sf.backends.BaseGaussianState¶

class
BaseGaussianState
(state_data, num_modes, mode_names=None)[source]¶ Bases:
strawberryfields.backends.states.BaseState
Class for the representation of quantum states using the Gaussian formalism.
Note that this class uses the Gaussian representation convention
\[\bar{\mathbf{r}} = (\bar{x}_1,\bar{x}_2,\dots,\bar{x}_N,\bar{p}_1,\dots,\bar{p}_N)\] Parameters
state_data (tuple(mu, cov)) – A tuple containing the vector of means array
mu
and the covariance matrix arraycov
, in terms of the complex displacement.num_modes (int) – the number of modes in the state
pure (bool) – True if the state is a pure state, false if the state is mixed
mode_names (Sequence) – (optional) this argument contains a list providing mode names for each mode in the state
Attributes
Returns the underlying numerical (or symbolic) representation of the state.
Returns the value of \(\hbar\) used in the generation of the state.
Checks whether the state is a pure state.
Returns a dictionary mapping the mode names to mode indices.
Returns a dictionary mapping the mode index to mode names.
Gets the number of modes that the state represents.

EQ_TOLERANCE
= 1e10¶

data
¶ Returns the underlying numerical (or symbolic) representation of the state. The form of this data differs for different backends.

hbar
¶ Returns the value of \(\hbar\) used in the generation of the state.
The value of \(\hbar\) is a convention chosen in the definition of \(\x\) and \(\p\). See Operators for more details.
 Returns
\(\hbar\) value.
 Return type
float

is_pure
¶ Checks whether the state is a pure state.
 Returns
True if and only if the state is pure.
 Return type
bool

mode_indices
¶ Returns a dictionary mapping the mode names to mode indices.
The mode names are determined from the initialization argument
mode_names
. If these were not supplied, the names are generated automatically based on the mode indices. Returns
dictionary of the form
{"mode name":i,...}
 Return type
dict

mode_names
¶ Returns a dictionary mapping the mode index to mode names.
The mode names are determined from the initialization argument
mode_names
. If these were not supplied, the names are generated automatically based on the mode indices. Returns
dictionary of the form
{i:"mode name",...}
 Return type
dict

num_modes
¶ Gets the number of modes that the state represents.
 Returns
the number of modes in the state
 Return type
int
Methods
cov
()The covariance matrix describing the Gaussian state.
displacement
([modes])Returns the displacement parameter \(\alpha\) of the modes specified.
fidelity
(other_state, mode, **kwargs)Fidelity of the reduced state in the specified mode with a user supplied state.
fidelity_coherent
(alpha_list, **kwargs)The fidelity of the state with a product of coherent states.
fidelity_vacuum
(**kwargs)The fidelity of the state with the vacuum state.
fock_prob
(n, **kwargs)Probability of a particular Fock basis state.
is_coherent
(mode[, tol])Returns True if the Gaussian state of a particular mode is a coherent state.
is_squeezed
(mode[, tol])Returns True if the Gaussian state of a particular mode is a squeezed state.
mean_photon
(mode, **kwargs)Returns the mean photon number of a particular mode.
means
()The vector of means describing the Gaussian state.
poly_quad_expectation
(A[, d, k, phi])The multimode expectation values and variance of arbitrary 2nd order polynomials of quadrature operators.
quad_expectation
(mode[, phi])The \(\x_{\phi}\) operator expectation values and variance for the specified mode.
reduced_dm
(modes, **kwargs)Returns a reduced density matrix in the Fock basis.
reduced_gaussian
(modes)Returns the vector of means and the covariance matrix of the specified modes.
squeezing
([modes])Returns the squeezing parameters \((r,\phi)\) of the modes specified.
wigner
(mode, xvec, pvec)Calculates the discretized Wigner function of the specified mode.

cov
()[source]¶ The covariance matrix describing the Gaussian state.
The diagonal elements of the covariance matrix correspond to the variance in the position and momentum quadratures:
\[\begin{split}\mathbf{V}_{ii} = \begin{cases} (\Delta x_i)^2, & 0\leq i\leq N1\\ (\Delta p_{iN})^2, & N\leq i\leq 2(N1) \end{cases}\end{split}\]where \(\Delta x_i\) and \(\Delta p_i\) refer to the position and momentum quadrature variance of mode \(i\) respectively.
Note that if the covariance matrix is purely diagonal, then this corresponds to squeezing \(z=re^{i\phi}\) where \(\phi=0\), and \(\Delta x_i = e^{2r}\), \(\Delta p_i = e^{2r}\).
 Returns
the \(2N\times 2N\) covariance matrix.
 Return type
array

displacement
(modes=None)[source]¶ Returns the displacement parameter \(\alpha\) of the modes specified.
 Parameters
modes (int or Sequence[int]) – modes specified
 Returns
sequence of complex displacements \(\alpha\) corresponding to the list of specified modes
 Return type
Sequence[complex]

abstract
fidelity
(other_state, mode, **kwargs)[source]¶ Fidelity of the reduced state in the specified mode with a user supplied state. Note that this method only supports singlemode states.
 Parameters
other_state – a pure state vector array represented in the Fock basis (for Fock backends) or a Sequence
(mu, cov)
containing the means and covariance matrix (for Gaussian backends) Returns
The fidelity of the circuit state with
other_state
.

abstract
fidelity_coherent
(alpha_list, **kwargs)[source]¶ The fidelity of the state with a product of coherent states.
The fidelity is defined by
\[\bra{\vec{\alpha}}\rho\ket{\vec{\alpha}}\] Parameters
alpha_list (Sequence[complex]) – list of coherent state parameters, one for each mode
 Returns
the fidelity value
 Return type
float

abstract
fidelity_vacuum
(**kwargs)[source]¶ The fidelity of the state with the vacuum state.
 Returns
the fidelity of the state with the vacuum
 Return type
float

abstract
fock_prob
(n, **kwargs)[source]¶ Probability of a particular Fock basis state.
Computes the probability \(\braket{\vec{n}\psi}^2\) of measuring the given multimode Fock state based on the state \(\ket{\psi}\).
Warning
Computing the Fock probabilities of states has exponential scaling in the Gaussian representation (for example states output by a Gaussian backend as a
BaseGaussianState
). This shouldn’t affect smallscale problems, where only a few Fock basis state probabilities need to be calculated, but will become evident in larger scale problems. Parameters
n (Sequence[int]) – the Fock state \(\ket{\vec{n}}\) that we want to measure the probability of
**kwargs –
cutoff (int): (default 10) specifies the fock basis truncation when calculating of the fock basis probabilities. Note that the cutoff argument only applies for Gaussian representation; states represented in the Fock basis will use their own internal cutoff dimension.
 Returns
measurement probability
 Return type
float

is_coherent
(mode, tol=1e10)[source]¶ Returns True if the Gaussian state of a particular mode is a coherent state.
 Parameters
mode (int) – the specified mode
tol (float) – the numerical precision in determining if squeezing is not present
 Returns
True if and only if the state is a coherent state.
 Return type
bool

is_squeezed
(mode, tol=1e06)[source]¶ Returns True if the Gaussian state of a particular mode is a squeezed state.
 Parameters
mode (int) – the specified mode
tol (float) – the numerical precision in determining if squeezing is present
 Returns
True if and only if the state is a squeezed state.
 Return type
bool

abstract
mean_photon
(mode, **kwargs)[source]¶ Returns the mean photon number of a particular mode.
 Parameters
mode (int) – specifies the mode
**kwargs –
cutoff (int): (default 10) Fock basis trunction for calculation of mean photon number. Note that the cutoff argument only applies for Gaussian representation; states represented in the Fock basis will use their own internal cutoff dimension.
 Returns
the mean photon number and variance
 Return type
tuple

means
()[source]¶ The vector of means describing the Gaussian state.
For a \(N\) mode state, this has the form
\[\bar{\mathbf{r}} = \left(\bar{x}_0,\dots,\bar{x}_{N1},\bar{p}_0,\dots,\bar{p}_{N1}\right)\]where \(\bar{x}_i\) and \(\bar{p}_i\) refer to the mean position and momentum quadrature of mode \(i\) respectively.
 Returns
a length \(2N\) array containing the vector of means.
 Return type
array

poly_quad_expectation
(A, d=None, k=0, phi=0, **kwargs)[source]¶ The multimode expectation values and variance of arbitrary 2nd order polynomials of quadrature operators.
An arbitrary 2nd order polynomial of quadrature operators over $N$ modes can always be written in the following form:
\[P(\mathbf{r}) = \mathbf{r}^T A\mathbf{r} + \mathbf{r}^T \mathbf{d} + k I\]where:
\(A\in\mathbb{R}^{2N\times 2N}\) is a symmetric matrix representing the quadratic coefficients,
\(\mathbf{d}\in\mathbb{R}^{2N}\) is a real vector representing the linear coefficients,
\(k\in\mathbb{R}\) represents the constant term, and
\(\mathbf{r} = (\x_1,\dots,\x_N,\p_1,\dots,\p_N)\) is the vector of quadrature operators in \(xp\)ordering.
This method returns the expectation value of this secondorder polynomial,
\[\langle P(\mathbf{r})\rangle,\]as well as the variance
\[\Delta P(\mathbf{r})^2 = \braket{P(\mathbf{r})^2}  \braket{P(\mathbf{r})}^2\] Parameters
A (array) – a real symmetric 2Nx2N NumPy array, representing the quadratic coefficients of the second order quadrature polynomial.
d (array) – a real length2N NumPy array, representing the linear coefficients of the second order quadrature polynomial. Defaults to the zero vector.
k (float) – the constant term. Default 0.
phi (float) – quadrature angle, clockwise from the positive \(x\) axis. If provided, the vectori of quadrature operators \(\mathbf{r}\) is first rotated by angle \(\phi\) in the phase space.
 Returns
expectation value and variance
 Return type
tuple (float, float)

quad_expectation
(mode, phi=0, **kwargs)[source]¶ The \(\x_{\phi}\) operator expectation values and variance for the specified mode.
The \(\x_{\phi}\) operator is defined as follows,
\[\x_{\phi} = \cos\phi~\x + \sin\phi~\p\]with corresponding expectation value
\[\bar{x_{\phi}}=\langle x_{\phi}\rangle = \text{Tr}(\x_{\phi}\rho_{mode})\]and variance
\[\Delta x_{\phi}^2 = \langle x_{\phi}^2\rangle  \braket{x_{\phi}}^2\] Parameters
mode (int) – the requested mode
phi (float) –
quadrature angle, clockwise from the positive \(x\) axis.
\(\phi=0\) corresponds to the \(x\) expectation and variance (default)
\(\phi=\pi/2\) corresponds to the \(p\) expectation and variance
 Returns
expectation value and variance
 Return type
tuple (float, float)

abstract
reduced_dm
(modes, **kwargs)[source]¶ Returns a reduced density matrix in the Fock basis.
 Parameters
modes (int or Sequence[int]) – specifies the mode(s) to return the reduced density matrix for.
**kwargs –
cutoff (int): (default 10) specifies where to truncate the returned density matrix. Note that the cutoff argument only applies for Gaussian representation; states represented in the Fock basis will use their own internal cutoff dimension.
 Returns
the reduced density matrix for the specified modes
 Return type
array

reduced_gaussian
(modes)[source]¶ Returns the vector of means and the covariance matrix of the specified modes.
 Parameters
modes (int of Sequence[int]) – indices of the requested modes
 Returns
where means is an array containing the vector of means, and cov is a square array containing the covariance matrix.
 Return type
tuple (means, cov)

squeezing
(modes=None)[source]¶ Returns the squeezing parameters \((r,\phi)\) of the modes specified.
 Parameters
modes (int or Sequence[int]) – modes specified
 Returns
sequence of tuples containing the squeezing parameters \((r,\phi)\) of the specified modes.
 Return type
List[(float, float)]

wigner
(mode, xvec, pvec)[source]¶ Calculates the discretized Wigner function of the specified mode.
 Parameters
mode (int) – the mode to calculate the Wigner function for
xvec (array) – array of discretized \(x\) quadrature values
pvec (array) – array of discretized \(p\) quadrature values
 Returns
2D array of size [len(xvec), len(pvec)], containing reduced Wigner function values for specified x and p values.
 Return type
array
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