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wrap_power_trajectory.py
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wrap_power_trajectory.py
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import sdf
import matplotlib
matplotlib.use('agg')
#%matplotlib inline
import matplotlib.pyplot as plt
import numpy as np
#from numpy import ma
from matplotlib import colors, ticker, cm
from matplotlib.mlab import bivariate_normal
from optparse import OptionParser
import os
######## Constant defined here ########
pi = 3.1415926535897932384626
q0 = 1.602176565e-19 # C
m0 = 9.10938291e-31 # kg
v0 = 2.99792458e8 # m/s^2
kb = 1.3806488e-23 # J/K
mu0 = 4.0e-7*pi # N/A^2
epsilon0 = 8.8541878176203899e-12 # F/m
h_planck = 6.62606957e-34 # J s
wavelength= 1.0e-6
frequency = v0*2*pi/wavelength
exunit = m0*v0*frequency/q0
bxunit = m0*frequency/q0
denunit = frequency**2*epsilon0*m0/q0**2
print('electric field unit: '+str(exunit))
print('magnetic field unit: '+str(bxunit))
print('density unit nc: '+str(denunit))
font = {'family' : 'monospace',
'style' : 'normal',
'color' : 'black',
'weight' : 'normal',
'size' : 20,
}
directory = './txt_1300/'
px = np.loadtxt(directory+'px2d_x.txt')
py = np.loadtxt(directory+'py2d_x.txt')
xx = np.loadtxt(directory+'xx2d_x.txt')
yy = np.loadtxt(directory+'yy2d_x.txt')
workx2d = np.loadtxt(directory+'workx2d_x.txt')
worky2d = np.loadtxt(directory+'worky2d_x.txt')
fieldex = np.loadtxt(directory+'fieldex2d_x.txt')/4.0
fieldey = np.loadtxt(directory+'fieldey2d_x.txt')/4.0
fieldbz = np.loadtxt(directory+'fieldbz2d_x.txt')/4.0
ey_averaged = -8.0/3.2*yy
bz_averaged = -8.0/3.2*yy
laser_ey = fieldey-ey_averaged
laser_bz = fieldbz-bz_averaged
gg = (px**2+py**2+1)**0.5
R = gg-px
theta = np.arctan2(py,px)
number=400
tt = np.linspace(5.0,130,1250)
#tt = tt[:,np.newaxis]
select_x = np.array([21,17,2,57,58,68,72,78,172,107])
line_y1 = np.linspace(-12,-3.2,1001)
line_x1 = np.zeros_like(line_y1)+5
line_y2 = np.linspace(3.2,12,1001)
line_x2 = np.zeros_like(line_y2)+5
line_x3 = np.linspace(5,200.0,1001)
line_y3 = np.zeros_like(line_x3)+3.2
line_x4 = np.linspace(5,200.0,1001)
line_y4 = np.zeros_like(line_x4)-3.2
index=68
norm_x = matplotlib.colors.Normalize(vmin=1.,vmax=501.)
start = 40
#cbar=plt.colorbar( ticks=np.linspace(np.min(1), np.max(501), 5) )
#cbar.set_label('$\gamma$',fontdict=font)
#cbar.ax.set_yticklabels(cbar.ax.get_yticklabels(),fontsize=20)
# plt.legend(loc='upper right')
ax = plt.subplot(5,2,1)
plt.scatter(xx[index,:], yy[index,:], c=gg[index,:], norm=norm_x, s=6, cmap='autumn', edgecolors='None')
#plt.xlabel('Energy [MeV]',fontdict=font)
plt.ylabel('y [$\lambda$]',fontdict=font)
plt.xticks(fontsize=20); plt.yticks(fontsize=20);
#plt.yscale('log')
plt.xlim(4,126)
#plt.legend(loc='best',fontsize=20,framealpha=0.5)
ax = plt.subplot(5,2,3)
y1 = -(fieldex)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
plt.scatter(xx[index,:], yy[ind, c=gg[index,:], norm=norm_x, s=6, cmap='autumn', edgecolors='None')
ax = plt.subplot(5,2,5)
y1 = -(fieldey*py/px)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
ax = plt.subplot(5,2,7)
y1 = -(fieldey*py/px)[index,start:]-(fieldex)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
ax = plt.subplot(5,2,9)
plt.scatter(xx[index,:], gg[index,:], c=gg[index,:], norm=norm_x, s=6, cmap='autumn', edgecolors='None')
directory = './txt_1300/'
px = np.loadtxt(directory+'px2d_y.txt')
py = np.loadtxt(directory+'py2d_y.txt')
xx = np.loadtxt(directory+'xx2d_y.txt')
yy = np.loadtxt(directory+'yy2d_y.txt')
workx2d = np.loadtxt(directory+'workx2d_y.txt')
worky2d = np.loadtxt(directory+'worky2d_y.txt')
fieldex = np.loadtxt(directory+'fieldex2d_y.txt')/4.0
fieldey = np.loadtxt(directory+'fieldey2d_y.txt')/4.0
fieldbz = np.loadtxt(directory+'fieldbz2d_y.txt')/4.0
ey_averaged = -8.0/3.2*yy
bz_averaged = -8.0/3.2*yy
laser_ey = fieldey-ey_averaged
laser_bz = fieldbz-bz_averaged
gg = (px**2+py**2+1)**0.5
R = gg-px
theta = np.arctan2(py,px)
number=400
#tt = tt[:,np.newaxis]
line_y1 = np.linspace(-12,-3.2,1001)
line_x1 = np.zeros_like(line_y1)+5
line_y2 = np.linspace(3.2,12,1001)
line_x2 = np.zeros_like(line_y2)+5
line_x3 = np.linspace(5,200.0,1001)
line_y3 = np.zeros_like(line_x3)+3.2
line_x4 = np.linspace(5,200.0,1001)
line_y4 = np.zeros_like(line_x4)-3.2
index=3
norm_x = matplotlib.colors.Normalize(vmin=1.,vmax=301.)
#cbar=plt.colorbar( ticks=np.linspace(np.min(1), np.max(501), 5) )
#cbar.set_label('$\gamma$',fontdict=font)
#cbar.ax.set_yticklabels(cbar.ax.get_yticklabels(),fontsize=20)
# plt.legend(loc='upper right')
ax = plt.subplot(5,2,2)
plt.scatter(xx[index,:],yy[index,:], c=gg[index,:], norm=norm_x, s=6, cmap='winter', edgecolors='None')
ax = plt.subplot(5,2,4)
y1 = -(fieldex)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
ax = plt.subplot(5,2,6)
y1 = -(fieldey*py/px)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
ax = plt.subplot(5,2,8)
y1 = -(fieldey*py/px)[index,start:]-(fieldex)[index,start:]
y2 = np.zeros_like(y1)
ax.fill_between(xx[index,start:],y1,y2, where=y1>=y2, facecolor='green',alpha=0.3,interpolate=True)
ax.fill_between(xx[index,start:],y1,y2, where=y1<=y2, facecolor='red',alpha=0.3,interpolate=True)
ax = plt.subplot(5,2,10)
plt.scatter(xx[index,:],gg[index,:], c=gg[index,:], norm=norm_x, s=6, cmap='winter', edgecolors='None')
#cbar=plt.colorbar( ticks=np.linspace(np.min(1), np.max(301), 5) )
#cbar.set_label('$\gamma$',fontdict=font)
#cbar.ax.set_yticklabels(cbar.ax.get_yticklabels(),fontsize=20)
# plt.legend(loc='upper right')
#plt.xlim(-5,130)
#plt.ylim(-3.8,3.8)
#plt.xlabel('x [$\lambda$]',fontdict=font)
#plt.ylabel('y [$\lambda$]',fontdict=font)
#plt.xticks(fontsize=20); plt.yticks(fontsize=20);
#plt.title('electron at y='+str(round(y[n,0]/2/np.pi,4)),fontdict=font)
fig = plt.gcf()
fig.set_size_inches(32.0, 25)
fig.savefig('./figure_wrap_up/'+'trajectory_pwer.png',format='png',dpi=160)
plt.close("all")