Jan-15-2020, 11:51 PM
Hi All,
I am new to the python and trying to do some curve fitting for my lab data. I have found an Elliott Fit code from Dr. Valerio D'Innocenzo's doctoral thesis and changed a bit to work for my data but it is not working. It was giving me errors like :
" RuntimeWarning: overflow encountered in cosh
return (1 / (abs(np.cosh((e-x))/ gamma)) * 2 * np.pi * np.sqrt(Eb) / (1 - np.exp(-2 * np.pi / (np.sqrt(D)))) * 1 / (1 - npc * (x - Eg))) "
My experimental data is in 2nd column and energy values in 1st column.
Can anyone help me fix it?
Thanks,
Shashi
I am new to the python and trying to do some curve fitting for my lab data. I have found an Elliott Fit code from Dr. Valerio D'Innocenzo's doctoral thesis and changed a bit to work for my data but it is not working. It was giving me errors like :
" RuntimeWarning: overflow encountered in cosh
return (1 / (abs(np.cosh((e-x))/ gamma)) * 2 * np.pi * np.sqrt(Eb) / (1 - np.exp(-2 * np.pi / (np.sqrt(D)))) * 1 / (1 - npc * (x - Eg))) "
My experimental data is in 2nd column and energy values in 1st column.
Can anyone help me fix it?
Thanks,
Shashi
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.ticker as ticker
# ODEpack tool for differential equation integration
from numpy.distutils.fcompiler import none
from scipy.integrate import odeint, quad
# Optimization tool
import scipy.optimize as opt
#Interpolation tool
from scipy.interpolate import interp1d
def Elliots_fit (p, a_exp , e):
Eb, Eg, gamma, npc, k = p
#Descrete transitions to the excitonic states
absex = np.zeros((e.size))
n = np.linspace(1, 500, 500)
for i in range(0, e.size):
expr = 4*np.pi*(Eb**(3/2)) / (n**3)*(1/(np.cosh((e[i] - Eg + Eb/n**2) / gamma)))
S = expr.cumsum(axis=0)
absex[i] = S[-1]
#Band to band absorption with Sommerfeld correction
abseh = np.zeros((e.size))
def fun_eh(x, e, gamma, Eb, Eg, npc):
D = (x-Eg)/Eb
return (1 / (abs(np.cosh((e-x))/ gamma)) * 2 * np.pi * np.sqrt(Eb) / (1 - np.exp(-2 * np.pi / (np.sqrt(D)))) * 1 / (1 - npc * (x - Eg)))
for i in range(0, e.size):
q = quad(fun_eh, Eg, np.inf, args=(e[i], gamma, Eb, Eg, npc))
abseh[i] = q[0]
#Complete Abs simulation (background added)
abs_sim = np.zeros((e.size))
for i in range(0, e.size):
abs_sim[i] = (e[i] / Eb**(3/2))*(absex[i] + abseh[i])
return (abs_sim*k-abs_exp_fit)
#Data loading
data = np.loadtxt('transmission_data.txt')
# plt.plot(e, data[:,2])
e_exp = data [:,0] # concerted from nm to eV
a_exp = data[:,1] # My data
#Intial Values
Eb = 0.030 # exciton binding energy (eV)
gamma = 0.029 # inhomogeneous line broadening (eV)
Eg = 2.402 # semiconductor bandgap (eV)
npc = -0.31 # non−parabolic coefficient
k = 0.0035
#Energy axis generation
# ix0 = np.searchsorted(e_exp ,1.58862)
# ix1 = np.searchsorted(e_exp ,1.42976)
# e = np.linspace(e_exp[ix1], e_exp[ix0-1], 500) # energy axes (eV)
e = np.linspace(e_exp[len(e_exp)-1], e_exp[0], 3440) # energy axes (eV)
p0 = np.array([Eb, Eg, gamma, npc, k],dtype=np.float64 )#b = np.array([[1,2,3,4,5],[6,7,8,9,10]],dtype=np.float64)
#Fit Calling
#Interpolating the simulated abs over the exp x−axis
f = interp1d(e_exp ,a_exp)
abs_exp_fit = f(e)
opt_out = opt.leastsq(Elliots_fit ,p0, args =( abs_exp_fit , e), full_output=1)
fitted_param = opt_out[0]
#Standard error evaluation
fitting = Elliots_fit(fitted_param, abs_exp_fit, e)
plt.plot(e, abs_exp_fit)
plt.plot(e, fitting)
if (len( abs_exp_fit ) > len(p0)) and opt_out [1] is not None:
s_sq = (( fitting-abs_exp_fit )**2).sum()((len( abs_exp_fit )-len(p0)))
pcov = opt_out[1] * s_sq
else:
pcov = np.inf
error = []
for i in range(len(opt_out [0])):
try:
error.append( np.absolute(pcov[i][i])**0.5)
except:
error.append( 0.00 )
pfit_leastsq = opt_out [0]
perr_leastsq = np.array(error)
