def test_compare_solvers_coherent_state_memc():
"""
correlation: comparing me and mc for driven oscillator in fock state
"""
N = 2
a = destroy(N)
H = a.dag() * a + a + a.dag()
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
psi0 = fock(N, 1)
taulist = np.linspace(0, 1.0, 3)
corr1 = correlation_2op_2t(H,
psi0, [0, 0.5],
taulist,
c_ops,
a.dag(),
a,
solver="me")
corr2 = correlation_2op_2t(H,
psi0, [0, 0.5],
taulist,
c_ops,
a.dag(),
a,
solver="mc")
# pretty lax criterion, but would otherwise require a quite long simulation
# time
assert_(abs(corr1 - corr2).max() < 0.25)
def test_compare_solvers_coherent_state_mees():
"""
correlation: comparing me and es for oscillator in coherent initial state
"""
N = 20
a = destroy(N)
H = a.dag() * a
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
rho0 = coherent_dm(N, np.sqrt(4.0))
taulist = np.linspace(0, 5.0, 100)
corr1 = correlation_2op_2t(H,
rho0,
None,
taulist,
c_ops,
a.dag(),
a,
solver="me")
corr2 = correlation_2op_2t(H,
rho0,
None,
taulist,
c_ops,
a.dag(),
a,
solver="es")
assert_(max(abs(corr1 - corr2)) < 1e-4)
def test_fn_list_td_corr2():
"""
correlation: multi time-dependent factor
"""
# test for bug of issue #1048
sm = destroy(2)
args = {}
def step_func(t, args={}):
return np.arctan(t - 2) / np.pi + 0.5
def inv_step_func(t, args={}):
return np.arctan(-(t - 2)) / np.pi + 0.5
H1 = [[(sm + sm.dag()), step_func], [qeye(2), inv_step_func]]
H2 = [[qeye(2), inv_step_func], [(sm + sm.dag()), step_func]]
tlist = np.linspace(0, 5, 6)
corr1 = correlation_2op_2t(H1,
fock(2, 0),
tlist,
tlist, [sm],
sm.dag(),
sm,
args=args)
corr2 = correlation_2op_2t(H2,
fock(2, 0),
tlist,
tlist, [sm],
sm.dag(),
sm,
args=args)
assert_(np.sum(np.abs(corr1 - corr2)) < 1e-5)
def test_compare_solvers_coherent_state_memc():
"""
correlation: comparing me and mc for driven oscillator in ground state
"""
N = 20
a = destroy(N)
H = a.dag() * a + a + a.dag()
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
psi0 = fock(N, 0)
taulist = np.linspace(0, 1.0, 5)
corr1 = correlation_2op_2t(H,
psi0, [0],
taulist,
c_ops,
a.dag(),
a,
solver="me")[0]
corr2 = correlation_2op_2t(H,
psi0, [0],
taulist,
c_ops,
a.dag(),
a,
solver="mc")[0]
assert_(max(abs(corr1 - corr2)) < 5e-2)
def test_c_ops_fn_list_td_corr():
"""
correlation: comparing 3LS emission corr., c_ops td (fn-list td format)
"""
# calculate zero-delay HOM cross-correlation, for incoherently pumped
# 3LS ladder system g2ab[0]
# with following parameters:
# gamma = 1, 99% initialized, tp = 0.5
# Then: g2ab(0)~0.185
tlist = np.linspace(0, 6, 20)
ket0 = fock(3, 0)
ket1 = fock(3, 1)
ket2 = fock(3, 2)
sm01 = ket0 * ket1.dag()
sm12 = ket1 * ket2.dag()
psi0 = fock(3, 2)
tp = 1
# define "pi" pulse as when 99% of population has been transferred
Om = np.sqrt(-np.log(1e-2) / (tp * np.sqrt(np.pi)))
c_ops = [
sm01,
[
sm12 * Om, lambda t, args: np.exp(-(t - args["t_off"])**2 /
(2 * args["tp"]**2))
]
]
args = {"tp": tp, "t_off": 2}
H = qeye(3) * 0
# HOM cross-correlation depends on coherences (g2[0]=0)
c1 = correlation_2op_2t(H,
psi0,
tlist,
tlist,
c_ops,
sm01.dag(),
sm01,
args=args)
c2 = correlation_2op_2t(H,
psi0,
tlist,
tlist,
c_ops,
sm01.dag(),
sm01,
args=args,
reverse=True)
n = mesolve(H, psi0, tlist, c_ops, [sm01.dag() * sm01],
args=args).expect[0]
n_f = Cubic_Spline(tlist[0], tlist[-1], n)
corr_ab = -c1 * c2 + np.array([[n_f(t) * n_f(t + tau) for tau in tlist]
for t in tlist])
dt = tlist[1] - tlist[0]
gab = abs(np.trapz(np.trapz(corr_ab, axis=0))) * dt**2
assert_(abs(gab - 0.185) < 1e-2)
def test_hamiltonian_order_unimportant():
# Testing for regression on issue 1048.
sp = qutip.sigmap()
H = [[qutip.sigmax(), lambda t, _: _step(t-2)],
[qutip.qeye(2), lambda t, _: _step(-(t-2))]]
start = qutip.basis(2, 0)
times = np.linspace(0, 5, 6)
forwards = qutip.correlation_2op_2t(H, start, times, times, [sp],
sp.dag(), sp)
backwards = qutip.correlation_2op_2t(H[::-1], start, times, times, [sp],
sp.dag(), sp)
np.testing.assert_allclose(forwards, backwards, atol=1e-6)
def test_c_ops_fn_list_td_corr():
"""
correlation: comparing 3LS emission corr., c_ops td (fn-list td format)
"""
# calculate zero-delay HOM cross-correlation, for incoherently pumped
# 3LS ladder system g2ab[0]
# with following parameters:
# gamma = 1, 99% initialized, tp = 0.5
# Then: g2ab(0)~0.185
tlist = np.linspace(0, 6, 20)
ket0 = fock(3, 0)
ket1 = fock(3, 1)
ket2 = fock(3, 2)
sm01 = ket0 * ket1.dag()
sm12 = ket1 * ket2.dag()
psi0 = fock(3, 2)
tp = 1
# define "pi" pulse as when 99% of population has been transferred
Om = np.sqrt(-np.log(1e-2) / (tp * np.sqrt(np.pi)))
c_ops = [sm01,
[sm12 * Om,
lambda t, args:
np.exp(-(t - args["t_off"]) ** 2 / (2 * args["tp"] ** 2))]]
args = {"tp": tp, "t_off": 2}
H = qeye(3) * 0
# HOM cross-correlation depends on coherences (g2[0]=0)
c1 = correlation_2op_2t(H, psi0, tlist, tlist, c_ops,
sm01.dag(), sm01, args=args)
c2 = correlation_2op_2t(H, psi0, tlist, tlist, c_ops,
sm01.dag(), sm01, args=args, reverse=True)
n = mesolve(
H, psi0, tlist, c_ops, [sm01.dag() * sm01], args=args
).expect[0]
n_f = Cubic_Spline(tlist[0], tlist[-1], n)
corr_ab = - c1 * c2 + np.array(
[[n_f(t) * n_f(t + tau) for tau in tlist]
for t in tlist])
dt = tlist[1] - tlist[0]
gab = abs(np.trapz(np.trapz(corr_ab, axis=0))) * dt ** 2
assert_(abs(gab - 0.185) < 1e-2)
def test_compare_solvers_coherent_state_memc():
"""
correlation: comparing me and mc for driven oscillator in ground state
"""
N = 20
a = destroy(N)
H = a.dag() * a + a + a.dag()
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
psi0 = fock(N, 0)
taulist = np.linspace(0, 1.0, 5)
corr1 = correlation_2op_2t(H, psi0, [0], taulist, c_ops, a.dag(), a,
solver="me")[0]
corr2 = correlation_2op_2t(H, psi0, [0], taulist, c_ops, a.dag(), a,
solver="mc")[0]
assert_(max(abs(corr1 - corr2)) < 5e-2)
def test_compare_solvers_coherent_state_mees():
"""
correlation: comparing me and es for oscillator in coherent initial state
"""
N = 20
a = destroy(N)
H = a.dag() * a
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
rho0 = coherent_dm(N, np.sqrt(4.0))
taulist = np.linspace(0, 5.0, 100)
corr1 = correlation_2op_2t(H, rho0, None, taulist, c_ops, a.dag(), a,
solver="me")
corr2 = correlation_2op_2t(H, rho0, None, taulist, c_ops, a.dag(), a,
solver="es")
assert_(max(abs(corr1 - corr2)) < 1e-4)
def test_np_str_list_td_corr():
"""
correlation: comparing 3LS emission corr., c_ops td (np-list td format)
"""
# calculate zero-delay HOM cross-correlation, for incoherently pumped
# 3LS ladder system g2ab[0]
# with following parameters:
# gamma = 1, 99% initialized, tp = 0.5
# Then: g2ab(0)~0.185
tlist = np.linspace(0, 6, 20)
ket0 = fock(3, 0)
ket1 = fock(3, 1)
ket2 = fock(3, 2)
sm01 = ket0 * ket1.dag()
sm12 = ket1 * ket2.dag()
psi0 = fock(3, 2)
tp = 1
t_off = 2
# define "pi" pulse as when 99% of population has been transferred
Om = np.sqrt(-np.log(1e-2) / (tp * np.sqrt(np.pi)))
c_ops = [sm01,
[sm12 * Om, np.exp(-(tlist - t_off) ** 2 / (2 * tp ** 2))]]
H = qeye(3) * 0
# HOM cross-correlation depends on coherences (g2[0]=0)
c1 = correlation_2op_2t(H, psi0, tlist, tlist, c_ops,
sm01.dag(), sm01)
c2 = correlation_2op_2t(H, psi0, tlist, tlist, c_ops,
sm01.dag(), sm01, reverse=True)
n = mesolve(
H, psi0, tlist, c_ops, sm01.dag() * sm01
).expect[0]
n_f = interp1d(tlist, n, kind="cubic", fill_value=0, bounds_error=False)
corr_ab = - c1 * c2 + np.array(
[[n_f(t) * n_f(t + tau) for tau in tlist]
for t in tlist])
dt = tlist[1] - tlist[0]
gab = abs(np.trapz(np.trapz(corr_ab, axis=0))) * dt ** 2
assert_(abs(gab - 0.185) < 1e-2)
def test_coefficient_c_ops_3ls(self, dependence_3ls):
# Calculate zero-delay HOM cross-correlation for incoherently pumped
# three-level system, g2_ab[0] with gamma = 1.
dimension = 3
H = qutip.qzero(dimension)
start = qutip.basis(dimension, 2)
times = _3ls_times
project_0_1 = qutip.projection(dimension, 0, 1)
project_1_2 = qutip.projection(dimension, 1, 2)
population_1 = qutip.projection(dimension, 1, 1)
# Define the pi pulse to be when 99% of the population is transferred.
rabi = np.sqrt(-np.log(0.01) / (_3ls_args['tp'] * np.sqrt(np.pi)))
c_ops = [project_0_1, [rabi * project_1_2, dependence_3ls]]
forwards = qutip.correlation_2op_2t(H,
start,
times,
times,
c_ops,
project_0_1.dag(),
project_0_1,
args=_3ls_args)
backwards = qutip.correlation_2op_2t(H,
start,
times,
times,
c_ops,
project_0_1.dag(),
project_0_1,
args=_3ls_args,
reverse=True)
n_expect = qutip.mesolve(H,
start,
times,
c_ops,
args=_3ls_args,
e_ops=[population_1]).expect[0]
correlation_ab = -forwards * backwards + _n_correlation(
times, n_expect)
g2_ab_0 = _trapz_2d(np.real(correlation_ab), times)
assert abs(g2_ab_0 - 0.185) < 1e-2
def test_compare_solvers_coherent_state_memc():
"""
correlation: comparing me and mc for driven oscillator in fock state
"""
N = 2
a = destroy(N)
H = a.dag() * a + a + a.dag()
G1 = 0.75
n_th = 2.00
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
psi0 = fock(N, 1)
taulist = np.linspace(0, 1.0, 3)
corr1 = correlation_2op_2t(H, psi0, [0, 0.5], taulist, c_ops, a.dag(), a,
solver="me")
corr2 = correlation_2op_2t(H, psi0, [0, 0.5], taulist, c_ops, a.dag(), a,
solver="mc")
# pretty lax criterion, but would otherwise require a quite long simulation
# time
assert_(abs(corr1 - corr2).max() < 0.2)
N = 15
taus = np.linspace(0, 10.0, 200)
a = qutip.destroy(N)
H = 2 * np.pi * a.dag() * a
# collapse operator
G1 = 0.75
n_th = 2.00 # bath temperature in terms of excitation number
c_ops = [np.sqrt(G1 * (1 + n_th)) * a, np.sqrt(G1 * n_th) * a.dag()]
# start with a coherent state
rho0 = qutip.coherent_dm(N, 2.0)
# first calculate the occupation number as a function of time
n = qutip.mesolve(H, rho0, taus, c_ops, [a.dag() * a]).expect[0]
# calculate the correlation function G1 and normalize with n to obtain g1
G1 = qutip.correlation_2op_2t(H, rho0, None, taus, c_ops, a.dag(), a)
g1 = G1 / np.sqrt(n[0] * n)
plt.plot(taus, np.real(g1), 'b', lw=2)
plt.plot(taus, n, 'r', lw=2)
plt.title('Decay of a coherent state to an incoherent (thermal) state')
plt.xlabel(r'$\tau$')
plt.legend([
r'First-order coherence function $g^{(1)}(\tau)$',
r'Occupation number $n(\tau)$',
])
plt.show()
import numpy as np
import matplotlib.pyplot as plt
import qutip
times = np.linspace(0, 10.0, 200)
a = qutip.destroy(10)
x = a.dag() + a
H = a.dag() * a
alpha = 2.5
rho0 = qutip.coherent_dm(10, alpha)
corr = qutip.correlation_2op_2t(H, rho0, times, times, [np.sqrt(0.25) * a], x,
x)
plt.pcolor(np.real(corr))
plt.xlabel(r'Time $t_2$')
plt.ylabel(r'Time $t_1$')
plt.title(r'Correlation $\left<x(t)x(0)\right>$')
plt.show()