Copyright (C) 2011 and later, Paul D. Nation & Robert J. Johansson
In [1]:
%matplotlib inline
import matplotlib.pyplot as plt
In [2]:
import numpy as np
import qutip.settings
from qutip import *
In [3]:
from qutip.ipynbtools import HTMLProgressBar
In [4]:
from matplotlib import rcParams
rcParams['font.family'] = 'STIXGeneral'
rcParams['mathtext.fontset'] = 'stix'
rcParams['font.size'] = '14'
In [5]:
N = 15
w0 = 1.0 * 2 * np.pi
g = 0.2 * 2 * np.pi
times = np.linspace(0, 15, 150)
dt = times[1] - times[0]
gamma = 0.01
kappa = 0.1
ntraj = 150
In [6]:
a = tensor(destroy(N), identity(2))
sm = tensor(identity(N), destroy(2))
In [7]:
H = w0 * a.dag() * a + w0 * sm.dag() * sm + g * (sm * a.dag() + sm.dag() * a)
In [8]:
rho0 = tensor(fock(N, 5), fock(2, 0))
In [9]:
e_ops = [a.dag() * a, a + a.dag(), sm.dag() * sm]
In [10]:
c_ops = [np.sqrt(gamma) * sm] # collapse operator for qubit
sc_ops = [np.sqrt(kappa) * a] # stochastic collapse for resonator
In [11]:
result_ref = mesolve(H, rho0, times, c_ops+sc_ops, e_ops)
In [12]:
result1 = photocurrent_mesolve(H, rho0, times, c_ops=c_ops, sc_ops=sc_ops, e_ops=e_ops,
ntraj=1, nsubsteps=100,
store_measurement=True,
options=Options(store_states=True))
Run the smesolve solver in parallel by passing the keyword argument map_func=parallel_map:
In [13]:
result2 = photocurrent_mesolve(H, rho0, times, c_ops=c_ops, sc_ops=sc_ops, e_ops=e_ops,
ntraj=ntraj, nsubsteps=100,
store_measurement=True,
options=Options(store_states=True),
progress_bar=HTMLProgressBar(),
map_func=parallel_map)
In [14]:
fig, axes = plt.subplots(2, 3, figsize=(16, 8), sharex=True)
axes[0,0].plot(times, result1.expect[0], label=r'Stochastic ME (ntraj = 1)', lw=2)
axes[0,0].plot(times, result_ref.expect[0], label=r'Lindblad ME', lw=2)
axes[0,0].set_title("Cavity photon number (ntraj = 1)")
axes[0,0].legend()
axes[1,0].plot(times, result2.expect[0], label=r'Stochatic ME (ntraj = %d)' % ntraj, lw=2)
axes[1,0].plot(times, result_ref.expect[0], label=r'Lindblad ME', lw=2)
axes[1,0].set_title("Cavity photon number (ntraj = 10)")
axes[1,0].legend()
axes[0,1].plot(times, result1.expect[2], label=r'Stochastic ME (ntraj = 1)', lw=2)
axes[0,1].plot(times, result_ref.expect[2], label=r'Lindblad ME', lw=2)
axes[0,1].set_title("Qubit excition probability (ntraj = 1)")
axes[0,1].legend()
axes[1,1].plot(times, result2.expect[2], label=r'Stochatic ME (ntraj = %d)' % ntraj, lw=2)
axes[1,1].plot(times, result_ref.expect[2], label=r'Lindblad ME', lw=2)
axes[1,1].set_title("Qubit excition probability (ntraj = %d)" % ntraj)
axes[1,1].legend()
axes[0,2].step(times, dt * np.cumsum(result1.measurement[0].real), lw=2)
axes[0,2].set_title("Cummulative photon detections (ntraj = 1)")
axes[1,2].step(times, dt * np.cumsum(np.array(result2.measurement).sum(axis=0).real) / ntraj, lw=2)
axes[1,2].set_title("Cummulative avg. photon detections (ntraj = %d)" % ntraj)
fig.tight_layout()
In [15]:
from qutip.ipynbtools import version_table
version_table()
Out[15]: