def _diagonal_operator(diag):
"""Creates an operator representing a
multiplication with a diagonal matrix"""
diag = diag.ravel()[:, np.newaxis]
def diag_matvec(vec):
if vec.ndim > 1:
return diag * vec
else:
return diag.ravel() * vec
linop = LinearOperator(shape=(len(diag), len(diag)),
matvec=diag_matvec,
rmatvec=diag_matvec,
dtype=np.float64)
linop.matvec = diag_matvec
linop.rmatvec = diag_matvec
return linop
def get_grad_linop(X, Y, invcovB, invcovN, alpha):
"""
Linear operator implementing the gradient of the functional
\frac{1}{2} \|Y - XB\|^2_{\Sigma_n} + \frac{1}{2} \|B\|^2_{\Sigma_s}
which reads
grad_B = X^T(XB - Y)\Sigma_n^{-1} + \lambda B\Sigma_s^{-1}
"""
N, P = X.shape
T = invcovB.shape[0]
if P <= N:
XTX = aslinearoperator(X.T.dot(X))
XTYinvcovN = invcovN.rmatvec(Y.T.dot(X)).T
def matvec(vecB):
XTXB = XTX.matvec(vecB.reshape(T, P).T)
XTXB_invcovN = invcovN.rmatvec(XTXB.T).T
B_incovB = invcovB.rmatvec(vecB.reshape(T, P)).T
result = XTXB_invcovN - XTYinvcovN + alpha * B_incovB
return result.T.ravel()
else:
# raise(Exception)
def matvec(vecB):
XB_minus_Y_invcovN = invcovN.rmatvec(
(X.dot(vecB.reshape(T, P).T) - Y).T).T
XT_XB_minus_Y_invcovN = X.T.dot(XB_minus_Y_invcovN)
B_incovB = invcovB.rmatvec(vecB.reshape(T, P)).T
result = XT_XB_minus_Y_invcovN + alpha * B_incovB
return result.T.ravel()
linop = LinearOperator(shape=tuple([X.shape[1] * Y.shape[1]] * 2),
matvec=matvec,
rmatvec=matvec,
dtype=np.dtype('float64'))
linop.matvec = matvec
linop.rmatvec = matvec
linop.dtype = np.dtype('float64')
return linop
def _woodbury_inverse(Ainv, Cinv, U, V):
"""Uses Woodbury Matrix Identity to invert the Matrix
(A + UCV) ^ (-1)
See http://en.wikipedia.org/wiki/Woodbury_matrix_identity"""
def matvec(x):
# this is probably wildly suboptimal, but it works
Ainv_x = Ainv.matvec(x)
Cinv_mat = Cinv.matvec(np.eye(Cinv.shape[0]))
VAinvU = V.dot(Ainv.matvec(U))
inv_Cinv_plus_VAinvU = np.linalg.inv(Cinv_mat + VAinvU)
VAinv_x = V.dot(Ainv_x)
inv_blabla_VAinv_x = inv_Cinv_plus_VAinvU.dot(VAinv_x)
whole_big_block = Ainv.matvec(
U.dot(inv_blabla_VAinv_x))
return Ainv_x - whole_big_block
shape = Ainv.shape
linop = LinearOperator(shape=shape, matvec=matvec)
linop.matvec = matvec
linop.rmatvec = matvec
return linop
#!/usr/bin/env python
# encoding:utf-8
import numpy as np
from scipy.sparse.linalg import LinearOperator
def mv(v):
print("v:{}".format(v))
print("v:{}".format(v.shape))
return np.array([2 * v[0], 3 * v[1]])
A = LinearOperator((2, 3), matvec=mv)
print("A.matvec:{}".format(A.matvec(np.ones(3))))
def calculate_delta(gamma, #3-dim array (Nz,Nx,Ny) of complex shear
P_kd, #line-of-sight kappa-delta transform
P_gk, #gamma-kappa transform
S_dd, #expected signal covariance of delta
# (can be arbitrary form)
N, #shear noise
alpha, #weiner filter strength
M_factor = 1 #optional scaling of M before cg-method
):
"""
Implement equation A3 from Simon & Taylor 2009
Note: their notation Q -> our notation P_kd
Also, here we factor N_d^-1 out of M: M should be Hermitian for
the cg method. The Simon 09 expression is Hermitian only if N_d is
proportional to the identity, which will not be the case for
deweighted border pixels.
"""
P_kd = as_Lens3D_matrix(P_kd)
P_gk = as_Lens3D_matrix(P_gk)
S_dd = as_Lens3D_matrix(S_dd)
N = as_Lens3D_matrix(N)
P_gk_cross = P_gk.conj_transpose()
P_kd_T = P_kd.transpose()
print "calculating delta:"
print " shape of P_gk:",P_gk.shape
print " shape of P_kd:",P_kd.shape
print "constructing linear operator M"
#define an operator which performs matrix-vector
# multiplication representing M
def matvec(v):
v0 = P_gk_cross.view_as_Lens3D_vec(v)
v1 = N.matvec(v0)
v1 *= alpha
v2 = P_gk_cross.matvec( v0 )
v2 = P_kd_T.matvec( v2 )
v2 = S_dd.matvec( v2 )
v2 = P_kd.matvec( v2 )
v2 = P_gk.matvec( v2 )
ret = numpy.zeros(v.shape,dtype=complex)
ret += v1.vec
ret += v2.vec
return P_gk_cross.view_as_same_type( ret * M_factor , v )
M = LinearOperator(P_gk.shape,
matvec=matvec,
dtype=complex)
v = numpy.random.random(M.shape[1])
t0 = time()
v2 = M.matvec(v)
t = time()-t0
print " M multiplication: %.3g sec" % t
#print M.matvec(numpy.ones(M.shape[1]))[:10]
#exit()
print "constructing preconditioner for M"
#define an operator which can quickly approximate the inverse of
# M using fourier-space inversions. This inverse will be exact for
# a noiseless reconstruction on an infinite field
P_gk_I = P_gk.inverse(False)
#P_kd_I = P_kd.inverse()
S_dd_I = S_dd.inverse(False)
#P_kd_I_T = P_kd_I.transpose()
P_gk_I_cross = P_gk_I.conj_transpose()
def matvec_pc(v):
v0 = P_gk_I.view_as_Lens3D_vec(v)
v0 = P_gk_I.matvec(v0)
#v0 = P_kd_I.matvec(v0)
v0 = S_dd_I.matvec(v0)
#v0 = P_kd_I_T.matvec(v0)
v0 = P_gk_I_cross.matvec(v0)
return P_gk_I.view_as_same_type(v0,v)
M_pc = LinearOperator( (M.shape[1],M.shape[0]),
matvec = matvec_pc,
dtype = M.dtype )
v = numpy.random.random(M_pc.shape[1])
t0 = time()
v3 = M_pc.matvec(v)
t_pc = time()-t0
print " preconditioner multiplication: %.3g sec" % t_pc
step1_vec = gamma.vec
use_cg = True
#---define callback function---
def callback(self):
callback.N += 1
if callback.N%100 == 0: print callback.N,'iterations'
callback.N = 0
#------------------------------
t0 = time()
print "calculating cg:"
ret,errcode = cg( M, step1_vec,
x0 = numpy.zeros(M.shape[1],dtype=step1_vec.dtype),
callback=callback,
M = M_pc)
if errcode != 0:
raise ValueError, "calculate_delta: cg iterations did not converge: err = %s" % (str(errcode))
tf = time()
print " cg: total time = %.2g sec" % (tf-t0)
print " number of iterations = %i" % callback.N
print " time per iteration = %.2g sec" % ( (tf-t0)/callback.N )
ret *= M_factor
ret = P_gk_cross * ret
ret = P_kd_T * ret
delta = S_dd * ret
return P_kd.view_as_Lens3D_vec(delta)
def estimate_condition_number(P_kd,
P_gk,
S_dd,
N,
alpha,
compute_exact = False):
P_kd = as_Lens3D_matrix(P_kd)
P_gk = as_Lens3D_matrix(P_gk)
S_dd = as_Lens3D_matrix(S_dd)
N = as_Lens3D_matrix(N)
P_gk_cross = P_gk.conj_transpose()
P_kd_T = P_kd.transpose()
def matvec(v):
v0 = P_gk_cross.view_as_Lens3D_vec(v)
v2 = P_gk_cross.matvec( v0 )
v2 = P_kd_T.matvec( v2 )
v2 = S_dd.matvec( v2 )
v2 = P_kd.matvec( v2 )
v2 = P_gk.matvec( v2 )
v1 = N.matvec(v0)
v1 *= alpha
ret = numpy.zeros(v.shape,dtype=complex)
ret += v1.vec
ret += v2.vec
return P_gk_cross.view_as_same_type( ret , v )
M = LinearOperator(P_gk.shape,
matvec=matvec,
dtype=complex)
#compute the exact condition number
if compute_exact:
v = numpy.random.random(M.shape[1])
t0 = time()
v2 = M.matvec(v)
t = time()-t0
print " - constructing matrix representation (est. %s)" \
% printtime(t*M.shape[0])
t0 = time()
M_rep = get_mat_rep(M)
print " time to get mat rep: %.2g sec" % (time()-t0)
print " - computing SVD"
t0 = time()
sig = numpy.linalg.svd(M_rep,compute_uv=False)
print " time for SVD: %.2g sec" % (time()-t0)
print 'true condition number: %.2e / %.2e = %.2e' \
% (sig[0],sig[-1],
sig[0]/sig[-1])
#estimate condition number, assuming the noiseless matrix
# is rank-deficient. This will be true if there are more
# source lens-planes than mass lens-planes
eval_max,evec_max = arpack.eigen(M,1)
print 'estimated condition number: %.2e / %.2e = %.2e' \
% ( abs(eval_max[0]) , numpy.min(N.data),
abs(eval_max[0]) / numpy.min(N.data) )
class ConvolutionMatrix(object):
""" Convolution matrix container.
"""
def __init__(self, A=None, mv=None, rmv=None, shape=None):
self.A = A
if A is not None:
self.shape = A.shape
def mv(v):
return A @ v
def rmv(v):
return A.conjugate().T @ v
elif any([mv is not None, rmv is not None]):
if shape:
self.shape = shape
else:
print('If A is not given, its shape must be provided.')
raise Exception(RuntimeError)
if not callable(mv):
print(
'Input mv was not a function. Both mv and rmv shoud be functions, or both empty.'
)
raise Exception(RuntimeError)
elif not callable(rmv):
print(
'Input rmv was not a function. Both mv and rmv shoud be functions, or both empty.'
)
raise Exception(RuntimeError)
else:
# One of both inputs are needed for ConvolutionMatrix creation
print(
'A was not an ndarray, and both multiplication functions A(x) and At(x) were not provided.'
)
raise Exception(RuntimeError)
self.m = self.shape[0]
self.n = self.shape[1]
self.matrix = LinearOperator(self.shape, matvec=mv, rmatvec=rmv)
self.check_adjoint()
def validate_input(self, b0, opts):
assert (np.abs(b0) == b0).all, 'b must be real-valued and non-negative'
if opts.customx0:
assert np.shape(opts.customx0) == (
n, 1), 'customx0 must be a column vector of length n'
def check_adjoint(self):
""" Check that A and At are indeed ajoints of one another
"""
y = np.random.randn(self.m)
Aty = self.matrix.rmatvec(y)
x = np.random.randn(self.n)
Ax = self.matrix.matvec(x)
inner_product1 = Ax.conjugate().T @ y
inner_product2 = x.conjugate().T @ Aty
error = np.abs(inner_product1 -
inner_product2) / np.abs(inner_product1)
assert error < 1e-3, 'Invalid measurement operator: At is not the adjoint of A. Error = %.1f' % error
print('Both matrices were adjoints', error)
def hermitic(self):
return
def lsqr(self, b, tol, maxit, x0):
""" Solution of the least squares problem for ConvolutionMatrix
Gkp, opts.tol/100, opts.max_inner_iters, gk
"""
if b.shape[1] > 0:
b = b.reshape(-1)
if x0.shape[1] > 0:
x0 = x0.reshape(-1)
# x, istop, itn, r1norm = lsqr(self.matrix, b, atol=tol, btol=tol, iter_lim=maxit, x0=x0)
ret = lsqr(self.matrix,
b,
damp=0.01,
atol=tol / 100,
btol=tol / 100,
iter_lim=maxit,
x0=x0)
x = ret[0]
return x
def hmul(self, x):
""" Hermitic mutliplication
returns At*x
"""
return self.matrix.rmatvec(x)
def __mul__(self, x):
return self.matrix.matvec(x)
def __matmul__(self, x):
"""Implementation of left ConvolutionMatrix multiplication, i.e. A@x"""
return self.matrix.dot(x)
def __rmatmul__(self, x):
"""Implementation of right ConvolutionMatrix multiplication, i.e. x@A"""
return
def __rmul__(self, x):
if type(x) is float:
lvec = np.ones(self.shape[1]) * x
else:
lvec = x
return x * self.A # This is not optimal
def calc_yeigs(self, m, b0, idx, squared=True):
if squared:
v = (idx * b0**2).reshape(-1)
else:
v = (idx * b0).reshape(-1)
def ymatvec(x):
return 1 / m * self.matrix.rmatvec(v * self.matrix.matvec(x))
yfun = LinearOperator((self.n, self.n), matvec=ymatvec)
[eval, x0] = eigs(yfun, k=1, which='LR', tol=1E-5)
return x0
def right_eigvec(self, k=1, tol=1e-10, init=None):
""" Compute dominant right eigenvector of transfermatrix with tensors A.
"""
# Build list of correct matrices
A = [self.mps1.B[i] for i in range(self.mps1.L)]
B = [self.mps2.B[i] for i in range(self.mps2.L)]
def __apply_right(vec):
# Reshape vec
vec = np.reshape(vec, (A[-1].shape[2], B[-1].shape[2]))
# Contract as if transfer matrix
vec = np.tensordot(vec, A[-1],
axes=(0, 2)) # (rt rb)(d lt rt) -> (rb d lt)
vec = np.tensordot(vec, np.conjugate(B[-1]),
axes=((0, 1),
(2, 0))) # (rb d lt)(d lb rb) -> (lt lb)
if len(A) > 1:
for s in range(len(A) - 2, -1, -1):
vec = np.tensordot(vec, A[s], axes=(0, 2))
vec = np.tensordot(vec,
np.conjugate(B[s]),
axes=((0, 1), (2, 0)))
return np.reshape(vec, A[0].shape[1] * B[0].shape[1])
E = LinearOperator(
(A[0].shape[1] * B[0].shape[1], A[-1].shape[2] * B[-1].shape[2]),
matvec=__apply_right,
dtype=np.complex128)
if init == None:
newinit = np.random.rand(A[-1].shape[2],
B[-1].shape[2]) + 1j * np.random.rand(
A[-1].shape[2], B[-1].shape[2])
if A[-1].shape[2] == B[-1].shape[2]:
newinit = 0.5 * (newinit + np.conjugate(np.transpose(newinit)))
else:
if init.shape[0] != A[-1].shape[2] or init.shape[1] != B[-1].shape[
2]:
newinit = np.zeros((A[-1].shape[2], B[-1].shape[2]),
dtype=np.complex128)
newinit[:init.shape[0], :init.shape[1]] = init
else:
newinit = init
init = np.reshape(newinit, A[-1].shape[2] * B[-1].shape[2])
if E.shape[0] == 1 and E.shape[1] == 1:
return E.matvec(np.array([1])), np.array([1])
ev, eigvec = sp.sparse.linalg.eigs(E,
k=k,
which='LM',
v0=init,
maxiter=1e4,
tol=tol)
return ev, np.array([
np.array(np.reshape(eigvec[:, i], (A[0].shape[1], B[0].shape[1])))
for i in range(k)
])
def left_eigvec(self, k=1, tol=1e-10, init=None):
""" Compute dominant left eigenvector of transfermatrix with tensor A.
"""
# Build list of correct matrices
A = [
np.tensordot(
np.diag(self.mps1.Lambda[(i - 1) % self.mps1.L]),
np.tensordot(self.mps1.B[i],
np.diag(self.mps1.Lambda[i]**(-1))))
for i in range(self.mps1.L)
]
B = [
np.tensordot(
np.diag(self.mps2.Lambda[(i - 1) % self.mps2.L]),
np.tensordot(self.mps2.B[i],
np.diag(self.mps2.Lambda[i]**(-1))))
for i in range(self.mps2.L)
]
def __apply_left(vec):
# Reshape vec
vec = np.reshape(vec, (A[0].shape[1], B[0].shape[1]))
# Contract as if transfer matrix
vec = np.tensordot(vec, A[0],
axes=(0, 1)) # (lt lb)(d lt rt) -> (lb d rt)
vec = np.tensordot(vec, np.conjugate(B[0]),
axes=((0, 1),
(1, 0))) #(lb d rt)(d lb rb) -> (rt rb)
if len(A) > 1:
for s in range(1, len(A)):
vec = np.tensordot(vec, A[s], axes=(0, 1))
vec = np.tensordot(vec,
np.conjugate(B[s]),
axes=((0, 1), (1, 0)))
return np.reshape(vec, A[-1].shape[2] * B[-1].shape[2])
E = LinearOperator(
(A[-1].shape[2] * B[-1].shape[2], A[0].shape[1] * B[0].shape[1]),
matvec=__apply_left,
dtype=np.complex128)
if init == None:
init = np.random.rand(A[0].shape[1],
B[0].shape[1]) + 1j * np.random.rand(
A[0].shape[1], B[0].shape[1])
# Hermitian initial guess!
if A[0].shape[0] == B[0].shape[1]:
init = 0.5 * (init + np.conjugate(np.transpose(init)))
init = np.reshape(init, A[0].shape[1] * B[0].shape[1])
if E.shape[0] == 1 and E.shape[1] == 1:
return E.matvec(np.array([1])), np.array([1])
ev, eigvec = sp.sparse.linalg.eigs(E,
k=k,
which='LM',
v0=init,
maxiter=1e4,
tol=tol)
return ev, np.array([
np.array(np.reshape(eigvec[:, i],
(A[-1].shape[2], B[-1].shape[2])))
for i in range(k)
])
def vcycle_stat(nu, nu1, nu2, m, u_guess, f, level):
"""
Function to run one vcycle of the multigrid method using the stationary
method as a smoother. In this case we try to solve the initial system.
Parameters
----------
nu : positive real number
regularization parameter
nu1 : integer
number of pre-smoothing steps used
nu2 : integer
number of post-smoothing steps used
m : integer
size of the current matrix
u_guess : ndarray
initial guess of the current run
f : ndarray
function of the current right-hand side of the system
level : int
maximum number of levels the algorithm should do in the recursion
Returns
-------
u : ndarray
solution after the last post-smoothing step
res_norm : list
list with the norm of the residuals
"""
norm = create_norm(m)
#construct linear operator
op = get_system(m, nu)
C = LinearOperator((m**2, m**2), op)
if level == 1:
system = np.zeros((m**2, m**2))
for i in range(0, m**2):
e = np.zeros(m**2)
e[i] = 1
system[i, :] = C.matvec(e)
u_sol = np.linalg.solve(system, f) #######
res_norm = norm(f - C(u_sol))
return (u_sol, res_norm)
else:
### PRE-SMOOTHING
u_nu1, _, _ = solver_stationary_fixedRight(u_guess,
nu,
f,
m,
maxIter=nu1)
### RECURSION
# restriction matrix (full weighted restriction matrix) to get
# the smaller system
R = RMatrix(m)
# projection matrix, to get back to the full system
P = 4 * R.T
res_temp = f - C(u_nu1)
f_new = R.dot(res_temp)
# get new matrix size
m_new = int((m + 1) / 2 - 1)
## init with zero vector
u_init = np.zeros(m_new**2)
u_temp, _ = vcycle_stat(nu, nu1, nu2, m_new, u_init, f_new, level - 1)
# project the current solution into the higher dimensional space
u_new = u_nu1 + P.dot(u_temp)
### POST-SMOOTHING
u_nu2, _, _ = solver_stationary_fixedRight(u_new,
nu,
f,
m,
maxIter=nu2)
res_norm = norm(f - C(u_nu2))
return (u_nu2, res_norm)
pylab.colorbar()
pylab.show()
exit()
#test Sigma->gamma
if False:
print "testing Sigma->gamma"
def matvec(v):
v1 = P_kd.matvec(v)
return P_gk.matvec(v1)
M = LinearOperator(P_kd.shape,matvec=matvec,dtype=complex)
kappa_test = P_kd.matvec(Sigma)
gamma_test = M.matvec(Sigma.vec)
gamma_test = P_kd.view_as_Lens3D_vec(gamma_test)
for i in range(gamma.Nz):
pylab.figure( figsize=(6,8) )
pylab.subplot(211)
kappa.imshow_lens_plane(i)
gamma.fieldplot_lens_plane(i)
pylab.title(r"$\kappa,\gamma\ \rm{true}\ (z=%.2f)$" % z_gamma[i])
pylab.subplot(212)
kappa_test.imshow_lens_plane(i)
gamma_test.fieldplot_lens_plane(i)
pylab.title(r"$\kappa,\gamma\ \rm{test}\ (z=%.2f)$" % z_gamma[i])
pylab.show()
exit()
return Av
L_op = LinearOperator((N, N), matvec=LinOp_func)
# creating the dense version of A as above
A = np.zeros_like(A_dense)
A += np.diag(np.diag(A_dense))
A += np.diag(np.diag(A_dense, k=diag_shift), k=diag_shift)
A += np.diag(np.diag(A_dense, k=-diag_shift), k=-diag_shift)
print('A:\n', A)
# calculating the product using LinearOperator
prod_linOp = L_op.matvec(np.ones(N))
# crudely calculating the product
prod_crude = A * np.ones((N, 1))
# raises error if they are not equal. Else nothing is printed
np.testing.assert_array_almost_equal(np.reshape(prod_linOp, (N, 1)),
prod_crude)
# solving the eigenvalue problem
# using numpy.linalg.eig
eigval_1, __ = np.linalg.eig(A)
# using the scipy.sparse.linalg.eigs
eigval_2, __ = scipy.sparse.linalg.eigsh(L_op, k=N - 1, which='SM')
print('\n\n')
def make_kle(self, KLE_sigma, KLE_L, KLE_num_eig, nrow, ncol, nlay, Lx, Ly): print "making KLE, this will take a long time for large dimensions" print KLE_sigma, KLE_L, KLE_num_eig, nrow, ncol, nlay, Lx, Ly # initialise swig wrapped cpp class C_matrix = correlation.C_matrix(KLE_sigma, KLE_L) C_matrix.set_dims(nrow, ncol, Lx, Ly) out_vec = np.zeros((nrow*ncol), 'd') def KLE_Av(v): C_matrix.av_no_C(nrow*ncol, v, out_vec) return out_vec KLE_A = LinearOperator((nrow*ncol,nrow*ncol), matvec=KLE_Av, dtype='d') t1 = time.time() eig_vals, eig_vecs = eigsh( KLE_A, k=KLE_num_eig) t2 = time.time() # sometimes one gets -v rather than v? for i in range(KLE_num_eig): print "NORM", np.linalg.norm(eig_vecs[:,i]) assert np.allclose(KLE_A.matvec(eig_vecs[:,i]), eig_vals[i]*eig_vecs[:,i]) print "==================================" print "SVD took ", t2-t1, "seconds and " print "they seem to indeed be eigen vectors" print "==================================" # plot eigenvectors from mpl_toolkits.mplot3d import axes3d import matplotlib.pyplot as plt fig = plt.figure(figsize=plt.figaspect(0.2)) for i in range(eig_vecs.shape[1]): ax = fig.add_subplot(1, eig_vecs.shape[1], i, projection='3d') x = np.arange(0, nrow*Lx, Lx) X = np.empty((nrow, ncol)) for col in range(ncol): X[:,col] = x y = np.arange(0, ncol*Ly, Ly) Y = np.empty((nrow, ncol)) for row in range(nrow): Y[row,:] = y Z = eig_vecs[:,i].reshape((nrow, ncol)) ax.plot_wireframe(X, Y, Z) plt.show() # plot eigenvals # import matplotlib.pyplot as plt plt.plot(eig_vals, 'o-') plt.show() print "eig_vals", eig_vals np.savez(working_directory+'kle.npz', eig_vals=eig_vals, eig_vecs=eig_vecs, KLE_L=KLE_L, KLE_sigma=KLE_sigma, KLE_num_eig=KLE_num_eig, nrow=nrow, ncol=ncol, Lx=Lx, Ly=Ly) return eig_vals, eig_vecs
# how you'd use it ########################################## # mu = np.zeros(nrow*ncol) # could be the mean of any data you have # scale = 1. # # evaluate KLE with given modes # # other parameters (other than modes) are mu, scale, eig_vecs, eig_vals (or really sigma and L on which they depend) # def KLE(modes): # coefs = np.sqrt(eig_vals) * modes # elementwise # truncated_M = mu + scale * np.dot( eig_vecs, coefs) # unflattened = truncated_M.reshape(nrow,ncol) # return unflattened # modes = np.ones(num_eig) # print KLE(modes) ############################################ print "==================================" print "done in ", t1-t0, "seconds" print "==================================" for i in range(num_eig): assert np.allclose(A.matvec(eig_vecs[:,i]), eig_vals[i]*eig_vecs[:,i]) print "==================================" print "they are indeed eigenvectors" print "=================================="
