J.R. Johansson and P.D. Nation
For more information about QuTiP see http://qutip.org
In [1]:
%matplotlib inline
import matplotlib.pylab as plt
import matplotlib as mpl
from mpl_toolkits.mplot3d import Axes3D
from matplotlib import cm
In [2]:
from qutip import *
#from qutip.visualization import wigner_cmap
In [3]:
x = 1.0 / sqrt(2) * (basis(10, 4) + basis(10, 2))
xvec = arange(-5, 5, 10.0 / 100)
yvec = xvec
W = wigner(x, xvec, yvec)
cmap = wigner_cmap(W)
X, Y = meshgrid(xvec, yvec)
In [4]:
fig = plt.figure(figsize=(8,6))
plt.contourf(X, Y, W, 50, cmap=cmap)
plt.colorbar();
In [5]:
fig = plt.figure(figsize=(10,8))
ax = Axes3D(fig, azim=-30, elev=73)
ax.plot_surface(X, Y, W, cmap=cmap, rstride=1, cstride=1, alpha=1, linewidth=0)
ax.set_zlim3d(-0.25, 0.25)
for a in ax.w_zaxis.get_ticklines() + ax.w_zaxis.get_ticklabels():
a.set_visible(False)
nrm = mpl.colors.Normalize(W.min(), W.max())
cax, kw = mpl.colorbar.make_axes(ax, shrink=.66, pad=.02)
cb1 = mpl.colorbar.ColorbarBase(cax, cmap=cmap, norm=nrm)
cb1.set_label('Pseudoprobability')
In [6]:
N = 20;
alpha = -1.0; # Coherent amplitude of field
epsilon = 0.5j; # Squeezing parameter
a = destroy(N);
D = (alpha*a.dag()-conj(alpha)*a).expm(); # Displacement
S = (0.5*conj(epsilon)*a*a-0.5*epsilon*a.dag()*a.dag()).expm(); # Squeezing
psi = D*S*basis(N,0); # Apply to vacuum state
g = 2;
In [7]:
xvec = arange(-40.,40.)*5./40
X,Y = meshgrid(xvec, xvec)
W=wigner(psi,xvec,xvec)
fig1 = plt.figure()
ax = Axes3D(fig1)
ax.plot_surface(X, Y, W, rstride=2, cstride=2, cmap=cm.jet, alpha=0.7)
ax.contour(X, Y, W, 15,zdir='x', offset=-6)
ax.contour(X, Y, W, 15,zdir='y', offset=6)
ax.contour(X, Y, W, 15,zdir='z', offset=-0.3)
ax.set_xlim3d(-6,6)
ax.set_xlim3d(-6,6)
ax.set_zlim3d(-0.3,0.4)
plt.title('Wigner function of squeezed state');
In [8]:
Q = qfunc(psi,xvec,xvec,g);
fig2 = plt.figure()
ax = Axes3D(fig2)
ax.plot_surface(X, Y, Q, rstride=2, cstride=2, cmap=cm.jet, alpha=0.7)
ax.contour(X, Y, Q,zdir='x', offset=-6)
ax.contour(X, Y, Q,zdir='y', offset=6)
ax.contour(X, Y, Q, 15,zdir='z', offset=-0.4)
ax.set_xlim3d(-6,6)
ax.set_xlim3d(-6,6)
ax.set_zlim3d(-0.3,0.4)
plt.title('Q function of squeezed state');
In [9]:
N = 20;
#amplitudes of coherent states
alpha1=-2.0-2j
alpha2=2.0+2j
#define ladder oeprators
a = destroy(N);
#define displacement oeprators
D1=(alpha1*dag(a)-conj(alpha1)*a).expm()
D2=(alpha2*dag(a)-conj(alpha2)*a).expm()
#sum of coherent states
psi = sqrt(2)**-1*(D1+D2)*basis(N,0); # Apply to vacuum state
In [10]:
#calculate Wigner function
yvec = xvec = arange(-100.,100.)*5./100
g=2.
W = wigner(psi,xvec,yvec)
c = plt.contourf(xvec,yvec,real(W),100)
plt.xlim([-5,5])
plt.ylim([-5,5])
plt.title('Wigner function of Schrodinger cat')
cbar = plt.colorbar(c)
cbar.ax.set_ylabel('Pseudoprobability');
In [11]:
#calculate Q function
Q = qfunc(psi,xvec,yvec)
qplt = plt.contourf(xvec,yvec,real(Q),100)
plt.xlim([-5,5])
plt.ylim([-5,5])
plt.title('Q function of Schrodinger cat')
cbar = plt.colorbar(qplt)
cbar.ax.set_ylabel('Probability');
In [12]:
from qutip.ipynbtools import version_table
version_table()
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