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import numpy as np
from qutip import *
import matplotlib.pyplot as plt
%matplotlib inline
from IPython.display import Image
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one, two, three = three_level_basis()
sig11 = one * one.dag()
sig22 = two * two.dag()
sig33 = three * three.dag()
sig13 = one * three.dag()
sig23 = two * three.dag()
sig12 = one * two.dag()
Image("fig/EIT_levels.png")
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# Loop over the detuning Delta and generate rho and chi
# constants based on Jenkins EIT masters thesis
# It seems like the values they quote aren't right. They don't match the code.
γ = 1 # decay rate on probe transition
Γ = 1 # decay rate on control transition
γc = 0.05 # coherence decay rate (i.e. long-lived state |2>)
ΔC = 0 # control field detuning
ΩP = 0.01 # Rabi freq. for probe
ΩC = 1.0 # Rabi freq. for control
# collapse operators
c1 = np.sqrt(γ)*sig13 # 1-3 coherence decay (probe transition)
c2 = np.sqrt(Γ)*sig23 # 2-3 coherence decay (control transition)
c3 = np.sqrt(γc)*sig12 # ground state coherence decay
collapse = [c1,c2,c3]
deltalist = np.linspace(-3,3,301)
#deltalist = [1e-15]
rho_33 = []
chi = []
#probelist = np.arange(0.0,10.0,0.5)
#for ΩP in probelist:
# ΔP = 0
# H = -1/2*Qobj([[0,0,ΩP],[0,2*(ΔP - ΔC),ΩC],[ΩP, ΩC, 2*ΔP]])
# rho_ss = steadystate(H,collapse)
# rho_33.append(rho_ss[2,2]) # jenkins approach
for ΔP in deltalist:
H = -1/2*Qobj([[0,0,ΩP],[0,2*(ΔP - ΔC),ΩC],[ΩP, ΩC, 2*ΔP]])
rho_ss = steadystate(H,collapse)
# prob.append(expect(sig33.dag(),rho_ss)) # this also works
rho_33.append(rho_ss[2,2]) # jenkins approach
chi.append(expect(sig13,rho_ss))
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#plt.plot(probelist,np.real(rho_33))
#plt.title("Excited state population")
#plt.xlabel("$\Omega_p$")
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H
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plt.plot(deltalist,np.real(rho_33))
plt.title("Excited state population")
plt.xlabel("$\Delta$")
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plt.plot(deltalist,np.real(chi),label="Index n")
plt.plot(deltalist,np.imag(chi),label="Abs.")
plt.legend()
plt.title("$\chi$")
plt.xlabel("$\Delta$")
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This agrees with the standard results, and the interpretation of slow light within the EIT window.
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