Two-Level: Weak Pulse
Define and Solve
[1]:
mb_solve_json = """
{
"atom": {
"fields": [
{
"coupled_levels": [[0, 1]],
"detuning": 0.0,
"rabi_freq": 1.0e-3,
"rabi_freq_t_args": {
"ampl": 1.0,
"centre": 0.0,
"fwhm": 1.0
},
"rabi_freq_t_func": "gaussian"
}
],
"num_states": 2
},
"t_min": -2.0,
"t_max": 10.0,
"t_steps": 100,
"z_min": -0.2,
"z_max": 1.2,
"z_steps": 20,
"z_steps_inner": 2,
"interaction_strengths": [
1.0
]
}
"""
[2]:
from maxwellbloch import mb_solve
mb_solve_00 = mb_solve.MBSolve().from_json_str(mb_solve_json)
[3]:
Omegas_zt, states_zt = mb_solve_00.mbsolve()
z-step 2/20 (10%)
z-step 4/20 (20%)
z-step 6/20 (30%)
z-step 8/20 (40%)
z-step 10/20 (50%)
z-step 12/20 (60%)
z-step 14/20 (70%)
z-step 16/20 (80%)
z-step 18/20 (90%)
/home/docs/checkouts/readthedocs.org/user_builds/maxwellbloch/envs/v0.10.0/lib/python3.11/site-packages/qutip/solver/solver_base.py:598: FutureWarning: e_ops will be keyword only from qutip 5.3 for all solver
warnings.warn(
Field Output
[4]:
import matplotlib.pyplot as plt
%matplotlib inline
import numpy as np
import seaborn as sns
sns.set_style("darkgrid")
fig = plt.figure(1, figsize=(16, 6))
ax = fig.add_subplot(111)
cmap_range = np.linspace(0.0, 1.0e-3, 11)
cf = ax.contourf(
mb_solve_00.tlist,
mb_solve_00.zlist,
np.abs(mb_solve_00.Omegas_zt[0] / (2 * np.pi)),
cmap_range,
cmap=plt.cm.Blues,
)
ax.set_title(r"Rabi Frequency ($\Gamma / 2\pi $)")
ax.set_xlabel(r"Time ($1/\Gamma$)")
ax.set_ylabel("Distance ($L$)")
for y in [0.0, 1.0]:
ax.axhline(y, c="grey", lw=1.0, ls="dotted")
plt.colorbar(cf);