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A single step in the simulation of the DensityMatrixSimulator.
Inherits From: StepResultBase
, StepResult
cirq.DensityMatrixStepResult(
sim_state: 'cirq.SimulationStateBase[cirq.DensityMatrixSimulationState]',
dtype: Type[np.complexfloating] = np.complex64
)
Args | |
---|---|
sim_state
|
The qubit:SimulationState lookup for this step. |
dtype
|
The numpy.dtype used by the simulation. One of
numpy.complex64 or numpy.complex128 .
|
Attributes | |
---|---|
measurements
|
A dictionary from measurement gate key to measurement results, ordered by the qubits that the measurement operates on. |
Methods
density_matrix
density_matrix(
copy=True
)
Returns the density matrix at this step in the simulation.
The density matrix that is stored in this result is returned in the
computational basis with these basis states defined by the qubit_map.
In particular the value in the qubit_map is the index of the qubit,
and these are translated into binary vectors where the last qubit is
the 1s bit of the index, the second-to-last is the 2s bit of the index,
and so forth (i.e. big endian ordering). The density matrix is a
2 ** num_qubits
square matrix, with rows and columns ordered by
the computational basis as just described.
Example | |
---|---|
qubit_map
|
{QubitA: 0, QubitB: 1, QubitC: 2}
Then the returned density matrix will have (row and column) indices
mapped to qubit basis states like the following table
| | QubitA | QubitB | QubitC | | :-: | :----: | :----: | :----: | | 0 | 0 | 0 | 0 | | 1 | 0 | 0 | 1 | | 2 | 0 | 1 | 0 | | 3 | 0 | 1 | 1 | | 4 | 1 | 0 | 0 | | 5 | 1 | 0 | 1 | | 6 | 1 | 1 | 0 | | 7 | 1 | 1 | 1 | |
Args | |
---|---|
copy
|
If True, then the returned state is a copy of the density matrix. If False, then the density matrix is not copied, potentially saving memory. If one only needs to read derived parameters from the density matrix and store then using False can speed up simulation by eliminating a memory copy. |
sample
sample(
qubits: List['cirq.Qid'],
repetitions: int = 1,
seed: 'cirq.RANDOM_STATE_OR_SEED_LIKE' = None
) -> np.ndarray
Samples from the system at this point in the computation.
Note that this does not collapse the state vector.
Args | |
---|---|
qubits
|
The qubits to be sampled in an order that influence the returned measurement results. |
repetitions
|
The number of samples to take. |
seed
|
A seed for the pseudorandom number generator. |
Returns | |
---|---|
Measurement results with True corresponding to the |1⟩ state.
The outer list is for repetitions, and the inner corresponds to
measurements ordered by the supplied qubits. These lists
are wrapped as a numpy ndarray.
|
sample_measurement_ops
sample_measurement_ops(
measurement_ops: List['cirq.GateOperation'],
repetitions: int = 1,
seed: 'cirq.RANDOM_STATE_OR_SEED_LIKE' = None,
*,
_allow_repeated=False
) -> Dict[str, np.ndarray]
Samples from the system at this point in the computation.
Note that this does not collapse the state vector.
In contrast to sample
which samples qubits, this takes a list of
cirq.GateOperation
instances whose gates are cirq.MeasurementGate
instances and then returns a mapping from the key in the measurement
gate to the resulting bit strings. Different measurement operations must
not act on the same qubits.
Args | |
---|---|
measurement_ops
|
GateOperation instances whose gates are
MeasurementGate instances to be sampled form.
|
repetitions
|
The number of samples to take. |
seed
|
A seed for the pseudorandom number generator. |
_allow_repeated
|
If True, adds extra dimension to the result, corresponding to the number of times a key is repeated. |
Returns: A dictionary from measurement gate key to measurement results. Measurement results are stored in a 2-dimensional numpy array, the first dimension corresponding to the repetition and the second to the actual boolean measurement results (ordered by the qubits being measured.)
Raises | |
---|---|
ValueError
|
If the operation's gates are not MeasurementGate
instances or a qubit is acted upon multiple times by different
operations from measurement_ops .
|