <ncourty@irisa.fr>2018-09-07 11:58:42 +0200
commitd99abf078537acf6cf49480b9790a9c450889031 (patch)
treec9e1138752af5ea4b33d9d46766033386098dd28
parent5180023fc49d15ad83faccc5674d5966fe9a0385 (diff)
Wasserstein convolutional barycenter
-rw-r--r--README.md4
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-rw-r--r--examples/plot_convolutional_barycenter.py92
-rw-r--r--ot/bregman.py106
7 files changed, 201 insertions, 1 deletions
diff --git a/README.md b/README.md
index dded582..1105362 100644
--- a/README.md
+++ b/README.md
@@ -227,4 +227,6 @@ You can also post bug reports and feature requests in Github issues. Make sure t
[19] Seguy, V., Bhushan Damodaran, B., Flamary, R., Courty, N., Rolet, A.& Blondel, M. [Large-scale Optimal Transport and Mapping Estimation](https://arxiv.org/pdf/1711.02283.pdf). International Conference on Learning Representation (2018)
-[20] Cuturi, M. and Doucet, A. (2014) [Fast Computation of Wasserstein Barycenters](http://proceedings.mlr.press/v32/cuturi14.html). International Conference in Machine Learning \ No newline at end of file
+[20] Cuturi, M. and Doucet, A. (2014) [Fast Computation of Wasserstein Barycenters](http://proceedings.mlr.press/v32/cuturi14.html). International Conference in Machine Learning
+
+[21] Solomon, J., De Goes, F., Peyré, G., Cuturi, M., Butscher, A., Nguyen, A. & Guibas, L. (2015). [Convolutional wasserstein distances: Efficient optimal transportation on geometric domains](https://dl.acm.org/citation.cfm?id=2766963). ACM Transactions on Graphics (TOG), 34(4), 66. \ No newline at end of file
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diff --git a/examples/plot_convolutional_barycenter.py b/examples/plot_convolutional_barycenter.py
new file mode 100644
index 0000000..d231da9
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+++ b/examples/plot_convolutional_barycenter.py
@@ -0,0 +1,92 @@
+
+#%%
+# -*- coding: utf-8 -*-
+"""
+============================================
+Convolutional Wasserstein Barycenter example
+============================================
+
+This example is designed to illustrate how the Convolutional Wasserstein Barycenter
+function of POT works.
+"""
+
+# Author: Nicolas Courty <ncourty@irisa.fr>
+#
+# License: MIT License
+
+
+import numpy as np
+import pylab as pl
+import ot
+
+##############################################################################
+# Data preparation
+# ----------------
+#
+# The four distributions are constructed from 4 simple images
+
+
+f1 = 1 - pl.imread('../data/redcross.png')[:, :, 2]
+f2 = 1 - pl.imread('../data/duck.png')[:, :, 2]
+f3 = 1 - pl.imread('../data/heart.png')[:, :, 2]
+f4 = 1 - pl.imread('../data/tooth.png')[:, :, 2]
+
+A = []
+f1=f1/np.sum(f1)
+f2=f2/np.sum(f2)
+f3=f3/np.sum(f3)
+f4=f4/np.sum(f4)
+A.append(f1)
+A.append(f2)
+A.append(f3)
+A.append(f4)
+A=np.array(A)
+
+nb_images = 5
+
+# those are the four corners coordinates that will be interpolated by bilinear
+# interpolation
+v1=np.array((1,0,0,0))
+v2=np.array((0,1,0,0))
+v3=np.array((0,0,1,0))
+v4=np.array((0,0,0,1))
+
+
+##############################################################################
+# Barycenter computation and visualization
+# ----------------------------------------
+#
+
+pl.figure(figsize=(10,10))
+pl.title('Convolutional Wasserstein Barycenters in POT')
+cm='Blues'
+# regularization parameter
+reg=0.004
+for i in range(nb_images):
+ for j in range(nb_images):
+ pl.subplot(nb_images,nb_images,i*nb_images+j+1)
+ tx=float(i)/(nb_images-1)
+ ty=float(j)/(nb_images-1)
+
+ # weights are constructed by bilinear interpolation
+ tmp1=(1-tx)*v1+tx*v2
+ tmp2=(1-tx)*v3+tx*v4
+ weights=(1-ty)*tmp1+ty*tmp2
+
+ if i==0 and j==0:
+ pl.imshow(f1,cmap=cm)
+ pl.axis('off')
+ elif i==0 and j==(nb_images-1):
+ pl.imshow(f3,cmap=cm)
+ pl.axis('off')
+ elif i==(nb_images-1) and j==0:
+ pl.imshow(f2,cmap=cm)
+ pl.axis('off')
+ elif i==(nb_images-1) and j==(nb_images-1):
+ pl.imshow(f4,cmap=cm)
+ pl.axis('off')
+ else:
+ # call to barycenter computation
+ pl.imshow(ot.convolutional_barycenter2d(A,reg,weights),cmap=cm)
+ pl.axis('off')
+pl.show() \ No newline at end of file
diff --git a/ot/bregman.py b/ot/bregman.py
index c755f51..05f4d9d 100644
--- a/ot/bregman.py
+++ b/ot/bregman.py
@@ -918,6 +918,112 @@ def barycenter(A, M, reg, weights=None, numItermax=1000,
else:
return geometricBar(weights, UKv)
+def convolutional_barycenter2d(A,reg,weights=None,numItermax = 10000, stopThr=1e-9, verbose=False, log=False):
+ """Compute the entropic regularized wasserstein barycenter of distributions A
+ where A is a collection of 2D images.
+
+ The function solves the following optimization problem:
+
+ .. math::
+ \mathbf{a} = arg\min_\mathbf{a} \sum_i W_{reg}(\mathbf{a},\mathbf{a}_i)
+
+ where :
+
+ - :math:`W_{reg}(\cdot,\cdot)` is the entropic regularized Wasserstein distance (see ot.bregman.sinkhorn)
+ - :math:`\mathbf{a}_i` are training distributions (2D images) in the mast two dimensions of matrix :math:`\mathbf{A}`
+ - reg is the regularization strength scalar value
+
+ The algorithm used for solving the problem is the Sinkhorn-Knopp matrix scaling algorithm as proposed in [21]_
+
+ Parameters
+ ----------
+ A : np.ndarray (n,w,h)
+ n distributions (2D images) of size w x h
+ reg : float
+ Regularization term >0
+ weights : np.ndarray (n,)
+ Weights of each image on the simplex (barycentric coodinates)
+ numItermax : int, optional
+ Max number of iterations
+ stopThr : float, optional
+ Stop threshol on error (>0)
+ verbose : bool, optional
+ Print information along iterations
+ log : bool, optional
+ record log if True
+
+
+ Returns
+ -------
+ a : (w,h) ndarray
+ 2D Wasserstein barycenter
+ log : dict
+ log dictionary return only if log==True in parameters
+
+
+ References
+ ----------
+
+ .. [21] Solomon, J., De Goes, F., Peyré, G., Cuturi, M., Butscher, A., Nguyen, A. & Guibas, L. (2015).
+ Convolutional wasserstein distances: Efficient optimal transportation on geometric domains
+ ACM Transactions on Graphics (TOG), 34(4), 66
+
+
+ """
+
+ if weights is None:
+ weights = np.ones(A.shape[0]) / A.shape[0]
+ else:
+ assert(len(weights) == A.shape[0])
+
+ if log:
+ log = {'err': []}
+
+ b=np.zeros_like(A[0,:,:])
+ U=np.ones_like(A)
+ KV=np.ones_like(A)
+ threshold = 1e-30 # in order to avoids numerical precision issues
+
+ cpt = 0
+ err=1
+
+ # build the convolution operator
+ t = np.linspace(0,1,A.shape[1])
+ [Y,X] = np.meshgrid(t,t)
+ xi1 = np.exp(-(X-Y)**2/reg)
+ K = lambda x: np.dot(np.dot(xi1,x),xi1)
+
+ while (err>stopThr and cpt<numItermax):
+
+ bold=b
+ cpt = cpt +1
+
+ b=np.zeros_like(A[0,:,:])
+ for r in range(A.shape[0]):
+ KV[r,:,:]=K(A[r,:,:]/np.maximum(threshold,K(U[r,:,:])))
+ b += weights[r] * np.log(np.maximum(threshold, U[r,:,:]*KV[r,:,:]))
+ b = np.exp(b)
+ for r in range(A.shape[0]):
+ U[r,:,:]=b/np.maximum(threshold,KV[r,:,:])
+
+ if cpt%10==1:
+ err=np.sum(np.abs(bold-b))
+ # log and verbose print
+ if log:
+ log['err'].append(err)
+
+ if verbose:
+ if cpt%200 ==0:
+ print('{:5s}|{:12s}'.format('It.','Err')+'\n'+'-'*19)
+ print('{:5d}|{:8e}|'.format(cpt,err))
+
+ if log:
+ log['niter']=cpt
+ log['U']=U
+ return b,log
+ else:
+ return b
+
def unmix(a, D, M, M0, h0, reg, reg0, alpha, numItermax=1000,
stopThr=1e-3, verbose=False, log=False):