MultiQubitFrame¶
- class MultiQubitFrame(list_operators: list[Operator])[source]¶
-
Class that collects all information that any frame of multiple qubits should specify.
This is a representation of an operator-valued vector space frame. The effects are specified as a list of
Operator
.Note
This is a base class which collects functionality common to various subclasses. As an end-user you would not use this class directly. Check out
povm_toolbox.quantum_info
for more general information.Initialize from explicit operators.
- Parameters:
list_operators (list[Operator]) – list that contains the explicit frame operators. The length of the list is the number of operators of the frame.
- Raises:
ValueError – if the frame operators do not have a correct shape. They should all be hermitian and of the same dimension.
Attributes
- dimension¶
The dimension of the Hilbert space on which the effects act.
- informationally_complete¶
If the frame spans the entire Hilbert space.
- num_operators¶
The number of effects of the frame.
- operators¶
Return the list of frame operators.
- pauli_operators¶
Convert the internal frame operators to Pauli form.
Warning
The conversion to Pauli form can be computationally intensive.
- Returns:
The frame operators in Pauli form. Each frame operator is returned as a dictionary mapping Pauli labels to coefficients.
- Raises:
QiskitError – when the frame operators could not be converted to Pauli form (e.g. when they are not N-qubit operators).
Inherited Attributes
- num_subsystems¶
The number of subsystems which the frame operators act on.
For qubits, this is always \(\log_2(\)
dimension
\()\).
Methods
- analysis(hermitian_op: SparsePauliOp | Operator, frame_op_idx: int | set[int] | None = None) float | dict[int, float] | ndarray [source]¶
Return the frame coefficients of
hermitian_op
.This method implements the analysis operator \(A\) of the frame \(\{F_k\}_k\):
\[A: \mathcal{O} \mapsto \{ \mathrm{Tr}\left[F_k \mathcal{O} \right] \}_k,\]where \(c_k = \mathrm{Tr}\left[F_k \mathcal{O} \right]\) are called the frame coefficients of the Hermitian operator \(\mathcal{O}\).
- Parameters:
hermitian_op (SparsePauliOp | Operator) – a hermitian operator whose frame coefficients to compute.
frame_op_idx (int | set[int] | None) – label or set of labels indicating which coefficients are queried. If
None
, all coefficients are queried.
- Returns:
Frame coefficients, specified by
frame_op_idx
, of the Hermitian operatorhermitian_op
. If a specific coefficient was queried, afloat
is returned. If a specific set of coefficients was queried, a dictionary mapping labels to coefficients is returned. If all coefficients were queried, an array with all coefficients is returned.- Raises:
TypeError – when the provided single or sequence of labels
frame_op_idx
does not have a valid type.ValueError – when the dimension of the provided
hermitian_op
does not match the dimension of the frame operators.
- Return type:
- classmethod from_vectors(frame_vectors: ndarray) Self [source]¶
Initialize a frame from non-normalized bloch vectors.
The non-normalized Bloch vectors are given by \(|\tilde{\psi}_k \rangle = \sqrt{\gamma_k} |\psi_k \rangle\). The resulting frame operators are \(F_k = \gamma_k |\psi_k \rangle \langle \psi_k |\) where \(\gamma_k\) is the trace of the \(k\)’th frame operator.
- Parameters:
frame_vectors (ndarray) – list of vectors \(|\tilde{\psi_k} \rangle\). The length of the list corresponds to the number of operators of the frame. Each vector is of shape \((\mathrm{dim},)\) where \(\mathrm{dim}\) is the
dimension
of the Hilbert space on which the frame acts.- Returns:
The frame corresponding to the vectors.
- Return type:
Self