def test_squeezing(self):
"""Test squeezing gives correct means and cov"""
self.eng.reset()
q = self.eng.register
x = 0.2
p = 0.3
r = 0.42
phi = 0.123
H, t = squeezing(r, phi, hbar=self.hbar)
with self.eng:
Xgate(x) | q[0]
Zgate(p) | q[0]
GaussianPropagation(H, t) | q[0]
state = self.eng.run('gaussian')
# test the covariance matrix
res = state.cov()
S = rot(phi / 2) @ np.diag(np.exp([-r, r])) @ rot(phi / 2).T
V = S @ S.T * self.hbar / 2
self.assertTrue(np.allclose(res, V))
# test the vector of means
res = state.means()
exp = S @ np.array([x, p])
self.assertTrue(np.allclose(res, exp))
def test_rotation(self):
"""Test rotation gives correct means and cov"""
self.eng.reset()
q = self.eng.register
x = 0.2
p = 0.3
phi = 0.123
H, t = rotation(phi, hbar=self.hbar)
with self.eng:
Xgate(x) | q[0]
Zgate(p) | q[0]
Sgate(2) | q[0]
GaussianPropagation(H, t) | q[0]
state = self.eng.run('gaussian')
# test the covariance matrix
res = state.cov()
V = np.diag([np.exp(-4), np.exp(4)]) * self.hbar / 2
expected = rot(phi) @ V @ rot(phi).T
self.assertTrue(np.allclose(res, expected))
# test the vector of means
res = state.means()
exp = rot(phi) @ np.diag(np.exp([-2, 2])) @ np.array([x, p])
self.assertTrue(np.allclose(res, exp))
def test_quadratic_phase(self):
"""Test quadratic phase gives correct means and cov"""
self.eng.reset()
q = self.eng.register
x = 0.2
p = 0.3
s = 0.432
H, t = quadratic_phase(s)
with self.eng:
Xgate(x) | q[0]
Zgate(p) | q[0]
GaussianPropagation(H, t) | q[0]
state = self.eng.run('gaussian')
# test the covariance matrix
res = state.cov()
expected = np.array([[1, s], [s, 1 + s**2]]) * self.hbar / 2
self.assertTrue(np.allclose(res, expected))
# test the vector of means
res = state.means()
expected = np.array([x, p + s * x])
self.assertTrue(np.allclose(res, expected))
def test_displaced_oscillator(self):
"""Test that a forced quantum oscillator produces the correct
self.logTestName()
trajectory in the phase space"""
H = QuadOperator('q0 q0', 0.5)
H += QuadOperator('p0 p0', 0.5)
H -= QuadOperator('q0', self.F)
res = []
tlist = np.arange(0, self.t, self.dt)
for t in tlist: #pylint: disable=unused-variable
self.eng.reset()
q = self.eng.register
with self.eng:
Xgate(self.x0) | q[0]
Zgate(self.p0) | q[0]
GaussianPropagation(H, self.t) | q
state = self.eng.run('gaussian')
res.append(state.means().tolist())
res = np.array(res)[-1]
expected = self.displaced_oscillator_soln(self.t)
self.assertTrue(np.allclose(res, expected))
def test_rotation(self, hbar):
"""Test rotation gives correct means and cov"""
prog = sf.Program(1)
eng = sf.Engine("gaussian")
x = 0.2
p = 0.3
phi = 0.123
H, t = rotation(phi, hbar=hbar)
with prog.context as q:
Xgate(x) | q[0]
Zgate(p) | q[0]
Sgate(2) | q[0]
GaussianPropagation(H, t) | q[0]
state = eng.run(prog).state
# test the covariance matrix
res = state.cov()
V = np.diag([np.exp(-4), np.exp(4)]) * hbar / 2
expected = rot(phi) @ V @ rot(phi).T
assert np.allclose(res, expected)
# test the vector of means
res = state.means()
exp = rot(phi) @ np.diag(np.exp([-2, 2])) @ np.array([x, p])
assert np.allclose(res, exp)
def test_squeezing(self, hbar):
"""Test squeezing gives correct means and cov"""
prog = sf.Program(1)
eng = sf.Engine("gaussian")
x = 0.2
p = 0.3
r = 0.42
phi = 0.123
H, t = squeezing(r, phi, hbar=hbar)
with prog.context as q:
Xgate(x) | q[0]
Zgate(p) | q[0]
GaussianPropagation(H, t) | q[0]
state = eng.run(prog).state
# test the covariance matrix
res = state.cov()
S = rot(phi / 2) @ np.diag(np.exp([-r, r])) @ rot(phi / 2).T
V = S @ S.T * hbar / 2
assert np.allclose(res, V)
# test the vector of means
res = state.means()
exp = S @ np.array([x, p])
assert np.allclose(res, exp)
def test_displaced_oscillator(self):
"""Test that a forced quantum oscillator produces the correct
self.logTestName()
trajectory in the phase space"""
H = QuadOperator('q0 q0', 0.5)
H += QuadOperator('p0 p0', 0.5)
H -= QuadOperator('q0', self.F)
res = []
tlist = np.arange(0, self.t, self.dt)
eng = sf.Engine("gaussian")
for idx, t in enumerate(tlist): #pylint: disable=unused-variable
prog = sf.Program(1)
with prog.context as q:
Xgate(self.x0) | q[0]
Zgate(self.p0) | q[0]
GaussianPropagation(H, self.t) | q
state = eng.run(prog).state
eng.reset()
res.append(state.means().tolist())
res = np.array(res)[-1]
expected = self.displaced_oscillator_soln(self.t)
assert np.allclose(res, expected)
def test_quadratic_phase(self, hbar):
"""Test quadratic phase gives correct means and cov"""
prog = sf.Program(1)
eng = sf.Engine("gaussian")
x = 0.2
p = 0.3
s = 0.432
H, t = quadratic_phase(s)
with prog.context as q:
Xgate(x) | q[0]
Zgate(p) | q[0]
GaussianPropagation(H, t) | q[0]
state = eng.run(prog).state
# test the covariance matrix
res = state.cov()
expected = np.array([[1, s], [s, 1 + s**2]]) * hbar / 2
assert np.allclose(res, expected)
# test the vector of means
res = state.means()
expected = np.array([x, p + s * x])
assert np.allclose(res, expected)
def init_layer(q):
"""Create an initial state with defined
squeezing and displacement"""
Xgate(0.2) | q[0]
Xgate(0.4) | q[1]
Zgate(0.3) | q[1]
Sgate(0.1) | q[0]
Sgate(-0.1) | q[1]
return q
def decompose(self, reg):
"""Return the decomposed commands"""
cmds = []
cmds += [Command(GaussianTransform(self.S), reg)]
if self.disp:
cmds += [
Command(Xgate(x), reg) for x in self.d[:self.ns] if x != 0.
]
cmds += [
Command(Zgate(z), reg) for z in self.d[self.ns:] if z != 0.
]
return cmds
r = np.abs(alpha)
phi = np.angle(alpha)
with prog.context as q:
# prepare initial states
Coherent(r, phi) | q[0]
Squeezed(-2) | q[1]
Squeezed(2) | q[2]
# apply gates
BS = BSgate(pi / 4, 0)
BS | (q[1], q[2])
BS | (q[0], q[1])
# Perform homodyne measurements
MeasureX | q[0]
MeasureP | q[1]
# Displacement gates conditioned on
# the measurements
Xgate(sqrt(2) * q[0].par) | q[2]
Zgate(sqrt(2) * q[1].par) | q[2]
eng = sf.Engine("fock", backend_options={"cutoff_dim": 15})
result = eng.run(prog)
# view output state and fidelity
print(result.samples)
print(result.state)
print(result.state.fidelity_coherent([0, 0, alpha]))