2023-09-30 17:53:06 +00:00
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# -*- coding: utf-8 -*-
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"""
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Created on Tue Aug 30 14:25:12 2022
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2023-12-14 19:49:44 +00:00
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@author: timofej
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2023-09-30 17:53:06 +00:00
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"""
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from plot import qtplot
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import sys
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import os
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import json
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import pyqtgraph as qt
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import pyqtgraph.exporters
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import math as m
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import numpy as np
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from scipy.fftpack import fft, fftfreq
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from scipy.stats import cauchy
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vect = np.vectorize
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@vect
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def log2(x):
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try:
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return m.log2(x)
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except ValueError:
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if x==0:
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return float(0)
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else:
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raise
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basepath = f'/cloud/Public/_data/neuropercolation/2lay/steps=1000100/'
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vals = [[],[]]
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TOTP_eps=[]
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TOTP_eps = []
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SIGP_eps = []
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SN_eps = []
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STON_eps = []
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FMAX_eps = []
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FWHM_eps = []
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Q_eps = []
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LHM_eps = []
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UHM_eps = []
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SOS_eps = []
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SPECC_eps=[]
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LORENTZ_eps=[]
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dims=[9]
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runsteps = 1000000
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for dim in dims:
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path=basepath+f'dim={dim:02}/'
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eps_space = np.linspace(0.005, 0.5, 100)
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eps_space=eps_space[1::2]
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TOTP = []
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SIGP = []
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SN = []
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STON = []
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FMAX = []
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FWHM = []
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Q = []
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LHM=[]
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UHM=[]
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SOS=[]
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#%%
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for eps in eps_space:
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eps=round(eps,3)
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halfh_parts = []
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sigtonoi_parts = []
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noisefloor_parts = []
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totalpower_parts = []
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sigpower_parts = []
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sn_parts = []
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freqmax_parts = []
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freqfwhm_parts = []
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specc_list = []
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lorentz_list = []
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subfreqmax_parts = []
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subfreqfwhm_parts = []
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totlorentz_list = []
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lhm_list=[]
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uhm_list=[]
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parts = 1
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partlen = int(runsteps/parts)
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for part in range(0,runsteps,partlen):
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with open(path+f"eps={eps:.3f}_activation.txt", 'r', encoding='utf-8') as f:
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activation = json.load(f)[100+part:100+part+partlen]
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phases = []
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for act in activation:
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ph = m.atan2(*act[::-1])
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phase = act[0] + act[1]*1j #m.e**(ph*1j)
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phases.append(phase)
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spectrum = abs(fft(phases))**2
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freqs = fftfreq(partlen, 1)
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accum = 1#int(500/parts)
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if accum==1:
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try:
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with open(path+f"eps={eps:.3f}_smooth_spectrum.txt", 'r', encoding='utf-8') as f:
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specc = json.load(f)
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freqqs = np.array([freqs[pos] for pos in range(-int(partlen/2),int(partlen/2))])
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print(f'Loaded specc for eps={eps:.3f}')
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except:
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freqqs = np.array([freqs[pos] for pos in range(-int(partlen/2),int(partlen/2))])
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spec = np.array([spectrum[pos] for pos in range(-int(partlen/2),int(partlen/2))])
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kernelres=2500
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kernelbase = np.linspace(-1,1,2*kernelres+1)
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kernel = np.exp(-1/(1-np.abs(kernelbase)**2))
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kernel=kernel/np.sum(kernel)
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spec_ext = np.hstack((spec[-kernelres:],spec,spec[:kernelres]))
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specc=np.convolve(spec_ext,kernel,mode='same')[kernelres:-kernelres]
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with open(path+f"eps={eps:.3f}_smooth_spectrum.txt", 'w', encoding='utf-8') as f:
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json.dump(list(specc),f,indent=1)
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else:
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freqqs = np.array([freqs[pos]
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for pos in range(int((-partlen+accum)/2), int((partlen+accum)/2),accum)])
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specc = np.array([( spectrum[pos-int(accum/2)]/2 + sum(spectrum[pos-int(accum/2)+1:pos+int(accum/2)-1]) + spectrum[pos+int(accum/2)-1] + spectrum[pos+int(accum/2)]/2 )/accum
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for pos in range(int((-partlen+accum)/2), int((partlen+accum)/2),accum)])
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halfh = (max(specc)+min(specc))/2
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#sigtonoi = sum([specc[pos] for pos in range(len(specc)) if specc[pos]>=halfh])/sum([specc[pos] for pos in range(len(specc)) if specc[pos]<halfh])
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fars = int(runsteps/accum/100)
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noisefloor = min(np.average(specc[:fars]),np.average(specc[-fars:]))
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speccnorm = specc - noisefloor
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totalpower = sum(specc)
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sigpower = sum(speccnorm)
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sig = max(specc)
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sn = sigpower/(totalpower-sigpower)
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sigtonoi = sig/(totalpower-sig)
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halfh_parts.append(halfh)
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sigtonoi_parts.append(sigtonoi)
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noisefloor_parts.append(noisefloor)
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totalpower_parts.append(totalpower)
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sigpower_parts.append(sig)
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sn_parts.append(sn)
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specc_list.append(specc)
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cumspecc = [speccnorm[0]]
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for pos in range(1,len(speccnorm)):
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cumspecc.append(cumspecc[pos-1]+speccnorm[pos])
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for pos in range(len(specc)):
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if cumspecc[pos+1]>=sigpower/2:
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median = pos
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stepdiff = speccnorm[pos]
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halfdiff = sum(speccnorm[:pos+1]) - sigpower/2
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freqstep = freqqs[pos] - freqqs[pos-1]
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freqmax = freqqs[pos] - freqstep * halfdiff/stepdiff
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break
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for pos in range(median, len(speccnorm)):
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if cumspecc[pos+1]>=sigpower*3/4:
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stepdiff = speccnorm[pos]
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halfdiff = sum(speccnorm[:pos+1]) - sigpower*3/4
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freqstep = freqqs[pos] - freqqs[pos-1]
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freqquart3 = freqqs[pos] - freqstep * halfdiff/stepdiff
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break
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for pos in range(median+1):
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if cumspecc[pos+1]>=sigpower/4:
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stepdiff = speccnorm[pos]
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halfdiff = sum(speccnorm[:pos+1]) - sigpower/4
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freqstep = freqqs[pos] - freqqs[pos-1]
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freqquart1 = freqqs[pos] - freqstep * halfdiff/stepdiff
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break
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freqfwhm = freqquart3-freqquart1
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gamma = freqfwhm/2
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freqmax_parts.append(freqmax)
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freqfwhm_parts.append(freqfwhm)
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print(gamma**2/median**2)
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lorentz = sigpower/m.pi * accum/partlen * gamma/((freqqs-freqmax)**2+gamma**2) + noisefloor
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lorentz_list.append(lorentz)
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speccpdf = speccnorm/sigpower
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deviation = np.sqrt(sum((specc-lorentz)**2)/len(specc))/sigpower
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maxpos = 0
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for i in range(len(freqqs)):
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if abs(freqqs[i]-freqmax)<abs(freqqs[maxpos]-freqmax):
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maxpos = i
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pos=maxpos
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try:
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while lorentz[pos]>lorentz[maxpos]/2:
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pos-=1
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lhm=freqqs[pos]
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except:
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lhm=freqqs[0]
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pos=maxpos
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try:
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while lorentz[pos]>lorentz[maxpos]/2:
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pos+=1
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uhm=freqqs[pos]
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except:
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uhm=freqqs[-1]
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SPECC = np.average(specc_list,axis=0)
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LORENTZ = np.average(lorentz_list,axis=0)
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DEV = np.sqrt(sum((SPECC-LORENTZ)**2)/len(SPECC))/sum(SPECC)
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TOTP.append(np.average(totalpower_parts))
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SIGP.append(np.average(sigpower_parts))
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SN.append(np.average(sn_parts))
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STON.append(sigtonoi)
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FMAX.append(np.average(freqmax_parts))
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FWHM.append(np.average(freqfwhm_parts))
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LHM.append(lhm)
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UHM.append(uhm)
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Q.append(np.average(freqmax_parts)/np.average(freqfwhm_parts))
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SOS.append(DEV)
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#%%
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with open(path+f"signal/SN_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(SN, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/FMAX_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(FMAX, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/FWHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(FWHM, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/LHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(LHM, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/UHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(UHM, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/TOTP_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(TOTP, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/SIGP_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(SIGP, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/Q_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(Q, f, ensure_ascii=False, indent=4)
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with open(path+f"signal/STON_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(STON, f, ensure_ascii=False, indent=4)
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#%%
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plotpath = path + 'spectra/'
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# qtplot(f'Frequency spectrum for dim={dim} eps={eps:.3f}',
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# [freqqs]*2,
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# [LORENTZ,SPECC],
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# [f'lorentz regression dev={DEV}','spectrum'],
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# x_tag = 'frequency f',
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# y_tag = 'spectral power p',
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# y_log = False,
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# export=True,
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# lw=1,
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# path=plotpath,
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# filename=f'Lorentz and Cauchy fit to spectrum {parts} parts accum={accum} eps={round(eps,3):.3f}.png',
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# close=True)
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#%%
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print("Power {}, Signal {}".format(round(totalpower), round(sigpower)))
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print("Done {:.3f}: DEV {}, FMAX {}, FWHM {}".format(eps, round(deviation,3), round(freqmax,5), round(FWHM[-1],5)))
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LORENTZ_eps.append(LORENTZ)
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SPECC_eps.append(SPECC)
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#%%
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# vareps=chr(949)
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# qtplot(f'Frequency spectra to noise level',
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# [freqqs[50::100]]*len(eps_space),
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# [SPECC[50::100] for SPECC in SPECC_eps],
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# [f'{vareps}={eps:.3f}' for eps in eps_space],
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# x_tag = 'frequency f',
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# y_tag = 'energy spectral density',
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# y_log = True,
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# export=False,
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# lw=2,
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# path=plotpath,
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# filename=f'Lorentz and Cauchy fit to spectrum log {parts} parts accum={accum} eps={round(eps,3):.3f}.png',
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# close=False)
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#%%
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TOTP_eps.append(TOTP)
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SIGP_eps.append(SIGP)
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SN_eps.append(SN)
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STON_eps.append(STON)
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FMAX_eps.append(FMAX)
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FWHM_eps.append(FWHM)
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Q_eps.append(Q)
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LHM_eps.append(LHM)
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UHM_eps.append(UHM)
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SOS_eps.append(SOS)
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#%%
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sigpath = basepath + 'signal/'
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if not os.path.exists(sigpath):
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os.makedirs(sigpath)
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# qtplot(f'Signal to noise for dim={dim} eps={eps:.3f}',
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# [eps_space],
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# [SN],
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# ['signalpower to noisefloor'],
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# x_tag = 'epsilon',
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# y_tag = 'ratio',
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# y_log = False,
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# export=True,
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# path=sigpath,
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# filename=f'SN_plot.png',
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# close=True)
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qtplot(f'Q facor for odd automaton sizes',
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[eps_space]*3,
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Q_eps,
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[f'dim={dim}x{dim}' for dim in dims],
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y_tag = 'purity',
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y_log = False,
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export=True,
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path=sigpath,
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filename=f'Q_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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# with open(path+f"signal/FMAX_1_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'r', encoding='utf-8') as f:
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# FMAX=json.load(f)
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# with open(path+f"signal/FWHM_1_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'r', encoding='utf-8') as f:
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# FWHM=json.load(f)
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qtplot(f'Dominant frequency',
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2023-12-10 21:47:15 +00:00
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[[0]+list(eps_space[:20])]*3,
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[[0]+FMAX[:20],[0]+LHM[:20],[0]+UHM[:20]],
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2023-09-30 17:53:06 +00:00
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# [f'dim={dim}x{dim}' for dim in dims],
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2023-12-10 21:47:15 +00:00
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['FMAX', 'FMAX-FWHM/2', 'FMAX+FWHM/2'],
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colors=['r','r','g'],
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2023-09-30 17:53:06 +00:00
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y_tag = 'frequency f',
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2023-12-10 21:47:15 +00:00
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y_log = False,
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2023-09-30 17:53:06 +00:00
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export=True,
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path=sigpath,
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filename=f'FMAX+FWHMto50_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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qtplot(f'Dominant frequency',
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[[0]+list(eps_space[:-1])]*3,
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[[0]+FMAX[:-1] for FMAX in FMAX_eps],#, [[0]+LHM[i][:50] for LHM in LHM_eps], [[0]+UHM[i][:50] for UHM in UHM_eps],
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[f'dim={dim}x{dim}' for dim in dims],
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#[['dominant frequency', 'lesser half maximum', 'upper half maximum'],
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#colors=['g','r','r'],
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y_tag = 'frequency f',
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y_log = True,
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export=True,
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path=sigpath,
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filename=f'FMAX+FWHMto50_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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qtplot(f'Total and signal energy to noise level',
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[eps_space]*6,
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list(np.array(SIGP_eps)/runsteps*accum)+list(np.array(TOTP_eps)/runsteps*accum),
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[f'signal energy for dim={dim:02d}' for dim in dims]+[f'total energy for dim={dim:02d}' for dim in dims],
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colors=['b','g','r','c','y','m'],
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y_tag = f'energy',
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y_log = True,
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export=True,
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path=sigpath,
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filename=f'POWER_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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qtplot(f'Signal-to-noise ratio to noise level',
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[eps_space]*len(dims),
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STON_eps,
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[f'dim={dim:02d}x{dim:02d}' for dim in dims],
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y_tag = f'ratio S/N',
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y_log = True,
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export=True,
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path=sigpath,
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filename=f'SN_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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qtplot(f'Goodness of fit to Lorentz curve',
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[eps_space]*len(dims),
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SOS_eps,
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[f'dim={dim:02d}x{dim:02d}' for dim in dims],
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y_tag = f'mean deviation',
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y_log = False,
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export=True,
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path=sigpath,
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filename=f'DEV_plot_{parts}parts_accum={accum}.png',
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close=False)
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#%%
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with open(basepath+f"signal/SN_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(SN_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/FMAX_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(FMAX_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/FWHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(FWHM_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/LHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(LHM_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/UHM_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(UHM_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/TOTP_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(TOTP_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/SIGP_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(SIGP_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/Q_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(Q_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/STON_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(STON_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/Q_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(Q_eps, f, ensure_ascii=False, indent=4)
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with open(basepath+f"signal/STON_{parts}_accum={accum}_dim={dim}_runsteps={runsteps}.txt", 'w', encoding='utf-8') as f:
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json.dump(STON_eps, f, ensure_ascii=False, indent=4)
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def plot_execute():
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if sys.flags.interactive != 1 or not hasattr(qt.QtCore, 'PYQT_VERSION'):
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qt.QtGui.QApplication.exec_()
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