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https://gitlab.science.ru.nl/mthesis-edeboone/m-thesis-introduction.git
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ZH: show phase due to t_trace[0] from measurement
This is not required to be known when finding the phase as lib.find_beacon_in_traces already accounts for it.
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4c834ad8e7
commit
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2 changed files with 48 additions and 8 deletions
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@ -92,7 +92,7 @@ if __name__ == "__main__":
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# TODO: refine masking
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# use beacon but remove where E_AxB-Beacon != 0
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if True:
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if True:
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if not True:
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t_mask = np.isclose(h5ant['E_AxB'][1], h5ant['traces'][4], rtol=1e-3, atol=1e-3)
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else:
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t_mask = np.ones(len(t_trace), dtype=bool)
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@ -156,24 +156,52 @@ if __name__ == "__main__":
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amplitude = amps[idx]
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orientation = orients[idx]
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# Correct for phase by t_trace[0]
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corr_phase = lib.phase_mod(2*np.pi*f_beacon*t_trace[0])
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if False:
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# Subtract phase due to not starting at t=0
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# This is already done in beacon_find_traces
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phase = lib.phase_mod(phase + corr_phase)
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# for reporting using plots
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found_data[i] = frequency, phase, amplitude
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if (show_plots or fig_dir) and (i == 60 or i == 72):
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if (show_plots or fig_dir) and (i == 0 or i == 72 or i == 70):
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p2t = lambda phase: phase/(2*np.pi*f_beacon)
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fig, ax = plt.subplots()
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ax.set_title(f"Beacon at antenna {h5ant.attrs['name']}\nF:{frequency:.2e}, P:{phase:.4f}, A:{amplitude:.1e}")
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ax.set_xlabel("t [ns]")
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ax.set_ylabel("Amplitude")
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for i, trace in enumerate(test_traces):
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ax.plot(t_trace, test_traces[i], marker='.', label='trace '+orients[i])
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if True:
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# let the trace start at t=0
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t_0 = min(t_trace)
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extra_phase = corr_phase
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else:
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t_0 = 0
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extra_phase = -1*corr_phase
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myt = np.linspace(min(t_trace), max(t_trace), 10*len(t_trace))
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ax.plot(myt, lib.sine_beacon(frequency, myt, amplitude=amplitude, phase=phase), ls='dashed', label='simulated beacon')
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for j, trace in enumerate(test_traces):
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ax.plot(t_trace - t_0, test_traces[j], marker='.', label='trace '+orients[j])
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myt = np.linspace(min(t_trace), max(t_trace), 10*len(t_trace)) - t_0
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ax.plot(myt, lib.sine_beacon(frequency, myt, amplitude=amplitude, t0=0, phase=phase+extra_phase), ls='dotted', label='simulated beacon')
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ax.axvline( p2t(lib.phase_mod(-1*(phase+extra_phase), low=0)), color='r', ls='dashed', label='$t_\\varphi$')
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ax.axvline(0,color='grey',alpha=0.5)
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ax.axhline(0,color='grey',alpha=0.5)
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ax.legend()
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if fig_dir:
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old_xlims = ax.get_xlim()
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ax.set_xlim(min(t_trace)-t_0-10,min(t_trace)-t_0+40)
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fig.savefig(path.join(fig_dir, __file__ + f".A{h5ant.attrs['name']}.zoomed.pdf"))
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ax.set_xlim(*old_xlims)
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fig.savefig(path.join(fig_dir, __file__ + f".A{h5ant.attrs['name']}.pdf"))
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# save to file
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@ -1,5 +1,12 @@
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#!/usr/bin/env python3
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"""
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Test the functions in lib concerning
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beacon generation and phase measuring
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work correctly together.
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"""
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import matplotlib.pyplot as plt
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import numpy as np
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@ -7,20 +14,25 @@ import lib
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seed = 12345
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dt = 1 # ns
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t = np.arange(0, 10*int(1e3), dt)
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frequency = 45e-3 # GHz
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N = 5e2
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t = np.arange(0, 10*int(1e3), dt, dtype=float)
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rng = np.random.default_rng(seed)
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phase_res = np.zeros(int(N))
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# Vary both the base time and the phase
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for i in range(int(N)):
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t_extra = (2*rng.uniform(size=1) - 1) *1e3
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t += t_extra
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phase = lib.phase_mod(np.pi*(2*rng.uniform(size=1) -1)) # rad
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beacon = lib.sine_beacon(frequency, t, t0=0, phase=phase)
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measured = lib.find_beacon_in_traces([beacon], t, frequency, frequency_fit=False)
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t -= t_extra
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phase_res[i] = lib.phase_mod(measured[1][0] - phase)
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fig, ax = plt.subplots()
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