def _dense_solve(self, rhs, adjoint=False, adjoint_arg=False): """Solve by conversion to a dense matrix.""" if self.is_square is False: # pylint: disable=g-bool-id-comparison raise NotImplementedError( "Solve is not yet implemented for non-square operators.") rhs = linalg.adjoint(rhs) if adjoint_arg else rhs if self._can_use_cholesky(): return linalg_ops.cholesky_solve( linalg_ops.cholesky(self.to_dense()), rhs) return linear_operator_util.matrix_solve_with_broadcast( self.to_dense(), rhs, adjoint=adjoint)
def _solve(self, rhs, adjoint=False, adjoint_arg=False): if self.base_operator.is_non_singular is False: raise ValueError( "Solve not implemented unless this is a perturbation of a " "non-singular LinearOperator.") # The Woodbury formula gives: # https://en.wikipedia.org/wiki/Woodbury_matrix_identity # (L + UDV^H)^{-1} # = L^{-1} - L^{-1} U (D^{-1} + V^H L^{-1} U)^{-1} V^H L^{-1} # = L^{-1} - L^{-1} U C^{-1} V^H L^{-1} # where C is the capacitance matrix, C := D^{-1} + V^H L^{-1} U # Note also that, with ^{-H} being the inverse of the adjoint, # (L + UDV^H)^{-H} # = L^{-H} - L^{-H} V C^{-H} U^H L^{-H} l = self.base_operator if adjoint: # If adjoint, U and V have flipped roles in the operator. v, u = self._get_uv_as_tensors() # Capacitance should still be computed with u=self.u and v=self.v, which # after the "flip" on the line above means u=v, v=u. I.e. no need to # "flip" in the capacitance call, since the call to # matrix_solve_with_broadcast below is done with the `adjoint` argument, # and this takes care of things. capacitance = self._make_capacitance(u=v, v=u) else: u, v = self._get_uv_as_tensors() capacitance = self._make_capacitance(u=u, v=v) # L^{-1} rhs linv_rhs = l.solve(rhs, adjoint=adjoint, adjoint_arg=adjoint_arg) # V^H L^{-1} rhs vh_linv_rhs = _linalg.matmul(v, linv_rhs, adjoint_a=True) # C^{-1} V^H L^{-1} rhs if self._use_cholesky: capinv_vh_linv_rhs = linalg_ops.cholesky_solve( linalg_ops.cholesky(capacitance), vh_linv_rhs) else: capinv_vh_linv_rhs = linear_operator_util.matrix_solve_with_broadcast( capacitance, vh_linv_rhs, adjoint=adjoint) # U C^{-1} V^H M^{-1} rhs u_capinv_vh_linv_rhs = _linalg.matmul(u, capinv_vh_linv_rhs) # L^{-1} U C^{-1} V^H L^{-1} rhs linv_u_capinv_vh_linv_rhs = l.solve(u_capinv_vh_linv_rhs, adjoint=adjoint) # L^{-1} - L^{-1} U C^{-1} V^H L^{-1} return linv_rhs - linv_u_capinv_vh_linv_rhs
def _solve(self, rhs, adjoint=False, adjoint_arg=False): if self.base_operator.is_non_singular is False: raise ValueError( "Solve not implemented unless this is a perturbation of a " "non-singular LinearOperator.") # The Woodbury formula gives: # https://en.wikipedia.org/wiki/Woodbury_matrix_identity # (L + UDV^H)^{-1} # = L^{-1} - L^{-1} U (D^{-1} + V^H L^{-1} U)^{-1} V^H L^{-1} # = L^{-1} - L^{-1} U C^{-1} V^H L^{-1} # where C is the capacitance matrix, C := D^{-1} + V^H L^{-1} U # Note also that, with ^{-H} being the inverse of the adjoint, # (L + UDV^H)^{-H} # = L^{-H} - L^{-H} V C^{-H} U^H L^{-H} l = self.base_operator if adjoint: v = self.u u = self.v else: v = self.v u = self.u # L^{-1} rhs linv_rhs = l.solve(rhs, adjoint=adjoint, adjoint_arg=adjoint_arg) # V^H L^{-1} rhs vh_linv_rhs = _linalg.matmul(v, linv_rhs, adjoint_a=True) # C^{-1} V^H L^{-1} rhs if self._use_cholesky: capinv_vh_linv_rhs = linalg_ops.cholesky_solve( linalg_ops.cholesky(self._make_capacitance()), vh_linv_rhs) else: capinv_vh_linv_rhs = linear_operator_util.matrix_solve_with_broadcast( self._make_capacitance(), vh_linv_rhs, adjoint=adjoint) # U C^{-1} V^H M^{-1} rhs u_capinv_vh_linv_rhs = _linalg.matmul(u, capinv_vh_linv_rhs) # L^{-1} U C^{-1} V^H L^{-1} rhs linv_u_capinv_vh_linv_rhs = l.solve(u_capinv_vh_linv_rhs, adjoint=adjoint) # L^{-1} - L^{-1} U C^{-1} V^H L^{-1} return linv_rhs - linv_u_capinv_vh_linv_rhs