mirror of
https://gitlab.science.ru.nl/mthesis-edeboone/m-thesis-introduction.git
synced 2024-12-22 19:43:30 +01:00
176 lines
6.9 KiB
Python
Executable file
176 lines
6.9 KiB
Python
Executable file
#!/usr/bin/env python3
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# vim: fdm=indent ts=4
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import h5py
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from itertools import combinations, zip_longest
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import matplotlib.pyplot as plt
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import numpy as np
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import aa_generate_beacon as beacon
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import lib
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if __name__ == "__main__":
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from os import path
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import sys
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fname = "ZH_airshower/mysim.sry"
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show_plots = True
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save_result = True
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ref_ant_id = None # leave None for all baselines
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####
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fname_dir = path.dirname(fname)
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antennas_fname = path.join(fname_dir, beacon.antennas_fname)
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time_diffs_fname = antennas_fname
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# Read in antennas from file
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f_beacon, tx, antennas = beacon.read_beacon_hdf5(antennas_fname)
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# run over all baselines
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if ref_ant_id is None:
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print("Doing all baselines")
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baselines = list(combinations(antennas,2))
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# use ref_ant
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else:
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ref_ant = antennas[ref_ant_id]
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print(f"Doing all baselines with {ref_ant.name}")
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baselines = list(zip_longest([], antennas, fillvalue=ref_ant))
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freq_names = antennas[0].beacon_info.keys()
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if len(freq_names) > 1:
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raise NotImplementedError
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freq_name = next(iter(freq_names))
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# Determine integer multiple of periods to shift
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# and True phase differences
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time_diffs = np.empty( (len(baselines), 3) )
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for i, base in enumerate(baselines):
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if i%50==0:
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print(i, "out of", len(baselines))
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# which traces to keep track of
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traces = [ base[0].E_AxB, base[1].E_AxB ]
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# read f_beacon from the first antenna
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f_beacon = base[0].beacon_info[freq_name]['freq']
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# how many samples do we need to shift
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sample_shifts, maxima = lib.coherence_sum_maxima(traces[0], traces[1], periodic=False)
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best_sample_shift = sample_shifts[np.argmax(maxima)]
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# turn sample_shift into time
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sampling_dt = (base[1].t[1] - base[1].t[0]) # ns
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delta_t_coherence = sampling_dt*best_sample_shift # ns
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# get the amount of periods to move
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k_period, t_rest = np.divmod(delta_t_coherence, 1/f_beacon)
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# always keep the reference before traces[1]
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if t_rest < 0: # np.divmod already does this
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k_period -= 1
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t_rest = 1/f_beacon + t_rest
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# Get true phase diffs
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try:
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true_phases = np.array([ant.beacon_info[freq_name]['true_phase'] for ant in base])
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true_phases_diff = lib.phase_mod(lib.phase_mod(true_phases[0]) - lib.phase_mod(true_phases[1]))
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except IndexError:
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# true_phase not determined yet
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print(f"Missing true_phases for {freq_name} in baseline {base[0].name},{base[1].name}")
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true_phases_diff = np.nan
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# save k_period with antenna names
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time_diffs[i] = [true_phases_diff, k_period, f_beacon]
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# Plotting for one or two iterations
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if show_plots and (i in [ 1, 57 ] or k_period > 3):
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# More than three periods is quite much so report it
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# Show correlation maxima plot
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if not True:
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fig, ax = plt.subplots()
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ax.set_title(f"Correlation Maxima {i}")
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ax.set_xlabel("k")
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ax.set_ylabel("Maximum correlation")
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ax.plot(ks, maxima)
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ax.plot(best_k, maxima[max_idx], marker='X')
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# Delta t due to the beacon
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# Note that we want to show some overlapping waveforms
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# Therefore we use the phase from the original waveforms
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# and not the true_phases (we lost t_d information there)
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phases = np.array([ant.beacon_info[freq_name]['phase'] for ant in base])
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phases_diff = lib.phase_mod(lib.phase_mod(phases[0]) - lib.phase_mod(phases[1]))
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delta_t_beacon = phases_diff/(2*np.pi*f_beacon)
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# Do we make it a shared plot with both the
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# signal and the beacon?
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beacons = None
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if True:
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try:
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beacons = [ base[0].beacon, base[1].beacon ]
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except:
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# No beacon waveforms available..
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pass
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# Start the figure
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fig, axs = plt.subplots(1+(beacons is not None), 1, sharex=True)
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if beacons is None:
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axs = [axs]
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print('i',i,f"B({base[0].name},{base[1].name})", 'k[T]',k_period, 'rest[ns]',t_rest, 'T[ns]',1/f_beacon, 'dT_coher[ns]', delta_t_coherence, 'dT_beac[ns]', delta_t_beacon)
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fig.suptitle(
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", ".join([
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f"$\\Delta$t_beacon [ns]: {delta_t_beacon:.2f}",
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f"$\\Delta\\varphi$: {phases_diff:.4f}",
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f"$\\Delta\\sigma_\\varphi$: {true_phases_diff:.4f}",
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f"",
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])
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)
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axs[-1].set_xlabel('t [ns]')
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axs[0].set_ylabel('Amplitude [a.u.]')
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# plot vertical lines indicating f_beacon
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min_t, max_t = min(base[0].t[0], base[1].t[0]), max(base[0].t[-1], base[1].t[-1])
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N_lines = int( (max_t - min_t)*f_beacon) +1
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for i, t in enumerate(np.arange(N_lines)/f_beacon):
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for ax in axs:
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ax.axvline( min_t + t, color='k', alpha=0.3)
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# Plot traces
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l1 = axs[0].plot(base[0].t, traces[0], label=f'Ref: {base[0].name}', alpha=0.8)
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l2 = axs[0].plot(base[1].t, traces[1], label=f'Orig: {base[1].name}', alpha=0.3, marker='+', ms=5)
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axs[0].plot(base[0].t + k_period/f_beacon + t_rest, traces[1], label='Coherence', alpha=0.3, marker='x', ms=5)
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l3 = axs[0].plot(base[1].t - delta_t_beacon +k_period/f_beacon, traces[1], label=f'$\\Delta t_{{\\varphi}}$ + ($k={k_period:.0f}$)T', alpha=0.8)
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axs[0].legend(fancybox=True, framealpha=0.5)
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# Plot beacon if available
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if beacons is not None:
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ax = axs[1]
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ax.set_title("Original Beacons")
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ax.plot(base[0].t, beacons[0], label=f'Ref: {base[0].name}', alpha=0.8, color=l1[0].get_color())
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ax.plot(base[1].t, beacons[1], label=f'Orig: {base[1].name}', alpha=0.3, marker='+', ms=5, color=l2[0].get_color())
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ax.plot(base[1].t -delta_t_beacon +k_period/f_beacon, beacons[1], label=f'$\\Delta t_{{\\varphi}}$ + ($k={k_period:.0f}$)T', alpha=0.8, color=l3[0].get_color())
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if False:
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if False:
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fig.savefig(__file__ + f"_i{i}_k{k_period}_zoomed_out.pdf")
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ax.set_xlim(base[0].t[0]-1/f_beacon, base[0].t[0] + 5/f_beacon)
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fig.savefig(__file__ + f"_i{i}_k{k_period}.pdf")
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# Report back to CLI
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print("Period Multiples resolved from", antennas_fname)
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if save_result:
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# Save integer periods to antennas
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beacon.write_baseline_time_diffs_hdf5(time_diffs_fname, baselines, time_diffs[:,0], time_diffs[:,1], time_diffs[:,2])
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print("Timediffs saved to", time_diffs_fname)
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plt.show()
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