def get_aggregate(A, strength, aggregate, diagonal_dominance, B, **kwargs):
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
if 'B' in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'predefined':
C = kwargs['C'].tocsr()
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate)
if fn == 'standard':
AggOp = standard_aggregation(C, **kwargs)[0]
elif fn == 'naive':
AggOp = naive_aggregation(C, **kwargs)[0]
elif fn == 'lloyd':
AggOp = lloyd_aggregation(C, **kwargs)[0]
elif fn == 'pairwise':
AggOp = pairwise_aggregation(A, B, **kwargs)[0]
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
return AggOp
def test_naive_aggregation(self):
for A in self.cases:
S = symmetric_strength_of_connection(A)
(expected, expected_Cpts) = reference_naive_aggregation(S)
(result, Cpts) = naive_aggregation(S)
assert_equal((result - expected).nnz, 0)
assert_equal(Cpts.shape[0], expected_Cpts.shape[0])
assert_equal(np.setdiff1d(Cpts, expected_Cpts).shape[0], 0)
def test_naive_aggregation(self):
for A in self.cases:
S = symmetric_strength_of_connection(A)
(expected, expected_Cpts) = reference_naive_aggregation(S)
(result, Cpts) = naive_aggregation(S)
assert_equal((result - expected).nnz, 0)
assert_equal(Cpts.shape[0], expected_Cpts.shape[0])
assert_equal(np.setdiff1d(Cpts, expected_Cpts).shape[0], 0)
def test_naive_aggregation(self):
for A in self.cases:
S = symmetric_strength_of_connection(A)
(expected, expected_Cpts) = reference_naive_aggregation(S)
(result, Cpts) = naive_aggregation(S)
assert_equal((result - expected).nnz, 0)
assert_equal(Cpts.shape[0], expected_Cpts.shape[0])
assert_equal(np.setdiff1d(Cpts, expected_Cpts).shape[0], 0)
# S is diagonal - no dofs aggregated
S = spdiags([[1, 1, 1, 1]], [0], 4, 4, format='csr')
(result, Cpts) = naive_aggregation(S)
expected = np.eye(4)
assert_equal(result.toarray(), expected)
assert_equal(Cpts.shape[0], 4)
def test_naive_aggregation(self):
for A in self.cases:
S = symmetric_strength_of_connection(A)
(expected, expected_Cpts) = reference_naive_aggregation(S)
(result, Cpts) = naive_aggregation(S)
assert_equal((result - expected).nnz, 0)
assert_equal(Cpts.shape[0], expected_Cpts.shape[0])
assert_equal(np.setdiff1d(Cpts, expected_Cpts).shape[0], 0)
# S is diagonal - no dofs aggregated
S = spdiags([[1, 1, 1, 1]], [0], 4, 4, format='csr')
(result, Cpts) = naive_aggregation(S)
expected = np.eye(4)
assert_equal(result.toarray(), expected)
assert_equal(Cpts.shape[0], 4)
def test_symmetric(self):
for A in self.cases:
# theta = 0, no entries dropped
theta = 0.0
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
assert_almost_equal(cost[0], 3.5)
for theta in [0.1, 0.25, 0.5, 0.75, 0.9]:
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
assert (cost[0] <= 3.5)
assert (cost[0] > 0.0)
# theta = 1, only largest entries in each row remain
theta = 1.0
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
est = 1.5 + 2.0 * float(A.shape[0]) / A.nnz
assert_almost_equal(cost[0], est)
def test_symmetric(self):
for A in self.cases:
# theta = 0, no entries dropped
theta = 0.0
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
assert_almost_equal(cost[0], 3.5)
for theta in [0.1,0.25,0.5,0.75,0.9]:
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
assert(cost[0] <= 3.5)
assert(cost[0] > 0.0)
# theta = 1, only largest entries in each row remain
theta = 1.0
cost = [0]
symmetric_strength_of_connection(A, theta, cost)
est = 1.5 + 2.0*float(A.shape[0]) / A.nnz
assert_almost_equal(cost[0],est)
def extend_hierarchy(levels, strength, aggregate, smooth, improve_candidates,
diagonal_dominance=False, keep=True):
"""Service routine to implement the strength of connection, aggregation,
tentative prolongation construction, and prolongation smoothing. Called by
smoothed_aggregation_solver.
"""
A = levels[-1].A
B = levels[-1].B
if A.symmetry == "nonsymmetric":
AH = A.H.asformat(A.format)
BH = levels[-1].BH
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength[len(levels)-1])
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
if 'B' in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'predefined':
C = kwargs['C'].tocsr()
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] = kwargs['cost'][0]
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
levels[-1].complexity['diag_dom'] = kwargs['cost'][0]
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate[len(levels)-1])
if fn == 'standard':
AggOp = standard_aggregation(C, **kwargs)[0]
elif fn == 'naive':
AggOp = naive_aggregation(C, **kwargs)[0]
elif fn == 'lloyd':
AggOp = lloyd_aggregation(C, **kwargs)[0]
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
levels[-1].complexity['aggregation'] = kwargs['cost'][0] * (float(C.nnz)/A.nnz)
# Improve near nullspace candidates by relaxing on A B = 0
temp_cost = [0.0]
fn, kwargs = unpack_arg(improve_candidates[len(levels)-1], cost=False)
if fn is not None:
b = np.zeros((A.shape[0], 1), dtype=A.dtype)
B = relaxation_as_linear_operator((fn, kwargs), A, b, temp_cost) * B
levels[-1].B = B
if A.symmetry == "nonsymmetric":
BH = relaxation_as_linear_operator((fn, kwargs), AH, b, temp_cost) * BH
levels[-1].BH = BH
levels[-1].complexity['candidates'] = temp_cost[0] * B.shape[1]
# Compute the tentative prolongator, T, which is a tentative interpolation
# matrix from the coarse-grid to the fine-grid. T exactly interpolates
# B_fine = T B_coarse. Orthogonalization complexity ~ 2nk^2, k=B.shape[1].
temp_cost=[0.0]
T, B = fit_candidates(AggOp, B, cost=temp_cost)
if A.symmetry == "nonsymmetric":
TH, BH = fit_candidates(AggOp, BH, cost=temp_cost)
levels[-1].complexity['tentative'] = temp_cost[0]/A.nnz
# Smooth the tentative prolongator, so that it's accuracy is greatly
# improved for algebraically smooth error.
fn, kwargs = unpack_arg(smooth[len(levels)-1])
if fn == 'jacobi':
P = jacobi_prolongation_smoother(A, T, C, B, **kwargs)
elif fn == 'richardson':
P = richardson_prolongation_smoother(A, T, **kwargs)
elif fn == 'energy':
P = energy_prolongation_smoother(A, T, C, B, None, (False, {}),
**kwargs)
elif fn is None:
P = T
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
levels[-1].complexity['smooth_P'] = kwargs['cost'][0]
# Compute the restriction matrix, R, which interpolates from the fine-grid
# to the coarse-grid. If A is nonsymmetric, then R must be constructed
# based on A.H. Otherwise R = P.H or P.T.
symmetry = A.symmetry
if symmetry == 'hermitian':
R = P.H
elif symmetry == 'symmetric':
R = P.T
elif symmetry == 'nonsymmetric':
fn, kwargs = unpack_arg(smooth[len(levels)-1])
if fn == 'jacobi':
R = jacobi_prolongation_smoother(AH, TH, C, BH, **kwargs).H
elif fn == 'richardson':
R = richardson_prolongation_smoother(AH, TH, **kwargs).H
elif fn == 'energy':
R = energy_prolongation_smoother(AH, TH, C, BH, None, (False, {}),
**kwargs)
R = R.H
elif fn is None:
R = T.H
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
levels[-1].complexity['smooth_R'] = kwargs['cost'][0]
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].AggOp = AggOp # aggregation operator
levels[-1].T = T # tentative prolongator
levels[-1].P = P # smoothed prolongator
levels[-1].R = R # restriction operator
# Form coarse grid operator, get complexity
levels[-1].complexity['RAP'] = mat_mat_complexity(R,A) / float(A.nnz)
RA = R * A
levels[-1].complexity['RAP'] += mat_mat_complexity(RA,P) / float(A.nnz)
A = RA * P # Galerkin operator, Ac = RAP
A.symmetry = symmetry
levels.append(multilevel_solver.level())
levels[-1].A = A
levels[-1].B = B # right near nullspace candidates
if A.symmetry == "nonsymmetric":
levels[-1].BH = BH # left near nullspace candidates
def extend_hierarchy(levels, strength, CF, keep):
""" helper function for local methods """
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = split.RS(C)
elif fn == 'PMIS':
splitting = split.PMIS(C)
elif fn == 'PMISc':
splitting = split.PMISc(C)
elif fn == 'CLJP':
splitting = split.CLJP(C)
elif fn == 'CLJPc':
splitting = split.CLJPc(C)
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
P = direct_interpolation(A, C, splitting)
# Generate the restriction matrix that maps from the fine-grid to the
# coarse-grid
R = P.T.tocsr()
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].splitting = splitting # C/F splitting
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels.append(multilevel_solver.level())
# Form next level through Galerkin product
A = R * A * P
levels[-1].A = A
def extend_hierarchy(levels, strength, aggregate, smooth, improve_candidates, diagonal_dominance=False, keep=True):
"""Service routine to implement the strength of connection, aggregation,
tentative prolongation construction, and prolongation smoothing. Called by
smoothed_aggregation_solver.
"""
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
B = levels[-1].B
if A.symmetry == "nonsymmetric":
AH = A.H.asformat(A.format)
BH = levels[-1].BH
# Compute the strength-of-connection matrix C, where larger
# C[i, j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength[len(levels) - 1])
if fn == "symmetric":
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == "classical":
C = classical_strength_of_connection(A, **kwargs)
elif fn == "distance":
C = distance_strength_of_connection(A, **kwargs)
elif (fn == "ode") or (fn == "evolution"):
if "B" in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == "energy_based":
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == "predefined":
C = kwargs["C"].tocsr()
elif fn == "algebraic_distance":
C = algebraic_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError("unrecognized strength of connection method: %s" % str(fn))
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate[len(levels) - 1])
if fn == "standard":
AggOp, Cnodes = standard_aggregation(C, **kwargs)
elif fn == "naive":
AggOp, Cnodes = naive_aggregation(C, **kwargs)
elif fn == "lloyd":
AggOp, Cnodes = lloyd_aggregation(C, **kwargs)
elif fn == "predefined":
AggOp = kwargs["AggOp"].tocsr()
Cnodes = kwargs["Cnodes"]
else:
raise ValueError("unrecognized aggregation method %s" % str(fn))
# Improve near nullspace candidates by relaxing on A B = 0
fn, kwargs = unpack_arg(improve_candidates[len(levels) - 1])
if fn is not None:
b = np.zeros((A.shape[0], 1), dtype=A.dtype)
B = relaxation_as_linear_operator((fn, kwargs), A, b) * B
levels[-1].B = B
if A.symmetry == "nonsymmetric":
BH = relaxation_as_linear_operator((fn, kwargs), AH, b) * BH
levels[-1].BH = BH
# Compute the tentative prolongator, T, which is a tentative interpolation
# matrix from the coarse-grid to the fine-grid. T exactly interpolates
# B_fine[:, 0:blocksize(A)] = T B_coarse[:, 0:blocksize(A)].
T, dummy = fit_candidates(AggOp, B[:, 0 : blocksize(A)])
del dummy
if A.symmetry == "nonsymmetric":
TH, dummyH = fit_candidates(AggOp, BH[:, 0 : blocksize(A)])
del dummyH
# Create necessary root node matrices
Cpt_params = (True, get_Cpt_params(A, Cnodes, AggOp, T))
T = scale_T(T, Cpt_params[1]["P_I"], Cpt_params[1]["I_F"])
if A.symmetry == "nonsymmetric":
TH = scale_T(TH, Cpt_params[1]["P_I"], Cpt_params[1]["I_F"])
# Set coarse grid near nullspace modes as injected fine grid near
# null-space modes
B = Cpt_params[1]["P_I"].T * levels[-1].B
if A.symmetry == "nonsymmetric":
BH = Cpt_params[1]["P_I"].T * levels[-1].BH
# Smooth the tentative prolongator, so that it's accuracy is greatly
# improved for algebraically smooth error.
fn, kwargs = unpack_arg(smooth[len(levels) - 1])
if fn == "energy":
P = energy_prolongation_smoother(A, T, C, B, levels[-1].B, Cpt_params=Cpt_params, **kwargs)
elif fn is None:
P = T
else:
raise ValueError(
"unrecognized prolongation smoother \
method %s"
% str(fn)
)
# Compute the restriction matrix R, which interpolates from the fine-grid
# to the coarse-grid. If A is nonsymmetric, then R must be constructed
# based on A.H. Otherwise R = P.H or P.T.
symmetry = A.symmetry
if symmetry == "hermitian":
R = P.H
elif symmetry == "symmetric":
R = P.T
elif symmetry == "nonsymmetric":
fn, kwargs = unpack_arg(smooth[len(levels) - 1])
if fn == "energy":
R = energy_prolongation_smoother(AH, TH, C, BH, levels[-1].BH, Cpt_params=Cpt_params, **kwargs)
R = R.H
elif fn is None:
R = T.H
else:
raise ValueError(
"unrecognized prolongation smoother \
method %s"
% str(fn)
)
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].AggOp = AggOp # aggregation operator
levels[-1].T = T # tentative prolongator
levels[-1].Fpts = Cpt_params[1]["Fpts"] # Fpts
levels[-1].P_I = Cpt_params[1]["P_I"] # Injection operator
levels[-1].I_F = Cpt_params[1]["I_F"] # Identity on F-pts
levels[-1].I_C = Cpt_params[1]["I_C"] # Identity on C-pts
levels[-1].P = P # smoothed prolongator
levels[-1].R = R # restriction operator
levels[-1].Cpts = Cpt_params[1]["Cpts"] # Cpts (i.e., rootnodes)
levels.append(multilevel_solver.level())
A = R * A * P # Galerkin operator
A.symmetry = symmetry
levels[-1].A = A
levels[-1].B = B # right near nullspace candidates
if A.symmetry == "nonsymmetric":
levels[-1].BH = BH # left near nullspace candidates
def initial_setup_stage(A,
symmetry,
pdef,
candidate_iters,
epsilon,
max_levels,
max_coarse,
aggregate,
prepostsmoother,
smooth,
strength,
work,
initial_candidate=None):
"""
Computes a complete aggregation and the first near-nullspace candidate
following Algorithm 3 in Brezina et al.
Parameters
----------
candidate_iters
number of test relaxation iterations
epsilon
minimum acceptable relaxation convergence factor
References
----------
.. [1] Brezina, Falgout, MacLachlan, Manteuffel, McCormick, and Ruge
"Adaptive Smoothed Aggregation ($\alpha$SA) Multigrid"
SIAM Review Volume 47, Issue 2 (2005)
http://www.cs.umn.edu/~maclach/research/aSA2.pdf
"""
# Define relaxation routine
def relax(A, x):
fn, kwargs = unpack_arg(prepostsmoother)
if fn == 'gauss_seidel':
gauss_seidel(A,
x,
np.zeros_like(x),
iterations=candidate_iters,
sweep='symmetric')
elif fn == 'gauss_seidel_nr':
gauss_seidel_nr(A,
x,
np.zeros_like(x),
iterations=candidate_iters,
sweep='symmetric')
elif fn == 'gauss_seidel_ne':
gauss_seidel_ne(A,
x,
np.zeros_like(x),
iterations=candidate_iters,
sweep='symmetric')
elif fn == 'jacobi':
jacobi(A,
x,
np.zeros_like(x),
iterations=1,
omega=1.0 / rho_D_inv_A(A))
elif fn == 'richardson':
polynomial(A,
x,
np.zeros_like(x),
iterations=1,
coefficients=[1.0 / approximate_spectral_radius(A)])
elif fn == 'gmres':
x[:] = (gmres(A, np.zeros_like(x), x0=x,
maxiter=candidate_iters)[0]).reshape(x.shape)
else:
raise TypeError('Unrecognized smoother')
# flag for skipping steps f-i in step 4
skip_f_to_i = True
# step 1
A_l = A
if initial_candidate is None:
x = sp.rand(A_l.shape[0], 1).astype(A_l.dtype)
# The following type check matches the usual 'complex' type,
# but also numpy data types such as 'complex64', 'complex128'
# and 'complex256'.
if A_l.dtype.name.startswith('complex'):
x = x + 1.0j * sp.rand(A_l.shape[0], 1)
else:
x = np.array(initial_candidate, dtype=A_l.dtype)
# step 2
relax(A_l, x)
work[:] += A_l.nnz * candidate_iters * 2
# step 3
# not advised to stop the iteration here: often the first relaxation pass
# _is_ good, but the remaining passes are poor
# if x_A_x/x_A_x_old < epsilon:
# # relaxation alone is sufficient
# print 'relaxation alone works: %g'%(x_A_x/x_A_x_old)
# return x, []
# step 4
As = [A]
xs = [x]
Ps = []
AggOps = []
StrengthOps = []
while A.shape[0] > max_coarse and max_levels > 1:
# The real check to break from the while loop is below
# Begin constructing next level
fn, kwargs = unpack_arg(strength[len(As) - 1]) # step 4b
if fn == 'symmetric':
C_l = symmetric_strength_of_connection(A_l, **kwargs)
# Diagonal must be nonzero
C_l = C_l + eye(C_l.shape[0], C_l.shape[1], format='csr')
elif fn == 'classical':
C_l = classical_strength_of_connection(A_l, **kwargs)
# Diagonal must be nonzero
C_l = C_l + eye(C_l.shape[0], C_l.shape[1], format='csr')
if isspmatrix_bsr(A_l):
C_l = amalgamate(C_l, A_l.blocksize[0])
elif (fn == 'ode') or (fn == 'evolution'):
C_l = evolution_strength_of_connection(
A_l, np.ones((A_l.shape[0], 1), dtype=A.dtype), **kwargs)
elif fn == 'predefined':
C_l = kwargs['C'].tocsr()
elif fn is None:
C_l = A_l.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# In SA, strength represents "distance", so we take magnitude of
# complex values
if C_l.dtype.name.startswith('complex'):
C_l.data = np.abs(C_l.data)
# Create a unified strength framework so that large values represent
# strong connections and small values represent weak connections
if (fn == 'ode') or (fn == 'evolution') or (fn == 'energy_based'):
C_l.data = 1.0 / C_l.data
# aggregation
fn, kwargs = unpack_arg(aggregate[len(As) - 1])
if fn == 'standard':
AggOp = standard_aggregation(C_l, **kwargs)[0]
elif fn == 'lloyd':
AggOp = lloyd_aggregation(C_l, **kwargs)[0]
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
T_l, x = fit_candidates(AggOp, x) # step 4c
fn, kwargs = unpack_arg(smooth[len(As) - 1]) # step 4d
if fn == 'jacobi':
P_l = jacobi_prolongation_smoother(A_l, T_l, C_l, x, **kwargs)
elif fn == 'richardson':
P_l = richardson_prolongation_smoother(A_l, T_l, **kwargs)
elif fn == 'energy':
P_l = energy_prolongation_smoother(A_l, T_l, C_l, x, None,
(False, {}), **kwargs)
elif fn is None:
P_l = T_l
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
# R should reflect A's structure # step 4e
if symmetry == 'symmetric':
A_l = P_l.T.asformat(P_l.format) * A_l * P_l
elif symmetry == 'hermitian':
A_l = P_l.H.asformat(P_l.format) * A_l * P_l
StrengthOps.append(C_l)
AggOps.append(AggOp)
Ps.append(P_l)
As.append(A_l)
# skip to step 5 as in step 4e
if (A_l.shape[0] <= max_coarse) or (len(AggOps) + 1 >= max_levels):
break
if not skip_f_to_i:
x_hat = x.copy() # step 4g
relax(A_l, x) # step 4h
work[:] += A_l.nnz * candidate_iters * 2
if pdef is True:
x_A_x = np.dot(np.conjugate(x).T, A_l * x)
xhat_A_xhat = np.dot(np.conjugate(x_hat).T, A_l * x_hat)
err_ratio = (x_A_x / xhat_A_xhat)**(1.0 / candidate_iters)
else:
# use A.H A inner-product
Ax = A_l * x
# Axhat = A_l * x_hat
x_A_x = np.dot(np.conjugate(Ax).T, Ax)
xhat_A_xhat = np.dot(np.conjugate(x_hat).T, A_l * x_hat)
err_ratio = (x_A_x / xhat_A_xhat)**(1.0 / candidate_iters)
if err_ratio < epsilon: # step 4i
# print "sufficient convergence, skipping"
skip_f_to_i = True
if x_A_x == 0:
x = x_hat # need to restore x
else:
# just carry out relaxation, don't check for convergence
relax(A_l, x) # step 4h
work[:] += 2 * A_l.nnz * candidate_iters
# store xs for diagnostic use and for use in step 5
xs.append(x)
# step 5
# Extend coarse-level candidate to the finest level
# --> note that we start with the x from the second coarsest level
x = xs[-1]
# make sure that xs[-1] has been relaxed by step 4h, i.e. relax(As[-2], x)
for lev in range(len(Ps) - 2, -1, -1): # lev = coarsest ... finest-1
P = Ps[lev] # I: lev --> lev+1
A = As[lev] # A on lev+1
x = P * x
relax(A, x)
work[:] += A.nnz * candidate_iters * 2
# Set predefined strength of connection and aggregation
if len(AggOps) > 1:
aggregate = [('predefined', {
'AggOp': AggOps[i]
}) for i in range(len(AggOps))]
strength = [('predefined', {
'C': StrengthOps[i]
}) for i in range(len(StrengthOps))]
return x, aggregate, strength # first candidate
def initial_setup_stage(A, symmetry, pdef, candidate_iters, epsilon,
max_levels, max_coarse, aggregate, prepostsmoother,
smooth, strength, work, initial_candidate=None):
"""Compute aggregation and the first near-nullspace candidate following Algorithm 3 in Brezina et al.
Parameters
----------
candidate_iters
number of test relaxation iterations
epsilon
minimum acceptable relaxation convergence factor
References
----------
.. [1] Brezina, Falgout, MacLachlan, Manteuffel, McCormick, and Ruge
"Adaptive Smoothed Aggregation (aSA) Multigrid"
SIAM Review Volume 47, Issue 2 (2005)
http://www.cs.umn.edu/~maclach/research/aSA2.pdf
"""
# Define relaxation routine
def relax(A, x):
fn, kwargs = unpack_arg(prepostsmoother)
if fn == 'gauss_seidel':
gauss_seidel(A, x, np.zeros_like(x),
iterations=candidate_iters, sweep='symmetric')
elif fn == 'gauss_seidel_nr':
gauss_seidel_nr(A, x, np.zeros_like(x),
iterations=candidate_iters, sweep='symmetric')
elif fn == 'gauss_seidel_ne':
gauss_seidel_ne(A, x, np.zeros_like(x),
iterations=candidate_iters, sweep='symmetric')
elif fn == 'jacobi':
jacobi(A, x, np.zeros_like(x), iterations=1,
omega=1.0 / rho_D_inv_A(A))
elif fn == 'richardson':
polynomial(A, x, np.zeros_like(x), iterations=1,
coefficients=[1.0/approximate_spectral_radius(A)])
elif fn == 'gmres':
x[:] = (gmres(A, np.zeros_like(x), x0=x,
maxiter=candidate_iters)[0]).reshape(x.shape)
else:
raise TypeError('Unrecognized smoother')
# flag for skipping steps f-i in step 4
skip_f_to_i = True
# step 1
A_l = A
if initial_candidate is None:
x = sp.rand(A_l.shape[0], 1).astype(A_l.dtype)
# The following type check matches the usual 'complex' type,
# but also numpy data types such as 'complex64', 'complex128'
# and 'complex256'.
if A_l.dtype.name.startswith('complex'):
x = x + 1.0j*sp.rand(A_l.shape[0], 1)
else:
x = np.array(initial_candidate, dtype=A_l.dtype)
# step 2
relax(A_l, x)
work[:] += A_l.nnz * candidate_iters*2
# step 3
# not advised to stop the iteration here: often the first relaxation pass
# _is_ good, but the remaining passes are poor
# if x_A_x/x_A_x_old < epsilon:
# # relaxation alone is sufficient
# print 'relaxation alone works: %g'%(x_A_x/x_A_x_old)
# return x, []
# step 4
As = [A]
xs = [x]
Ps = []
AggOps = []
StrengthOps = []
while A.shape[0] > max_coarse and max_levels > 1:
# The real check to break from the while loop is below
# Begin constructing next level
fn, kwargs = unpack_arg(strength[len(As)-1]) # step 4b
if fn == 'symmetric':
C_l = symmetric_strength_of_connection(A_l, **kwargs)
# Diagonal must be nonzero
C_l = C_l + eye(C_l.shape[0], C_l.shape[1], format='csr')
elif fn == 'classical':
C_l = classical_strength_of_connection(A_l, **kwargs)
# Diagonal must be nonzero
C_l = C_l + eye(C_l.shape[0], C_l.shape[1], format='csr')
if isspmatrix_bsr(A_l):
C_l = amalgamate(C_l, A_l.blocksize[0])
elif (fn == 'ode') or (fn == 'evolution'):
C_l = evolution_strength_of_connection(A_l,
np.ones(
(A_l.shape[0], 1),
dtype=A.dtype),
**kwargs)
elif fn == 'predefined':
C_l = kwargs['C'].tocsr()
elif fn is None:
C_l = A_l.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# In SA, strength represents "distance", so we take magnitude of
# complex values
if C_l.dtype.name.startswith('complex'):
C_l.data = np.abs(C_l.data)
# Create a unified strength framework so that large values represent
# strong connections and small values represent weak connections
if (fn == 'ode') or (fn == 'evolution') or (fn == 'energy_based'):
C_l.data = 1.0 / C_l.data
# aggregation
fn, kwargs = unpack_arg(aggregate[len(As) - 1])
if fn == 'standard':
AggOp = standard_aggregation(C_l, **kwargs)[0]
elif fn == 'lloyd':
AggOp = lloyd_aggregation(C_l, **kwargs)[0]
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
T_l, x = fit_candidates(AggOp, x) # step 4c
fn, kwargs = unpack_arg(smooth[len(As)-1]) # step 4d
if fn == 'jacobi':
P_l = jacobi_prolongation_smoother(A_l, T_l, C_l, x, **kwargs)
elif fn == 'richardson':
P_l = richardson_prolongation_smoother(A_l, T_l, **kwargs)
elif fn == 'energy':
P_l = energy_prolongation_smoother(A_l, T_l, C_l, x, None,
(False, {}), **kwargs)
elif fn is None:
P_l = T_l
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
# R should reflect A's structure # step 4e
if symmetry == 'symmetric':
A_l = P_l.T.asformat(P_l.format) * A_l * P_l
elif symmetry == 'hermitian':
A_l = P_l.H.asformat(P_l.format) * A_l * P_l
StrengthOps.append(C_l)
AggOps.append(AggOp)
Ps.append(P_l)
As.append(A_l)
# skip to step 5 as in step 4e
if (A_l.shape[0] <= max_coarse) or (len(AggOps) + 1 >= max_levels):
break
if not skip_f_to_i:
x_hat = x.copy() # step 4g
relax(A_l, x) # step 4h
work[:] += A_l.nnz*candidate_iters*2
if pdef is True:
x_A_x = np.dot(np.conjugate(x).T, A_l*x)
xhat_A_xhat = np.dot(np.conjugate(x_hat).T, A_l*x_hat)
err_ratio = (x_A_x/xhat_A_xhat)**(1.0/candidate_iters)
else:
# use A.H A inner-product
Ax = A_l * x
# Axhat = A_l * x_hat
x_A_x = np.dot(np.conjugate(Ax).T, Ax)
xhat_A_xhat = np.dot(np.conjugate(x_hat).T, A_l*x_hat)
err_ratio = (x_A_x/xhat_A_xhat)**(1.0/candidate_iters)
if err_ratio < epsilon: # step 4i
# print "sufficient convergence, skipping"
skip_f_to_i = True
if x_A_x == 0:
x = x_hat # need to restore x
else:
# just carry out relaxation, don't check for convergence
relax(A_l, x) # step 4h
work[:] += 2 * A_l.nnz * candidate_iters
# store xs for diagnostic use and for use in step 5
xs.append(x)
# step 5
# Extend coarse-level candidate to the finest level
# --> note that we start with the x from the second coarsest level
x = xs[-1]
# make sure that xs[-1] has been relaxed by step 4h, i.e. relax(As[-2], x)
for lev in range(len(Ps)-2, -1, -1): # lev = coarsest ... finest-1
P = Ps[lev] # I: lev --> lev+1
A = As[lev] # A on lev+1
x = P * x
relax(A, x)
work[:] += A.nnz*candidate_iters*2
# Set predefined strength of connection and aggregation
if len(AggOps) > 1:
aggregate = [('predefined', {'AggOp': AggOps[i]})
for i in range(len(AggOps))]
strength = [('predefined', {'C': StrengthOps[i]})
for i in range(len(StrengthOps))]
return x, aggregate, strength # first candidate
def extend_hierarchy(levels, strength, CF, interp, keep):
""" helper function for local methods """
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
block_starts = levels[-1].block_starts
verts = levels[-1].verts
# If this is a system, apply the unknown approach by coarsening and generating interpolation based on each diagonal block of A
if (block_starts):
A_diag = extract_diagonal_blocks(A, block_starts)
else:
A_diag = [A]
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
C_diag = []
P_diag = []
splitting = []
next_lvl_block_starts = [0]
block_cnt = 0
for mat in A_diag:
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C_diag.append( symmetric_strength_of_connection(mat, **kwargs) )
elif fn == 'classical':
C_diag.append( classical_strength_of_connection(mat, **kwargs) )
elif fn == 'distance':
C_diag.append( distance_strength_of_connection(mat, **kwargs) )
elif (fn == 'ode') or (fn == 'evolution'):
C_diag.append( evolution_strength_of_connection(mat, **kwargs) )
elif fn == 'energy_based':
C_diag.append( energy_based_strength_of_connection(mat, **kwargs) )
elif fn == 'algebraic_distance':
C_diag.append( algebraic_distance(mat, **kwargs) )
elif fn == 'affinity':
C_diag.append( affinity_distance(mat, **kwargs) )
elif fn is None:
C_diag.append( mat )
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting.append( split.RS(C_diag[-1]) )
elif fn == 'PMIS':
splitting.append( split.PMIS(C_diag[-1]) )
elif fn == 'PMISc':
splitting.append( split.PMISc(C_diag[-1]) )
elif fn == 'CLJP':
splitting.append( split.CLJP(C_diag[-1]) )
elif fn == 'CLJPc':
splitting.append( split.CLJPc(C_diag[-1]) )
elif fn == 'Shifted2DCoarsening':
splitting.append( split.Shifted2DCoarsening(C_diag[-1]) )
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
fn, kwargs = unpack_arg(interp)
if fn == 'standard':
P_diag.append( standard_interpolation(mat, C_diag[-1], splitting[-1]) )
elif fn == 'direct':
P_diag.append( direct_interpolation(mat, C_diag[-1], splitting[-1]) )
else:
raise ValueError('unknown interpolation method (%s)' % interp)
next_lvl_block_starts.append( next_lvl_block_starts[-1] + P_diag[-1].shape[1])
block_cnt = block_cnt + 1
P = block_diag(P_diag)
# Generate the restriction matrix that maps from the fine-grid to the
# coarse-grid
R = P.T.tocsr()
# Store relevant information for this level
splitting = numpy.concatenate(splitting)
if keep:
C = block_diag(C_diag)
levels[-1].C = C # strength of connection matrix
levels[-1].splitting = splitting # C/F splitting
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels.append(multilevel_solver.level())
# Form next level through Galerkin product
# !!! For systems, how do I propogate the block structure information down to the next grid? Especially if the blocks are different sizes? !!!
A = R * A * P
levels[-1].A = A
if (block_starts):
levels[-1].block_starts = next_lvl_block_starts
else:
levels[-1].block_starts = None
# If called for, output a visualization of the C/F splitting
if (verts.any()):
new_verts = numpy.empty([P.shape[1], 2])
cnt = 0
for i in range(len(splitting)):
if (splitting[i]):
new_verts[cnt] = verts[i]
cnt = cnt + 1
levels[-1].verts = new_verts
else:
levels[-1].verts = numpy.zeros(1)
def extend_hierarchy(levels,
strength,
aggregate,
smooth,
improve_candidates,
diagonal_dominance=False,
keep=True):
"""Extend the multigrid hierarchy.
Service routine to implement the strength of connection, aggregation,
tentative prolongation construction, and prolongation smoothing. Called by
smoothed_aggregation_solver.
"""
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
B = levels[-1].B
if A.symmetry == "nonsymmetric":
AH = A.H.asformat(A.format)
BH = levels[-1].BH
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength[len(levels) - 1])
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
if 'B' in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'predefined':
C = kwargs['C'].tocsr()
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate[len(levels) - 1])
if fn == 'standard':
AggOp = standard_aggregation(C, **kwargs)[0]
elif fn == 'naive':
AggOp = naive_aggregation(C, **kwargs)[0]
elif fn == 'lloyd':
AggOp = lloyd_aggregation(C, **kwargs)[0]
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
# Improve near nullspace candidates by relaxing on A B = 0
fn, kwargs = unpack_arg(improve_candidates[len(levels) - 1])
if fn is not None:
b = np.zeros((A.shape[0], 1), dtype=A.dtype)
B = relaxation_as_linear_operator((fn, kwargs), A, b) * B
levels[-1].B = B
if A.symmetry == "nonsymmetric":
BH = relaxation_as_linear_operator((fn, kwargs), AH, b) * BH
levels[-1].BH = BH
# Compute the tentative prolongator, T, which is a tentative interpolation
# matrix from the coarse-grid to the fine-grid. T exactly interpolates
# B_fine = T B_coarse.
T, B = fit_candidates(AggOp, B)
if A.symmetry == "nonsymmetric":
TH, BH = fit_candidates(AggOp, BH)
# Smooth the tentative prolongator, so that it's accuracy is greatly
# improved for algebraically smooth error.
fn, kwargs = unpack_arg(smooth[len(levels) - 1])
if fn == 'jacobi':
P = jacobi_prolongation_smoother(A, T, C, B, **kwargs)
elif fn == 'richardson':
P = richardson_prolongation_smoother(A, T, **kwargs)
elif fn == 'energy':
P = energy_prolongation_smoother(A, T, C, B, None, (False, {}),
**kwargs)
elif fn is None:
P = T
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
# Compute the restriction matrix, R, which interpolates from the fine-grid
# to the coarse-grid. If A is nonsymmetric, then R must be constructed
# based on A.H. Otherwise R = P.H or P.T.
symmetry = A.symmetry
if symmetry == 'hermitian':
R = P.H
elif symmetry == 'symmetric':
R = P.T
elif symmetry == 'nonsymmetric':
fn, kwargs = unpack_arg(smooth[len(levels) - 1])
if fn == 'jacobi':
R = jacobi_prolongation_smoother(AH, TH, C, BH, **kwargs).H
elif fn == 'richardson':
R = richardson_prolongation_smoother(AH, TH, **kwargs).H
elif fn == 'energy':
R = energy_prolongation_smoother(AH, TH, C, BH, None, (False, {}),
**kwargs)
R = R.H
elif fn is None:
R = T.H
else:
raise ValueError('unrecognized prolongation smoother method %s' %
str(fn))
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].AggOp = AggOp # aggregation operator
levels[-1].T = T # tentative prolongator
levels[-1].P = P # smoothed prolongator
levels[-1].R = R # restriction operator
levels.append(multilevel_solver.level())
A = R * A * P # Galerkin operator
A.symmetry = symmetry
levels[-1].A = A
levels[-1].B = B # right near nullspace candidates
if A.symmetry == "nonsymmetric":
levels[-1].BH = BH # left near nullspace candidates
def extend_hierarchy(levels, strength, CF, interpolation, restriction, keep):
""" helper function for local methods """
A = levels[-1].A
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] = kwargs['cost'][0]
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = split.RS(C, **kwargs)
elif fn == 'PMIS':
splitting = split.PMIS(C, **kwargs)
elif fn == 'PMISc':
splitting = split.PMISc(C, **kwargs)
elif fn == 'CLJP':
splitting = split.CLJP(C, **kwargs)
elif fn == 'CLJPc':
splitting = split.CLJPc(C, **kwargs)
elif fn == 'CR':
splitting = CR(C, **kwargs)
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
levels[-1].complexity['CF'] = kwargs['cost'][0]
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
fn, kwargs = unpack_arg(interpolation)
if fn == 'standard':
P = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'injection':
P = injection_interpolation(A, splitting, **kwargs)
else:
raise ValueError('unknown interpolation method (%s)' % interpolation)
levels[-1].complexity['interpolate'] = kwargs['cost'][0]
# Generate the restriction matrix that maps from the fine-grid to the
# coarse-grid. Must make sure transpose matrices remain in CSR or BSR
fn, kwargs = unpack_arg(restriction)
if isspmatrix_csr(A):
if restriction == 'galerkin':
R = P.T.tocsr()
elif fn == 'standard':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'distance_two':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'direct':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'injection': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
R = R.T.tocsr()
else:
raise ValueError('unknown interpolation method (%s)' %
interpolation)
else:
if restriction == 'galerkin':
R = P.T.tobsr()
elif fn == 'standard':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'distance_two':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'direct':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'injection': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
R = R.T.tobsr()
else:
raise ValueError('unknown interpolation method (%s)' %
interpolation)
levels[-1].complexity['restriction'] = kwargs['cost'][0]
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels[-1].splitting = splitting # C/F splitting
# Form coarse grid operator, get complexity
levels[-1].complexity['RAP'] = mat_mat_complexity(R, A) / float(A.nnz)
RA = R * A
levels[-1].complexity['RAP'] += mat_mat_complexity(RA, P) / float(A.nnz)
A = RA * P # Galerkin operator, Ac = RAP
# Make sure coarse-grid operator is in correct sparse format
if (isspmatrix_csr(P) and (not isspmatrix_csr(A))):
A = A.tocsr()
elif (isspmatrix_bsr(P) and (not isspmatrix_bsr(A))):
A = A.tobsr()
# Form next level through Galerkin product
levels.append(multilevel_solver.level())
levels[-1].A = A
def extend_hierarchy(levels, strength, CF, interp, restrict, filter_operator,
coarse_grid_P, coarse_grid_R, keep):
""" helper function for local methods """
# Filter operator. Need to keep original matrix on fineest level for
# computing residuals
if (filter_operator is not None) and (filter_operator[1] != 0):
if len(levels) == 1:
A = deepcopy(levels[-1].A)
else:
A = levels[-1].A
filter_matrix_rows(A, filter_operator[1], diagonal=True, lump=filter_operator[0])
else:
A = levels[-1].A
# Check if matrix was filtered to be diagonal --> coarsest grid
if A.nnz == A.shape[0]:
return 1
# Zero initial complexities for strength, splitting and interpolation
levels[-1].complexity['CF'] = 0.0
levels[-1].complexity['strength'] = 0.0
levels[-1].complexity['interpolate'] = 0.0
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] += kwargs['cost'][0] * A.nnz / float(A.nnz)
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = RS(C, **kwargs)
elif fn == 'PMIS':
splitting = PMIS(C, **kwargs)
elif fn == 'PMISc':
splitting = PMISc(C, **kwargs)
elif fn == 'CLJP':
splitting = CLJP(C, **kwargs)
elif fn == 'CLJPc':
splitting = CLJPc(C, **kwargs)
elif fn == 'CR':
splitting = CR(C, **kwargs)
elif fn == 'weighted_matching':
splitting, soc = weighted_matching(C, **kwargs)
if soc is not None:
C = soc
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
levels[-1].complexity['CF'] += kwargs['cost'][0] * C.nnz / float(A.nnz)
temp = np.sum(splitting)
if (temp == len(splitting)) or (temp == 0):
return 1
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
r_flag = False
fn, kwargs = unpack_arg(interp)
if fn == 'standard':
P = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'inject':
P = injection_interpolation(A, splitting, **kwargs)
elif fn == 'neumann':
P = neumann_ideal_interpolation(A, splitting, **kwargs)
elif fn == 'scaledAfc':
P = scaled_Afc_interpolation(A, splitting, **kwargs)
elif fn == 'air':
if isspmatrix_bsr(A):
temp_A = bsr_matrix(A.T)
P = local_AIR(temp_A, splitting, **kwargs)
P = bsr_matrix(P.T)
else:
temp_A = csr_matrix(A.T)
P = local_AIR(temp_A, splitting, **kwargs)
P = csr_matrix(P.T)
elif fn == 'restrict':
r_flag = True
else:
raise ValueError('unknown interpolation method (%s)' % interp)
levels[-1].complexity['interpolate'] += kwargs['cost'][0] * A.nnz / float(A.nnz)
# Build restriction operator
fn, kwargs = unpack_arg(restrict)
if fn is None:
R = P.T
elif fn == 'air':
R = local_AIR(A, splitting, **kwargs)
elif fn == 'neumann':
R = neumann_AIR(A, splitting, **kwargs)
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
if isspmatrix_bsr(A):
R = R.T.tobsr()
else:
R = R.T.tocsr()
elif fn == 'inject': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
if isspmatrix_bsr(A):
R = R.T.tobsr()
else:
R = R.T.tocsr()
elif fn == 'standard':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'distance_two':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'direct':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
else:
raise ValueError('unknown restriction method (%s)' % restrict)
# If set P = R^T
if r_flag:
P = R.T
# Optional different interpolation for RAP
fn, kwargs = unpack_arg(coarse_grid_P)
if fn == 'standard':
P_temp = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P_temp = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P_temp = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P_temp = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'inject':
P_temp = injection_interpolation(A, splitting, **kwargs)
elif fn == 'neumann':
P_temp = neumann_ideal_interpolation(A, splitting, **kwargs)
elif fn == 'air':
if isspmatrix_bsr(A):
temp_A = bsr_matrix(A.T)
P_temp = local_AIR(temp_A, splitting, **kwargs)
P_temp = bsr_matrix(P_temp.T)
else:
temp_A = csr_matrix(A.T)
P_temp = local_AIR(temp_A, splitting, **kwargs)
P_temp = csr_matrix(P_temp.T)
else:
P_temp = P
# Optional different restriction for RAP
fn, kwargs = unpack_arg(coarse_grid_R)
if fn == 'air':
R_temp = local_AIR(A, splitting, **kwargs)
elif fn == 'neumann':
R_temp = neumann_AIR(A, splitting, **kwargs)
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R_temp = one_point_interpolation(A, temp_C, splitting, **kwargs)
if isspmatrix_bsr(A):
R_temp = R_temp.T.tobsr()
else:
R_temp = R_temp.T.tocsr()
elif fn == 'inject': # Don't need A^T or C^T here
R_temp = injection_interpolation(A, splitting, **kwargs)
if isspmatrix_bsr(A):
R_temp = R_temp.T.tobsr()
else:
R_temp = R_temp.T.tocsr()
elif fn == 'standard':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tocsr()
elif fn == 'distance_two':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tocsr()
elif fn == 'direct':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tocsr()
else:
R_temp = R
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels[-1].splitting = splitting # C/F splitting
# Form coarse grid operator, get complexity
#levels[-1].complexity['RAP'] = mat_mat_complexity(R_temp,A) / float(A.nnz)
#RA = R_temp * A
#levels[-1].complexity['RAP'] += mat_mat_complexity(RA,P_temp) / float(A.nnz)
#A = RA * P_temp
# RL: RAP = R*(A*P)
levels[-1].complexity['RAP'] = mat_mat_complexity(A, P_temp) / float(A.nnz)
AP = A * P_temp
levels[-1].complexity['RAP'] += mat_mat_complexity(R_temp, AP) / float(A.nnz)
A = R_temp * AP
# Make sure coarse-grid operator is in correct sparse format
if (isspmatrix_csr(P) and (not isspmatrix_csr(A))):
A = A.tocsr()
elif (isspmatrix_bsr(P) and (not isspmatrix_bsr(A))):
A = A.tobsr()
A.eliminate_zeros()
levels.append(multilevel_solver.level())
levels[-1].A = A
return 0
def extend_hierarchy(levels, strength, CF, interp, restrict, filter_operator,
coarse_grid_P, coarse_grid_R, keep):
""" helper function for local methods """
# Filter operator. Need to keep original matrix on fineest level for
# computing residuals
if (filter_operator is not None) and (filter_operator[1] != 0):
if len(levels) == 1:
A = deepcopy(levels[-1].A)
else:
A = levels[-1].A
filter_matrix_rows(A,
filter_operator[1],
diagonal=True,
lump=filter_operator[0])
else:
A = levels[-1].A
# Check if matrix was filtered to be diagonal --> coarsest grid
if A.nnz == A.shape[0]:
return 1
# Zero initial complexities for strength, splitting and interpolation
levels[-1].complexity['CF'] = 0.0
levels[-1].complexity['strength'] = 0.0
levels[-1].complexity['interpolate'] = 0.0
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] += kwargs['cost'][0] * A.nnz / float(
A.nnz)
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = RS(C, **kwargs)
elif fn == 'PMIS':
splitting = PMIS(C, **kwargs)
elif fn == 'PMISc':
splitting = PMISc(C, **kwargs)
elif fn == 'CLJP':
splitting = CLJP(C, **kwargs)
elif fn == 'CLJPc':
splitting = CLJPc(C, **kwargs)
elif fn == 'CR':
splitting = CR(C, **kwargs)
elif fn == 'weighted_matching':
splitting, soc = weighted_matching(C, **kwargs)
if soc is not None:
C = soc
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
levels[-1].complexity['CF'] += kwargs['cost'][0] * C.nnz / float(A.nnz)
temp = np.sum(splitting)
if (temp == len(splitting)) or (temp == 0):
return 1
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
r_flag = False
fn, kwargs = unpack_arg(interp)
if fn == 'standard':
P = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'inject':
P = injection_interpolation(A, splitting, **kwargs)
elif fn == 'neumann':
P = neumann_ideal_interpolation(A, splitting, **kwargs)
elif fn == 'scaledAfc':
P = scaled_Afc_interpolation(A, splitting, **kwargs)
elif fn == 'air':
if isspmatrix_bsr(A):
temp_A = bsr_matrix(A.T)
P = local_AIR(temp_A, splitting, **kwargs)
P = bsr_matrix(P.T)
else:
temp_A = csr_matrix(A.T)
P = local_AIR(temp_A, splitting, **kwargs)
P = csr_matrix(P.T)
elif fn == 'restrict':
r_flag = True
else:
raise ValueError('unknown interpolation method (%s)' % interp)
levels[-1].complexity['interpolate'] += kwargs['cost'][0] * A.nnz / float(
A.nnz)
# Build restriction operator
fn, kwargs = unpack_arg(restrict)
if fn is None:
R = P.T
elif fn == 'air':
R = local_AIR(A, splitting, **kwargs)
elif fn == 'neumann':
R = neumann_AIR(A, splitting, **kwargs)
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
if isspmatrix_bsr(A):
R = R.T.tobsr()
else:
R = R.T.tocsr()
elif fn == 'inject': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
if isspmatrix_bsr(A):
R = R.T.tobsr()
else:
R = R.T.tocsr()
elif fn == 'standard':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'distance_two':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'direct':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
else:
raise ValueError('unknown restriction method (%s)' % restrict)
# If set P = R^T
if r_flag:
P = R.T
# Optional different interpolation for RAP
fn, kwargs = unpack_arg(coarse_grid_P)
if fn == 'standard':
P_temp = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P_temp = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P_temp = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P_temp = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'inject':
P_temp = injection_interpolation(A, splitting, **kwargs)
elif fn == 'neumann':
P_temp = neumann_ideal_interpolation(A, splitting, **kwargs)
elif fn == 'air':
if isspmatrix_bsr(A):
temp_A = bsr_matrix(A.T)
P_temp = local_AIR(temp_A, splitting, **kwargs)
P_temp = bsr_matrix(P_temp.T)
else:
temp_A = csr_matrix(A.T)
P_temp = local_AIR(temp_A, splitting, **kwargs)
P_temp = csr_matrix(P_temp.T)
else:
P_temp = P
# Optional different restriction for RAP
fn, kwargs = unpack_arg(coarse_grid_R)
if fn == 'air':
R_temp = local_AIR(A, splitting, **kwargs)
elif fn == 'neumann':
R_temp = neumann_AIR(A, splitting, **kwargs)
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R_temp = one_point_interpolation(A, temp_C, splitting, **kwargs)
if isspmatrix_bsr(A):
R_temp = R_temp.T.tobsr()
else:
R_temp = R_temp.T.tocsr()
elif fn == 'inject': # Don't need A^T or C^T here
R_temp = injection_interpolation(A, splitting, **kwargs)
if isspmatrix_bsr(A):
R_temp = R_temp.T.tobsr()
else:
R_temp = R_temp.T.tocsr()
elif fn == 'standard':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = standard_interpolation(temp_A, temp_C, splitting,
**kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = standard_interpolation(temp_A, temp_C, splitting,
**kwargs)
R_temp = R_temp.T.tocsr()
elif fn == 'distance_two':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = distance_two_interpolation(temp_A, temp_C, splitting,
**kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = distance_two_interpolation(temp_A, temp_C, splitting,
**kwargs)
R_temp = R_temp.T.tocsr()
elif fn == 'direct':
if isspmatrix_bsr(A):
temp_A = A.T.tobsr()
temp_C = C.T.tobsr()
R_temp = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tobsr()
else:
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R_temp = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R_temp = R_temp.T.tocsr()
else:
R_temp = R
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels[-1].splitting = splitting # C/F splitting
# Form coarse grid operator, get complexity
#levels[-1].complexity['RAP'] = mat_mat_complexity(R_temp,A) / float(A.nnz)
#RA = R_temp * A
#levels[-1].complexity['RAP'] += mat_mat_complexity(RA,P_temp) / float(A.nnz)
#A = RA * P_temp
# RL: RAP = R*(A*P)
levels[-1].complexity['RAP'] = mat_mat_complexity(A, P_temp) / float(A.nnz)
AP = A * P_temp
levels[-1].complexity['RAP'] += mat_mat_complexity(R_temp, AP) / float(
A.nnz)
A = R_temp * AP
# Make sure coarse-grid operator is in correct sparse format
if (isspmatrix_csr(P) and (not isspmatrix_csr(A))):
A = A.tocsr()
elif (isspmatrix_bsr(P) and (not isspmatrix_bsr(A))):
A = A.tobsr()
A.eliminate_zeros()
levels.append(multilevel_solver.level())
levels[-1].A = A
return 0
def extend_hierarchy(levels, strength, CF, interpolation, restriction, keep):
""" helper function for local methods """
A = levels[-1].A
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] = kwargs['cost'][0]
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = split.RS(C, **kwargs)
elif fn == 'PMIS':
splitting = split.PMIS(C, **kwargs)
elif fn == 'PMISc':
splitting = split.PMISc(C, **kwargs)
elif fn == 'CLJP':
splitting = split.CLJP(C, **kwargs)
elif fn == 'CLJPc':
splitting = split.CLJPc(C, **kwargs)
elif fn == 'CR':
splitting = CR(C, **kwargs)
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
levels[-1].complexity['CF'] = kwargs['cost'][0]
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
fn, kwargs = unpack_arg(interpolation)
if fn == 'standard':
P = standard_interpolation(A, C, splitting, **kwargs)
elif fn == 'distance_two':
P = distance_two_interpolation(A, C, splitting, **kwargs)
elif fn == 'direct':
P = direct_interpolation(A, C, splitting, **kwargs)
elif fn == 'one_point':
P = one_point_interpolation(A, C, splitting, **kwargs)
elif fn == 'injection':
P = injection_interpolation(A, splitting, **kwargs)
else:
raise ValueError('unknown interpolation method (%s)' % interpolation)
levels[-1].complexity['interpolate'] = kwargs['cost'][0]
# Generate the restriction matrix that maps from the fine-grid to the
# coarse-grid. Must make sure transpose matrices remain in CSR or BSR
fn, kwargs = unpack_arg(restriction)
if isspmatrix_csr(A):
if restriction == 'galerkin':
R = P.T.tocsr()
elif fn == 'standard':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'distance_two':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'direct':
temp_A = A.T.tocsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
R = R.T.tocsr()
elif fn == 'injection': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
R = R.T.tocsr()
else:
raise ValueError('unknown interpolation method (%s)' % interpolation)
else:
if restriction == 'galerkin':
R = P.T.tobsr()
elif fn == 'standard':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = standard_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'distance_two':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = distance_two_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'direct':
temp_A = A.T.tobsr()
temp_C = C.T.tocsr()
R = direct_interpolation(temp_A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'one_point': # Don't need A^T here
temp_C = C.T.tocsr()
R = one_point_interpolation(A, temp_C, splitting, **kwargs)
R = R.T.tobsr()
elif fn == 'injection': # Don't need A^T or C^T here
R = injection_interpolation(A, splitting, **kwargs)
R = R.T.tobsr()
else:
raise ValueError('unknown interpolation method (%s)' % interpolation)
levels[-1].complexity['restriction'] = kwargs['cost'][0]
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels[-1].splitting = splitting # C/F splitting
# Form coarse grid operator, get complexity
levels[-1].complexity['RAP'] = mat_mat_complexity(R,A) / float(A.nnz)
RA = R * A
levels[-1].complexity['RAP'] += mat_mat_complexity(RA,P) / float(A.nnz)
A = RA * P # Galerkin operator, Ac = RAP
# Make sure coarse-grid operator is in correct sparse format
if (isspmatrix_csr(P) and (not isspmatrix_csr(A))):
A = A.tocsr()
elif (isspmatrix_bsr(P) and (not isspmatrix_bsr(A))):
A = A.tobsr()
# Form next level through Galerkin product
levels.append(multilevel_solver.level())
levels[-1].A = A
N = 40
n = N * N
grid_dims = [N, N]
stencil = diffusion_stencil_2d(epsilon, theta)
A = stencil_grid(stencil, grid_dims, format='csr')
[d, d, A] = symmetric_rescaling(A)
A = csr_matrix(A)
B = np.kron(np.ones((A.shape[0] / 1, 1), dtype=A.dtype), np.eye(1))
tol = 1e-12 # Drop tolerance for singular values
if SA:
if SOC == 'evol':
C = evolution_strength_of_connection(A, B, epsilon=SOC_drop, k=2)
else:
SOC = 'symm'
C = symmetric_strength_of_connection(A, theta=SOC_drop)
AggOp, Cpts = standard_aggregation(C)
else:
splitting = CR(A, method='habituated')
Cpts = [i for i in range(0, n) if splitting[i] == 1]
Fpts = [i for i in range(0, n) if i not in Cpts]
num_Fpts = len(Fpts)
num_Cpts = len(Cpts)
num_bad_guys = 1
cf_ratio = float(num_Cpts) / num_Fpts
# Permutation matrix to sort rows
permute = identity(n, format='csr')
permute.indices = np.concatenate((Fpts, Cpts))
def extend_hierarchy(levels, strength, aggregate, smooth, improve_candidates,
diagonal_dominance=False, keep=True):
"""Service routine to implement the strength of connection, aggregation,
tentative prolongation construction, and prolongation smoothing. Called by
smoothed_aggregation_solver.
"""
A = levels[-1].A
B = levels[-1].B
if A.symmetry == "nonsymmetric":
AH = A.H.asformat(A.format)
BH = levels[-1].BH
# Compute the strength-of-connection matrix C, where larger
# C[i, j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength[len(levels)-1])
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
if 'B' in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'predefined':
C = kwargs['C'].tocsr()
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn == 'affinity':
C = affinity_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
levels[-1].complexity['strength'] = kwargs['cost'][0]
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
levels[-1].complexity['diag_dom'] = kwargs['cost'][0]
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate[len(levels)-1])
if fn == 'standard':
AggOp, Cnodes = standard_aggregation(C, **kwargs)
elif fn == 'naive':
AggOp, Cnodes = naive_aggregation(C, **kwargs)
elif fn == 'lloyd':
AggOp, Cnodes = lloyd_aggregation(C, **kwargs)
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
Cnodes = kwargs['Cnodes']
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
levels[-1].complexity['aggregation'] = kwargs['cost'][0] * (float(C.nnz)/A.nnz)
# Improve near nullspace candidates by relaxing on A B = 0
temp_cost = [0.0]
fn, kwargs = unpack_arg(improve_candidates[len(levels)-1],cost=False)
if fn is not None:
b = np.zeros((A.shape[0], 1), dtype=A.dtype)
B = relaxation_as_linear_operator((fn, kwargs), A, b, temp_cost) * B
levels[-1].B = B
if A.symmetry == "nonsymmetric":
BH = relaxation_as_linear_operator((fn, kwargs), AH, b, temp_cost) * BH
levels[-1].BH = BH
levels[-1].complexity['candidates'] = temp_cost[0] * B.shape[1]
# Compute the tentative prolongator, T, which is a tentative interpolation
# matrix from the coarse-grid to the fine-grid. T exactly interpolates
# B_fine[:, 0:blocksize(A)] = T B_coarse[:, 0:blocksize(A)].
# Orthogonalization complexity ~ 2nk^2, k = blocksize(A).
temp_cost=[0.0]
T, dummy = fit_candidates(AggOp, B[:, 0:blocksize(A)], cost=temp_cost)
del dummy
if A.symmetry == "nonsymmetric":
TH, dummyH = fit_candidates(AggOp, BH[:, 0:blocksize(A)], cost=temp_cost)
del dummyH
levels[-1].complexity['tentative'] = temp_cost[0]/A.nnz
# Create necessary root node matrices
Cpt_params = (True, get_Cpt_params(A, Cnodes, AggOp, T))
T = scale_T(T, Cpt_params[1]['P_I'], Cpt_params[1]['I_F'])
levels[-1].complexity['tentative'] += T.nnz / float(A.nnz)
if A.symmetry == "nonsymmetric":
TH = scale_T(TH, Cpt_params[1]['P_I'], Cpt_params[1]['I_F'])
levels[-1].complexity['tentative'] += TH.nnz / float(A.nnz)
# Set coarse grid near nullspace modes as injected fine grid near
# null-space modes
B = Cpt_params[1]['P_I'].T*levels[-1].B
if A.symmetry == "nonsymmetric":
BH = Cpt_params[1]['P_I'].T*levels[-1].BH
# Smooth the tentative prolongator, so that it's accuracy is greatly
# improved for algebraically smooth error.
fn, kwargs = unpack_arg(smooth[len(levels)-1])
if fn == 'energy':
P = energy_prolongation_smoother(A, T, C, B, levels[-1].B,
Cpt_params=Cpt_params, **kwargs)
elif fn is None:
P = T
else:
raise ValueError('unrecognized prolongation smoother \
method %s' % str(fn))
levels[-1].complexity['smooth_P'] = kwargs['cost'][0]
# Compute the restriction matrix R, which interpolates from the fine-grid
# to the coarse-grid. If A is nonsymmetric, then R must be constructed
# based on A.H. Otherwise R = P.H or P.T.
symmetry = A.symmetry
if symmetry == 'hermitian':
R = P.H
elif symmetry == 'symmetric':
R = P.T
elif symmetry == 'nonsymmetric':
fn, kwargs = unpack_arg(smooth[len(levels)-1])
if fn == 'energy':
R = energy_prolongation_smoother(AH, TH, C, BH, levels[-1].BH,
Cpt_params=Cpt_params, **kwargs)
R = R.H
levels[-1].complexity['smooth_R'] = kwargs['cost'][0]
elif fn is None:
R = T.H
else:
raise ValueError('unrecognized prolongation smoother \
method %s' % str(fn))
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].AggOp = AggOp # aggregation operator
levels[-1].T = T # tentative prolongator
levels[-1].Fpts = Cpt_params[1]['Fpts'] # Fpts
levels[-1].P_I = Cpt_params[1]['P_I'] # Injection operator
levels[-1].I_F = Cpt_params[1]['I_F'] # Identity on F-pts
levels[-1].I_C = Cpt_params[1]['I_C'] # Identity on C-pts
levels[-1].P = P # smoothed prolongator
levels[-1].R = R # restriction operator
levels[-1].Cpts = Cpt_params[1]['Cpts'] # Cpts (i.e., rootnodes)
# Form coarse grid operator, get complexity
levels[-1].complexity['RAP'] = mat_mat_complexity(R,A) / float(A.nnz)
RA = R * A
levels[-1].complexity['RAP'] += mat_mat_complexity(RA,P) / float(A.nnz)
A = RA * P # Galerkin operator, Ac = RAP
A.symmetry = symmetry
levels.append(multilevel_solver.level())
levels[-1].A = A
levels[-1].B = B # right near nullspace candidates
if A.symmetry == "nonsymmetric":
levels[-1].BH = BH # left near nullspace candidates
def extend_hierarchy(levels, strength, CF, keep):
""" helper function for local methods """
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
# Compute the strength-of-connection matrix C, where larger
# C[i,j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength)
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
C = evolution_strength_of_connection(A, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn is None:
C = A
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Generate the C/F splitting
fn, kwargs = unpack_arg(CF)
if fn == 'RS':
splitting = split.RS(C)
elif fn == 'PMIS':
splitting = split.PMIS(C)
elif fn == 'PMISc':
splitting = split.PMISc(C)
elif fn == 'CLJP':
splitting = split.CLJP(C)
elif fn == 'CLJPc':
splitting = split.CLJPc(C)
else:
raise ValueError('unknown C/F splitting method (%s)' % CF)
# Generate the interpolation matrix that maps from the coarse-grid to the
# fine-grid
P = direct_interpolation(A, C, splitting)
# Generate the restriction matrix that maps from the fine-grid to the
# coarse-grid
R = P.T.tocsr()
# Store relevant information for this level
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].splitting = splitting # C/F splitting
levels[-1].P = P # prolongation operator
levels[-1].R = R # restriction operator
levels.append(multilevel_solver.level())
# Form next level through Galerkin product
A = R * A * P
levels[-1].A = A
def extend_hierarchy(levels, strength, aggregate, smooth, improve_candidates,
diagonal_dominance=False, keep=True, test_ind=0):
"""Service routine to implement the strength of connection, aggregation,
tentative prolongation construction, and prolongation smoothing. Called by
smoothed_aggregation_solver.
"""
def unpack_arg(v):
if isinstance(v, tuple):
return v[0], v[1]
else:
return v, {}
A = levels[-1].A
B = levels[-1].B
if A.symmetry == "nonsymmetric":
AH = A.H.asformat(A.format)
BH = levels[-1].BH
# Improve near nullspace candidates by relaxing on A B = 0
fn, kwargs = unpack_arg(improve_candidates[len(levels)-1])
if fn is not None:
b = np.zeros((A.shape[0], 1), dtype=A.dtype)
B = relaxation_as_linear_operator((fn, kwargs), A, b) * B
levels[-1].B = B
if A.symmetry == "nonsymmetric":
BH = relaxation_as_linear_operator((fn, kwargs), AH, b) * BH
levels[-1].BH = BH
# Compute the strength-of-connection matrix C, where larger
# C[i, j] denote stronger couplings between i and j.
fn, kwargs = unpack_arg(strength[len(levels)-1])
if fn == 'symmetric':
C = symmetric_strength_of_connection(A, **kwargs)
elif fn == 'classical':
C = classical_strength_of_connection(A, **kwargs)
elif fn == 'distance':
C = distance_strength_of_connection(A, **kwargs)
elif (fn == 'ode') or (fn == 'evolution'):
if 'B' in kwargs:
C = evolution_strength_of_connection(A, **kwargs)
else:
C = evolution_strength_of_connection(A, B, **kwargs)
elif fn == 'energy_based':
C = energy_based_strength_of_connection(A, **kwargs)
elif fn == 'predefined':
C = kwargs['C'].tocsr()
elif fn == 'algebraic_distance':
C = algebraic_distance(A, **kwargs)
elif fn is None:
C = A.tocsr()
else:
raise ValueError('unrecognized strength of connection method: %s' %
str(fn))
# Avoid coarsening diagonally dominant rows
flag, kwargs = unpack_arg(diagonal_dominance)
if flag:
C = eliminate_diag_dom_nodes(A, C, **kwargs)
# Compute the aggregation matrix AggOp (i.e., the nodal coarsening of A).
# AggOp is a boolean matrix, where the sparsity pattern for the k-th column
# denotes the fine-grid nodes agglomerated into k-th coarse-grid node.
fn, kwargs = unpack_arg(aggregate[len(levels)-1])
if fn == 'standard':
AggOp, Cnodes = standard_aggregation(C, **kwargs)
elif fn == 'naive':
AggOp, Cnodes = naive_aggregation(C, **kwargs)
elif fn == 'lloyd':
AggOp, Cnodes = lloyd_aggregation(C, **kwargs)
elif fn == 'pairwise':
AggOp, Cnodes = pairwise_aggregation(A, B, **kwargs)
elif fn == 'predefined':
AggOp = kwargs['AggOp'].tocsr()
Cnodes = kwargs['Cnodes']
else:
raise ValueError('unrecognized aggregation method %s' % str(fn))
# ----------------------------------------------------------------------------- #
# ------------------- New ideal interpolation constructed -------------------- #
# ----------------------------------------------------------------------------- #
# pdb.set_trace()
# splitting = CR(A)
# Cpts = [i for i in range(0,AggOp.shape[0]) if splitting[i]==1]
# Compute prolongation operator.
if test_ind==0:
T = new_ideal_interpolation(A=A, AggOp=AggOp, Cnodes=Cnodes, B=B[:, 0:blocksize(A)], SOC=C)
else:
T = py_ideal_interpolation(A=A, AggOp=AggOp, Cnodes=Cnodes, B=B[:, 0:blocksize(A)], SOC=C)
print "\nSize of sparsity pattern - ", T.nnz
# Smooth the tentative prolongator, so that it's accuracy is greatly
# improved for algebraically smooth error.
# fn, kwargs = unpack_arg(smooth[len(levels)-1])
# if fn == 'jacobi':
# P = jacobi_prolongation_smoother(A, T, C, B, **kwargs)
# elif fn == 'richardson':
# P = richardson_prolongation_smoother(A, T, **kwargs)
# elif fn == 'energy':
# P = energy_prolongation_smoother(A, T, C, B, None, (False, {}),
# **kwargs)
# elif fn is None:
# P = T
# else:
# raise ValueError('unrecognized prolongation smoother method %s' %
# str(fn))
P = T
# ----------------------------------------------------------------------------- #
# ----------------------------------------------------------------------------- #
# Compute the restriction matrix R, which interpolates from the fine-grid
# to the coarse-grid. If A is nonsymmetric, then R must be constructed
# based on A.H. Otherwise R = P.H or P.T.
symmetry = A.symmetry
if symmetry == 'hermitian':
# symmetrically scale out the diagonal, include scaling in P, R
A = P.H * A * P
[dum, Dinv, dum] = symmetric_rescaling(A,copy=False)
P = bsr_matrix(P * diags(Dinv,offsets=0,format='csr'), blocksize=A.blocksize)
del dum
R = P.H
elif symmetry == 'symmetric':
# symmetrically scale out the diagonal, include scaling in P, R
A = P.T * A * P
[dum, Dinv, dum] = symmetric_rescaling(A,copy=False)
P = bsr_matrix(P * diags(Dinv,offsets=0,format='csr'), blocksize=A.blocksize)
del dum
R = P.T
elif symmetry == 'nonsymmetric':
raise TypeError('New ideal interpolation not implemented for non-symmetric matrix.')
if keep:
levels[-1].C = C # strength of connection matrix
levels[-1].AggOp = AggOp # aggregation operator
levels[-1].Fpts = [i for i in range(0,AggOp.shape[0]) if i not in Cnodes]
levels[-1].P = P # smoothed prolongator
levels[-1].R = R # restriction operator
levels[-1].Cpts = Cnodes # Cpts (i.e., rootnodes)
levels.append(multilevel_solver.level())
A.symmetry = symmetry
levels[-1].A = A
levels[-1].B = R*B # right near nullspace candidates
test = A.tocsr()
print "\nSize of coarse operator - ", test.nnz
if A.symmetry == "nonsymmetric":
levels[-1].BH = BH # left near nullspace candidates
