Version 0.500

examples/example_crossphasemodulation_6.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber import pypho_fiber
+from pypho_cwlaser import pypho_cwlaser
+from pypho_optfi import pypho_optfi
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.patches as mpatches
+import matplotlib.pyplot as plt
+
+
+
+# Define network elements
+gp       = pypho_setup(nos = 4*16, sps = 1*128, symbolrate = 10e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'singlepulse') # Set pattern = "singlepulse"
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = 0.33)
+sig_f0   = pypho_cwlaser(glova = gp, power = 3, Df = 0,  teta = 1*np.pi/4.0)
+sig_f1   = pypho_lasmod(glova = gp, power = 0, Df = 500, teta = 1*np.pi/1.0)
+filter_f0 = pypho_optfi(glova = gp, Df = 0, B = 50)
+SSMF     = pypho_fiber(glova = gp, l = 80,  D = 9.0,   S = 0.0, alpha = 0.2, gamma = 1.4, phi_max = .1)
+
+# Simulation
+
+# Define wavelength channel
+
+E_f0  = sig_f0()                                              
+
+bits    = bitsrc()
+esig    = esigsrc(bitsequence = bits)
+E_f1       = sig_f1(esig = esig)  
+E = copy.deepcopy(E_f1)
+
+E[0]['E'][0] = E_f0[0]['E'][0] + E_f1[0]['E'][0]  # Multiplex all signals X-Pol
+E[0]['E'][1] = E_f0[0]['E'][1] + E_f1[0]['E'][1]  # Multiplex all signals Y-Pol 
+
+
+E_Tx = copy.deepcopy(E)
+# Plot Spectrum Input signals
+plt.figure(1)
+plt.subplot(2, 1, 1)
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][0]   )**2))), 'r')
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][1]   )**2))), 'g:')
+plt.title("Input spectrum", loc='left')
+plt.ylabel('Spec. density');
+plt.grid(True)
+
+# Fiber transmission
+       
+E = SSMF(E = E)    
+
+# Plot Spectrum Output signals
+plt.subplot(2, 1, 2)
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][0]   )**2))), 'r')
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][1]   )**2))), 'g:')
+plt.title("Output spectrum", loc='left')
+plt.ylabel('Spec. density'); plt.xlabel('Frequency deviation [GHz]');
+plt.grid(True)
+
+
+# Calculate phase shift
+L_eff = (1-np.exp(-SSMF.l*SSMF.alpha))/(SSMF.alpha)
+phi_x_max = - (np.max(np.abs(E_Tx[0]['E'][0])**2) + 2.0/3.0* np.max(np.abs(E_Tx[0]['E'][1])**2))* L_eff * SSMF.gamma *1e-3
+phi_y_max = - (np.max(np.abs(E_Tx[0]['E'][1])**2) + 2.0/3.0* np.max(np.abs(E_Tx[0]['E'][0])**2))* L_eff * SSMF.gamma *1e-3
+
+print 'L_eff = ', L_eff
+print 'phi_x_max = ', phi_x_max
+print 'phi_y_max = ', phi_y_max
+
+# Plot power of both pol axis as function of transmission distance
+plt.figure(2)
+
+plt.subplot(2, 1, 2)
+plt.ylabel('$10log |E_y|^2$'); plt.xlabel('Transmission distance [m]');
+plt.ylim((-120, 10))
+plt.grid(True)
+plt.subplot(2, 1, 1)
+plt.ylabel('$10log |E_y|^2$');
+plt.ylim((-120, 10)) 
+plt.grid(True)
+plt.legend()
+plt.show()
\ No newline at end of file

examples/example_dispersion_1.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber import pypho_fiber
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.pyplot as plt
+from scipy.interpolate import UnivariateSpline
+
+# Define network elements
+gp       = pypho_setup(nos = 16, sps = 256, symbolrate = 10e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'singlepulse')
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = 0.85)
+sig_1550 = pypho_lasmod(glova = gp, power = 0, Df = 0, teta = 0)
+SSMF     = pypho_fiber(glova = gp, l = 80.0e3,  D = 17,   S = 0, alpha = 0.2e-12, gamma = 0, phi_max=10.0)
+
+# Simulation
+bits = bitsrc()
+esig = esigsrc(bitsequence = bits)
+E_Tx = sig_1550(esig = esig)                                                      
+
+
+# Define your parameters here
+T_0 = 25.0e-12
+z = 100.0e3
+D = 17.0
+beta_2, beta_3 = DS2beta(17.0, 0, gp.lambda0)
+
+
+# Create a single pulse with gaussian shape (not power!)
+E_Tx[0]['E'][0] = E_Tx[0]['E'][0]*0 + np.exp(-(gp.timeax-gp.timeax[-1]/2)**2 / (2.0*T_0**2) )
+E = copy.deepcopy(E_Tx)
+
+# Fiber trannsmission
+E = SSMF(E = E, D = D, l = z) 
+
+# Plot Input and Output signal 
+plt.figure(1)
+plt.plot(gp.timeax*1.0e12, np.abs(E_Tx[0]['E'][0]), 'r', label='$E(0, t)$')
+plt.plot(gp.timeax*1.0e12, np.abs(E[0]['E'][0]), 'g', label='$E(z=100$km$, t)$')
+
+
+# Get FWHM of the input signal E_Tx
+spline = UnivariateSpline(gp.timeax*1.0e12, np.abs(E_Tx[0]['E'][0])-1*np.max(np.abs(E_Tx[0]['E'][0]))/2, s=0)
+r1, r2 = spline.roots() # find the roots
+plt.annotate(s='', xy=(r1,np.max(np.abs(E_Tx[0]['E'][0]))/2), xytext=(r2,np.max(np.abs(E_Tx[0]['E'][0]))/2), arrowprops=dict(arrowstyle='<->'))
+plt.text(r1+(r2-r1)/2.0, 0.01 +np.max(np.abs(E_Tx[0]['E'][0]))/2, '$T_{FWHM,0}$ = ' + str(np.round(r2-r1,2)) + ' ps', fontsize=12, horizontalalignment='center')
+T_FWHM_0 = (r2-r1) * 1e-12
+T_0_plot = T_FWHM_0 / 2.35482
+
+
+# Get FWHM of the output signal E
+spline = UnivariateSpline(gp.timeax*1.0e12, np.abs(E[0]['E'][0])-1*np.max(np.abs(E[0]['E'][0]))/2, s=0)
+r1, r2 = spline.roots() # find the roots
+plt.annotate(s='', xy=(r1,np.max(np.abs(E[0]['E'][0]))/2), xytext=(r2,np.max(np.abs(E[0]['E'][0]))/2), arrowprops=dict(arrowstyle='<->'))
+plt.text(r1+(r2-r1)/2.0, 0.01 + np.max(np.abs(E[0]['E'][0]))/2, '$T_{FWHM,1}$ = ' + str(np.round(r2-r1,2)) + ' ps', fontsize=12, horizontalalignment='center')
+T_FWHM_1 = (r2-r1) * 1e-12
+plt.ylabel('$|E|$ a.u.'); plt.xlabel('Time $t$ [ps]'); legend = plt.legend(loc='upper right')
+
+L_D = (T_0_plot)**2  / np.abs(beta_2)
+# Print the results
+print 'Input signal 1/e-pulse width by definition : T_0 = ' , T_0*1e12, ' ps'
+print 'Input signal 1/e-pulse width from plot : T_0 = ' , T_0_plot*1e12, ' ps'
+print 'Input signal FWHM-pulse width from plot : T_FWHM,0 = ' , T_FWHM_0*1e12, ' ps'
+print 'Output signal FWHM-pulse width from plot : T_FWHM,1 = ' , T_FWHM_1*1e12, ' ps'
+print 'Calculated output FWHM-pulse width : T_FWHM,1 = ' , T_FWHM_0 * np.sqrt(1 + (z/L_D)**2)*1e12, ' ps'
\ No newline at end of file

examples/example_dispersion_2.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber import pypho_fiber
+from pypho_eye import pypho_eye
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.patches as mpatches
+import matplotlib.pyplot as plt
+from scipy.interpolate import UnivariateSpline
+
+# Define some parameter
+T_FWHM = 50e-12       # FWHM-pulsewidth of the optical power
+T_e = T_FWHM / 1.66510  # 1/e-pulsewidth of the electrical field
+z = 29.756e3         # Fiber length
+D = 16.8                # Dispersion coefficient
+T_FWHM_norm_max = 0.75   # Maximum FWHM pulseiwdth of the 
+
+# Define network elements
+gp       = pypho_setup(nos = 4*16, sps = 1*256, symbolrate = 10e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'random') # Set pattern = "singlepulse"
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = T_FWHM*gp.symbolrate)
+sig_1550 = pypho_lasmod(glova = gp, power = 0, Df = 0, teta = 0)
+SSMF     = pypho_fiber(glova = gp, l = z,  D = D,   S = 0, alpha = 0.2e-12, gamma = 0, phi_max = 10.0)
+eye      = pypho_eye(glova = gp, polarisation = 'x,y')
+
+# Simulation
+bits = bitsrc()
+
+esig = esigsrc(bitsequence = bits)
+E_Tx = sig_1550(esig = esig)                                              
+
+E = copy.deepcopy(E_Tx)
+
+# Fiber trannsmission
+E = SSMF(E = E) 
+E[0]['E'][0] = E[0]['E'][0] /np.max(np.abs(E[0]['E'][0]))*1e-3
+E_Tx[0]['E'][0] = E_Tx[0]['E'][0] /np.max(np.abs(E_Tx[0]['E'][0]))*1e-3
+# Plot Input and Output signal
+beta_2, beta_3 = DS2beta(D, 0, gp.lambda0)
+L_D = (T_e)**2  / np.abs(beta_2)     # Pulse width T_e here of the electrical field
+ 
+plt.figure(1)
+eye(E = E_Tx[0]['E'], polarisation = 'x', style="r")
+eye(E = E[0]['E'], polarisation = 'x', style="g")
+
+red_patch = mpatches.Patch(color='red', label='Input signal')
+green_patch = mpatches.Patch(color='green', label='Output signal')
+plt.legend(handles=[red_patch, green_patch], loc=1)
+print 'Calculated output FWHM-pulse width : T_FWHM,1 = ' , T_FWHM * np.sqrt(1 + (z/L_D)**2)*1e12, ' ps'
+
+T_FWHM_norm_0 = T_FWHM*1e12 / 100.0
+print (  'Calculated max reach : ' , 100e-12**2 *(1/1.665095)**2 * 2.0*np.pi * 299792458 *  T_FWHM_norm_0*np.sqrt(  T_FWHM_norm_max**2 - T_FWHM_norm_0**2) / (16.8e-6 * 1550e-9**2 )  *1e-3 )
\ No newline at end of file

examples/example_dispersion_3.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber import pypho_fiber
+from pypho_eye import pypho_eye
+from pypho_optfi import pypho_optfi
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.patches as mpatches
+import matplotlib.pyplot as plt
+
+# Define network elements
+gp       = pypho_setup(nos = 4*16, sps = 1*256, symbolrate = 40e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'random') # Set pattern = "singlepulse"
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = 0.33)
+sig_1550 = pypho_lasmod(glova = gp, power = 0, Df = 0, teta = 0)
+sig_1546 = pypho_lasmod(glova = gp, power = 0, Df = +500, teta = 0)
+sig_1554 = pypho_lasmod(glova = gp, power = 0, Df = -500, teta = 0)
+filter_1550 = pypho_optfi(glova = gp, Df = 0, B = 100)
+filter_1546 = pypho_optfi(glova = gp, Df = +500, B = 100)
+filter_1554 = pypho_optfi(glova = gp, Df = -500, B = 100)
+SSMF     = pypho_fiber(glova = gp, l = 100e3,  D = 16.8,   S = 0.058, alpha = 0.2e-12, gamma = 0, phi_max = 10.0)
+DCF      = pypho_fiber(glova = gp, l = 16.8e3,  D = -100.0,   S = -0.058/16.8 * 100.0, alpha = 0.2e-12, gamma = 0, phi_max = 10.0)
+eye      = pypho_eye(glova = gp, polarisation = 'x,y')
+
+# Simulation
+bits = bitsrc()
+
+esig = esigsrc(bitsequence = bits)
+E_1550 = sig_1550(esig = esig)                                              
+E_1546 = sig_1546(esig = esig)
+E_1554 = sig_1554(esig = esig)
+
+
+# Plot Input signals
+plt.figure(1)
+plt.subplot(3, 1, 1)
+plt.title("$\lambda$=1546nm", loc='left')
+eye(E = E_1546[0]['E'], polarisation = 'x', style="0.5")
+
+plt.subplot(3, 1, 2)
+plt.title("$\lambda$=1550nm", loc='left')
+eye(E = E_1550[0]['E'], polarisation = 'x', style="0.5")
+
+plt.subplot(3, 1, 3)
+plt.title("$\lambda$=1554nm", loc='left')
+eye(E = E_1554[0]['E'], polarisation = 'x', style="0.5")
+
+E_Tx = copy.deepcopy(E_1550)
+E_Tx[0]['E'][0] = E_1550[0]['E'][0] + E_1546[0]['E'][0] + E_1554[0]['E'][0] # Multiplex all signals 
+E = copy.deepcopy(E_Tx)
+
+# Fiber trannsmission
+E = SSMF(E = E,l = 100e3,  D = 16.8, S = 0.058) 
+E =  DCF(E = E,l = 16.8e3, D = -100, S = -0.058/16.8 * 100) # For full dispersion compenstion set S = -0.058/16.8 * 100
+
+
+# Filter out the channels
+E_1550 = filter_1550(E = copy.deepcopy(E))
+E_1546 = filter_1546(E = copy.deepcopy(E))
+E_1554 = filter_1554(E = copy.deepcopy(E))
+
+# Plot Output signals
+#plt.figure(2)
+plt.subplot(3, 1, 1)
+eye(E = E_1546[0]['E'], polarisation = 'x', style="r")
+red_patch = mpatches.Patch(color='0.5', label='Input signal')
+green_patch = mpatches.Patch(color='red', label='Output signal')
+plt.legend(handles=[red_patch, green_patch], loc=1)
+
+plt.subplot(3, 1, 2)
+eye(E = E_1550[0]['E'], polarisation = 'x', style="r")
+plt.subplot(3, 1, 3)
+eye(E = E_1554[0]['E'], polarisation = 'x', style="r")
+

examples/example_fourwavemixing_4.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_fiber import pypho_fiber
+from pypho_cwlaser import pypho_cwlaser
+from pypho_optfi import pypho_optfi
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.patches as mpatches
+import matplotlib.pyplot as plt
+
+#  Define some paramaters
+
+delta_f = 25       # Frequency difference of the two cw-signals
+L = 20e3           # Fiber length in m
+l = 0.1e3           # Step fiber length in m
+k = 7               # Defines how man channels left and right will be analyzed
+chut = np.arange(-k*delta_f, k*delta_f+delta_f, delta_f)        # Channels under test
+
+
+P_FWM_x = np.zeros((chut.size, int(L/l)))
+P_FWM_y = np.zeros((chut.size, int(L/l)))
+
+# Define network elements
+gp       = pypho_setup(nos = 4*16, sps = 1*128, symbolrate = 10e9)
+sig_f0  = pypho_cwlaser(glova = gp, power = 3, Df = 0, teta = 1*np.pi/4.0)
+sig_f   = pypho_cwlaser(glova = gp, power = 3, Df = delta_f, teta = 1*np.pi/2.0)
+filter_df = pypho_optfi(glova = gp, Df = 0, B = 10)
+SSMF     = pypho_fiber(glova = gp, l = l,  D = 5.0,   S = 0.0, alpha = 0.2, gamma = 1.4, phi_max = .1)
+
+# Simulation
+
+# Define wavelength channel
+E_f0  = sig_f0()                                              
+E_fm1 = sig_f(Df = +delta_f, teta = np.pi/2)
+E_fp1 = sig_f(Df = -delta_f, teta = np.pi/2)
+E_fm2 = sig_f(Df = -2*delta_f, teta = np.pi/2)
+E_fp2 = sig_f(Df = +2*delta_f, teta = np.pi/2)
+E = copy.deepcopy(E_fm1)
+
+E[0]['E'][0] = E_f0[0]['E'][0] + E_fp1[0]['E'][0] + E_fm1[0]['E'][0] + E_fp2[0]['E'][0] + E_fm2[0]['E'][0] # Multiplex all signals X-Pol
+E[0]['E'][1] = E_f0[0]['E'][1] + E_fp1[0]['E'][1] + E_fm1[0]['E'][1] + E_fp2[0]['E'][1] + E_fm2[0]['E'][1] # Multiplex all signals Y-Pol 
+
+
+E_Tx = copy.deepcopy(E)
+# Plot Spectrum Input signals
+plt.figure(1)
+plt.subplot(2, 1, 1)
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][0]   )**2))), 'r')
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][1]   )**2))), 'g:')
+plt.title("Input spectrum", loc='left')
+plt.ylabel('Spec. density');
+plt.grid(True)
+
+# Fiber transmission
+c1 = 0
+for z in np.arange(0,L,l):
+    print(z)
+    c2 = 0
+    for ch in chut:         # Loop through wavelengths and save mean power value of both pol axis
+        E_filtered = filter_df(copy.deepcopy(E), Df = ch)
+        P_FWM_x[c2][c1] = np.mean( np.abs(E_filtered[0]['E'][0])**2 )
+        P_FWM_y[c2][c1] = np.mean( np.abs(E_filtered[0]['E'][1])**2 )
+        c2 = c2 + 1
+
+    c1 = c1 + 1        
+    E = SSMF(E = E)    
+
+# Plot Spectrum Output signals
+plt.subplot(2, 1, 2)
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][0]   )**2))), 'r')
+plt.plot((gp.freqax-gp.f0)*1e-9, np.log10(abs(fftshift(fft(E[0]['E'][1]   )**2))), 'g:')
+plt.title("Output spectrum", loc='left')
+plt.ylabel('Spec. density'); plt.xlabel('Frequency deviation [GHz]');
+plt.grid(True)
+
+# Plot power of both pol axis as function of transmission distance
+plt.figure(2)
+for i in np.arange(0,chut.size):
+    plt.subplot(2, 1, 1)
+    plt.plot(np.arange(0,L,l), 10*np.log10(P_FWM_x[i]*1e3), label=str(chut[i]) + ' GHz') 
+    plt.subplot(2, 1, 2)
+    plt.plot(np.arange(0,L,l), 10*np.log10(P_FWM_y[i]*1e3)) 
+
+plt.subplot(2, 1, 2)
+plt.ylabel('$10log |E_y|^2$'); plt.xlabel('Transmission distance [m]');
+plt.ylim((-120, 10))
+plt.grid(True)
+plt.subplot(2, 1, 1)
+plt.ylabel('$10log |E_y|^2$');
+plt.ylim((-120, 10)) 
+plt.grid(True)
+plt.legend()
+plt.show()
\ No newline at end of file

examples/example_selfphasemodulation_5.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber import pypho_fiber
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.pyplot as plt
+
+
+
+# Define network elements
+gp       = pypho_setup(nos = 16, sps = 1*128, symbolrate = 10e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'ones')
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = 0.33)
+sig     = pypho_lasmod(glova = gp, power = 0, Df = 0, teta = np.pi/8)
+SSMF     = pypho_fiber(glova = gp, l = 80e3,  D = 0.0,   S = 0.0, alpha = 0.2, gamma = 1.4, phi_max = .1)
+
+# Simulation
+
+# Define wavelength channel
+bits    = bitsrc()
+esig    = esigsrc(bitsequence = bits)
+E       = sig(esig = esig)                                              
+
+E_Tx = copy.deepcopy(E)
+
+
+# Fiber transmission
+       
+E = SSMF(E = E)    
+
+# Plot power and phase of both pol axis
+plt.figure(1)
+plt.subplot(2, 1, 1)
+plt.plot(gp.timeax*1.0e12, np.abs(E[0]['E'][0])**2, 'r', label='$E_x(0, t)$')
+plt.plot(gp.timeax*1.0e12, np.abs(E[0]['E'][1])**2, 'g', label='$E_y(0, t)$')
+plt.ylabel('$10log |E_{x,y}|^2$'); plt.xlabel('Time [ps]');
+plt.grid(True)
+plt.legend()
+
+
+plt.subplot(2, 1, 2)
+plt.plot(gp.timeax*1.0e12, np.angle(E[0]['E'][0]), 'r', label='$E_x(0, t)$')
+plt.plot(gp.timeax*1.0e12, np.angle(E[0]['E'][1]), 'g', label='$E_y(0, t)$')
+plt.ylabel('$ \phi_{x,y} $'); plt.xlabel('Time [ps]');
+plt.grid(True)
+plt.legend()
+plt.show()
+
+# Calculate phase shift
+L_eff = (1-np.exp(-SSMF.l*SSMF.alpha))/(SSMF.alpha)
+phi_x_max = - (np.max(np.abs(E_Tx[0]['E'][0])**2) + 2.0/3.0* np.max(np.abs(E_Tx[0]['E'][1])**2))* L_eff * SSMF.gamma *1e-3
+phi_y_max = - (np.max(np.abs(E_Tx[0]['E'][1])**2) + 2.0/3.0* np.max(np.abs(E_Tx[0]['E'][0])**2))* L_eff * SSMF.gamma *1e-3
+
+print 'L_eff = ', L_eff
+print 'phi_x_max = ', phi_x_max
+print 'phi_y_max = ', phi_y_max
\ No newline at end of file

examples/gausswidth.py

+##!/usr/bin/env python2
+# -*- coding: utf-8 -*-
+
+#Import functions and libraries
+# Relase 0.5
+# arne.striegler@hm.edu
+
+import sys
+sys.path.append('../')
+from pypho_setup import pypho_setup
+from pypho_bits import pypho_bits
+from pypho_signalsrc import pypho_signalsrc
+from pypho_lasmod import pypho_lasmod
+from pypho_fiber_mod import pypho_fiber
+from pypho_functions import *
+import numpy as np
+import copy
+import matplotlib.pyplot as plt
+from scipy.interpolate import UnivariateSpline
+
+# Define network elements
+gp       = pypho_setup(nos = 16, sps = 256, symbolrate = 10e9)
+bitsrc   = pypho_bits(glova = gp, nob = gp.nos, pattern = 'singlepulse')
+esigsrc  = pypho_signalsrc(glova = gp, pulseshape = 'gauss_rz' , fwhm = 0.85)
+sig_1550 = pypho_lasmod(glova = gp, power = 0, Df = 0, teta = 0)
+SSMF     = pypho_fiber(glova = gp, l = 80.0e3,  D = 17,   S = 0, alpha = 0.2e-12, gamma = 0, phi_max=10.0)
+
+# Simulation
+bits = bitsrc()
+esig = esigsrc(bitsequence = bits)
+E_Tx = sig_1550(esig = esig)                                                      
+
+
+# Define your parameters here
+T_0 = 25.0e-12
+z = 50.0e3
+D = 17.0
+beta_2, beta_3 = DS2beta(17.0, 0, gp.lambda0)
+
+
+# Create a single pulse with gaussian shape (not power!)
+E_Tx[0]['E'][0] = E_Tx[0]['E'][0]*0 + np.exp(-(gp.timeax-gp.timeax[-1]/2)**2 / (2.0*T_0**2) )
+E = copy.deepcopy(E_Tx)
+E[0]['E'][0] = E[0]['E'][0]*0 + np.sqrt(np.exp(-(gp.timeax-gp.timeax[-1]/2)**2 / (2.0*T_0**2) ) )
+
+Eq = copy.deepcopy(E_Tx)
+Eq[0]['E'][0] = Eq[0]['E'][0]*0 + (np.exp(-(gp.timeax-gp.timeax[-1]/2)**2 / (2.0*T_0**2) ) )**2
+
+
+# Plot Input and Output signal 
+plt.figure(1)
+plt.plot(gp.timeax*1.0e12, np.abs(E_Tx[0]['E'][0]), 'r', label='Power: Gauss')
+plt.plot(gp.timeax*1.0e12, np.abs(E[0]['E'][0]), 'g', label='Power: sqrt.Gauss')
+plt.plot(gp.timeax*1.0e12, np.abs(Eq[0]['E'][0]), 'b', label='Power: Gauss**2')
+
+
+# Get FWHM of the input signal E_Tx
+spline = UnivariateSpline(gp.timeax*1.0e12, np.abs(E_Tx[0]['E'][0])-1*np.max(np.abs(E_Tx[0]['E'][0]))/2, s=0)
+r1, r2 = spline.roots() # find the roots
+plt.annotate(s='', xy=(r1,np.max(np.abs(E_Tx[0]['E'][0]))/2), xytext=(r2,np.max(np.abs(E_Tx[0]['E'][0]))/2), arrowprops=dict(arrowstyle='<->'))
+plt.text(r1+(r2-r1)/2.0, 0.04 +np.max(np.abs(E_Tx[0]['E'][0]))/2, '$T_{FWHM_0}$ = ' + str(np.round(r2-r1,2)) + ' ps', fontsize=12, horizontalalignment='center')
+T_FWHM_0 = (r2-r1) * 1e-12
+T_e_0 = T_FWHM_0 / 2.35482
+
+
+# Get FWHM of the output signal E
+spline = UnivariateSpline(gp.timeax*1.0e12, np.abs(E[0]['E'][0])-1*np.max(np.abs(E[0]['E'][0]))/2, s=0)
+r1, r2 = spline.roots() # find the roots
+plt.annotate(s='', xy=(r1,np.max(np.abs(E[0]['E'][0]))/2), xytext=(r2,np.max(np.abs(E[0]['E'][0]))/2), arrowprops=dict(arrowstyle='<->'))
+plt.text(r1+(r2-r1)/2.0, -0.04 + np.max(np.abs(E[0]['E'][0]))/2, '$T_{FWHM_1}$ = ' + str(np.round(r2-r1,2)) + ' ps', fontsize=12, horizontalalignment='center')
+T_FWHM_1 = (r2-r1) * 1e-12
+T_e_1 = T_FWHM_1 / 2.35482
+
+
+# Get FWHM of the output signal E
+spline = UnivariateSpline(gp.timeax*1.0e12, np.abs(Eq[0]['E'][0])-1*np.max(np.abs(Eq[0]['E'][0]))/2, s=0)
+r1, r2 = spline.roots() # find the roots
+plt.annotate(s='', xy=(r1,np.max(np.abs(Eq[0]['E'][0]))/2), xytext=(r2,np.max(np.abs(Eq[0]['E'][0]))/2), arrowprops=dict(arrowstyle='<->'))
+plt.text(r1+(r2-r1)/2.0, -0.1 + np.max(np.abs(Eq[0]['E'][0]))/2, '$T_{FWHM_q}$ = ' + str(np.round(r2-r1,2)) + ' ps', fontsize=12, horizontalalignment='center')
+T_FWHM_q = (r2-r1) * 1e-12
+T_e_q = T_FWHM_q / 2.35482
+
+plt.ylabel('$|E|$ a.u.'); plt.xlabel('Time $t$ [ps]'); legend = plt.legend(loc='upper right')
+
+# Print the results
+print 'Power: Gauss : T_FWHM_0 = ' , T_FWHM_0*1e12, ' ps'
+print 'Power: Gauss : T_e_0 = ' , T_e_0*1e12, ' ps'
+print 'Power: sqrt.Gauss : T_FWHM_1,0 = ' , T_FWHM_1*1e12, ' ps'
+print 'Power: sqrt.Gauss : T_e_0,1 = ' , T_e_1*1e12, ' ps'
+print 'Power: Gauss**2 : T_FWHM_0 = ' , T_FWHM_q*1e12, ' ps'
+print 'Power: Gauss**2 : T_e_0 = ' , T_e_q*1e12, ' ps'
+

pypho_bits.py

+#!/usr/bin/env python
+# -*- coding: utf-8 -*-
+#
+#  pypho.py
+#  
+#  Copyright 2014 Arne Striegler (arne.striegler@hm.edu)
+#  
+#   
+#  
+
+# Create Bitpattern
+#
+########################################################################
+import numpy as np
+import sys
+import random
+from pypho_functions import *
+
+########################################################################
+
+class pypho_bits(object):
+    def __init__(self, glova = None, nob = None, pattern = None):
+        
+        if glova == None:            
+            print ("ERROR: You must define the global variables")
+            sys.exit("PyPho stopped!")
+            
+        self.glova       = glova
+        self.nob         = None
+        self.pattern     = None
+        
+        self.set(nob,pattern)
+        
+########################################################################        
+    def __call__(self, nob = None, pattern = None):        
+    
+        self.set(nob, pattern)
+    
+        return self.out(self.nob, self.pattern)
+
+########################################################################        
+    def out(self, nob = None, pattern = None):        
+    
+        self.set(nob, pattern)
+        
+        if self.pattern == "singlepulse":
+            self.bits = np.zeros(self.nob, dtype=np.int)
+            self.bits[self.glova.nos/2] = 1    
+            
+        elif self.pattern == "ones":
+            self.bits = np.ones(self.nob, dtype=np.int)
+                        
+        elif self.pattern == "random":    
+            self.bits         = self.rndm()                    
+        else:    
+            print ("ERROR: No valid pattern specified!")
+            sys.exit("PyPho stopped!")
+            
+    
+        return self.bits
+
+### Create Random Bit Sequence #########################################
+
+    def rndm(self):
+        
+        self.value_rndn = np.ones(self.nob)
+        self.value_rndn[self.nob/2:] = 0
+        random.shuffle(self.value_rndn)
+        self.value_rndn[0]     = 1
+        self.value_rndn[-1] = 0
+        self.bits = np.array(self.value_rndn)
+
+        return self.value_rndn
+
+
+### Get and set parameters #############################################
+
+# nos: Number of Bits
+    @property
+    def nos(self):
+        """Get number of bits"""
+        return self.bits.size
+    
+
+
+########################################################################