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import datetime
import os
import logging
logging_path = os.path.dirname(logging.getLoggerClass().root.handlers[0].baseFilename)
import numpy as np
from scipy import signal, optimize
import matplotlib.pyplot as plt
def gen_omega(length):
if (length % 2) == 1:
raise ValueError("Needs an even length array.")
halflength = int(length/2)
factor = 2.0 * np.pi / length
omega = np.zeros(length, dtype=np.float)
for i in range(halflength):
omega[i] = factor * i
for i in range(halflength, length):
omega[i] = factor * (i - length)
return omega
def subsample_align(sig, ref_sig):
"""Do subsample alignment for sig relative to the reference signal
ref_sig. The delay between the two must be less than sample
Returns the aligned signal"""
n = len(sig)
if (n % 2) == 1:
raise ValueError("Needs an even length signal.")
halflen = int(n/2)
fft_sig = np.fft.fft(sig)
omega = gen_omega(n)
def correlate_for_delay(tau):
# A subsample offset between two signals corresponds, in the frequency
# domain, to a linearly increasing phase shift, whose slope
# corresponds to the delay.
#
# Here, we build this phase shift in rotate_vec, and multiply it with
# our signal.
rotate_vec = np.exp(1j * tau * omega)
# zero-frequency is rotate_vec[0], so rotate_vec[N/2] is the
# bin corresponding to the [-1, 1, -1, 1, ...] time signal, which
# is both the maximum positive and negative frequency.
# I don't remember why we handle it differently.
rotate_vec[halflen] = np.cos(np.pi * tau)
corr_sig = np.fft.ifft(rotate_vec * fft_sig)
return -np.abs(np.sum(np.conj(corr_sig) * ref_sig))
optim_result = optimize.minimize_scalar(correlate_for_delay, bounds=(-1,1), method='bounded', options={'disp': True})
if optim_result.success:
best_tau = optim_result.x
if 1:
corr = np.vectorize(correlate_for_delay)
ixs = np.linspace(-1, 1, 100)
taus = corr(ixs)
dt = datetime.datetime.now().isoformat()
tau_path = (logging_path + "/" + dt + "_tau.pdf")
plt.plot(ixs, taus)
plt.title("Subsample correlation, minimum is best: {}".format(best_tau))
plt.savefig(tau_path)
plt.clf()
# Prepare rotate_vec = fft_sig with rotated phase
rotate_vec = np.exp(1j * best_tau * omega)
rotate_vec[halflen] = np.cos(np.pi * best_tau)
return np.fft.ifft(rotate_vec * fft_sig).astype(np.complex64)
else:
#print("Could not optimize: " + optim_result.message)
return np.zeros(0, dtype=np.complex64)
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