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# -*- coding: utf-8 -*-
"""
Gromov-Wasserstein and Fused-Gromov-Wasserstein conditional gradient solvers.
"""

# Author: Erwan Vautier <erwan.vautier@gmail.com>
#         Nicolas Courty <ncourty@irisa.fr>
#         Rémi Flamary <remi.flamary@unice.fr>
#         Titouan Vayer <titouan.vayer@irisa.fr>
#         Cédric Vincent-Cuaz <cedvincentcuaz@gmail.com>
#
# License: MIT License

import numpy as np


from ..utils import dist, UndefinedParameter, list_to_array
from ..optim import cg, line_search_armijo, solve_1d_linesearch_quad
from ..utils import check_random_state, unif
from ..backend import get_backend, NumpyBackend

from ._utils import init_matrix, gwloss, gwggrad
from ._utils import update_square_loss, update_kl_loss, update_feature_matrix


def gromov_wasserstein(C1, C2, p=None, q=None, loss_fun='square_loss', symmetric=None, log=False, armijo=False, G0=None,
                       max_iter=1e4, tol_rel=1e-9, tol_abs=1e-9, **kwargs):
    r"""
    Returns the Gromov-Wasserstein transport between :math:`(\mathbf{C_1}, \mathbf{p})` and :math:`(\mathbf{C_2}, \mathbf{q})`

    The function solves the following optimization problem:

    .. math::
        \mathbf{T}^* \in \mathop{\arg \min}_\mathbf{T} \quad \sum_{i,j,k,l}
        L(\mathbf{C_1}_{i,k}, \mathbf{C_2}_{j,l}) \mathbf{T}_{i,j} \mathbf{T}_{k,l}

        s.t. \ \mathbf{\gamma} \mathbf{1} &= \mathbf{p}

             \mathbf{\gamma}^T \mathbf{1} &= \mathbf{q}

             \mathbf{\gamma} &\geq 0

    Where :

    - :math:`\mathbf{C_1}`: Metric cost matrix in the source space
    - :math:`\mathbf{C_2}`: Metric cost matrix in the target space
    - :math:`\mathbf{p}`: distribution in the source space
    - :math:`\mathbf{q}`: distribution in the target space
    - `L`: loss function to account for the misfit between the similarity matrices

    .. note:: This function is backend-compatible and will work on arrays
        from all compatible backends. But the algorithm uses the C++ CPU backend
        which can lead to copy overhead on GPU arrays.
    .. note:: All computations in the conjugate gradient solver are done with
        numpy to limit memory overhead.

    Parameters
    ----------
    C1 : array-like, shape (ns, ns)
        Metric cost matrix in the source space
    C2 : array-like, shape (nt, nt)
        Metric cost matrix in the target space
    p : array-like, shape (ns,), optional
        Distribution in the source space.
        If let to its default value None, uniform distribution is taken.
    q : array-like, shape (nt,), optional
        Distribution in the target space.
        If let to its default value None, uniform distribution is taken.
    loss_fun : str, optional
        loss function used for the solver either 'square_loss' or 'kl_loss'
    symmetric : bool, optional
        Either C1 and C2 are to be assumed symmetric or not.
        If let to its default None value, a symmetry test will be conducted.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    verbose : bool, optional
        Print information along iterations
    log : bool, optional
        record log if True
    armijo : bool, optional
        If True the step of the line-search is found via an armijo research. Else closed form is used.
        If there are convergence issues use False.
    G0: array-like, shape (ns,nt), optional
        If None the initial transport plan of the solver is pq^T.
        Otherwise G0 must satisfy marginal constraints and will be used as initial transport of the solver.
    max_iter : int, optional
        Max number of iterations
    tol_rel : float, optional
        Stop threshold on relative error (>0)
    tol_abs : float, optional
        Stop threshold on absolute error (>0)
    **kwargs : dict
        parameters can be directly passed to the ot.optim.cg solver

    Returns
    -------
    T : array-like, shape (`ns`, `nt`)
        Coupling between the two spaces that minimizes:

            :math:`\sum_{i,j,k,l} L(\mathbf{C_1}_{i,k}, \mathbf{C_2}_{j,l}) \mathbf{T}_{i,j} \mathbf{T}_{k,l}`
    log : dict
        Convergence information and loss.

    References
    ----------
    .. [12] Gabriel Peyré, Marco Cuturi, and Justin Solomon,
        "Gromov-Wasserstein averaging of kernel and distance matrices."
        International Conference on Machine Learning (ICML). 2016.

    .. [13] Mémoli, Facundo. Gromov–Wasserstein distances and the
        metric approach to object matching. Foundations of computational
        mathematics 11.4 (2011): 417-487.

    .. [47] Chowdhury, S., & Mémoli, F. (2019). The gromov–wasserstein
        distance between networks and stable network invariants.
        Information and Inference: A Journal of the IMA, 8(4), 757-787.
    """
    arr = [C1, C2]
    if p is not None:
        arr.append(list_to_array(p))
    else:
        p = unif(C1.shape[0], type_as=C1)
    if q is not None:
        arr.append(list_to_array(q))
    else:
        q = unif(C2.shape[0], type_as=C2)
    if G0 is not None:
        G0_ = G0
        arr.append(G0)

    nx = get_backend(*arr)
    p0, q0, C10, C20 = p, q, C1, C2

    p = nx.to_numpy(p0)
    q = nx.to_numpy(q0)
    C1 = nx.to_numpy(C10)
    C2 = nx.to_numpy(C20)
    if symmetric is None:
        symmetric = np.allclose(C1, C1.T, atol=1e-10) and np.allclose(C2, C2.T, atol=1e-10)

    if G0 is None:
        G0 = p[:, None] * q[None, :]
    else:
        G0 = nx.to_numpy(G0_)
        # Check marginals of G0
        np.testing.assert_allclose(G0.sum(axis=1), p, atol=1e-08)
        np.testing.assert_allclose(G0.sum(axis=0), q, atol=1e-08)
    # cg for GW is implemented using numpy on CPU
    np_ = NumpyBackend()

    constC, hC1, hC2 = init_matrix(C1, C2, p, q, loss_fun, np_)

    def f(G):
        return gwloss(constC, hC1, hC2, G, np_)

    if symmetric:
        def df(G):
            return gwggrad(constC, hC1, hC2, G, np_)
    else:
        constCt, hC1t, hC2t = init_matrix(C1.T, C2.T, p, q, loss_fun, np_)

        def df(G):
            return 0.5 * (gwggrad(constC, hC1, hC2, G, np_) + gwggrad(constCt, hC1t, hC2t, G, np_))
    if loss_fun == 'kl_loss':
        armijo = True  # there is no closed form line-search with KL

    if armijo:
        def line_search(cost, G, deltaG, Mi, cost_G, **kwargs):
            return line_search_armijo(cost, G, deltaG, Mi, cost_G, nx=np_, **kwargs)
    else:
        def line_search(cost, G, deltaG, Mi, cost_G, **kwargs):
            return solve_gromov_linesearch(G, deltaG, cost_G, C1, C2, M=0., reg=1., nx=np_, **kwargs)
    if log:
        res, log = cg(p, q, 0., 1., f, df, G0, line_search, log=True, numItermax=max_iter, stopThr=tol_rel, stopThr2=tol_abs, **kwargs)
        log['gw_dist'] = nx.from_numpy(log['loss'][-1], type_as=C10)
        log['u'] = nx.from_numpy(log['u'], type_as=C10)
        log['v'] = nx.from_numpy(log['v'], type_as=C10)
        return nx.from_numpy(res, type_as=C10), log
    else:
        return nx.from_numpy(cg(p, q, 0., 1., f, df, G0, line_search, log=False, numItermax=max_iter, stopThr=tol_rel, stopThr2=tol_abs, **kwargs), type_as=C10)


def gromov_wasserstein2(C1, C2, p=None, q=None, loss_fun='square_loss', symmetric=None, log=False, armijo=False, G0=None,
                        max_iter=1e4, tol_rel=1e-9, tol_abs=1e-9, **kwargs):
    r"""
    Returns the Gromov-Wasserstein discrepancy between :math:`(\mathbf{C_1}, \mathbf{p})` and :math:`(\mathbf{C_2}, \mathbf{q})`

    The function solves the following optimization problem:

    .. math::
        \mathbf{GW} = \min_\mathbf{T} \quad \sum_{i,j,k,l}
        L(\mathbf{C_1}_{i,k}, \mathbf{C_2}_{j,l}) \mathbf{T}_{i,j} \mathbf{T}_{k,l}

        s.t. \ \mathbf{\gamma} \mathbf{1} &= \mathbf{p}

             \mathbf{\gamma}^T \mathbf{1} &= \mathbf{q}

             \mathbf{\gamma} &\geq 0

    Where :

    - :math:`\mathbf{C_1}`: Metric cost matrix in the source space
    - :math:`\mathbf{C_2}`: Metric cost matrix in the target space
    - :math:`\mathbf{p}`: distribution in the source space
    - :math:`\mathbf{q}`: distribution in the target space
    - `L`: loss function to account for the misfit between the similarity
      matrices

    Note that when using backends, this loss function is differentiable wrt the
    matrices (C1, C2) and weights (p, q) for quadratic loss using the gradients from [38]_.

    .. note:: This function is backend-compatible and will work on arrays
        from all compatible backends. But the algorithm uses the C++ CPU backend
        which can lead to copy overhead on GPU arrays.
    .. note:: All computations in the conjugate gradient solver are done with
        numpy to limit memory overhead.

    Parameters
    ----------
    C1 : array-like, shape (ns, ns)
        Metric cost matrix in the source space
    C2 : array-like, shape (nt, nt)
        Metric cost matrix in the target space
    p : array-like, shape (ns,), optional
        Distribution in the source space.
        If let to its default value None, uniform distribution is taken.
    q : array-like, shape (nt,), optional
        Distribution in the target space.
        If let to its default value None, uniform distribution is taken.
    loss_fun :  str
        loss function used for the solver either 'square_loss' or 'kl_loss'
    symmetric : bool, optional
        Either C1 and C2 are to be assumed symmetric or not.
        If let to its default None value, a symmetry test will be conducted.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    verbose : bool, optional
        Print information along iterations
    log : bool, optional
        record log if True
    armijo : bool, optional
        If True the step of the line-search is found via an armijo research. Else closed form is used.
        If there are convergence issues use False.
    G0: array-like, shape (ns,nt), optional
        If None the initial transport plan of the solver is pq^T.
        Otherwise G0 must satisfy marginal constraints and will be used as initial transport of the solver.
    max_iter : int, optional
        Max number of iterations
    tol_rel : float, optional
        Stop threshold on relative error (>0)
    tol_abs : float, optional
        Stop threshold on absolute error (>0)
    **kwargs : dict
        parameters can be directly passed to the ot.optim.cg solver

    Returns
    -------
    gw_dist : float
        Gromov-Wasserstein distance
    log : dict
        convergence information and Coupling matrix

    References
    ----------
    .. [12] Gabriel Peyré, Marco Cuturi, and Justin Solomon,
        "Gromov-Wasserstein averaging of kernel and distance matrices."
        International Conference on Machine Learning (ICML). 2016.

    .. [13] Mémoli, Facundo. Gromov–Wasserstein distances and the
        metric approach to object matching. Foundations of computational
        mathematics 11.4 (2011): 417-487.

    .. [38] C. Vincent-Cuaz, T. Vayer, R. Flamary, M. Corneli, N. Courty, Online
        Graph Dictionary Learning, International Conference on Machine Learning
        (ICML), 2021.

    .. [47] Chowdhury, S., & Mémoli, F. (2019). The gromov–wasserstein
        distance between networks and stable network invariants.
        Information and Inference: A Journal of the IMA, 8(4), 757-787.
    """
    # simple get_backend as the full one will be handled in gromov_wasserstein
    nx = get_backend(C1, C2)

    # init marginals if set as None
    if p is None:
        p = unif(C1.shape[0], type_as=C1)
    if q is None:
        q = unif(C2.shape[0], type_as=C2)

    T, log_gw = gromov_wasserstein(
        C1, C2, p, q, loss_fun, symmetric, log=True, armijo=armijo, G0=G0,
        max_iter=max_iter, tol_rel=tol_rel, tol_abs=tol_abs, **kwargs)

    log_gw['T'] = T
    gw = log_gw['gw_dist']

    if loss_fun == 'square_loss':
        gC1 = 2 * C1 * nx.outer(p, p) - 2 * nx.dot(T, nx.dot(C2, T.T))
        gC2 = 2 * C2 * nx.outer(q, q) - 2 * nx.dot(T.T, nx.dot(C1, T))
        gw = nx.set_gradients(gw, (p, q, C1, C2),
                              (log_gw['u'] - nx.mean(log_gw['u']),
                               log_gw['v'] - nx.mean(log_gw['v']), gC1, gC2))

    if log:
        return gw, log_gw
    else:
        return gw


def fused_gromov_wasserstein(M, C1, C2, p=None, q=None, loss_fun='square_loss', symmetric=None, alpha=0.5,
                             armijo=False, G0=None, log=False, max_iter=1e4, tol_rel=1e-9, tol_abs=1e-9, **kwargs):
    r"""
    Computes the FGW transport between two graphs (see :ref:`[24] <references-fused-gromov-wasserstein>`)

    .. math::
        \mathbf{T}^* \in \mathop{\arg \min}_\mathbf{T}  \quad (1 - \alpha) \langle \mathbf{T}, \mathbf{M} \rangle_F +
        \alpha \sum_{i,j,k,l} L(\mathbf{C_1}_{i,k}, \mathbf{C_2}_{j,l}) \mathbf{T}_{i,j} \mathbf{T}_{k,l}

        s.t. \ \mathbf{T} \mathbf{1} &= \mathbf{p}

             \mathbf{T}^T \mathbf{1} &= \mathbf{q}

             \mathbf{T} &\geq 0

    where :

    - :math:`\mathbf{M}` is the (`ns`, `nt`) metric cost matrix
    - :math:`\mathbf{p}` and :math:`\mathbf{q}` are source and target weights (sum to 1)
    - `L` is a loss function to account for the misfit between the similarity matrices

    .. note:: This function is backend-compatible and will work on arrays
        from all compatible backends. But the algorithm uses the C++ CPU backend
        which can lead to copy overhead on GPU arrays.
    .. note:: All computations in the conjugate gradient solver are done with
        numpy to limit memory overhead.

    The algorithm used for solving the problem is conditional gradient as discussed in :ref:`[24] <references-fused-gromov-wasserstein>`

    Parameters
    ----------
    M : array-like, shape (ns, nt)
        Metric cost matrix between features across domains
    C1 : array-like, shape (ns, ns)
        Metric cost matrix representative of the structure in the source space
    C2 : array-like, shape (nt, nt)
        Metric cost matrix representative of the structure in the target space
    p : array-like, shape (ns,), optional
        Distribution in the source space.
        If let to its default value None, uniform distribution is taken.
    q : array-like, shape (nt,), optional
        Distribution in the target space.
        If let to its default value None, uniform distribution is taken.
    loss_fun : str, optional
        Loss function used for the solver
    symmetric : bool, optional
        Either C1 and C2 are to be assumed symmetric or not.
        If let to its default None value, a symmetry test will be conducted.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    alpha : float, optional
        Trade-off parameter (0 < alpha < 1)
    armijo : bool, optional
        If True the step of the line-search is found via an armijo research. Else closed form is used.
        If there are convergence issues use False.
    G0: array-like, shape (ns,nt), optional
        If None the initial transport plan of the solver is pq^T.
        Otherwise G0 must satisfy marginal constraints and will be used as initial transport of the solver.
    log : bool, optional
        record log if True
    max_iter : int, optional
        Max number of iterations
    tol_rel : float, optional
        Stop threshold on relative error (>0)
    tol_abs : float, optional
        Stop threshold on absolute error (>0)
    **kwargs : dict
        parameters can be directly passed to the ot.optim.cg solver

    Returns
    -------
    T : array-like, shape (`ns`, `nt`)
        Optimal transportation matrix for the given parameters.
    log : dict
        Log dictionary return only if log==True in parameters.


    .. _references-fused-gromov-wasserstein:
    References
    ----------
    .. [24] Vayer Titouan, Chapel Laetitia, Flamary Rémi, Tavenard Romain
        and Courty Nicolas "Optimal Transport for structured data with
        application on graphs", International Conference on Machine Learning
        (ICML). 2019.

    .. [47] Chowdhury, S., & Mémoli, F. (2019). The gromov–wasserstein
        distance between networks and stable network invariants.
        Information and Inference: A Journal of the IMA, 8(4), 757-787.
    """
    arr = [C1, C2, M]
    if p is not None:
        arr.append(list_to_array(p))
    else:
        p = unif(C1.shape[0], type_as=C1)
    if q is not None:
        arr.append(list_to_array(q))
    else:
        q = unif(C2.shape[0], type_as=C2)
    if G0 is not None:
        G0_ = G0
        arr.append(G0)

    nx = get_backend(*arr)
    p0, q0, C10, C20, M0, alpha0 = p, q, C1, C2, M, alpha

    p = nx.to_numpy(p0)
    q = nx.to_numpy(q0)
    C1 = nx.to_numpy(C10)
    C2 = nx.to_numpy(C20)
    M = nx.to_numpy(M0)
    alpha = nx.to_numpy(alpha0)

    if symmetric is None:
        symmetric = np.allclose(C1, C1.T, atol=1e-10) and np.allclose(C2, C2.T, atol=1e-10)

    if G0 is None:
        G0 = p[:, None] * q[None, :]
    else:
        G0 = nx.to_numpy(G0_)
        # Check marginals of G0
        np.testing.assert_allclose(G0.sum(axis=1), p, atol=1e-08)
        np.testing.assert_allclose(G0.sum(axis=0), q, atol=1e-08)
    # cg for GW is implemented using numpy on CPU
    np_ = NumpyBackend()

    constC, hC1, hC2 = init_matrix(C1, C2, p, q, loss_fun, np_)

    def f(G):
        return gwloss(constC, hC1, hC2, G, np_)

    if symmetric:
        def df(G):
            return gwggrad(constC, hC1, hC2, G, np_)
    else:
        constCt, hC1t, hC2t = init_matrix(C1.T, C2.T, p, q, loss_fun, np_)

        def df(G):
            return 0.5 * (gwggrad(constC, hC1, hC2, G, np_) + gwggrad(constCt, hC1t, hC2t, G, np_))

    if loss_fun == 'kl_loss':
        armijo = True  # there is no closed form line-search with KL

    if armijo:
        def line_search(cost, G, deltaG, Mi, cost_G, **kwargs):
            return line_search_armijo(cost, G, deltaG, Mi, cost_G, nx=np_, **kwargs)
    else:
        def line_search(cost, G, deltaG, Mi, cost_G, **kwargs):
            return solve_gromov_linesearch(G, deltaG, cost_G, C1, C2, M=(1 - alpha) * M, reg=alpha, nx=np_, **kwargs)
    if log:
        res, log = cg(p, q, (1 - alpha) * M, alpha, f, df, G0, line_search, log=True, numItermax=max_iter, stopThr=tol_rel, stopThr2=tol_abs, **kwargs)
        log['fgw_dist'] = nx.from_numpy(log['loss'][-1], type_as=C10)
        log['u'] = nx.from_numpy(log['u'], type_as=C10)
        log['v'] = nx.from_numpy(log['v'], type_as=C10)
        return nx.from_numpy(res, type_as=C10), log
    else:
        return nx.from_numpy(cg(p, q, (1 - alpha) * M, alpha, f, df, G0, line_search, log=False, numItermax=max_iter, stopThr=tol_rel, stopThr2=tol_abs, **kwargs), type_as=C10)


def fused_gromov_wasserstein2(M, C1, C2, p=None, q=None, loss_fun='square_loss', symmetric=None, alpha=0.5,
                              armijo=False, G0=None, log=False, max_iter=1e4, tol_rel=1e-9, tol_abs=1e-9, **kwargs):
    r"""
    Computes the FGW distance between two graphs see (see :ref:`[24] <references-fused-gromov-wasserstein2>`)

    .. math::
        \mathbf{GW} = \min_\mathbf{T} \quad (1 - \alpha) \langle \mathbf(T), \mathbf{M} \rangle_F + \alpha \sum_{i,j,k,l}
        L(\mathbf{C_1}_{i,k}, \mathbf{C_2}_{j,l}) \mathbf{T}_{i,j} \mathbf{T}_{k,l}

        s.t. \ \mathbf(T)\mathbf{1} &= \mathbf{p}

             \mathbf(T)^T \mathbf{1} &= \mathbf{q}

             \mathbf(T) &\geq 0

    where :

    - :math:`\mathbf{M}` is the (`ns`, `nt`) metric cost matrix
    - :math:`\mathbf{p}` and :math:`\mathbf{q}` are source and target weights (sum to 1)
    - `L` is a loss function to account for the misfit between the similarity matrices

    The algorithm used for solving the problem is conditional gradient as
    discussed in :ref:`[24] <references-fused-gromov-wasserstein2>`

    .. note:: This function is backend-compatible and will work on arrays
        from all compatible backends. But the algorithm uses the C++ CPU backend
        which can lead to copy overhead on GPU arrays.
    .. note:: All computations in the conjugate gradient solver are done with
        numpy to limit memory overhead.

    Note that when using backends, this loss function is differentiable wrt the
    matrices (C1, C2, M) and weights (p, q) for quadratic loss using the gradients from [38]_.

    Parameters
    ----------
    M : array-like, shape (ns, nt)
        Metric cost matrix between features across domains
    C1 : array-like, shape (ns, ns)
        Metric cost matrix representative of the structure in the source space.
    C2 : array-like, shape (nt, nt)
        Metric cost matrix representative of the structure in the target space.
    p : array-like, shape (ns,), optional
        Distribution in the source space.
        If let to its default value None, uniform distribution is taken.
    q : array-like, shape (nt,), optional
        Distribution in the target space.
        If let to its default value None, uniform distribution is taken.
    loss_fun : str, optional
        Loss function used for the solver.
    symmetric : bool, optional
        Either C1 and C2 are to be assumed symmetric or not.
        If let to its default None value, a symmetry test will be conducted.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    alpha : float, optional
        Trade-off parameter (0 < alpha < 1)
    armijo : bool, optional
        If True the step of the line-search is found via an armijo research.
        Else closed form is used. If there are convergence issues use False.
    G0: array-like, shape (ns,nt), optional
        If None the initial transport plan of the solver is pq^T.
        Otherwise G0 must satisfy marginal constraints and will be used as initial transport of the solver.
    log : bool, optional
        Record log if True.
    max_iter : int, optional
        Max number of iterations
    tol_rel : float, optional
        Stop threshold on relative error (>0)
    tol_abs : float, optional
        Stop threshold on absolute error (>0)
    **kwargs : dict
        Parameters can be directly passed to the ot.optim.cg solver.

    Returns
    -------
    fgw-distance : float
        Fused Gromov-Wasserstein distance for the given parameters.
    log : dict
        Log dictionary return only if log==True in parameters.


    .. _references-fused-gromov-wasserstein2:
    References
    ----------
    .. [24] Vayer Titouan, Chapel Laetitia, Flamary Rémi, Tavenard Romain
        and Courty Nicolas
        "Optimal Transport for structured data with application on graphs"
        International Conference on Machine Learning (ICML). 2019.

    .. [38] C. Vincent-Cuaz, T. Vayer, R. Flamary, M. Corneli, N. Courty, Online
        Graph Dictionary Learning, International Conference on Machine Learning
        (ICML), 2021.

    .. [47] Chowdhury, S., & Mémoli, F. (2019). The gromov–wasserstein
        distance between networks and stable network invariants.
        Information and Inference: A Journal of the IMA, 8(4), 757-787.
    """
    nx = get_backend(C1, C2, M)

    # init marginals if set as None
    if p is None:
        p = unif(C1.shape[0], type_as=C1)
    if q is None:
        q = unif(C2.shape[0], type_as=C2)

    T, log_fgw = fused_gromov_wasserstein(
        M, C1, C2, p, q, loss_fun, symmetric, alpha, armijo, G0, log=True,
        max_iter=max_iter, tol_rel=tol_rel, tol_abs=tol_abs, **kwargs)

    fgw_dist = log_fgw['fgw_dist']
    log_fgw['T'] = T

    if loss_fun == 'square_loss':
        gC1 = 2 * C1 * nx.outer(p, p) - 2 * nx.dot(T, nx.dot(C2, T.T))
        gC2 = 2 * C2 * nx.outer(q, q) - 2 * nx.dot(T.T, nx.dot(C1, T))
        if isinstance(alpha, int) or isinstance(alpha, float):
            fgw_dist = nx.set_gradients(fgw_dist, (p, q, C1, C2, M),
                                        (log_fgw['u'] - nx.mean(log_fgw['u']),
                                         log_fgw['v'] - nx.mean(log_fgw['v']),
                                         alpha * gC1, alpha * gC2, (1 - alpha) * T))
        else:
            lin_term = nx.sum(T * M)
            gw_term = (fgw_dist - (1 - alpha) * lin_term) / alpha
            fgw_dist = nx.set_gradients(fgw_dist, (p, q, C1, C2, M, alpha),
                                        (log_fgw['u'] - nx.mean(log_fgw['u']),
                                         log_fgw['v'] - nx.mean(log_fgw['v']),
                                         alpha * gC1, alpha * gC2, (1 - alpha) * T,
                                         gw_term - lin_term))

    if log:
        return fgw_dist, log_fgw
    else:
        return fgw_dist


def solve_gromov_linesearch(G, deltaG, cost_G, C1, C2, M, reg,
                            alpha_min=None, alpha_max=None, nx=None, **kwargs):
    """
    Solve the linesearch in the FW iterations

    Parameters
    ----------

    G : array-like, shape(ns,nt)
        The transport map at a given iteration of the FW
    deltaG : array-like (ns,nt)
        Difference between the optimal map found by linearization in the FW algorithm and the value at a given iteration
    cost_G : float
        Value of the cost at `G`
    C1 : array-like (ns,ns), optional
        Structure matrix in the source domain.
    C2 : array-like (nt,nt), optional
        Structure matrix in the target domain.
    M : array-like (ns,nt)
        Cost matrix between the features.
    reg : float
        Regularization parameter.
    alpha_min : float, optional
        Minimum value for alpha
    alpha_max : float, optional
        Maximum value for alpha
    nx : backend, optional
        If let to its default value None, a backend test will be conducted.
    Returns
    -------
    alpha : float
        The optimal step size of the FW
    fc : int
        nb of function call. Useless here
    cost_G : float
        The value of the cost for the next iteration


    .. _references-solve-linesearch:
    References
    ----------
    .. [24] Vayer Titouan, Chapel Laetitia, Flamary Rémi, Tavenard Romain and Courty Nicolas
        "Optimal Transport for structured data with application on graphs"
        International Conference on Machine Learning (ICML). 2019.
    """
    if nx is None:
        G, deltaG, C1, C2, M = list_to_array(G, deltaG, C1, C2, M)

        if isinstance(M, int) or isinstance(M, float):
            nx = get_backend(G, deltaG, C1, C2)
        else:
            nx = get_backend(G, deltaG, C1, C2, M)

    dot = nx.dot(nx.dot(C1, deltaG), C2.T)
    a = -2 * reg * nx.sum(dot * deltaG)
    b = nx.sum(M * deltaG) - 2 * reg * (nx.sum(dot * G) + nx.sum(nx.dot(nx.dot(C1, G), C2.T) * deltaG))

    alpha = solve_1d_linesearch_quad(a, b)
    if alpha_min is not None or alpha_max is not None:
        alpha = np.clip(alpha, alpha_min, alpha_max)

    # the new cost is deduced from the line search quadratic function
    cost_G = cost_G + a * (alpha ** 2) + b * alpha

    return alpha, 1, cost_G


def gromov_barycenters(
        N, Cs, ps=None, p=None, lambdas=None, loss_fun='square_loss', symmetric=True, armijo=False,
        max_iter=1000, tol=1e-9, warmstartT=False, verbose=False, log=False,
        init_C=None, random_state=None, **kwargs):
    r"""
    Returns the gromov-wasserstein barycenters of `S` measured similarity matrices :math:`(\mathbf{C}_s)_{1 \leq s \leq S}`

    The function solves the following optimization problem with block coordinate descent:

    .. math::

        \mathbf{C} = \mathop{\arg \min}_{\mathbf{C}\in \mathbb{R}^{N \times N}} \quad \sum_s \lambda_s \mathrm{GW}(\mathbf{C}, \mathbf{C}_s, \mathbf{p}, \mathbf{p}_s)

    Where :

    - :math:`\mathbf{C}_s`: metric cost matrix
    - :math:`\mathbf{p}_s`: distribution

    Parameters
    ----------
    N : int
        Size of the targeted barycenter
    Cs : list of S array-like of shape (ns, ns)
        Metric cost matrices
    ps : list of S array-like of shape (ns,), optional
        Sample weights in the `S` spaces.
        If let to its default value None, uniform distributions are taken.
    p : array-like, shape (N,), optional
        Weights in the targeted barycenter.
        If let to its default value None, uniform distribution is taken.
    lambdas : list of float, optional
        List of the `S` spaces' weights.
        If let to its default value None, uniform weights are taken.
    loss_fun : callable, optional
        tensor-matrix multiplication function based on specific loss function
    symmetric : bool, optional.
        Either structures are to be assumed symmetric or not. Default value is True.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    update : callable
        function(:math:`\mathbf{p}`, lambdas, :math:`\mathbf{T}`, :math:`\mathbf{Cs}`) that updates
        :math:`\mathbf{C}` according to a specific Kernel with the `S` :math:`\mathbf{T}_s` couplings
        calculated at each iteration
    max_iter : int, optional
        Max number of iterations
    tol : float, optional
        Stop threshold on relative error (>0)
    warmstartT: bool, optional
        Either to perform warmstart of transport plans in the successive
        fused gromov-wasserstein transport problems.s
    verbose : bool, optional
        Print information along iterations.
    log : bool, optional
        Record log if True.
    init_C : bool | array-like, shape(N,N)
        Random initial value for the :math:`\mathbf{C}` matrix provided by user.
    random_state : int or RandomState instance, optional
        Fix the seed for reproducibility

    Returns
    -------
    C : array-like, shape (`N`, `N`)
        Similarity matrix in the barycenter space (permutated arbitrarily)
    log : dict
        Log dictionary of error during iterations. Return only if `log=True` in parameters.

    References
    ----------
    .. [12] Gabriel Peyré, Marco Cuturi, and Justin Solomon,
        "Gromov-Wasserstein averaging of kernel and distance matrices."
        International Conference on Machine Learning (ICML). 2016.

    """
    Cs = list_to_array(*Cs)
    arr = [*Cs]
    if ps is not None:
        arr += list_to_array(*ps)
    else:
        ps = [unif(C.shape[0], type_as=C) for C in Cs]
    if p is not None:
        arr.append(list_to_array(p))
    else:
        p = unif(N, type_as=Cs[0])

    nx = get_backend(*arr)

    S = len(Cs)
    if lambdas is None:
        lambdas = [1. / S] * S

    # Initialization of C : random SPD matrix (if not provided by user)
    if init_C is None:
        generator = check_random_state(random_state)
        xalea = generator.randn(N, 2)
        C = dist(xalea, xalea)
        C /= C.max()
        C = nx.from_numpy(C, type_as=p)
    else:
        C = init_C

    if loss_fun == 'kl_loss':
        armijo = True

    cpt = 0
    err = 1

    if warmstartT:
        T = [None] * S
    error = []

    while (err > tol and cpt < max_iter):
        Cprev = C

        if warmstartT:
            T = [gromov_wasserstein(Cs[s], C, ps[s], p, loss_fun, symmetric=symmetric, armijo=armijo, G0=T[s],
                                    max_iter=max_iter, tol_rel=1e-5, tol_abs=0., verbose=verbose, log=False, **kwargs) for s in range(S)]
        else:
            T = [gromov_wasserstein(Cs[s], C, ps[s], p, loss_fun, symmetric=symmetric, armijo=armijo, G0=None,
                                    max_iter=max_iter, tol_rel=1e-5, tol_abs=0., verbose=verbose, log=False, **kwargs) for s in range(S)]
        if loss_fun == 'square_loss':
            C = update_square_loss(p, lambdas, T, Cs)

        elif loss_fun == 'kl_loss':
            C = update_kl_loss(p, lambdas, T, Cs)

        if cpt % 10 == 0:
            # we can speed up the process by checking for the error only all
            # the 10th iterations
            err = nx.norm(C - Cprev)
            error.append(err)

            if verbose:
                if cpt % 200 == 0:
                    print('{:5s}|{:12s}'.format(
                        'It.', 'Err') + '\n' + '-' * 19)
                print('{:5d}|{:8e}|'.format(cpt, err))

        cpt += 1

    if log:
        return C, {"err": error}
    else:
        return C


def fgw_barycenters(
        N, Ys, Cs, ps=None, lambdas=None, alpha=0.5, fixed_structure=False,
        fixed_features=False, p=None, loss_fun='square_loss', armijo=False,
        symmetric=True, max_iter=100, tol=1e-9, warmstartT=False, verbose=False,
        log=False, init_C=None, init_X=None, random_state=None, **kwargs):
    r"""Compute the fgw barycenter as presented eq (5) in :ref:`[24] <references-fgw-barycenters>`

    Parameters
    ----------
    N : int
        Desired number of samples of the target barycenter
    Ys: list of array-like, each element has shape (ns,d)
        Features of all samples
    Cs : list of array-like, each element has shape (ns,ns)
        Structure matrices of all samples
    ps : list of array-like, each element has shape (ns,), optional
        Masses of all samples.
        If let to its default value None, uniform distributions are taken.
    lambdas : list of float, optional
        List of the `S` spaces' weights.
        If let to its default value None, uniform weights are taken.
    alpha : float, optional
        Alpha parameter for the fgw distance.
    fixed_structure : bool
        Whether to fix the structure of the barycenter during the updates
    fixed_features : bool
        Whether to fix the feature of the barycenter during the updates
    p : array-like, shape (N,), optional
        Weights in the targeted barycenter.
        If let to its default value None, uniform distribution is taken.
    loss_fun : str
        Loss function used for the solver either 'square_loss' or 'kl_loss'
    symmetric : bool, optional
        Either structures are to be assumed symmetric or not. Default value is True.
        Else if set to True (resp. False), C1 and C2 will be assumed symmetric (resp. asymmetric).
    max_iter : int, optional
        Max number of iterations
    tol : float, optional
        Stop threshold on relative error (>0)
    warmstartT: bool, optional
        Either to perform warmstart of transport plans in the successive
        fused gromov-wasserstein transport problems.
    verbose : bool, optional
        Print information along iterations.
    log : bool, optional
        Record log if True.
    init_C : array-like, shape (N,N), optional
        Initialization for the barycenters' structure matrix. If not set
        a random init is used.
    init_X : array-like, shape (N,d), optional
        Initialization for the barycenters' features. If not set a
        random init is used.
    random_state : int or RandomState instance, optional
        Fix the seed for reproducibility

    Returns
    -------
    X : array-like, shape (`N`, `d`)
        Barycenters' features
    C : array-like, shape (`N`, `N`)
        Barycenters' structure matrix
    log : dict
        Only returned when log=True. It contains the keys:

        - :math:`\mathbf{T}`: list of (`N`, `ns`) transport matrices
        - :math:`(\mathbf{M}_s)_s`: all distance matrices between the feature of the barycenter and the other features :math:`(dist(\mathbf{X}, \mathbf{Y}_s))_s` shape (`N`, `ns`)


    .. _references-fgw-barycenters:
    References
    ----------
    .. [24] Vayer Titouan, Chapel Laetitia, Flamary Rémi, Tavenard Romain
        and Courty Nicolas
        "Optimal Transport for structured data with application on graphs"
        International Conference on Machine Learning (ICML). 2019.
    """
    Cs = list_to_array(*Cs)
    Ys = list_to_array(*Ys)
    arr = [*Cs, *Ys]
    if ps is not None:
        arr += list_to_array(*ps)
    else:
        ps = [unif(C.shape[0], type_as=C) for C in Cs]
    if p is not None:
        arr.append(list_to_array(p))
    else:
        p = unif(N, type_as=Cs[0])

    nx = get_backend(*arr)

    S = len(Cs)
    if lambdas is None:
        lambdas = [1. / S] * S

    d = Ys[0].shape[1]  # dimension on the node features

    if fixed_structure:
        if init_C is None:
            raise UndefinedParameter('If C is fixed it must be initialized')
        else:
            C = init_C
    else:
        if init_C is None:
            generator = check_random_state(random_state)
            xalea = generator.randn(N, 2)
            C = dist(xalea, xalea)
            C = nx.from_numpy(C, type_as=ps[0])
        else:
            C = init_C

    if fixed_features:
        if init_X is None:
            raise UndefinedParameter('If X is fixed it must be initialized')
        else:
            X = init_X
    else:
        if init_X is None:
            X = nx.zeros((N, d), type_as=ps[0])
        else:
            X = init_X

    T = [nx.outer(p, q) for q in ps]

    Ms = [dist(X, Ys[s]) for s in range(len(Ys))]

    if loss_fun == 'kl_loss':
        armijo = True

    cpt = 0
    err_feature = 1
    err_structure = 1

    if log:
        log_ = {}
        log_['err_feature'] = []
        log_['err_structure'] = []
        log_['Ts_iter'] = []

    while ((err_feature > tol or err_structure > tol) and cpt < max_iter):
        Cprev = C
        Xprev = X

        if not fixed_features:
            Ys_temp = [y.T for y in Ys]
            X = update_feature_matrix(lambdas, Ys_temp, T, p).T

        Ms = [dist(X, Ys[s]) for s in range(len(Ys))]

        if not fixed_structure:
            T_temp = [t.T for t in T]
            if loss_fun == 'square_loss':
                C = update_square_loss(p, lambdas, T_temp, Cs)

            elif loss_fun == 'kl_loss':
                C = update_kl_loss(p, lambdas, T_temp, Cs)

        if warmstartT:
            T = [fused_gromov_wasserstein(
                Ms[s], C, Cs[s], p, ps[s], loss_fun=loss_fun, alpha=alpha, armijo=armijo, symmetric=symmetric,
                G0=T[s], max_iter=max_iter, tol_rel=1e-5, tol_abs=0., verbose=verbose, **kwargs) for s in range(S)]
        else:
            T = [fused_gromov_wasserstein(
                Ms[s], C, Cs[s], p, ps[s], loss_fun=loss_fun, alpha=alpha, armijo=armijo, symmetric=symmetric,
                G0=None, max_iter=max_iter, tol_rel=1e-5, tol_abs=0., verbose=verbose, **kwargs) for s in range(S)]
        # T is N,ns
        err_feature = nx.norm(X - nx.reshape(Xprev, (N, d)))
        err_structure = nx.norm(C - Cprev)
        if log:
            log_['err_feature'].append(err_feature)
            log_['err_structure'].append(err_structure)
            log_['Ts_iter'].append(T)

        if verbose:
            if cpt % 200 == 0:
                print('{:5s}|{:12s}'.format(
                    'It.', 'Err') + '\n' + '-' * 19)
            print('{:5d}|{:8e}|'.format(cpt, err_structure))
            print('{:5d}|{:8e}|'.format(cpt, err_feature))

        cpt += 1

    if log:
        log_['T'] = T  # from target to Ys
        log_['p'] = p
        log_['Ms'] = Ms

    if log:
        return X, C, log_
    else:
        return X, C