Exemple #1
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    def inner(self,
              z: torch.Tensor,
              u: torch.Tensor,
              v=None,
              *,
              keepdim=False) -> torch.Tensor:
        """
        Inner product for tangent vectors at point :math:`z`.
        For the upper half space model, the inner product at point z = x + iy of the vectors u, v
        it is (z, u, v are complex symmetric matrices):

        g_{z}(u, v) = tr[ y^-1 u y^-1 \ov{v} ]

        :param z: torch.Tensor point on the manifold: b x 2 x n x n
        :param u: torch.Tensor tangent vector at point :math:`z`: b x 2 x n x n
        :param v: Optional[torch.Tensor] tangent vector at point :math:`z`: b x 2 x n x n
        :param keepdim: bool keep the last dim?
        :return: torch.Tensor inner product (broadcastable): b x 2 x 1 x 1
        """
        if v is None:
            v = u
        inv_imag_z = torch.inverse(sm.imag(z))
        inv_imag_z = sm.stick(inv_imag_z, torch.zeros_like(inv_imag_z))

        res = sm.bmm3(inv_imag_z, u, inv_imag_z)
        res = sm.bmm(res, sm.conjugate(v))
        real_part = sm.trace(sm.real(res), keepdim=True)  # b x 1
        real_part = torch.unsqueeze(real_part, -1)  # b x 1 x 1
        return sm.stick(real_part, real_part)  # b x 2 x 1 x 1
Exemple #2
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    def projx(self, z: torch.Tensor) -> torch.Tensor:
        """
        Project point :math:`z` on the manifold.

        In this space, we need to ensure that Y = Id - \overline(Z)Z is positive definite.

        Steps to project: Z complex symmetric matrix
        1) Z = SDS^-1
        2) D_tilde = clamp(D, max=1 - epsilon)
        3) Z_tilde = Ŝ D_tilde S^*

        :param z: points to be projected: (b, 2, n, n)
        """
        z = super().projx(z)

        eigenvalues, s = self.takagi_factorization.factorize(z)
        eigenvalues_tilde = torch.clamp(eigenvalues, max=1 - sm.EPS[z.dtype])

        diag_tilde = sm.diag_embed(eigenvalues_tilde)

        z_tilde = sm.bmm3(sm.conjugate(s), diag_tilde, sm.conj_trans(s))

        # we do this so no operation is applied on the matrices that already belong to the space.
        # This prevents modifying values due to numerical instabilities/floating point ops
        batch_wise_mask = torch.all(eigenvalues < 1 - sm.EPS[z.dtype],
                                    dim=-1,
                                    keepdim=True)
        already_in_space_mask = batch_wise_mask.unsqueeze(-1).unsqueeze(
            -1).expand_as(z)

        self.projected_points += len(z) - sum(batch_wise_mask).item()

        return torch.where(already_in_space_mask, z, z_tilde)
Exemple #3
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    def test_conjugate(self):
        x = get_random_symmetric_matrices(10, 4)
        x_imag = sm.imag(x)

        conj_x = sm.conjugate(x)

        self.assertAllEqual(-x_imag, sm.imag(conj_x))
        self.assertAllEqual(x_imag, sm.imag(x))
Exemple #4
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def get_id_minus_conjugate_z_times_z(z: torch.Tensor):
    """
    :param z: b x 2 x n x n
    :return: Id - \overline(z)z
    """
    identity = sm.identity_like(z)
    conj_z_z = sm.bmm(sm.conjugate(z), z)
    return sm.subtract(identity, conj_z_z)
Exemple #5
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    def test_takagi_factorization_very_large_values(self):
        a = get_random_symmetric_matrices(3, 3) * 1000

        eigenvalues, s = TakagiFactorization(3).factorize(a)

        diagonal = torch.diag_embed(eigenvalues)
        diagonal = sm.stick(diagonal, torch.zeros_like(diagonal))

        self.assertAllClose(
            a, sm.bmm3(sm.conjugate(s), diagonal, sm.conj_trans(s)))
Exemple #6
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    def test_takagi_factorization_real_neg_imag_neg(self):
        a = get_random_symmetric_matrices(3, 3)
        a = sm.stick(sm.real(a) * -1, sm.imag(a) * -1)

        eigenvalues, s = TakagiFactorization(3).factorize(a)

        diagonal = torch.diag_embed(eigenvalues)
        diagonal = sm.stick(diagonal, torch.zeros_like(diagonal))

        self.assertAllClose(
            a, sm.bmm3(sm.conjugate(s), diagonal, sm.conj_trans(s)))
Exemple #7
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    def test_takagi_factorization_real_identity(self):
        a = sm.identity_like(get_random_symmetric_matrices(3, 3))

        eigenvalues, s = TakagiFactorization(3).factorize(a)

        diagonal = torch.diag_embed(eigenvalues)
        diagonal = sm.stick(diagonal, torch.zeros_like(diagonal))

        self.assertAllClose(
            a, sm.bmm3(sm.conjugate(s), diagonal, sm.conj_trans(s)))
        self.assertAllClose(a, s)
        self.assertAllClose(torch.ones_like(eigenvalues), eigenvalues)
Exemple #8
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    def inner(self,
              z: torch.Tensor,
              u: torch.Tensor,
              v=None,
              *,
              keepdim=False) -> torch.Tensor:
        """
        Inner product for tangent vectors at point :math:`z`.
        For the bounded domain model, the inner product at point z of the vectors u, v
        it is (z, u, v are complex symmetric matrices):

        g_{z}(u, v) = tr[ (Id -  ẑz)^-1 u (Id - zẑ)^-1 \ov{v} ]

        :param z: torch.Tensor point on the manifold: b x 2 x n x n
        :param u: torch.Tensor tangent vector at point :math:`z`: b x 2 x n x n
        :param v: Optional[torch.Tensor] tangent vector at point :math:`z`: b x 2 x n x n
        :param keepdim: bool keep the last dim?
        :return: torch.Tensor inner product (broadcastable): b x 2 x 1 x 1
        """
        if v is None:
            v = u
        identity = sm.identity_like(z)
        conj_z = sm.conjugate(z)
        conj_z_z = sm.bmm(conj_z, z)
        z_conj_z = sm.bmm(z, conj_z)

        inv_id_minus_conj_z_z = sm.subtract(identity, conj_z_z)
        inv_id_minus_z_conj_z = sm.subtract(identity, z_conj_z)

        inv_id_minus_conj_z_z = sm.inverse(inv_id_minus_conj_z_z)
        inv_id_minus_z_conj_z = sm.inverse(inv_id_minus_z_conj_z)

        res = sm.bmm3(inv_id_minus_conj_z_z, u, inv_id_minus_z_conj_z)
        res = sm.bmm(res, sm.conjugate(v))
        real_part = sm.trace(sm.real(res), keepdim=True)
        real_part = torch.unsqueeze(real_part, -1)  # b x 1 x 1
        return sm.stick(real_part, real_part)  # # b x 2 x 1 x 1
Exemple #9
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    def test_takagi_factorization_real_diagonal(self):
        a = get_random_symmetric_matrices(3, 3) * 10
        a = torch.where(sm.identity_like(a) == 1, a, torch.zeros_like(a))

        eigenvalues, s = TakagiFactorization(3).factorize(a)

        diagonal = torch.diag_embed(eigenvalues)
        diagonal = sm.stick(diagonal, torch.zeros_like(diagonal))

        self.assertAllClose(
            a, sm.bmm3(sm.conjugate(s), diagonal, sm.conj_trans(s)))
        # real part of eigenvectors is made of vectors with one 1 and all zeros
        real_part = torch.sum(torch.abs(sm.real(s)), dim=-1)
        self.assertAllClose(torch.ones_like(real_part), real_part)
        # imaginary part of eigenvectors is all zeros
        self.assertAllClose(torch.zeros(1), torch.sum(sm.imag(s)))
Exemple #10
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    def egrad2rgrad(self, z: torch.Tensor, u: torch.Tensor) -> torch.Tensor:
        """
        Transform gradient computed using autodiff to the correct Riemannian gradient for the point :math:`x`.

        If you have a function f(z) on Mn, then the Riemannian gradient is
            grad_R(f(z)) = (Id + ẑz) * grad_E(f(z)) * (Id + zẑ)

        :param z: point on the manifold. Shape: (b, 2, n, n)
        :param u: gradient to be projected: Shape: same than z
        :return grad vector in the Riemannian manifold. Shape: same than z
        """
        id = sm.identity_like(z)
        conjz = sm.conjugate(z)
        id_plus_conjz_z = id + sm.bmm(conjz, z)
        id_plus_z_conjz = id + sm.bmm(z, conjz)
        riem_grad = sm.bmm3(id_plus_conjz_z, u, id_plus_z_conjz)
        return riem_grad