def nbody_prototype(mesh,
infield=False,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps,
dtype=tf.float32):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
# Compute a few things first, using simple tensorflow
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
# Parameters of the large scales decomposition
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin, shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
# Begin simulation
## Compute initial initial conditions distributed
input_field = tf.placeholder(dtype, [batch_size, nc, nc, nc])
if infield:
initc = mtf.import_tf_tensor(mesh, input_field, shape=part_shape)
else:
initc = mtfpm.linear_field(mesh, shape, bs, nc, pk, kv)
# Here we can run our nbody
if FLAGS.nbody:
state = mtfpm.lpt_init_single(
initc,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# Here we can run our nbody
final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape,
kv_lr, halo_size)
else:
final_state = mtfpm.lpt_init_single(
initc,
stages[-1],
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4],
final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
final_field = mtf.slicewise(
lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=dtype,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
return initc, final_field, input_field
def lpt_prototype(mesh,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
if halo_size >= 0.5 * min(nc // n_block_x, nc // n_block_y,
nc // n_block_z):
new_size = int(0.5 *
min(nc // n_block_x, nc // n_block_y, nc // n_block_z))
print('WARNING: REDUCING HALO SIZE from %d to %d' %
(halo_size, new_size))
halo_size = new_size
# Parameters of the large scales decomposition
downsampling_factor = 0
lnc = nc // 2**downsampling_factor
#
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype('float32'), shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
# Begin simulation
initc = mtfpm.linear_field(mesh, shape, bs, nc, pk, kv)
# # Reshaping array into high resolution mesh
# field = mtf.slicewise(lambda x:tf.expand_dims(tf.expand_dims(tf.expand_dims(x, axis=1),axis=1),axis=1),
# [initc],
# output_dtype=tf.float32,
# output_shape=hr_shape,
# name='my_reshape',
# splittable_dims=lr_shape[:-1]+hr_shape[1:4]+part_shape[1:3])
#
state = mtfpm.lpt_init_single(
initc,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# Here we can run our nbody
final_state = state #mtfpm.nbody(state, stages, lr_shape, hr_shape, k_dims, kv_lr, kv_hr, halo_size, downsampling_factor=downsampling_factor)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4],
final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
#final_field = mtf.reshape(final_field, [batch_dim, fx_dim, fy_dim, fz_dim])
# Hack usisng custom reshape because mesh is pretty dumb
final_field = mtf.slicewise(
lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=tf.float32,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
return initc, final_field
def benchmark_model(mesh):
"""
Initializes a 3D volume with random noise, and execute a forward FFT
"""
# Setup parameters
bs = FLAGS.box_size
nc = FLAGS.cube_size
batch_size = FLAGS.batch_size
a0 = FLAGS.a0
a = 1.0
nsteps = FLAGS.pm_steps
# Compute a few things first, using simple tensorflow
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Initialize the integration steps
stages = np.linspace(FLAGS.a0, 1.0, FLAGS.pm_steps, endpoint=True)
# Generate a batch of 3D initial conditions
initial_conditions = flowpm.linear_field(
nc, # size of the cube
bs, # Physical size of the cube
ipklin, # Initial power spectrum
batch_size=batch_size)
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
from flowpm.kernels import laplace_kernel, gradient_kernel
lap = tf.cast(laplace_kernel(kvec), tf.complex64)
grad_x = gradient_kernel(kvec, 0)
grad_y = gradient_kernel(kvec, 1)
grad_z = gradient_kernel(kvec, 2)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = 8
n_block_y = 4
n_block_z = 1
halo_size = 4
# Parameters of the large scales decomposition
downsampling_factor = 2
lnc = nc // 2**downsampling_factor
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
# Dimensions of the low resolution grid
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
batch_dim = mtf.Dimension("batch", batch_size)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype('float32'), shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
# kvec for high resolution blocks
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
initc = mtfpm.linear_field(mesh, shape, bs, nc, pk, kv)
state = mtfpm.lpt_init_single(
initc,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
#state = mtfpm.lpt_init(low, high, 0.1, kv_lr, kv_hr, halo_size, hr_shape, lr_shape,
# part_shape[1:], downsampling_factor=downsampling_factor, antialias=True,)
# Here we can run our nbody
final_state = state #mtfpm.nbody(state, stages, lr_shape, hr_shape, kv_lr, kv_hr, halo_size, downsampling_factor=downsampling_factor)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4], final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
#final_field = mtf.reshape(final_field, [batch_dim, fx_dim, fy_dim, fz_dim])
# Hack usisng custom reshape because mesh is pretty dumb
final_field = mtf.slicewise(lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=tf.float32,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
return mtf.reduce_sum(final_field)
def lpt_prototype(mesh,
initial_conditions,
derivs,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
stages = np.linspace(a0, a, nsteps, endpoint=True)
lap, grad_x, grad_y, grad_z = derivs
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
# Parameters of the large scales decomposition
downsampling_factor = 0
lnc = nc // 2**downsampling_factor
#
ffx_dim = mtf.Dimension("fnx", nc)
ffy_dim = mtf.Dimension("fny", nc)
ffz_dim = mtf.Dimension("fnz", nc)
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype('float32'), shape=[pk_dim])
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
field = mtf.import_tf_tensor(mesh, initial_conditions, shape=part_shape)
state = mtfpm.lpt_init_single(
field,
a,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
print('TOTO', state)
# Here we can run our nbody
final_state = state
# final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape,
# kv_lr, halo_size)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4],
final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
#final_field = mtf.reshape(final_field, [batch_dim, fx_dim, fy_dim, fz_dim])
# Hack usisng custom reshape because mesh is pretty dumb
final_field = mtf.slicewise(
lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=tf.float32,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
final_field = mtf.reshape(final_field,
[batch_dim, ffx_dim, ffy_dim, ffz_dim])
return final_field
def recon_model(mesh,
data,
bparams,
ipkerror,
R0,
x0,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps,
dtype=tf.float32):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
b1, b2, bs2 = bparams
kerror, perror = ipkerror[0].astype(np.float32), ipkerror[1].astype(
np.float32)
if dtype == tf.float32:
npdtype = "float32"
cdtype = tf.complex64
elif dtype == tf.float64:
npdtype = "float64"
cdtype = tf.complex128
print("Dtype : ", dtype, npdtype)
# Compute a few things first, using simple tensorflow
kny = 1 * np.pi * nc / bs
R1, R2 = 3., 3 * 1.2
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
if halo_size >= 0.5 * min(nc // n_block_x, nc // n_block_y,
nc // n_block_z):
new_size = int(0.5 *
min(nc // n_block_x, nc // n_block_y, nc // n_block_z))
print('WARNING: REDUCING HALO SIZE from %d to %d' %
(halo_size, new_size))
halo_size = new_size
# Parameters of the large scales decomposition
scalar = mtf.Dimension("scalar", 1)
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
#k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
klin = np.loadtxt('..//data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('..//data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype(npdtype), shape=[pk_dim])
pke_dim = mtf.Dimension("epk", len(perror))
pkerror = mtf.import_tf_tensor(mesh,
perror.astype(npdtype),
shape=[pke_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
splittables = lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3]
#
# Begin simulation
if x0 is None:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.random_normal_initializer(
mean=0.0, stddev=1, seed=None))
else:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.constant_initializer(x0))
state = mtfpm.lpt_init_single(
fieldvar,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape, kv_lr,
halo_size)
# paint the field
final_field = mtf.zeros(mesh, shape=part_shape)
final_field = mcomp.cic_paint_fr(final_field, final_state, part_shape,
hr_shape, halo_size, splittables, mesh)
##
#Get the fields for bias
hr_field = mcomp.fr_to_hr(final_field, hr_shape, halo_size, splittables,
mesh)
mstate = mpm.mtf_indices(hr_field.mesh,
shape=part_shape[1:],
dtype=tf.float32)
X = mtf.einsum([mtf.ones(hr_field.mesh, [batch_dim]), mstate],
output_shape=[batch_dim] + mstate.shape[:])
k_dims_pr = [d.shape[0] for d in kv]
k_dims_pr = [k_dims_pr[2], k_dims_pr[0], k_dims_pr[1]]
tfnc, tfbs = cswisef.float_to_mtf(nc * 1., mesh,
scalar), cswisef.float_to_mtf(
bs, mesh, scalar)
#
initc = fieldvar
d0 = initc - mtf.reduce_mean(initc)
#
d2 = initc * initc
d2 = d2 - mtf.reduce_mean(d2)
#
cfield = mesh_utils.r2c3d(d0, k_dims_pr, dtype=cdtype)
shearfield = mtf.zeros(mesh, shape=part_shape)
shearfield = shear(shearfield, cfield, kv, tfnc, tfbs)
s2 = shearfield - mtf.reduce_mean(shearfield)
dread = mcomp.cic_readout_fr(d0, [X],
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
d2read = mcomp.cic_readout_fr(d2, [X],
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
s2read = mcomp.cic_readout_fr(s2, [X],
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
ed, ed2, es2 = mtf.zeros(mesh, shape=part_shape), mtf.zeros(
mesh, shape=part_shape), mtf.zeros(mesh, shape=part_shape)
ed = mcomp.cic_paint_fr(ed,
final_state,
output_shape=part_shape,
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh,
weights=dread)
ed2 = mcomp.cic_paint_fr(ed2,
final_state,
output_shape=part_shape,
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh,
weights=d2read)
es2 = mcomp.cic_paint_fr(es2,
final_state,
output_shape=part_shape,
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh,
weights=s2read)
model = ed * b1 + ed2 * b2 + es2 * bs2
mtfdata = mtf.import_tf_tensor(mesh,
tf.convert_to_tensor(data),
shape=shape)
diff = model - mtfdata
# Get prior
k_dims_pr = [d.shape[0] for d in kv]
k_dims_pr = [k_dims_pr[2], k_dims_pr[0], k_dims_pr[1]]
cfield = mesh_utils.r2c3d(fieldvar, k_dims_pr, dtype=cdtype)
def _cwise_prior(kfield, pk, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = tf.sqrt((kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2)
kshape = kk.shape
kk = tf.reshape(kk, [-1])
pkmesh = tfp.math.interp_regular_1d_grid(
x=kk,
x_ref_min=1e-05,
x_ref_max=1000.0,
y_ref=pk,
grid_regularizing_transform=tf.log)
priormesh = tf.reshape(pkmesh, kshape)
return tf.abs(kfield) / priormesh**0.5
cpfield = mtf.cwise(_cwise_prior, [cfield, pk] + kv,
output_dtype=tf.float32)
prior = mtf.reduce_sum(mtf.square(cpfield)) * bs**3 #* nc**3
# Total loss
cdiff = mesh_utils.r2c3d(diff, k_dims_pr, dtype=cdtype)
def _cwise_diff(kfield, pk, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = tf.sqrt((kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2)
kshape = kk.shape
kk = tf.reshape(kk, [-1])
pkmesh = tfp.math.interp_regular_1d_grid(x=kk,
x_ref_min=kerror.min(),
x_ref_max=kerror.max(),
y_ref=pk)
priormesh = tf.reshape(pkmesh, kshape)
priormesh = tf.cast(priormesh**0.5, kfield.dtype)
return kfield / priormesh
cdiff = mtf.cwise(_cwise_diff, [cdiff, pkerror] + kv, output_dtype=cdtype)
def _cwise_smooth(kfield, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = (kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2
wts = tf.cast(tf.exp(-kk * (R0 * bs / nc)**2), kfield.dtype)
return kfield * wts
cdiff = mtf.cwise(_cwise_smooth, [cdiff] + kv, output_dtype=cdtype)
diff = mesh_utils.c2r3d(cdiff, diff.shape[-3:], dtype=dtype)
chisq = mtf.reduce_sum(mtf.square(diff))
loss = chisq + prior
fields = [fieldvar, final_field, model]
metrics = [chisq, prior, loss]
return fields, metrics, kv
def recon_model(mesh,
data,
R0,
x0,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps,
dtype=tf.float32):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
if dtype == tf.float32:
npdtype = "float32"
cdtype = tf.complex64
elif dtype == tf.float64:
npdtype = "float64"
cdtype = tf.complex128
print(dtype, npdtype)
# Compute a few things first, using simple tensorflow
stages = np.linspace(a0, a, nsteps, endpoint=True)
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
if halo_size >= 0.5 * min(nc // n_block_x, nc // n_block_y,
nc // n_block_z):
new_size = int(0.5 *
min(nc // n_block_x, nc // n_block_y, nc // n_block_z))
print('WARNING: REDUCING HALO SIZE from %d to %d' %
(halo_size, new_size))
halo_size = new_size
# Parameters of the large scales decomposition
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
klin = np.loadtxt('../data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype(npdtype), shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
# Begin simulation
if x0 is None:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.random_normal_initializer(
mean=0.0, stddev=1, seed=None))
else:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.constant_initializer(x0))
print("\nfieldvar : \n", fieldvar)
# Here we can run our nbody
if FLAGS.nbody:
state = mtfpm.lpt_init_single(
fieldvar,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# Here we can run our nbody
final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape,
kv_lr, halo_size)
else:
final_state = mtfpm.lpt_init_single(
fieldvar,
stages[-1],
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4],
final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
final_field = mtf.slicewise(
lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=dtype,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
mtfdata = mtf.import_tf_tensor(mesh,
tf.convert_to_tensor(data),
shape=shape)
# Get prior
k_dims_pr = [d.shape[0] for d in kv]
k_dims_pr = [k_dims_pr[2], k_dims_pr[0], k_dims_pr[1]]
cfield = mesh_utils.r2c3d(fieldvar, k_dims_pr, dtype=cdtype)
def _cwise_prior(kfield, pk, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = tf.sqrt((kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2)
kshape = kk.shape
kk = tf.reshape(kk, [-1])
pkmesh = tfp.math.interp_regular_1d_grid(
x=kk,
x_ref_min=1e-05,
x_ref_max=1000.0,
y_ref=pk,
grid_regularizing_transform=tf.log)
priormesh = tf.reshape(pkmesh, kshape)
return tf.abs(kfield) / priormesh**0.5
cpfield = mtf.cwise(_cwise_prior, [cfield, pk] + kv,
output_dtype=tf.float32)
prior = mtf.reduce_sum(mtf.square(cpfield)) * bs**3 #*nc**3
# Total loss
diff = (final_field - mtfdata)
R0 = tf.constant(R0)
print("R0 in the recon_model : ", R0)
def _cwise_smooth(kfield, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = (kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2
wts = tf.cast(tf.exp(-kk * (R0 * bs / nc)**2), kfield.dtype)
return kfield * wts
# Element-wise function that applies a Fourier kernel
plambda = FLAGS.plambda
def _cwise_logprob(finalfield, data):
galmean = tfp.distributions.Poisson(rate=plambda * (1 + finalfield))
logprob = galmean.log_prob(data)
return -1 * logprob
cfield = mesh_utils.r2c3d(final_field, k_dims_pr, dtype=cdtype)
cfield = mtf.cwise(_cwise_smooth, [cfield] + kv, output_dtype=cdtype)
final_fieldsm = mesh_utils.c2r3d(cfield, diff.shape[-3:], dtype=dtype)
chisq = mtf.cwise(_cwise_logprob, [final_fieldsm, mtfdata],
output_dtype=tf.float32) #
chisq = mtf.reduce_sum(chisq)
## #
loss = chisq + prior
def _cwise_sample(finalfield, data):
galmean = tfp.distributions.Poisson(rate=plambda * (1 + finalfield))
sample = galmean.sample()
return sample
sample = mtf.cwise(_cwise_sample, [final_fieldsm, mtfdata],
output_dtype=tf.float32) #
fields = [fieldvar, sample]
metrics = [chisq, prior, loss]
return fields, metrics, kv
def recon_prototype(mesh,
data,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps,
dtype=tf.float32):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
if dtype == tf.float32:
npdtype = "float32"
cdtype = tf.complex64
elif dtype == tf.float64:
npdtype = "float64"
cdtype = tf.complex128
print("Dtype : ", dtype, npdtype)
# Compute a few things first, using simple tensorflow
kny = 1 * np.pi * nc / bs
R1, R2 = 3., 3 * 1.2
stages = np.linspace(a0, a, nsteps, endpoint=True)
#graph = mtf.Graph()
#mesh = mtf.Mesh(graph, "my_mesh")
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
if halo_size >= 0.5 * min(nc // n_block_x, nc // n_block_y,
nc // n_block_z):
new_size = int(0.5 *
min(nc // n_block_x, nc // n_block_y, nc // n_block_z))
print('WARNING: REDUCING HALO SIZE from %d to %d' %
(halo_size, new_size))
halo_size = new_size
# Parameters of the large scales decomposition
scalar = mtf.Dimension("scalar", 1)
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
#k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype(npdtype), shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
#
# Begin simulation
## Compute initial initial conditions distributed
#initc = mtfpm.linear_field(mesh, shape, bs, nc, pk, kv)
fieldvar = mtf.get_variable(mesh, 'linear', part_shape)
input_field = tf.placeholder(data.dtype, [batch_size, nc, nc, nc])
mtfinp = mtf.import_tf_tensor(mesh, input_field, shape=part_shape)
linearop = mtf.assign(fieldvar, mtfinp)
#field = fieldvar
initc = fieldvar
print("initc : ", initc)
# Here we can run our nbody
if FLAGS.nbody:
state = mtfpm.lpt_init_single(
fieldvar,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# Here we can run our nbody
final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape,
kv_lr, halo_size)
else:
final_state = mtfpm.lpt_init_single(
initc,
stages[-1],
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
# paint the field
final_field = mtf.zeros(mesh, shape=hr_shape)
for block_size_dim in hr_shape[-3:]:
final_field = mtf.pad(final_field, [halo_size, halo_size],
block_size_dim.name)
final_field = mesh_utils.cic_paint(final_field, final_state[0], halo_size)
# Halo exchange
for blocks_dim, block_size_dim in zip(hr_shape[1:4],
final_field.shape[-3:]):
final_field = mpm.halo_reduce(final_field, blocks_dim, block_size_dim,
halo_size)
# Remove borders
for block_size_dim in hr_shape[-3:]:
final_field = mtf.slice(final_field, halo_size, block_size_dim.size,
block_size_dim.name)
final_field = mtf.slicewise(
lambda x: x[:, 0, 0, 0], [final_field],
output_dtype=dtype,
output_shape=[batch_dim, fx_dim, fy_dim, fz_dim],
name='my_dumb_reshape',
splittable_dims=part_shape[:-1] + hr_shape[:4])
##
x = final_field
ppars, mpars, kernel = setupfnn()
pwts, pbias, pmx, psx = ppars
mwts, mbias, mmx, msx, mmy, msy = mpars
msy, mmy = msy[0], mmy[0]
print("mmy : ", mmy)
size = 3
k_dims = [d.shape[0] for d in kv]
k_dims = [k_dims[2], k_dims[0], k_dims[1]]
tfnc, tfbs = float_to_mtf(nc * 1., mesh,
scalar), float_to_mtf(bs, mesh, scalar)
x1f = mesh_utils.r2c3d(x, k_dims, dtype=cdtype)
x1f = mtf.cwise(cwise_decic, [x1f] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x1d = mesh_utils.c2r3d(x1f, x.shape[-3:], dtype=dtype)
x1d = mtf.add(x1d, -1.)
x1f0 = mesh_utils.r2c3d(x1d, k_dims, dtype=cdtype)
x1f = mtf.cwise(cwise_fingauss,
[x1f0, float_to_mtf(R1, mesh, scalar)] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x1 = mesh_utils.c2r3d(x1f, x1d.shape[-3:], dtype=dtype)
x2f = mtf.cwise(cwise_fingauss,
[x1f0, float_to_mtf(R2, mesh, scalar)] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x2 = mesh_utils.c2r3d(x2f, x1d.shape[-3:], dtype=dtype)
x12 = x1 - x2
width = tf.placeholder(tf.float32, shape=())
def apply_pwts(x, x1, x2):
#y = tf.expand_dims(x, axis=-1)
y = tf.nn.conv3d(tf.expand_dims(x, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
y1 = tf.nn.conv3d(tf.expand_dims(x1, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
y2 = tf.nn.conv3d(tf.expand_dims(x2, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
#y = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
#y1 = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x1), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
#y2 = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x12), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
yy = tf.concat([y, y1, y2], axis=-1)
yy = yy - pmx
yy = yy / psx
yy1 = tf.nn.relu(tf.matmul(yy, pwts[0]) + pbias[0])
yy2 = tf.nn.relu(tf.matmul(yy1, pwts[1]) + pbias[1])
yy3 = tf.matmul(yy2, pwts[2]) + pbias[2]
pmodel = tf.nn.sigmoid(width * yy3)
return pmodel[..., 0]
pmodel = mtf.slicewise(
apply_pwts,
[x, x1, x12],
output_dtype=tf.float32,
output_shape=part_shape, # + [mtf.Dimension('c_dim', 81)],
name='apply_pwts',
splittable_dims=lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3])
def apply_mwts(x, x1, x2):
#y = tf.expand_dims(x, axis=-1)
zz = tf.concat([
tf.expand_dims(x, -1),
tf.expand_dims(x1, -1),
tf.expand_dims(x2, -1)
],
axis=-1)
zz = zz - mmx
zz = zz / msx
zz1 = tf.nn.elu(tf.matmul(zz, mwts[0]) + mbias[0])
zz2 = tf.nn.elu(tf.matmul(zz1, mwts[1]) + mbias[1])
zz3 = tf.matmul(zz2, mwts[2]) + mbias[2]
mmodel = zz3 * msy + mmy
return mmodel[..., 0]
mmodel = mtf.slicewise(
apply_mwts,
[x, x1, x12],
output_dtype=tf.float32,
output_shape=part_shape, # + [mtf.Dimension('c_dim', 81)],
name='apply_mwts',
splittable_dims=lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3])
model = pmodel * mmodel
mtfdata = mtf.import_tf_tensor(mesh,
tf.convert_to_tensor(data),
shape=shape)
# Get prior
#k_dims = [d.shape[0] for d in kv]
#k_dims = [k_dims[2], k_dims[0], k_dims[1]]
k_dims_pr = [d.shape[0] for d in kv]
k_dims_pr = [k_dims_pr[2], k_dims_pr[0], k_dims_pr[1]]
cfield = mesh_utils.r2c3d(fieldvar, k_dims_pr, dtype=cdtype)
def _cwise_prior(kfield, pk, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = tf.sqrt((kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2)
kshape = kk.shape
kk = tf.reshape(kk, [-1])
pkmesh = tfp.math.interp_regular_1d_grid(
x=kk,
x_ref_min=1e-05,
x_ref_max=1000.0,
y_ref=pk,
grid_regularizing_transform=tf.log)
priormesh = tf.reshape(pkmesh, kshape)
return tf.abs(kfield) / priormesh**0.5
cpfield = mtf.cwise(_cwise_prior, [cfield, pk] + kv,
output_dtype=tf.float32)
prior = mtf.reduce_sum(mtf.square(cpfield)) * bs**3 * nc**3
# Total loss
#diff = (model - mtfdata)
modelf = mesh_utils.r2c3d(model, k_dims, dtype=cdtype)
modelsmf = mtf.cwise(cwise_fingauss,
[modelf, float_to_mtf(R1, mesh, scalar)] + kv +
[tfnc, tfbs],
output_dtype=cdtype)
modelsm = mesh_utils.c2r3d(modelsmf, x1d.shape[-3:], dtype=dtype)
#dataf = mesh_utils.r2c3d(mtfdata, k_dims, dtype=cdtype)
#datasmf = mtf.cwise(cwise_fingauss, [dataf, float_to_mtf(R1, mesh, scalar)] + kv + [tfnc, tfbs], output_dtype=cdtype)
#datasm = mesh_utils.c2r3d(datasmf, x1d.shape[-3:], dtype=dtype)
##Anneal
R0 = tf.placeholder(tf.float32, shape=())
M0 = tf.placeholder(tf.float32, shape=())
off, istd = tf.placeholder(tf.float32, shape=data.shape), tf.placeholder(
tf.float32, shape=data.shape)
mtfoff = mtf.import_tf_tensor(mesh, off, shape=shape)
mtfistd = mtf.import_tf_tensor(mesh, istd, shape=shape)
diff = mtf.log(modelsm + M0) - mtf.log(mtfdata + M0)
#diff = diff / 0.25
#diff = (diff + mtfoff)*mtfistd #For some reason, doing things wrong this one
diff = (diff + mtfoff) / 0.25
def _cwise_smooth(kfield, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = (kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2
wts = tf.cast(tf.exp(-kk * (R0 * bs / nc)**2), kfield.dtype)
return kfield * wts
cdiff = mesh_utils.r2c3d(diff, k_dims_pr, dtype=cdtype)
cdiff = mtf.cwise(_cwise_smooth, [cdiff] + kv, output_dtype=cdtype)
diff = mesh_utils.c2r3d(cdiff, diff.shape[-3:], dtype=dtype)
chisq = mtf.reduce_sum(mtf.square(diff))
loss = chisq + prior
#return initc, final_field, loss, linearop, input_field
nyq = np.pi * nc / bs
def _cwise_highpass(kfield, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = (kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2
wts = tf.cast(tf.exp(-kk * (R0 * bs / nc + 1 / nyq)**2), kfield.dtype)
return kfield * (1 - wts)
var_grads = mtf.gradients([loss], [fieldvar])
cgrads = mesh_utils.r2c3d(var_grads[0], k_dims_pr, dtype=cdtype)
cgrads = mtf.cwise(_cwise_highpass, [cgrads] + kv, output_dtype=cdtype)
var_grads = [mesh_utils.c2r3d(cgrads, diff.shape[-3:], dtype=dtype)]
lr = tf.placeholder(tf.float32, shape=())
update_op = mtf.assign(fieldvar, fieldvar - var_grads[0] * lr)
return initc, model, loss, var_grads, update_op, linearop, input_field, lr, R0, M0, width, chisq, prior, off, istd
def recon_model(mesh,
datasm,
rsdfactor,
M0,
R0,
width,
off,
istd,
x0,
nc=FLAGS.nc,
bs=FLAGS.box_size,
batch_size=FLAGS.batch_size,
a0=FLAGS.a0,
a=FLAGS.af,
nsteps=FLAGS.nsteps,
dtype=tf.float32):
"""
Prototype of function computing LPT deplacement.
Returns output tensorflow and mesh tensorflow tensors
"""
if dtype == tf.float32:
npdtype = "float32"
cdtype = tf.complex64
elif dtype == tf.float64:
npdtype = "float64"
cdtype = tf.complex128
print("Dtype : ", dtype, npdtype)
# Compute a few things first, using simple tensorflow
kny = 1 * np.pi * nc / bs
R1, R2 = 3., 3 * 1.2
stages = np.linspace(a0, a, nsteps, endpoint=True)
#graph = mtf.Graph()
#mesh = mtf.Mesh(graph, "my_mesh")
# Define the named dimensions
# Parameters of the small scales decomposition
n_block_x = FLAGS.nx
n_block_y = FLAGS.ny
n_block_z = 1
halo_size = FLAGS.hsize
if halo_size >= 0.5 * min(nc // n_block_x, nc // n_block_y,
nc // n_block_z):
new_size = int(0.5 *
min(nc // n_block_x, nc // n_block_y, nc // n_block_z))
print('WARNING: REDUCING HALO SIZE from %d to %d' %
(halo_size, new_size))
halo_size = new_size
# Parameters of the large scales decomposition
scalar = mtf.Dimension("scalar", 1)
fx_dim = mtf.Dimension("nx", nc)
fy_dim = mtf.Dimension("ny", nc)
fz_dim = mtf.Dimension("nz", nc)
tfx_dim = mtf.Dimension("tx", nc)
tfy_dim = mtf.Dimension("ty", nc)
tfz_dim = mtf.Dimension("tz", nc)
tx_dim = mtf.Dimension("tx_lr", nc)
ty_dim = mtf.Dimension("ty_lr", nc)
tz_dim = mtf.Dimension("tz_lr", nc)
nx_dim = mtf.Dimension('nx_block', n_block_x)
ny_dim = mtf.Dimension('ny_block', n_block_y)
nz_dim = mtf.Dimension('nz_block', n_block_z)
sx_dim = mtf.Dimension('sx_block', nc // n_block_x)
sy_dim = mtf.Dimension('sy_block', nc // n_block_y)
sz_dim = mtf.Dimension('sz_block', nc // n_block_z)
#k_dims = [tx_dim, ty_dim, tz_dim]
batch_dim = mtf.Dimension("batch", batch_size)
klin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[0]
plin = np.loadtxt('../flowpm/data/Planck15_a1p00.txt').T[1]
ipklin = iuspline(klin, plin)
pk_dim = mtf.Dimension("npk", len(plin))
pk = mtf.import_tf_tensor(mesh, plin.astype(npdtype), shape=[pk_dim])
# Compute necessary Fourier kernels
kvec = flowpm.kernels.fftk((nc, nc, nc), symmetric=False)
kx = mtf.import_tf_tensor(mesh,
kvec[0].squeeze().astype('float32'),
shape=[tfx_dim])
ky = mtf.import_tf_tensor(mesh,
kvec[1].squeeze().astype('float32'),
shape=[tfy_dim])
kz = mtf.import_tf_tensor(mesh,
kvec[2].squeeze().astype('float32'),
shape=[tfz_dim])
kv = [ky, kz, kx]
# kvec for low resolution grid
kvec_lr = flowpm.kernels.fftk([nc, nc, nc], symmetric=False)
kx_lr = mtf.import_tf_tensor(mesh,
kvec_lr[0].squeeze().astype('float32'),
shape=[tx_dim])
ky_lr = mtf.import_tf_tensor(mesh,
kvec_lr[1].squeeze().astype('float32'),
shape=[ty_dim])
kz_lr = mtf.import_tf_tensor(mesh,
kvec_lr[2].squeeze().astype('float32'),
shape=[tz_dim])
kv_lr = [ky_lr, kz_lr, kx_lr]
shape = [batch_dim, fx_dim, fy_dim, fz_dim]
lr_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
hr_shape = [batch_dim, nx_dim, ny_dim, nz_dim, sx_dim, sy_dim, sz_dim]
part_shape = [batch_dim, fx_dim, fy_dim, fz_dim]
splittables = lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3]
#
# Begin simulation
if x0 is None:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.random_normal_initializer(
mean=0.0, stddev=1, seed=None))
else:
fieldvar = mtf.get_variable(mesh,
'linear',
part_shape,
initializer=tf.constant_initializer(x0))
##
state = mtfpm.lpt_init_single(
fieldvar,
a0,
kv_lr,
halo_size,
lr_shape,
hr_shape,
part_shape[1:],
antialias=True,
)
final_state = mtfpm.nbody_single(state, stages, lr_shape, hr_shape, kv_lr,
halo_size)
final_field = mtf.zeros(mesh, shape=part_shape)
final_field = mcomp.cic_paint_fr(final_field,
final_state,
output_shape=part_shape,
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
##
x = final_field
ppars, mpars, kernel = setupfnn()
pwts, pbias, pmx, psx = ppars
mwts, mbias, mmx, msx, mmy, msy = mpars
msy, mmy = msy[0], mmy[0]
size = 3
k_dims = [d.shape[0] for d in kv]
k_dims = [k_dims[2], k_dims[0], k_dims[1]]
tfnc, tfbs = float_to_mtf(nc * 1., mesh,
scalar), float_to_mtf(bs, mesh, scalar)
x1f = mesh_utils.r2c3d(x, k_dims, dtype=cdtype)
x1f = mtf.cwise(cwise_decic, [x1f] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x1d = mesh_utils.c2r3d(x1f, x.shape[-3:], dtype=dtype)
x1d = mtf.add(x1d, -1.)
x1f0 = mesh_utils.r2c3d(x1d, k_dims, dtype=cdtype)
x1f = mtf.cwise(cwise_fingauss,
[x1f0, float_to_mtf(R1, mesh, scalar)] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x1 = mesh_utils.c2r3d(x1f, x1d.shape[-3:], dtype=dtype)
x2f = mtf.cwise(cwise_fingauss,
[x1f0, float_to_mtf(R2, mesh, scalar)] + kv + [tfnc, tfbs],
output_dtype=cdtype)
x2 = mesh_utils.c2r3d(x2f, x1d.shape[-3:], dtype=dtype)
x12 = x1 - x2
def apply_pwts(x, x1, x2):
#y = tf.expand_dims(x, axis=-1)
y = tf.nn.conv3d(tf.expand_dims(x, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
y1 = tf.nn.conv3d(tf.expand_dims(x1, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
y2 = tf.nn.conv3d(tf.expand_dims(x2, axis=-1), kernel, [1, 1, 1, 1, 1],
'SAME')
#y = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
#y1 = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x1), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
#y2 = tf.nn.conv3d(tf.expand_dims(tfwrap3D(x12), -1), kernel, [1, 1, 1, 1, 1], 'VALID')
yy = tf.concat([y, y1, y2], axis=-1)
yy = yy - pmx
yy = yy / psx
yy1 = tf.nn.relu(tf.matmul(yy, pwts[0]) + pbias[0])
yy2 = tf.nn.relu(tf.matmul(yy1, pwts[1]) + pbias[1])
yy3 = tf.matmul(yy2, pwts[2]) + pbias[2]
pmodel = tf.nn.sigmoid(tf.constant(width) * yy3)
return pmodel[..., 0]
pmodel = mtf.slicewise(
apply_pwts,
[x, x1, x12],
output_dtype=tf.float32,
output_shape=part_shape, # + [mtf.Dimension('c_dim', 81)],
name='apply_pwts',
splittable_dims=lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3])
def apply_mwts(x, x1, x2):
#y = tf.expand_dims(x, axis=-1)
zz = tf.concat([
tf.expand_dims(x, -1),
tf.expand_dims(x1, -1),
tf.expand_dims(x2, -1)
],
axis=-1)
zz = zz - mmx
zz = zz / msx
zz1 = tf.nn.elu(tf.matmul(zz, mwts[0]) + mbias[0])
zz2 = tf.nn.elu(tf.matmul(zz1, mwts[1]) + mbias[1])
zz3 = tf.matmul(zz2, mwts[2]) + mbias[2]
mmodel = zz3 * msy + mmy
return mmodel[..., 0]
mmodel = mtf.slicewise(
apply_mwts,
[x, x1, x12],
output_dtype=tf.float32,
output_shape=part_shape, # + [mtf.Dimension('c_dim', 81)],
name='apply_mwts',
splittable_dims=lr_shape[:-1] + hr_shape[1:4] + part_shape[1:3])
model = pmodel * mmodel
##RSD below
hr_field = mcomp.fr_to_hr(final_field, hr_shape, halo_size, splittables,
mesh)
mstate = mpm.mtf_indices(hr_field.mesh,
shape=part_shape[1:],
dtype=tf.float32)
X = mtf.einsum([mtf.ones(hr_field.mesh, [batch_dim]), mstate],
output_shape=[batch_dim] + mstate.shape[:])
massf = mesh_utils.r2c3d(final_field, k_dims, dtype=cdtype)
masssmf = mtf.cwise(cwise_fingauss,
[massf, float_to_mtf(R1, mesh, scalar)] + kv +
[tfnc, tfbs],
output_dtype=cdtype)
masssm = mesh_utils.c2r3d(masssmf, final_field.shape[-3:], dtype=dtype)
masssm = masssm + 1e-5
imasssm = mtf.pow(x, -1.)
vzweights = final_state[1]
vzweights = mtf.slicewise(lambda x: x[:, :, :, :, -1], [vzweights],
output_dtype=tf.float32,
output_shape=vzweights.shape[:-1],
name='get_vz',
splittable_dims=vzweights.shape[1:-1])
print("weights : ", vzweights)
momz = mtf.zeros(mesh, shape=part_shape)
momz = mcomp.cic_paint_fr(final_field, final_state, output_shape=part_shape, hr_shape=hr_shape, \
halo_size=halo_size, splittables=splittables, mesh=mesh, weights=vzweights)
momzf = mesh_utils.r2c3d(momz, k_dims, dtype=cdtype)
momzsmf = mtf.cwise(cwise_fingauss,
[momzf, float_to_mtf(R1, mesh, scalar)] + kv +
[tfnc, tfbs],
output_dtype=cdtype)
momzsm = mesh_utils.c2r3d(momzsmf, momz.shape[-3:], dtype=dtype)
#Shift
velzsm = mtf.divide(momzsm, masssm)
vz = mcomp.cic_readout_fr(velzsm, [X],
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
vz = mtf.multiply(vz, rsdfactor)
print("vz : ", vz)
Xrsd = mtf.slicewise(lambda x, vz: x + tf.stack(
[tf.zeros_like(vz), tf.zeros_like(vz), vz], 4), [X, vzweights],
output_dtype=tf.float32,
output_shape=X.shape,
name='add_vz',
splittable_dims=X.shape[1:-1])
print(Xrsd)
modelread = mcomp.cic_readout_fr(model, [X],
hr_shape=hr_shape,
halo_size=halo_size,
splittables=splittables,
mesh=mesh)
modelrsd = mtf.zeros(mesh, shape=part_shape)
modelrsd = mcomp.cic_paint_fr(modelrsd, [Xrsd], output_shape=part_shape, hr_shape=hr_shape, \
halo_size=halo_size, splittables=splittables, mesh=mesh, weights=modelread)
model = modelrsd
print(modelrsd)
#Likelihood and prior here
mtfdatasm = mtf.import_tf_tensor(mesh,
tf.convert_to_tensor(datasm),
shape=shape)
# Get prior
k_dims_pr = [d.shape[0] for d in kv]
k_dims_pr = [k_dims_pr[2], k_dims_pr[0], k_dims_pr[1]]
cfield = mesh_utils.r2c3d(fieldvar, k_dims_pr, dtype=cdtype)
def _cwise_prior(kfield, pk, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = tf.sqrt((kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2)
kshape = kk.shape
kk = tf.reshape(kk, [-1])
pkmesh = tfp.math.interp_regular_1d_grid(
x=kk,
x_ref_min=1e-05,
x_ref_max=1000.0,
y_ref=pk,
grid_regularizing_transform=tf.log)
priormesh = tf.reshape(pkmesh, kshape)
return tf.abs(kfield) / priormesh**0.5
cpfield = mtf.cwise(_cwise_prior, [cfield, pk] + kv,
output_dtype=tf.float32)
prior = mtf.reduce_sum(mtf.square(cpfield)) * bs**3 * nc**3
# Total loss
#diff = (model - mtfdata)
modelf = mesh_utils.r2c3d(model, k_dims, dtype=cdtype)
modelsmf = mtf.cwise(cwise_fingauss,
[modelf, float_to_mtf(R1, mesh, scalar)] + kv +
[tfnc, tfbs],
output_dtype=cdtype)
modelsm = mesh_utils.c2r3d(modelsmf, x1d.shape[-3:], dtype=dtype)
##Anneal
M0 = tf.constant(M0)
diff = mtf.log(modelsm + M0) - mtf.log(mtfdatasm + M0)
if off is not None:
mtfoff = mtf.import_tf_tensor(mesh, off, shape=shape)
diff = diff + mtfoff
if istd is not None:
mtfistd = mtf.import_tf_tensor(mesh, istd, shape=shape)
diff = (diff + mtfoff
) * mtfistd #For some reason, doing things wrong this one
else:
diff = diff / 0.25
def _cwise_smooth(kfield, kx, ky, kz):
kx = tf.reshape(kx, [-1, 1, 1])
ky = tf.reshape(ky, [1, -1, 1])
kz = tf.reshape(kz, [1, 1, -1])
kk = (kx / bs * nc)**2 + (ky / bs * nc)**2 + (kz / bs * nc)**2
wts = tf.cast(tf.exp(-kk * (R0 * bs / nc)**2), kfield.dtype)
return kfield * wts
cdiff = mesh_utils.r2c3d(diff, k_dims_pr, dtype=cdtype)
cdiff = mtf.cwise(_cwise_smooth, [cdiff] + kv, output_dtype=cdtype)
diff = mesh_utils.c2r3d(cdiff, diff.shape[-3:], dtype=dtype)
chisq = mtf.reduce_sum(mtf.square(diff))
loss = chisq + prior
fields = [fieldvar, final_field, model]
metrics = [chisq, prior, loss]
return fields, metrics, kv
