#!/usr/bin/env python3 # -*- coding: utf-8 -*- """ Created on Mon Aug 21 14:59:22 2023 @author: astral """ import json import math as m import numpy as np from numpy.linalg import norm from datetime import datetime from random import sample as choose from plot import qtplot eps_space = list(np.linspace(0.01,0.2,20)) def resultant(sample): phase_x = [m.cos(ind) for ind in sample] phase_y = [m.sin(ind) for ind in sample] return (np.average(phase_x), np.average(phase_y)) def H2(x): return -x*m.log2(x)-(1-x)*m.log2(1-x) extremes = None maxdt = 300 for dim in [9]: for eps in eps_space[:10]: path=f'/cloud/Public/_data/neuropercolation/4lay/cons=7-knight_steps=1000100/dim=07/batch=0/' try: with open(path+f"eps={round(eps,3):.3f}_phase_diff.txt", 'r', encoding='utf-8') as f: phase_diff = json.load(f) except: with open(path+f"eps={round(eps,3):.3f}_activation.txt", 'r', encoding='utf-8') as f: activation = json.load(f)[100:] osc = list(zip(*activation)) phase = np.array([[np.arctan2(*act[::-1]) for act in osc[i]] for i in range(2)]) phase_diff = (phase[1]-phase[0]+m.pi)%(2*m.pi)-m.pi with open(path+f"eps={round(eps,3):.3f}_phase_diff.txt", 'w', encoding='utf-8') as f: json.dump(list(phase_diff), f, indent=1) all_res = norm(resultant(phase_diff)) av_diff = np.arccos(all_res) try: with open(path+f"eps={round(eps,3):.3f}_ei.txt", 'r', encoding='utf-8') as f: ei = json.load(f) except: with open(path+f"eps={round(eps,3):.3f}_channels.txt", 'r', encoding='utf-8') as f: channels = json.load(f)[100:] ei = [np.sum(cha)*(1-H2(eps)) for cha in channels] with open(path+f"eps={round(eps,3):.3f}_ei.txt", 'w', encoding='utf-8') as f: json.dump(ei, f, indent=1) pha_center = av_diff pha_dev = m.pi orth_ind = sorted([i for i,val in enumerate(ei[:-maxdt]) if (pha_center-pha_dev)<=abs(phase_diff[i])<=(pha_center+pha_dev)], key = lambda i: ei[i]) thres = 0.04*m.pi last_sync = lambda i: i if abs(phase_diff[i])<0.08*m.pi else last_sync(i-1) last_orth = lambda i: i if 0.42*m.pithres] diff00_ind = [last_sync(i) for i,pha in trav_out] diff00m_ind = [last_sync(i) for i,pha in trav_out if pha<0] diff00p_ind = [last_sync(i) for i,pha in trav_out if pha>0] trav_in = [(i,pha) for i,pha in enumerate(phase_diff[:-maxdt]) if m.pi/2-thres0] print(f'{len(diff00_ind)}/{len(trav_out)} synced states and {len(diff90_ind)}/{len(trav_in)} orthogonal states') #print(all_res, av_diff) in_ei = [] out_ei = [] inm_res = [] inp_res = [] outm_res = [] outp_res = [] for dt in range(maxdt): inm_res.append( resultant([phase_diff[i+dt] for i in diff90m_ind]) ) outm_res.append( resultant([phase_diff[i+dt] for i in diff00m_ind]) ) inp_res.append( resultant([phase_diff[i+dt] for i in diff90p_ind]) ) outp_res.append( resultant([phase_diff[i+dt] for i in diff00p_ind]) ) in_ei.append( np.average([ei[i+dt] for i in diff90_ind]) ) out_ei.append( np.average([ei[i+dt] for i in diff00_ind]) ) if dt%100==99: print(f'Done dt={dt}') im_res = list(zip(*inm_res)) om_res = list(zip(*outm_res)) ip_res = list(zip(*inp_res)) op_res = list(zip(*outp_res)) space = np.linspace(0,2*m.pi,101) av_ei = np.average(ei) qtplot(f'Transitions resultants for eps={round(eps,3):.3f} with dim={dim} with 4 layers', [im_res[0], om_res[0], ip_res[0], op_res[0], np.cos(space)], [im_res[1], om_res[1], ip_res[1], op_res[1], np.sin(space)], ['Resultant ev inward -', 'Resultant ev outward -', 'Resultant ev inward +', 'Resultant ev outward +', 'Unit Circle'], x_tag = 'x', y_tag = 'y', lw=1, export=True, path=path, filename=f'Transitions resultant pm for eps={round(eps,3):.3f} dim={dim}.png', close=False) qtplot(f'Transitions ei for eps={round(eps,3):.3f} with dim={dim} with 4 layers', [np.array(range(maxdt))]*3, [in_ei, out_ei, [av_ei]*maxdt], ['EI ev inward', 'EI ev outward', 'Average EI'], x_tag = 'dt', y_tag = 'average ei', export=True, path=path, filename=f'Transitions EI for eps={round(eps,3):.3f} dim={dim} .png', close=False) print(f'Done eps={eps:.3f} with dim={dim} at {datetime.now()}') # qtplot(f'Resultant and EI evolution for dim={dim} with 4 layers', # [[0]+eps_space]*2, # [max(av_ei)*diff_res, av_ei], # ['Resultant', 'avEI'], # export=True, # path=path, # filename=f'Resultant and EI for dim={dim}.png', # close=True)