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authorRémi Flamary <remi.flamary@gmail.com>2018-09-24 10:33:41 +0200
committerRémi Flamary <remi.flamary@gmail.com>2018-09-24 10:33:41 +0200
commit414331cbec21f00333e9de36a8790666c373e93c (patch)
tree5e5fab72c66d2e885c2d98bfc9567b527dfdb62e /ot/bregman.py
parent75fe96c183852971bb7be1da39af202b9f7d6e6c (diff)
parentc9b99df8fffec1dcc6802ef43b6192774817c5fb (diff)
Merge readme with master
Diffstat (limited to 'ot/bregman.py')
-rw-r--r--ot/bregman.py110
1 files changed, 110 insertions, 0 deletions
diff --git a/ot/bregman.py b/ot/bregman.py
index 1f5150a..418de57 100644
--- a/ot/bregman.py
+++ b/ot/bregman.py
@@ -1070,6 +1070,116 @@ def barycenter(A, M, reg, weights=None, numItermax=1000,
return geometricBar(weights, UKv)
+def convolutional_barycenter2d(A, reg, weights=None, numItermax=10000, stopThr=1e-9, stabThr=1e-30, 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)
+ stabThr : float, optional
+ Stabilization threshold to avoid numerical precision issue
+ 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)
+
+ 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)
+
+ def K(x):
+ return 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(stabThr, K(U[r, :, :])))
+ b += weights[r] * np.log(np.maximum(stabThr, U[r, :, :] * KV[r, :, :]))
+ b = np.exp(b)
+ for r in range(A.shape[0]):
+ U[r, :, :] = b / np.maximum(stabThr, 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):
"""