Commit dcf8a19c authored by Martin Reinecke's avatar Martin Reinecke

remove spurious file

parent f35278d7
Pipeline #12514 passed with stage
in 5 minutes and 39 seconds
from nifty import *
from mpi4py import MPI
import plotly.offline as py
import plotly.graph_objs as go
comm = MPI.COMM_WORLD
rank = comm.rank
def plot_maps(x, name):
trace = [None]*len(x)
keys = x.keys()
field = x[keys[0]]
domain = field.domain[0]
shape = len(domain.shape)
max_n = domain.shape[0]*domain.distances[0]
step = domain.distances[0]
x_axis = np.arange(0, max_n, step)
if shape == 1:
for ii in xrange(len(x)):
trace[ii] = go.Scatter(x= x_axis, y=x[keys[ii]].val.get_full_data(), name=keys[ii])
fig = go.Figure(data=trace)
py.plot(fig, filename=name)
elif shape == 2:
for ii in xrange(len(x)):
py.plot([go.Heatmap(z=x[keys[ii]].val.get_full_data().real)], filename=keys[ii])
else:
raise TypeError("Only 1D and 2D field plots are supported")
def plot_power(x, name):
layout = go.Layout(
xaxis=dict(
type='log',
autorange=True
),
yaxis=dict(
type='log',
autorange=True
)
)
trace = [None]*len(x)
keys = x.keys()
field = x[keys[0]]
domain = field.domain[0]
x_axis = domain.kindex
for ii in xrange(len(x)):
trace[ii] = go.Scatter(x= x_axis, y=x[keys[ii]].val.get_full_data(), name=keys[ii])
fig = go.Figure(data=trace, layout=layout)
py.plot(fig, filename=name)
np.random.seed(42)
if __name__ == "__main__":
distribution_strategy = 'not'
# setting spaces
npix = np.array([500]) # number of pixels
total_volume = 1. # total length
# setting signal parameters
lambda_s = .05 # signal correlation length
sigma_s = 10. # signal variance
#setting response operator parameters
length_convolution = .025
exposure = 1.
# calculating parameters
k_0 = 4. / (2 * np.pi * lambda_s)
a_s = sigma_s ** 2. * lambda_s * total_volume
# creation of spaces
# x1 = RGSpace([npix,npix], distances=total_volume / npix,
# zerocenter=False)
# k1 = RGRGTransformation.get_codomain(x1)
x1 = HPSpace(32)
k1 = HPLMTransformation.get_codomain(x1)
p1 = PowerSpace(harmonic_partner=k1, logarithmic=False)
# creating Power Operator with given spectrum
spec = (lambda k: a_s / (1 + (k / k_0) ** 2) ** 2)
p_field = Field(p1, val=spec)
S_op = create_power_operator(k1, spec)
# creating FFT-Operator and Response-Operator with Gaussian convolution
Fft_op = FFTOperator(domain=x1, target=k1,
domain_dtype=np.float64,
target_dtype=np.complex128)
R_op = ResponseOperator(x1, sigma=[length_convolution],
exposure=[exposure])
# drawing a random field
sk = p_field.power_synthesize(real_signal=True, mean=0.)
s = Fft_op.adjoint_times(sk)
signal_to_noise = 1
N_op = DiagonalOperator(R_op.target, diagonal=s.var()/signal_to_noise, bare=True)
n = Field.from_random(domain=R_op.target,
random_type='normal',
std=s.std()/np.sqrt(signal_to_noise),
mean=0.)
d = R_op(s) + n
# Wiener filter
j = Fft_op.times(R_op.adjoint_times(N_op.inverse_times(d)))
D = HarmonicPropagatorOperator(S=S_op, N=N_op, R=R_op)
mk = D(j)
m = Fft_op.adjoint_times(mk)
# z={}
# z["signal"] = s
# z["reconstructed_map"] = m
# z["data"] = d
# z["lambda"] = R_op(s)
# z["j"] = j
#
# plot_maps(z, "Wiener_filter.html")
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