def testFullyConnectedLayerParamsTensorToMat2d(self):
with ops.Graph().as_default(), self.test_session() as sess:
random_seed.set_random_seed(200)
layer_params = self._fully_connected_layer_params()
output = utils.layer_params_to_mat2d(layer_params[0])
self.assertListEqual([2, 2], output.get_shape().as_list())
self.assertAllClose(sess.run(output), np.array([[1., 2.], [4., 3.]]))
def testConvLayerParamsTupleToMat2d(self):
with ops.Graph().as_default():
random_seed.set_random_seed(200)
layer_params = self._conv_layer_params()
output = utils.layer_params_to_mat2d(layer_params)
self.assertListEqual([2 * 2 * 3 + 1, 4],
output.get_shape().as_list())
def testFullyConnectedLayerParamsTensorToMat2d(self):
with ops.Graph().as_default(), self.test_session() as sess:
random_seed.set_random_seed(200)
layer_params = self._fully_connected_layer_params()
output = utils.layer_params_to_mat2d(layer_params[0])
self.assertListEqual([2, 2], output.get_shape().as_list())
self.assertAllClose(sess.run(output), np.array([[1., 2.], [4.,
3.]]))
def multiply_matpower(self, vector, exp):
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = self._output_factor.right_multiply_matpower(
reshaped_vector, exp, self._output_damping_func)
reshaped_out = self._input_factor.left_multiply_matpower(
reshaped_out, exp, self._input_damping_func)
if self._renorm_coeff != 1.0:
reshaped_out *= math_ops.cast(
self._renorm_coeff**exp, dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_matpower(self, vector, exp):
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = self._output_factor.right_multiply_matpower(
reshaped_vector, exp, self._output_damping_func)
reshaped_out = self._input_factor.left_multiply_matpower(
reshaped_out, exp, self._input_damping_func)
if self._renorm_coeff != 1.0:
renorm_coeff = math_ops.cast(self._renorm_coeff, dtype=reshaped_out.dtype)
reshaped_out *= math_ops.cast(renorm_coeff**exp, dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_inverse(self, vector):
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = self._output_factor.right_multiply_inverse(
reshaped_vector, self._output_damping)
reshaped_out = self._input_factor.left_multiply_inverse(
reshaped_out, self._input_damping)
if self._renorm_coeff != 1.0:
reshaped_out /= math_ops.cast(self._renorm_coeff,
dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_inverse(self, vector):
left_factor_inv = self._input_factor.get_inverse(self._input_damping)
right_factor_inv = self._output_factor.get_inverse(self._output_damping)
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = math_ops.matmul(left_factor_inv,
math_ops.matmul(reshaped_vector,
right_factor_inv))
if self._renorm_coeff != 1.0:
reshaped_out /= math_ops.cast(
self._renorm_coeff, dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector):
left_factor = self._input_factor.get_cov()
right_factor = self._output_factor.get_cov()
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = (math_ops.matmul(reshaped_vector, right_factor) +
self._output_damping * reshaped_vector)
reshaped_out = (math_ops.matmul(left_factor, reshaped_out) +
self._input_damping * reshaped_out)
if self._renorm_coeff != 1.0:
reshaped_out *= math_ops.cast(self._renorm_coeff,
dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector):
left_factor = self._input_factor.get_cov()
right_factor = self._output_factor.get_cov()
reshaped_vector = utils.layer_params_to_mat2d(vector)
reshaped_out = (math_ops.matmul(reshaped_vector, right_factor) +
self._output_damping * reshaped_vector)
reshaped_out = (math_ops.matmul(left_factor, reshaped_out) +
self._input_damping * reshaped_out)
if self._renorm_coeff != 1.0:
reshaped_out *= math_ops.cast(
self._renorm_coeff, dtype=reshaped_out.dtype)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector):
"""Approximate damped Fisher-vector product.
Args:
vector: Tensor or 2-tuple of Tensors. if self._has_bias, Tensor of shape
[input_size, output_size] corresponding to layer's weights. If not, a
2-tuple of the former and a Tensor of shape [output_size] corresponding
to the layer's bias.
Returns:
Tensor of the same shape, corresponding to the Fisher-vector product.
"""
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = reshaped_vect * (self._factor.get_cov() + self._damping)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector):
"""Approximate damped Fisher-vector product.
Args:
vector: Tensor or 2-tuple of Tensors. if self._has_bias, Tensor of shape
[input_size, output_size] corresponding to layer's weights. If not, a
2-tuple of the former and a Tensor of shape [output_size] corresponding
to the layer's bias.
Returns:
Tensor of the same shape, corresponding to the Fisher-vector product.
"""
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = reshaped_vect * (self._factor.get_cov() + self._damping)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_matpower(self, vector, exp):
"""Multiplies the vector by the (damped) matrix-power of the block.
Args:
vector: Tensor or 2-tuple of Tensors. if self._has_bias, Tensor of shape
[input_size, output_size] corresponding to layer's weights. If not, a
2-tuple of the former and a Tensor of shape [output_size] corresponding
to the layer's bias.
exp: A scalar representing the power to raise the block before multiplying
it by the vector.
Returns:
The vector left-multiplied by the (damped) matrix-power of the block.
"""
reshaped_vec = utils.layer_params_to_mat2d(vector)
reshaped_out = self._factor.left_multiply_matpower(
reshaped_vec, exp, self._damping_func)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_matpower(self, vector, exp):
"""Multiplies the vector by the (damped) matrix-power of the block.
Args:
vector: Tensor or 2-tuple of Tensors. if self._has_bias, Tensor of shape
[input_size, output_size] corresponding to layer's weights. If not, a
2-tuple of the former and a Tensor of shape [output_size] corresponding
to the layer's bias.
exp: A scalar representing the power to raise the block before multiplying
it by the vector.
Returns:
The vector left-multiplied by the (damped) matrix-power of the block.
"""
reshaped_vec = utils.layer_params_to_mat2d(vector)
reshaped_out = self._factor.left_multiply_matpower(
reshaped_vec, exp, self._damping_func)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_inverse(self, vector):
# pylint: disable=invalid-name
Z = utils.layer_params_to_mat2d(vector)
# Derivations were done for "batch_dim==1" case so we need to convert to
# that orientation:
Z = array_ops.transpose(Z)
if self._option == SeriesFBApproximation.option1:
# Note that L_A = A0^(-1/2) * U_A and L_G = G0^(-1/2) * U_G.
L_A, psi_A = self._input_factor.get_option1quants(self._damping_input)
L_G, psi_G = self._output_factor.get_option1quants(self._damping_output)
def gamma(x):
# We are assuming that each case has the same number of time-steps.
# If this stops being the case one shouldn't simply replace this T
# with its average value. Instead, one needs to go back to the
# definition of the gamma function from the paper.
T = self._num_timesteps
return (1 - x)**2 / (T * (1 - x**2) - 2 * x * (1 - x**T))
# Y = gamma( psi_G*psi_A^T ) (computed element-wise)
# Even though Y is Z-independent we are recomputing it from the psi's
# each since Y depends on both A and G quantities, and it is relatively
# cheap to compute.
Y = gamma(array_ops.reshape(psi_G, [int(psi_G.shape[0]), -1]) * psi_A)
# Z = L_G^T * Z * L_A
# This is equivalent to the following computation from the original
# pseudo-code:
# Z = G0^(-1/2) * Z * A0^(-1/2)
# Z = U_G^T * Z * U_A
Z = math_ops.matmul(L_G, math_ops.matmul(Z, L_A), transpose_a=True)
# Z = Z .* Y
Z *= Y
# Z = L_G * Z * L_A^T
# This is equivalent to the following computation from the original
# pseudo-code:
# Z = U_G * Z * U_A^T
# Z = G0^(-1/2) * Z * A0^(-1/2)
Z = math_ops.matmul(L_G, math_ops.matmul(Z, L_A, transpose_b=True))
elif self._option == SeriesFBApproximation.option2:
# Note that P_A = A_1^T * A_0^(-1) and P_G = G_1^T * G_0^(-1),
# and K_A = A_0^(-1/2) * E_A and K_G = G_0^(-1/2) * E_G.
P_A, K_A, mu_A = self._input_factor.get_option2quants(self._damping_input)
P_G, K_G, mu_G = self._output_factor.get_option2quants(
self._damping_output)
# Our approach differs superficially from the pseudo-code in the paper
# in order to reduce the total number of matrix-matrix multiplies.
# In particular, the first three computations in the pseudo code are
# Z = G0^(-1/2) * Z * A0^(-1/2)
# Z = Z - hPsi_G^T * Z * hPsi_A
# Z = E_G^T * Z * E_A
# Noting that hPsi = C0^(-1/2) * C1 * C0^(-1/2), so that
# C0^(-1/2) * hPsi = C0^(-1) * C1 * C0^(-1/2) = P^T * C0^(-1/2)
# the entire computation can be written as
# Z = E_G^T * (G0^(-1/2) * Z * A0^(-1/2)
# - hPsi_G^T * G0^(-1/2) * Z * A0^(-1/2) * hPsi_A) * E_A
# = E_G^T * (G0^(-1/2) * Z * A0^(-1/2)
# - G0^(-1/2) * P_G * Z * P_A^T * A0^(-1/2)) * E_A
# = E_G^T * G0^(-1/2) * Z * A0^(-1/2) * E_A
# - E_G^T* G0^(-1/2) * P_G * Z * P_A^T * A0^(-1/2) * E_A
# = K_G^T * Z * K_A - K_G^T * P_G * Z * P_A^T * K_A
# This final expression is computed by the following two lines:
# Z = Z - P_G * Z * P_A^T
Z -= math_ops.matmul(P_G, math_ops.matmul(Z, P_A, transpose_b=True))
# Z = K_G^T * Z * K_A
Z = math_ops.matmul(K_G, math_ops.matmul(Z, K_A), transpose_a=True)
# Z = Z ./ (1*1^T - mu_G*mu_A^T)
# Be careful with the outer product. We don't want to accidentally
# make it an inner-product instead.
tmp = 1.0 - array_ops.reshape(mu_G, [int(mu_G.shape[0]), -1]) * mu_A
# Prevent some numerical issues by setting any 0.0 eigs to 1.0
tmp += 1.0 * math_ops.cast(math_ops.equal(tmp, 0.0), dtype=tmp.dtype)
Z /= tmp
# We now perform the transpose/reverse version of the operations
# derived above, whose derivation from the original pseudo-code is
# analgous.
# Z = K_G * Z * K_A^T
Z = math_ops.matmul(K_G, math_ops.matmul(Z, K_A, transpose_b=True))
# Z = Z - P_G^T * Z * P_A
Z -= math_ops.matmul(P_G, math_ops.matmul(Z, P_A), transpose_a=True)
# Z = normalize (1/E[T]) * Z
# Note that this normalization is done because we compute the statistics
# by averaging, not summing, over time. (And the gradient is presumably
# summed over time, not averaged, and thus their scales are different.)
Z /= math_ops.cast(self._num_timesteps, Z.dtype)
# Convert back to the "batch_dim==0" orientation.
Z = array_ops.transpose(Z)
return utils.mat2d_to_layer_params(vector, Z)
def multiply_matpower(self, vector, exp):
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = self._factor.left_multiply_matpower(
reshaped_vect, exp, self._damping_func)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_matpower(self, vector, exp):
if exp != -1:
raise NotImplementedError("FullyConnectedSeriesFB only supports inverse"
"multiplications.")
# pylint: disable=invalid-name
Z = utils.layer_params_to_mat2d(vector)
# Derivations were done for "batch_dim==1" case so we need to convert to
# that orientation:
Z = array_ops.transpose(Z)
if self._option == SeriesFBApproximation.option1:
# Note that L_A = A0^(-1/2) * U_A and L_G = G0^(-1/2) * U_G.
L_A, psi_A = self._input_factor.get_option1quants(
self._input_damping_func)
L_G, psi_G = self._output_factor.get_option1quants(
self._output_damping_func)
def gamma(x):
# We are assuming that each case has the same number of time-steps.
# If this stops being the case one shouldn't simply replace this T
# with its average value. Instead, one needs to go back to the
# definition of the gamma function from the paper.
T = self._num_timesteps
return (1 - x)**2 / (T * (1 - x**2) - 2 * x * (1 - x**T))
# Y = gamma( psi_G*psi_A^T ) (computed element-wise)
# Even though Y is Z-independent we are recomputing it from the psi's
# each since Y depends on both A and G quantities, and it is relatively
# cheap to compute.
Y = gamma(array_ops.reshape(psi_G, [int(psi_G.shape[0]), -1]) * psi_A)
# Z = L_G^T * Z * L_A
# This is equivalent to the following computation from the original
# pseudo-code:
# Z = G0^(-1/2) * Z * A0^(-1/2)
# Z = U_G^T * Z * U_A
Z = math_ops.matmul(L_G, math_ops.matmul(Z, L_A), transpose_a=True)
# Z = Z .* Y
Z *= Y
# Z = L_G * Z * L_A^T
# This is equivalent to the following computation from the original
# pseudo-code:
# Z = U_G * Z * U_A^T
# Z = G0^(-1/2) * Z * A0^(-1/2)
Z = math_ops.matmul(L_G, math_ops.matmul(Z, L_A, transpose_b=True))
elif self._option == SeriesFBApproximation.option2:
# Note that P_A = A_1^T * A_0^(-1) and P_G = G_1^T * G_0^(-1),
# and K_A = A_0^(-1/2) * E_A and K_G = G_0^(-1/2) * E_G.
P_A, K_A, mu_A = self._input_factor.get_option2quants(
self._input_damping_func)
P_G, K_G, mu_G = self._output_factor.get_option2quants(
self._output_damping_func)
# Our approach differs superficially from the pseudo-code in the paper
# in order to reduce the total number of matrix-matrix multiplies.
# In particular, the first three computations in the pseudo code are
# Z = G0^(-1/2) * Z * A0^(-1/2)
# Z = Z - hPsi_G^T * Z * hPsi_A
# Z = E_G^T * Z * E_A
# Noting that hPsi = C0^(-1/2) * C1 * C0^(-1/2), so that
# C0^(-1/2) * hPsi = C0^(-1) * C1 * C0^(-1/2) = P^T * C0^(-1/2)
# the entire computation can be written as
# Z = E_G^T * (G0^(-1/2) * Z * A0^(-1/2)
# - hPsi_G^T * G0^(-1/2) * Z * A0^(-1/2) * hPsi_A) * E_A
# = E_G^T * (G0^(-1/2) * Z * A0^(-1/2)
# - G0^(-1/2) * P_G * Z * P_A^T * A0^(-1/2)) * E_A
# = E_G^T * G0^(-1/2) * Z * A0^(-1/2) * E_A
# - E_G^T* G0^(-1/2) * P_G * Z * P_A^T * A0^(-1/2) * E_A
# = K_G^T * Z * K_A - K_G^T * P_G * Z * P_A^T * K_A
# This final expression is computed by the following two lines:
# Z = Z - P_G * Z * P_A^T
Z -= math_ops.matmul(P_G, math_ops.matmul(Z, P_A, transpose_b=True))
# Z = K_G^T * Z * K_A
Z = math_ops.matmul(K_G, math_ops.matmul(Z, K_A), transpose_a=True)
# Z = Z ./ (1*1^T - mu_G*mu_A^T)
# Be careful with the outer product. We don't want to accidentally
# make it an inner-product instead.
tmp = 1.0 - array_ops.reshape(mu_G, [int(mu_G.shape[0]), -1]) * mu_A
# Prevent some numerical issues by setting any 0.0 eigs to 1.0
tmp += 1.0 * math_ops.cast(math_ops.equal(tmp, 0.0), dtype=tmp.dtype)
Z /= tmp
# We now perform the transpose/reverse version of the operations
# derived above, whose derivation from the original pseudo-code is
# analgous.
# Z = K_G * Z * K_A^T
Z = math_ops.matmul(K_G, math_ops.matmul(Z, K_A, transpose_b=True))
# Z = Z - P_G^T * Z * P_A
Z -= math_ops.matmul(P_G, math_ops.matmul(Z, P_A), transpose_a=True)
# Z = normalize (1/E[T]) * Z
# Note that this normalization is done because we compute the statistics
# by averaging, not summing, over time. (And the gradient is presumably
# summed over time, not averaged, and thus their scales are different.)
Z /= math_ops.cast(self._num_timesteps, Z.dtype)
# Convert back to the "batch_dim==0" orientation.
Z = array_ops.transpose(Z)
return utils.mat2d_to_layer_params(vector, Z)
def multiply(self, vector):
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = reshaped_vect * (self._factor.get_cov() + self._damping)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector): reshaped_vect = utils.layer_params_to_mat2d(vector) reshaped_out = reshaped_vect * (self._factor.get_cov() + self._damping) return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply(self, vector):
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = self._factor.left_multiply(
reshaped_vect, self._damping)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def multiply_matpower(self, vector, exp):
reshaped_vect = utils.layer_params_to_mat2d(vector)
reshaped_out = self._factor.left_multiply_matpower(
reshaped_vect, exp, self._damping_func)
return utils.mat2d_to_layer_params(vector, reshaped_out)
def testConvLayerParamsTupleToMat2d(self):
with ops.Graph().as_default():
random_seed.set_random_seed(200)
layer_params = self._conv_layer_params()
output = utils.layer_params_to_mat2d(layer_params)
self.assertListEqual([2 * 2 * 3 + 1, 4], output.get_shape().as_list())
