def func(f1, b, set):
"""
This function Perform the gate application on the initial state of qubit and then the state tomography,
at the same time compute the analytical bloch state.
INCOME:
f1="string", b="string"
fig_data="svg",fig_data2="svg"
"""
#### Create the bloch-sphere on qutip
b1 = Bloch()
b2 = Bloch()
## create the analyical quantum state and perform tranformation
## Add states to the bloch sphere and plot it
b1.add_states(analytic(f1, b))
if not set:
states = qtomography(f1, b)
b2.add_vectors(states)
else:
### implements for
states = qtomography_s(f1, b)
for i in states:
b2.add_points(i)
b2.add_vectors(np.average(states, axis=0))
###
b2.render()
fig_data = print_figure(b2.fig, 'svg')
b1.render()
fig_data2 = print_figure(b1.fig, 'svg')
#b1.show()
#b2.show()
b1.clear()
b2.clear()
return fig_data, fig_data2
def bloch_plot(self, points=None, F=None):
"""
Plot the current state on the Bloch sphere using
qutip.
"""
# create instance of 3d plot
bloch = Bloch(figsize=[9, 9])
bloch.add_vectors([0, 0, 1])
bloch.xlabel = ['$<F_x>$', '']
bloch.ylabel = ['$<F_y>$', '']
bloch.zlabel = ['$<F_z>$', '']
if self.spin == 'half':
if points is None:
# convert current state into density operator
rho = np.outer(self.state.H, self.state)
# get Bloch vector representation
points = self.get_bloch_vec(rho)
# Can only plot systems of dimension 2 at this time
assert len(
points
) == 3, "System dimension must be spin 1/2 for Bloch sphere plot"
# create instance of 3d plot
bloch = Bloch(figsize=[9, 9])
elif self.spin == 'one':
#points is list of items in format [[x1,x2],[y1,y2],[z1,z2]]
if points is None:
points = [getStars(self.state)]
bloch.point_color = ['g', 'r',
'b'] #ensures point and line are same colour
bloch.point_marker = ['o', 'd', 'o']
#bloch.point_color = ['g','r'] #ensures point and line are same colour
#bloch.point_marker = ['o','d']
for p in points:
bloch.add_points([p[0][0], p[1][0], p[2][0]])
bloch.add_points([p[0][1], p[1][1], p[2][1]])
bloch.add_points(p, meth='l')
'''
bloch.point_color = ['b','b'] #ensures point and line are same colour
bloch.point_marker = ['o','o']
for p in points:
bloch.add_points(p)
bloch.add_points(p, meth='l')
'''
# add state
#bloch.render(bloch.fig, bloch.axes)
#bloch.fig.savefig("bloch.png",dpi=600, transparent=True)
bloch.show()
def bloch_field(self, time):
"""
Plot magnetic field vector normalised to the bloch sphere
"""
# seperate coordinates into axis set
xb = self.fields[0](time)
yb = self.fields[1](time)
zb = self.fields[2](time)
# add to list and normalise
points = [list(xb), list(yb), list(zb)]
sqsum = 0.0
for i, point in enumerate(points[0]):
# compute magnitude and store largest value
sqsum_test = np.sqrt(points[0][i]**2 + points[1][i]**2 +
points[2][i]**2)
if sqsum_test > sqsum:
sqsum = sqsum_test
points = points / sqsum
# create Bloch sphere instance
bloch = Bloch()
# add points and show
bloch.add_points(points)
bloch.show()
def draw_sphere_zenith(zenith_points, hv_points, root):
b = Bloch()
b.point_color = ['m', 'k', 'g', 'b', 'w', 'c', 'y', 'r']
b.zlabel = ['$z$', '']
b.point_marker = ['o']
b.point_size = [30]
b.frame_width = 1.2
fig = plt.figure(figsize=(20, 20))
b.fig = fig
x = (basis(2, 0) + (1 + 0j) * basis(2, 1)).unit()
y = (basis(2, 0) + (0 + 1j) * basis(2, 1)).unit()
z = (basis(2, 0) + (0 + 0j) * basis(2, 1)).unit()
b.add_states([x, y, z])
for i in range(len(zenith_points)):
# Transform xyz to zxy coordinates
tmp1 = np.array(
[zenith_points[i][2], zenith_points[i][0], zenith_points[i][1]])
tmp2 = np.vstack(
[hv_points[i][:, 2], hv_points[i][:, 0], hv_points[i][:, 1]]).T
tmp = np.vstack([tmp1, -tmp1, tmp2]).T
b.add_points(tmp)
# tmp1 = np.array([zenith_points[-1][2], zenith_points[-1][0], zenith_points[-1][1]])
# tmp = np.array([tmp1, -tmp1]).T
# b.add_points(tmp)
name = os.path.join(root, 'zenith_on_sphere.jpg')
b.save(name=name)
def draw_consensus_rectified_sphere(hv_points, root):
b = Bloch()
b.point_color = ['m', 'k', 'g', 'b', 'w', 'c', 'y', 'r']
b.zlabel = ['$z$', '']
b.point_marker = ['o']
b.point_size = [80]
b.frame_width = 1.2
fig = plt.figure(figsize=(20, 20))
b.fig = fig
x = (basis(2, 0) + (1 + 0j) * basis(2, 1)).unit()
y = (basis(2, 0) + (0 + 1j) * basis(2, 1)).unit()
z = (basis(2, 0) + (0 + 0j) * basis(2, 1)).unit()
b.add_states([x, y, z])
for i in range(len(hv_points)):
# Transform xyz to zxy coordinates
tmp2 = np.vstack(
[hv_points[i][:, 2], hv_points[i][:, 0], hv_points[i][:, 1]]).T
tmp = tmp2.T
b.add_points(tmp)
# b.add_points([ 0.99619469809174555, 0.087155742747658166, 0])
# b.add_points([0.99619469809174555, -0.087155742747658166, 0])
# b.add_points(tmp)
name = os.path.join(root, 'consensus_zenith_on_rectified_sphere.jpg')
b.save(name=name)
def bloch_plot(self, filename, points=None, save=False):
"""
Plot the current state on the Bloch sphere using
qutip.
"""
if points is None:
# convert current state into density operator
rho = np.outer(self.state.H, self.state)
# get Bloch vector representation
points = self.get_bloch_vec(rho)
# Can only plot systems of dimension 2 at this time
assert len(
points
) == 3, "System dimension must be spin 1/2 for Bloch sphere plot"
# create instance of 3d plot
bloch = Bloch(fig=1, figsize=[9, 9], view=[190, 10])
# add state
bloch.add_points(points)
bloch.render()
if save is True:
print('Bloch plot saved to Sim Results folder')
path = 'C:/Users/Boundsy/Desktop/Uni Work/PHS2360/Sim Results/' + str(
filename) + '.png'
bloch.fig.savefig(path, dpi=800, transparent=True)
def PlotStateAnalyzer(InputState, hwpAngle, qwpAngle):
QWPstate = QWP(qwpAngle) @ InputState
OutputState = HWP(hwpAngle) @ QWP(qwpAngle) @ InputState
pntsX = [
StateToBloch(QWP(th) @ InputState)[0] for th in arange(0, pi, pi / 64)
]
pntsY = [
StateToBloch(QWP(th) @ InputState)[1] for th in arange(0, pi, pi / 64)
]
pntsZ = [
StateToBloch(QWP(th) @ InputState)[2] for th in arange(0, pi, pi / 64)
]
pnts = [pntsX, pntsY, pntsZ]
pntsX2 = [
StateToBloch(HWP(th) @ QWP(qwpAngle) @ InputState)[0]
for th in arange(0, pi, pi / 64)
]
pntsY2 = [
StateToBloch(HWP(th) @ QWP(qwpAngle) @ InputState)[1]
for th in arange(0, pi, pi / 64)
]
pntsZ2 = [
StateToBloch(HWP(th) @ QWP(qwpAngle) @ InputState)[2]
for th in arange(0, pi, pi / 64)
]
pnts2 = [pntsX2, pntsY2, pntsZ2]
bsph = Bloch()
bsph.add_points(pnts)
bsph.add_points(pnts2)
bsph.add_vectors(StateToBloch(OutputState))
bsph.add_vectors(StateToBloch(InputState))
bsph.add_vectors(StateToBloch(QWPstate))
return bsph.show()
def bloch_animate(self, pnts, name="Bloch_animate"):
"""
Animates the path of a state through the set of pure states - requires ffmpeg
"""
from pylab import figure
import matplotlib.animation as animation
from mpl_toolkits.mplot3d import Axes3D
# set up plot environment
fig = figure()
ax = Axes3D(fig, azim=-40, elev=30)
sphere = Bloch(axes=ax)
# define animation function (from qutip docs)
def animate(i):
sphere.clear()
sphere.add_points(
[pnts[0][:i + 1], pnts[1][:i + 1], pnts[2][:i + 1]])
sphere.make_sphere()
return ax
def init():
sphere.vector_color = ['r']
return ax
ani = animation.FuncAnimation(fig,
animate,
np.arange(len(pnts[0])),
init_func=init,
repeat=False)
ani.save(name + ".mp4", fps=20)
def create_gif(qstates, qstart, qtarget, name):
'''
Inputs:
# qstates: list of states as np.arrays
# qstart, qtarget: respectively the target ans start state
# name: name of the output gif
'''
b = Bloch()
duration = 5 #framerate
images = []
for (qstate, i) in zip(qstates, range(0, len(qstates))):
b.clear()
b.point_color = "r" # options: 'r', 'g', 'b' etc.
b.point_marker = ['o']
b.point_size = [40]
b.add_states(qutip_qstate(qstart))
b.add_states(qutip_qstate(qtarget))
for previous in range(i):
b.add_states(qutip_qstate(qstates[previous]),
"point") #plots previous visited states as points
b.add_states(qutip_qstate(qstate))
filename = 't.png'
b.save(filename)
images.append(imageio.imread(filename))
imageio.mimsave(name, images, 'GIF', fps=duration)
def __enter__(self):
from qutip import Bloch3d, Bloch
plt.ion()
self.fig = plt.figure(figsize=self.figsize)
self.ax = Axes3D(self.fig, azim=-30, elev=15)
self.ball = Bloch(axes=self.ax)
self.ball.zlabel = [r'$|N\rangle$', r'$|S\rangle$']
return self
def plot_quantum_state(amplitudes):
"""
Thin function to abstract the plotting on the Bloch sphere.
"""
bloch_sphere = Bloch()
vec = get_vector(amplitudes[0], amplitudes[1])
bloch_sphere.add_vectors(vec)
bloch_sphere.show()
bloch_sphere.clear()
def PlotStateQWP(InputState, qwpAngle):
OutputState = QWP(qwpAngle) @ InputState
pntsX = [
StateToBloch(QWP(th) @ InputState)[0] for th in arange(0, pi, pi / 64)
]
pntsY = [
StateToBloch(QWP(th) @ InputState)[1] for th in arange(0, pi, pi / 64)
]
pntsZ = [
StateToBloch(QWP(th) @ InputState)[2] for th in arange(0, pi, pi / 64)
]
pnts = [pntsX, pntsY, pntsZ]
bsph = Bloch()
bsph.add_points(pnts)
bsph.add_vectors(StateToBloch(OutputState))
bsph.add_vectors(StateToBloch(InputState))
return bsph.show()
def bloch_from_dataframe(df, fig, axes):
"""
Plot Bloch sphere
:param df: pd.DataFrame
:param axes:
:return:
"""
bloch = Bloch(fig=fig, axes=axes)
bloch.vector_color = plt.get_cmap('viridis')(np.linspace(0, 1, len(df)))
bloch.add_states([
Qobj([[row.Jxx, row.beta + 1j * row.gamma],
[row.beta - 1j * row.gamma, row.Jyy]])
for _, row in df.iterrows()
])
bloch.make_sphere()
def animate_bloch(vectors, duration=0.1, save_all=False):
numberOfLoops = 1 #Enter '1' to apply only ONE mode [Excitation or Relaxation] or '2' to to apply only BOTH modes [Excitation and Relaxation] starting with the selected mode
if numberOfLoops == 1:
maxAngle = 2 * np.pi
elif numberOfLoops == 2:
maxAngle = 4 * np.pi
mode = 1 #Enter '0' to activate Excitation Mode or '1' to activate Relaxation Mode
omega = np.pi / 6 #Enter the angular frequency
z = 0
sqAngle = np.pi / 2
a = 5
vectorM = Bloch()
# vectorM.view = [90,90] #Activate this line to view magnetization’s trajectory on x-y plane
images = []
for t in np.arange(omega, maxAngle, 0.1):
if mode == 0:
z = np.pi / 2 * np.sin(t / (4))
if t == 2 * np.pi:
mode = 1
elif mode == 1:
z = np.pi / 2 * np.cos(t / (4))
if t == 2 * np.pi:
mode = 0
else:
pass
vectorM.clear()
vectorM.add_vectors([
np.sin(omega) * np.cos(t),
np.sin(omega) * np.sin(t),
np.cos(omega)
])
vectorM.add_vectors(
[np.sin(z) * np.cos(a * t),
np.sin(z) * np.sin(a * t),
np.cos(z)])
vectorM.add_vectors([
np.sin(sqAngle) * np.cos(t),
np.sin(sqAngle) * np.sin(t),
np.cos(sqAngle)
])
filename = 'temp_file.png'
vectorM.save(filename)
images.append(imageio.imread(filename))
imageio.mimsave('bloch_anim.gif', images, duration=duration)
def field_plot(self, params, bloch=[False, 1]):
"""
Plots the signal components given simulation parameters over the specified time doman
"""
# get time varying fields and simulation data
time, cparams, Bfields = field_get(params=params)
# plot magnetic field vector on Bloch sphere
if bloch[0]:
Bfields = Bfields[::bloch[1], :]
# normalise each magnetic field vector
for i in range(len(Bfields)):
norm = np.sqrt(Bfields[i, 0]**2 + Bfields[i, 1]**2 +
Bfields[i, 2]**2)
Bfields[i, 0] /= norm
Bfields[i, 1] /= norm
Bfields[i, 2] /= norm
# extract x,y,z fields
Bx = Bfields[:, 0]
By = Bfields[:, 1]
Bz = Bfields[:, 2]
# define bloch object
b = Bloch()
b.add_points([Bx, By, Bz])
b.show()
else:
# plot fields
fig, ax = plt.subplots(nrows=3, ncols=1, sharex=True, sharey=False)
for i, row in enumerate(ax):
# plot each component, skipping zero time value
row.plot(time, Bfields[:, i])
row.set_title("Field vector along {} axis".format(
['x', 'y', 'z'][i]))
plt.ylabel('Frequency (Hz)')
plt.xlabel("Time (s)")
#plt.ylabel("Ampltiude ($Hz/Gauss$)")
plt.show()
def animate(states):
fig = figure()
ax = Axes3D(fig,azim=-40,elev=30)
sphere = Bloch(axes=ax)
def animate(i):
sphere.clear()
sphere.add_states([states[i]])
sphere.make_sphere()
return ax
def init():
sphere.vector_color = ['r']
return ax
ani = animation.FuncAnimation(fig, animate, np.arange(len(states)),
init_func=init, blit=False, repeat=True)
ani.save('decoherence.mp4', fps=20)
def maj_vid(self, points):
#takes screenshots of majorana stars over time to produce vid
if points is None:
points = [getStars(self.state)]
i = 0
for p in points:
bloch = Bloch(figsize=[9, 9])
bloch.xlabel = ['$<F_x>$', '']
bloch.ylabel = ['$<F_y>$', '']
bloch.zlabel = ['$<F_z>$', '']
bloch.point_color = ['g', 'r',
'b'] #ensures point and line are same colour
bloch.point_marker = ['o', 'd', 'o']
bloch.add_points([p[0][0], p[1][0], p[2][0]])
bloch.add_points([p[0][1], p[1][1], p[2][1]])
bloch.add_points(p, meth='l')
bloch.render(bloch.fig, bloch.axes)
bloch.fig.savefig(
"bloch" + str(i).zfill(int(np.ceil(np.log10(len(points))))) +
".png",
dpi=600,
transparent=False)
i += 1
def draw_center_hvps_rectified_sphere(hv_points, root):
b = Bloch()
b.point_color = ['m', 'k', 'g', 'b', 'w', 'c', 'y', 'r']
b.zlabel = ['$z$', '']
b.point_marker = ['o']
b.point_size = [80]
b.frame_width = 1.2
fig = plt.figure(figsize=(20, 20))
b.fig = fig
x = (basis(2, 0) + (1 + 0j) * basis(2, 1)).unit()
y = (basis(2, 0) + (0 + 1j) * basis(2, 1)).unit()
z = (basis(2, 0) + (0 + 0j) * basis(2, 1)).unit()
b.add_states([x, y, z])
for i in range(len(hv_points)):
# Transform xyz to zxy coordinates
tmp1 = np.array([hv_points[i][2], hv_points[i][0], hv_points[i][1]])
tmp2 = np.vstack([tmp1, -tmp1]).T
tmp = tmp2
b.add_points(tmp)
name = os.path.join(root, 'consensus_hvps_center_on_rectified_sphere.jpg')
b.save(name=name)
def bloch_plot(self, points=None):
"""
Plot the current state on the Bloch sphere using
qutip.
"""
if points is None:
# convert current state into density operator
rho = np.outer(self.state.H, self.state)
# get Bloch vector representation
points = self.get_bloch_vec(rho)
# Can only plot systems of dimension 2 at this time
assert len(
points
) == 3, "System dimension must be spin 1/2 for Bloch sphere plot"
# create instance of 3d plot
bloch = Bloch(figsize=[9, 9])
# add state
bloch.add_points(points)
bloch.add_vectors([0, 0, 1])
bloch.render(bloch.fig, bloch.axes)
bloch.fig.savefig("bloch.png", dpi=600, transparent=True)
bloch.show()
def PlotBlochState(state):
bsph = Bloch()
bsph.add_vectors(StateToBloch(state))
return bsph.show()
def bloch_plot2(self,
filename,
save=False,
vecList=[],
vecColour=[],
view=[190, 10],
points=None,
folder=False,
fig=False,
ax=False):
"""
Plot the current state on the Bloch sphere using
qutip.
"""
if points is None:
# convert current state into density operator
rho = np.outer(self.state.H, self.state)
# get Bloch vector representation
points = self.get_bloch_vec(rho)
# Can only plot systems of dimension 2 at this time
assert len(
points
) == 3, "System dimension must be spin 1/2 for Bloch sphere plot"
# create instance of 3d plot
if not fig or not ax:
bloch = Bloch(figsize=[9, 9], view=view)
else:
bloch = Bloch(fig=fig, axes=ax, view=view)
# add state
bloch.add_points(points)
# bloch.zlabel = [r'$\left|+z\right>$',r'$\left|-z\right>$']
bloch.zlabel = [r'$\ket{+_z}$', r'$\ket{-_z}$']
# bloch.ylabel = [r'$\ket{+_y}$',r'$\ket{-_y}$']
# bloch.ylabel = [r'$\ket{+_y}$',r'$\ket{-_y}$']
# print(vecList.shape)
# add vectors
if vecList.shape[1] == 3:
if len(vecColour) >= vecList.shape[0] and len(vecColour) > 0:
bloch.vector_color = vecColour
else:
bloch.vector_color = ['#CC6600', 'royalblue', 'r', 'm', 'g']
bloch.add_vectors(vecList)
# add field vector
# bloch.add_vectors([1,0,0.15])
# bloch.add_vectors([0,0,1])
# bloch.add_vectors([1,0,0])
# render bloch sphere
if not fig or not ax:
bloch.render()
else:
# bloch.render(fig = fig, axes = ax)
bloch.render(fig=fig)
# save output
if save is True:
if not folder:
folder = 'C:/Users/Boundsy/Desktop/Uni Work/PHS2360/Sim Results/'
print('Bloch plot saved to ' + str(folder))
path1 = folder + str(filename) + '.png'
path2 = folder + str(filename) + '.pdf'
bloch.fig.savefig(path1, dpi=800, transparent=True)
bloch.fig.savefig(path2, dpi=800, transparent=True)
# return axes for annotations
return bloch.fig, bloch.axes
#!/usr/bin/env python3 # -*- coding: utf-8 -*- """ Created on Tue Jul 30 12:26:48 2019 @author: banano """ # from qutip import Bloch, Bloch3d b1 = Bloch() vec = [0,1,0] b1.add_vectors(vec) b1.vector_color = ['k'] b2 = Bloch() vec = [0,0,1] b2.add_vectors(vec) b2.vector_color = ['r'] b2.show() b1.show()
def __init__(self, fig):
#################################################################
#
# Initialize plotting exact plots tools
#
#################################################################
# p = np.linspace(-20., 20., 1000)[:, np.newaxis]
# q = np.linspace(-20., 20., 1000)[np.newaxis, :]
#
# self.hybrid = CAnalyticQCHybrid(p, q, kT=0.5)
#
# img_params = dict(
# extent=[q.min(), q.max(), p.min(), p.max()],
# origin='lower',
# cmap='seismic',
# # norm=WignerNormalize(vmin=-0.1, vmax=0.1)
# norm=WignerSymLogNorm(linthresh=1e-10, vmin=-0.01, vmax=0.1)
# )
p = np.linspace(-25, 25, 600)[:, np.newaxis]
q = np.linspace(-25, 25, 600)[np.newaxis, :]
self.hybrid = CAnalyticQCHybrid(p=p,
q=q,
omega=1.,
beta=2.,
alpha=0.95)
img_params = dict(
extent=[q.min(), q.max(), p.min(),
p.max()],
origin='lower',
cmap='seismic',
# norm=WignerNormalize(vmin=-0.1, vmax=0.1)
norm=WignerSymLogNorm(linthresh=1e-10, vmin=-0.01, vmax=0.1))
#################################################################
#
# Initialize Pauli propagator
#
#################################################################
self.pauli = SplitOpPauliLike1D(
X_amplitude=2. * q.max(),
X_gridDIM=512,
dt=0.0001,
K0="0.5 * P ** 2",
V0="0.5 * X ** 2",
V1="0.5 * 0.95 * X ** 2",
# kT=self.hybrid.kT, # parameters controlling the width of the initial wavepacket
).set_wavefunction("exp(-0.5 * X ** 2)")
#################################################################
#
# Initialize plotting facility
#
#################################################################
self.fig = fig
self.fig.suptitle(
"Quantum-classical hybrid $m=1$, $\omega=1$, $\\alpha=0.95$, $\\beta={:.1e}$ (a.u.) (a.u.)"
.format(self.hybrid.beta))
self.ax = fig.add_subplot(221)
self.ax.set_title('Classical density')
# generate empty plots
self.img_classical_density = self.ax.imshow([[0]], **img_params)
self.ax.set_xlabel('$q$ (a.u.)')
self.ax.set_ylabel('$p$ (a.u.)')
ax = fig.add_subplot(222)
ax.set_title('Quantum purity')
self.quantum_purity_plot, = ax.plot([0., 40], [1, 0.5],
label='hybrid')
self.pauli_quantum_purity_plot, = ax.plot([0., 40], [1, 0.5],
label='Pauli')
ax.set_xlabel('time (a.u.)')
ax.set_ylabel("quantum purity")
ax.legend()
self.time = []
self.qpurity = []
self.pauli_qpurity = []
ax = fig.add_subplot(223)
ax.set_title("Coordinate distribution")
self.c_coordinate_distribution, = ax.semilogy(
[self.hybrid.q.min(), self.hybrid.q.max()], [1e-11, 1e0],
label="hybrid")
self.pauli_coordinate_distribution, = ax.semilogy(
[self.hybrid.q.min(), self.hybrid.q.max()], [1e-11, 1e0],
label="Pauli")
ax.legend()
ax.set_xlabel('$q$ (a.u.)')
ax.set_ylabel('Probability density')
ax = fig.add_subplot(224, projection='3d', azim=90, elev=0)
self.bloch = Bloch(axes=ax)
self.bloch.make_sphere()
# ist qutip installiert?
# https://numpy.org/install/#python-numpy-install-guide
# importieren der numpy Library mit der Abkuerzung np
# um nicht immer numpy schreiben zu muessen
import numpy as np
# importieren der Python eigene Mathematik Library
import math
# Beispielseite zu qutip
# http://qutip.org/docs/3.1.0/guide/guide-bloch.html
# %% -1-
# Bloch() erzeugt eine Bloch
# mit b verweisen wir spaeter auf diese
b = Bloch()
# b.show() zeigt die aktuelle Blochkugel an
b.show()
print('-1-')
input('Press ENTER to continue.'
) # Ansonst wird Fenster sofort wieder geschlossen bzw. ueberschrieben.
# %% -2-
# hinzufuegen eines Vektor
# x,y,z
v = [1, 0, 0] # dazu geben wir einen Vektor in die x-Richtung an
b.add_vectors(
v) # mit b.add_vectors wird der Vektor v der Blochkugel hinzugefuegt
b.show()
print('-2-')
def __init__(self, fig):
#################################################################
#
# Initialize plotting exact plots tools
#
#################################################################
# p = np.linspace(-20., 20., 1000)[:, np.newaxis]
# q = np.linspace(-20., 20., 1000)[np.newaxis, :]
#
# self.hybrid = CAnalyticQCHybrid(p, q, kT=0.5)
#
# img_params = dict(
# extent=[q.min(), q.max(), p.min(), p.max()],
# origin='lower',
# cmap='seismic',
# # norm=WignerNormalize(vmin=-0.1, vmax=0.1)
# norm=WignerSymLogNorm(linthresh=1e-10, vmin=-0.01, vmax=0.1)
# )
p = np.linspace(-0.1, 0.1, 500)[:, np.newaxis]
q = np.linspace(-0.1, 0.1, 500)[np.newaxis, :]
self.hybrid = SolAGKEq(p=p, q=q, omega=1., beta=1e5, alpha=0.95)
img_params = dict(
extent=[q.min(), q.max(), p.min(),
p.max()],
origin='lower',
cmap='seismic',
#norm=WignerNormalize(vmin=-0.1, vmax=0.1)
norm=WignerSymLogNorm(linthresh=1e-10, vmin=-0.01, vmax=0.1))
# List to save the total hybrid energy for testing (it must be a conserved quantity)
self.total_energy = []
# List to save the x component of the Bloch vector
self.sigma_1 = []
#################################################################
#
# Initialize plotting facility
#
#################################################################
self.fig = fig
self.fig.suptitle(
"Quantum-classical hybrid $m=1$, $\omega=1$, $\\alpha=0.95$, $\\beta={:.1e}$ (a.u.) (a.u.)"
.format(self.hybrid.beta))
self.ax = fig.add_subplot(221)
self.ax.set_title('Classical density')
# generate empty plots
self.img_classical_density = self.ax.imshow([[0]], **img_params)
self.ax.set_xlabel('$q$ (a.u.)')
self.ax.set_ylabel('$p$ (a.u.)')
ax = fig.add_subplot(222)
ax.set_title('Quantum purity')
self.quantum_purity_plot, = ax.plot([0., 1000000], [1, 0.5])
ax.set_xlabel('time (a.u.)')
ax.set_ylabel("quantum purity")
self.time = []
self.qpurity = []
ax = fig.add_subplot(223)
ax.set_title("Coordinate distribution")
self.c_coordinate_distribution, = ax.semilogy(
[self.hybrid.q.min(), self.hybrid.q.max()], [1e-11, 1e0],
label="hybrid")
ax.legend()
ax.set_xlabel('$q$ (a.u.)')
ax.set_ylabel('Probability density')
ax = fig.add_subplot(224, projection='3d', azim=0, elev=0)
self.bloch = Bloch(axes=ax)
self.bloch.make_sphere()
