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authorNicolas Courty <Nico@pc-mna-08.univ-ubs.fr>2017-08-31 16:44:18 +0200
committerNicolas Courty <Nico@MacBook-Pro-de-Nicolas.local>2017-09-01 11:09:13 +0200
commit8c525174bb664cafa98dfff73dce9d42d7818f71 (patch)
treed353a0952f29c8cf3cb71bdd198f9acc4afa58da
parent93dee553a3dd5d6e3c5a5d325bb6333e8eb24dee (diff)
Minor corrections suggested by @agramfort + new barycenter example + test function
-rw-r--r--README.md2
-rwxr-xr-xdata/carre.pngbin0 -> 168 bytes
-rwxr-xr-xdata/coeur.pngbin0 -> 225 bytes
-rwxr-xr-xdata/rond.pngbin0 -> 230 bytes
-rwxr-xr-xdata/triangle.pngbin0 -> 254 bytes
-rw-r--r--examples/plot_gromov.py14
-rwxr-xr-xexamples/plot_gromov_barycenter.py240
-rw-r--r--ot/gromov.py36
-rw-r--r--test/test_gromov.py38
9 files changed, 302 insertions, 28 deletions
diff --git a/README.md b/README.md
index 257244b..22b20a4 100644
--- a/README.md
+++ b/README.md
@@ -185,4 +185,4 @@ You can also post bug reports and feature requests in Github issues. Make sure t
[11] Flamary, R., Cuturi, M., Courty, N., & Rakotomamonjy, A. (2016). [Wasserstein Discriminant Analysis](https://arxiv.org/pdf/1608.08063.pdf). arXiv preprint arXiv:1608.08063.
-[12] Peyré, Gabriel, Marco Cuturi, and Justin Solomon, [Gromov-Wasserstein averaging of kernel and distance matrices](http://proceedings.mlr.press/v48/peyre16.html) International Conference on Machine Learning (ICML). 2016.
+[12] Gabriel Peyré, Marco Cuturi, and Justin Solomon, [Gromov-Wasserstein averaging of kernel and distance matrices](http://proceedings.mlr.press/v48/peyre16.html) International Conference on Machine Learning (ICML). 2016.
diff --git a/data/carre.png b/data/carre.png
new file mode 100755
index 0000000..45ff0ef
--- /dev/null
+++ b/data/carre.png
Binary files differ
diff --git a/data/coeur.png b/data/coeur.png
new file mode 100755
index 0000000..3f511a6
--- /dev/null
+++ b/data/coeur.png
Binary files differ
diff --git a/data/rond.png b/data/rond.png
new file mode 100755
index 0000000..1c1a068
--- /dev/null
+++ b/data/rond.png
Binary files differ
diff --git a/data/triangle.png b/data/triangle.png
new file mode 100755
index 0000000..ca36d09
--- /dev/null
+++ b/data/triangle.png
Binary files differ
diff --git a/examples/plot_gromov.py b/examples/plot_gromov.py
index a33fde1..9bbdbde 100644
--- a/examples/plot_gromov.py
+++ b/examples/plot_gromov.py
@@ -1,8 +1,8 @@
# -*- coding: utf-8 -*-
"""
-====================
+==========================
Gromov-Wasserstein example
-====================
+==========================
This example is designed to show how to use the Gromov-Wassertsein distance
computation in POT.
"""
@@ -14,14 +14,14 @@ computation in POT.
import scipy as sp
import numpy as np
+import matplotlib.pylab as pl
import ot
-import matplotlib.pylab as pl
"""
Sample two Gaussian distributions (2D and 3D)
-====================
+=============================================
The Gromov-Wasserstein distance allows to compute distances with samples that do not belong to the same metric space.
For demonstration purpose, we sample two Gaussian distributions in 2- and 3-dimensional spaces.
"""
@@ -42,7 +42,7 @@ xt = np.random.randn(n, 3).dot(P) + mu_t
"""
Plotting the distributions
-====================
+==========================
"""
fig = pl.figure()
ax1 = fig.add_subplot(121)
@@ -54,7 +54,7 @@ pl.show()
"""
Compute distance kernels, normalize them and then display
-====================
+=========================================================
"""
C1 = sp.spatial.distance.cdist(xs, xs)
@@ -72,7 +72,7 @@ pl.show()
"""
Compute Gromov-Wasserstein plans and distance
-====================
+=============================================
"""
p = ot.unif(n)
diff --git a/examples/plot_gromov_barycenter.py b/examples/plot_gromov_barycenter.py
new file mode 100755
index 0000000..6a72b3b
--- /dev/null
+++ b/examples/plot_gromov_barycenter.py
@@ -0,0 +1,240 @@
+# -*- coding: utf-8 -*-
+"""
+=====================================
+Gromov-Wasserstein Barycenter example
+=====================================
+This example is designed to show how to use the Gromov-Wassertsein distance
+computation in POT.
+"""
+
+# Author: Erwan Vautier <erwan.vautier@gmail.com>
+# Nicolas Courty <ncourty@irisa.fr>
+#
+# License: MIT License
+
+
+import numpy as np
+import scipy as sp
+
+import scipy.ndimage as spi
+import matplotlib.pylab as pl
+from sklearn import manifold
+from sklearn.decomposition import PCA
+
+import ot
+
+"""
+
+Smacof MDS
+==========
+This function allows to find an embedding of points given a dissimilarity matrix
+that will be given by the output of the algorithm
+"""
+
+
+def smacof_mds(C, dim, maxIter=3000, eps=1e-9):
+ """
+ Returns an interpolated point cloud following the dissimilarity matrix C using SMACOF
+ multidimensional scaling (MDS) in specific dimensionned target space
+
+ Parameters
+ ----------
+ C : np.ndarray(ns,ns)
+ dissimilarity matrix
+ dim : Integer
+ dimension of the targeted space
+ maxIter : Maximum number of iterations of the SMACOF algorithm for a single run
+
+ eps : relative tolerance w.r.t stress to declare converge
+
+
+ Returns
+ -------
+ npos : R**dim ndarray
+ Embedded coordinates of the interpolated point cloud (defined with one isometry)
+
+
+ """
+
+ seed = np.random.RandomState(seed=3)
+
+ mds = manifold.MDS(
+ dim,
+ max_iter=3000,
+ eps=1e-9,
+ dissimilarity='precomputed',
+ n_init=1)
+ pos = mds.fit(C).embedding_
+
+ nmds = manifold.MDS(
+ 2,
+ max_iter=3000,
+ eps=1e-9,
+ dissimilarity="precomputed",
+ random_state=seed,
+ n_init=1)
+ npos = nmds.fit_transform(C, init=pos)
+
+ return npos
+
+
+"""
+Data preparation
+================
+The four distributions are constructed from 4 simple images
+"""
+
+
+def im2mat(I):
+ """Converts and image to matrix (one pixel per line)"""
+ return I.reshape((I.shape[0] * I.shape[1], I.shape[2]))
+
+
+carre = spi.imread('../data/carre.png').astype(np.float64) / 256
+rond = spi.imread('../data/rond.png').astype(np.float64) / 256
+triangle = spi.imread('../data/triangle.png').astype(np.float64) / 256
+fleche = spi.imread('../data/coeur.png').astype(np.float64) / 256
+
+shapes = [carre, rond, triangle, fleche]
+
+S = 4
+xs = [[] for i in range(S)]
+
+
+for nb in range(4):
+ for i in range(8):
+ for j in range(8):
+ if shapes[nb][i, j] < 0.95:
+ xs[nb].append([j, 8 - i])
+
+xs = np.array([np.array(xs[0]), np.array(xs[1]),
+ np.array(xs[2]), np.array(xs[3])])
+
+
+"""
+Barycenter computation
+======================
+The four distributions are constructed from 4 simple images
+"""
+ns = [len(xs[s]) for s in range(S)]
+N = 30
+
+"""Compute all distances matrices for the four shapes"""
+Cs = [sp.spatial.distance.cdist(xs[s], xs[s]) for s in range(S)]
+Cs = [cs / cs.max() for cs in Cs]
+
+ps = [ot.unif(ns[s]) for s in range(S)]
+p = ot.unif(N)
+
+
+lambdast = [[float(i) / 3, float(3 - i) / 3] for i in [1, 2]]
+
+Ct01 = [0 for i in range(2)]
+for i in range(2):
+ Ct01[i] = ot.gromov.gromov_barycenters(N, [Cs[0], Cs[1]], [
+ ps[0], ps[1]], p, lambdast[i], 'square_loss', 5e-4, numItermax=100, stopThr=1e-3)
+
+Ct02 = [0 for i in range(2)]
+for i in range(2):
+ Ct02[i] = ot.gromov.gromov_barycenters(N, [Cs[0], Cs[2]], [
+ ps[0], ps[2]], p, lambdast[i], 'square_loss', 5e-4, numItermax=100, stopThr=1e-3)
+
+Ct13 = [0 for i in range(2)]
+for i in range(2):
+ Ct13[i] = ot.gromov.gromov_barycenters(N, [Cs[1], Cs[3]], [
+ ps[1], ps[3]], p, lambdast[i], 'square_loss', 5e-4, numItermax=100, stopThr=1e-3)
+
+Ct23 = [0 for i in range(2)]
+for i in range(2):
+ Ct23[i] = ot.gromov.gromov_barycenters(N, [Cs[2], Cs[3]], [
+ ps[2], ps[3]], p, lambdast[i], 'square_loss', 5e-4, numItermax=100, stopThr=1e-3)
+
+"""
+Visualization
+=============
+"""
+
+"""The PCA helps in getting consistency between the rotations"""
+
+clf = PCA(n_components=2)
+npos = [0, 0, 0, 0]
+npos = [smacof_mds(Cs[s], 2) for s in range(S)]
+
+npost01 = [0, 0]
+npost01 = [smacof_mds(Ct01[s], 2) for s in range(2)]
+npost01 = [clf.fit_transform(npost01[s]) for s in range(2)]
+
+npost02 = [0, 0]
+npost02 = [smacof_mds(Ct02[s], 2) for s in range(2)]
+npost02 = [clf.fit_transform(npost02[s]) for s in range(2)]
+
+npost13 = [0, 0]
+npost13 = [smacof_mds(Ct13[s], 2) for s in range(2)]
+npost13 = [clf.fit_transform(npost13[s]) for s in range(2)]
+
+npost23 = [0, 0]
+npost23 = [smacof_mds(Ct23[s], 2) for s in range(2)]
+npost23 = [clf.fit_transform(npost23[s]) for s in range(2)]
+
+
+fig = pl.figure(figsize=(10, 10))
+
+ax1 = pl.subplot2grid((4, 4), (0, 0))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax1.scatter(npos[0][:, 0], npos[0][:, 1], color='r')
+
+ax2 = pl.subplot2grid((4, 4), (0, 1))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax2.scatter(npost01[1][:, 0], npost01[1][:, 1], color='b')
+
+ax3 = pl.subplot2grid((4, 4), (0, 2))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax3.scatter(npost01[0][:, 0], npost01[0][:, 1], color='b')
+
+ax4 = pl.subplot2grid((4, 4), (0, 3))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax4.scatter(npos[1][:, 0], npos[1][:, 1], color='r')
+
+ax5 = pl.subplot2grid((4, 4), (1, 0))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax5.scatter(npost02[1][:, 0], npost02[1][:, 1], color='b')
+
+ax6 = pl.subplot2grid((4, 4), (1, 3))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax6.scatter(npost13[1][:, 0], npost13[1][:, 1], color='b')
+
+ax7 = pl.subplot2grid((4, 4), (2, 0))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax7.scatter(npost02[0][:, 0], npost02[0][:, 1], color='b')
+
+ax8 = pl.subplot2grid((4, 4), (2, 3))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax8.scatter(npost13[0][:, 0], npost13[0][:, 1], color='b')
+
+ax9 = pl.subplot2grid((4, 4), (3, 0))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax9.scatter(npos[2][:, 0], npos[2][:, 1], color='r')
+
+ax10 = pl.subplot2grid((4, 4), (3, 1))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax10.scatter(npost23[1][:, 0], npost23[1][:, 1], color='b')
+
+ax11 = pl.subplot2grid((4, 4), (3, 2))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax11.scatter(npost23[0][:, 0], npost23[0][:, 1], color='b')
+
+ax12 = pl.subplot2grid((4, 4), (3, 3))
+pl.xlim((-1, 1))
+pl.ylim((-1, 1))
+ax12.scatter(npos[3][:, 0], npos[3][:, 1], color='r')
diff --git a/ot/gromov.py b/ot/gromov.py
index 7cf3b42..421ed3f 100644
--- a/ot/gromov.py
+++ b/ot/gromov.py
@@ -23,7 +23,7 @@ def square_loss(a, b):
Returns the value of L(a,b)=(1/2)*|a-b|^2
"""
- return (1 / 2) * (a - b)**2
+ return 0.5 * (a - b)**2
def kl_loss(a, b):
@@ -54,9 +54,9 @@ def tensor_square_loss(C1, C2, T):
Parameters
----------
- C1 : np.ndarray(ns,ns)
+ C1 : ndarray, shape (ns, ns)
Metric cost matrix in the source space
- C2 : np.ndarray(nt,nt)
+ C2 : ndarray, shape (nt, nt)
Metric costfr matrix in the target space
T : np.ndarray(ns,nt)
Coupling between source and target spaces
@@ -87,7 +87,7 @@ def tensor_square_loss(C1, C2, T):
return b
tens = -np.dot(h1(C1), T).dot(h2(C2).T)
- tens = tens - tens.min()
+ tens -= tens.min()
return np.array(tens)
@@ -112,9 +112,9 @@ def tensor_kl_loss(C1, C2, T):
Parameters
----------
- C1 : np.ndarray(ns,ns)
+ C1 : ndarray, shape (ns, ns)
Metric cost matrix in the source space
- C2 : np.ndarray(nt,nt)
+ C2 : ndarray, shape (nt, nt)
Metric costfr matrix in the target space
T : np.ndarray(ns,nt)
Coupling between source and target spaces
@@ -149,7 +149,7 @@ def tensor_kl_loss(C1, C2, T):
return np.log(b + 1e-15)
tens = -np.dot(h1(C1), T).dot(h2(C2).T)
- tens = tens - tens.min()
+ tens -= tens.min()
return np.array(tens)
@@ -175,9 +175,8 @@ def update_square_loss(p, lambdas, T, Cs):
"""
- tmpsum = np.sum([lambdas[s] * np.dot(T[s].T, Cs[s]).dot(T[s])
- for s in range(len(T))])
- ppt = np.dot(p, p.T)
+ tmpsum = sum([lambdas[s] * np.dot(T[s].T, Cs[s]).dot(T[s]) for s in range(len(T))])
+ ppt = np.outer(p, p)
return(np.divide(tmpsum, ppt))
@@ -203,9 +202,8 @@ def update_kl_loss(p, lambdas, T, Cs):
"""
- tmpsum = np.sum([lambdas[s] * np.dot(T[s].T, Cs[s]).dot(T[s])
- for s in range(len(T))])
- ppt = np.dot(p, p.T)
+ tmpsum = sum([lambdas[s] * np.dot(T[s].T, Cs[s]).dot(T[s]) for s in range(len(T))])
+ ppt = np.outer(p, p)
return(np.exp(np.divide(tmpsum, ppt)))
@@ -239,9 +237,9 @@ def gromov_wasserstein(C1, C2, p, q, loss_fun, epsilon, numItermax=1000, stopThr
Parameters
----------
- C1 : np.ndarray(ns,ns)
+ C1 : ndarray, shape (ns, ns)
Metric cost matrix in the source space
- C2 : np.ndarray(nt,nt)
+ C2 : ndarray, shape (nt, nt)
Metric costfr matrix in the target space
p : np.ndarray(ns,)
distribution in the source space
@@ -271,7 +269,7 @@ def gromov_wasserstein(C1, C2, p, q, loss_fun, epsilon, numItermax=1000, stopThr
C1 = np.asarray(C1, dtype=np.float64)
C2 = np.asarray(C2, dtype=np.float64)
- T = np.dot(p, q.T) # Initialization
+ T = np.outer(p, q) # Initialization
cpt = 0
err = 1
@@ -333,9 +331,9 @@ def gromov_wasserstein2(C1, C2, p, q, loss_fun, epsilon, numItermax=1000, stopTh
Parameters
----------
- C1 : np.ndarray(ns,ns)
+ C1 : ndarray, shape (ns, ns)
Metric cost matrix in the source space
- C2 : np.ndarray(nt,nt)
+ C2 : ndarray, shape (nt, nt)
Metric costfr matrix in the target space
p : np.ndarray(ns,)
distribution in the source space
@@ -434,8 +432,6 @@ def gromov_barycenters(N, Cs, ps, p, lambdas, loss_fun, epsilon, numItermax=1000
Cs = [np.asarray(Cs[s], dtype=np.float64) for s in range(S)]
lambdas = np.asarray(lambdas, dtype=np.float64)
- T = [0 for s in range(S)]
-
# Initialization of C : random SPD matrix
xalea = np.random.randn(N, 2)
C = dist(xalea, xalea)
diff --git a/test/test_gromov.py b/test/test_gromov.py
new file mode 100644
index 0000000..75eeaab
--- /dev/null
+++ b/test/test_gromov.py
@@ -0,0 +1,38 @@
+"""Tests for module gromov """
+
+# Author: Erwan Vautier <erwan.vautier@gmail.com>
+# Nicolas Courty <ncourty@irisa.fr>
+#
+# License: MIT License
+
+import numpy as np
+import ot
+
+
+def test_gromov():
+ n = 50 # nb samples
+
+ mu_s = np.array([0, 0])
+ cov_s = np.array([[1, 0], [0, 1]])
+
+ xs = ot.datasets.get_2D_samples_gauss(n, mu_s, cov_s)
+
+ xt = [xs[n - (i + 1)] for i in range(n)]
+ xt = np.array(xt)
+
+ p = ot.unif(n)
+ q = ot.unif(n)
+
+ C1 = ot.dist(xs, xs)
+ C2 = ot.dist(xt, xt)
+
+ C1 /= C1.max()
+ C2 /= C2.max()
+
+ G = ot.gromov_wasserstein(C1, C2, p, q, 'square_loss', epsilon=5e-4)
+
+ # check constratints
+ np.testing.assert_allclose(
+ p, G.sum(1), atol=1e-04) # cf convergence gromov
+ np.testing.assert_allclose(
+ q, G.sum(0), atol=1e-04) # cf convergence gromov