Z2Symmetries#
- class qiskit.quantum_info.Z2Symmetries(symmetries, sq_paulis, sq_list, tapering_values=None, *, tol=1e-14)[ソース]#
ベースクラス:
object
The $Z_2$ symmetry converter identifies symmetries from the problem hamiltonian and uses them to provide a tapered - more efficient - representation of operators as Paulis for this problem. For each identified symmetry, one qubit can be eliminated in the Pauli representation at the cost of having to test two symmetry sectors (for the two possible eigenvalues - tapering values - of the symmetry). In certain problems such as the finding of the main operator’s ground state, one can a priori identify the symmetry sector of the solution and thus effectively reduce the computational overhead.
The following attributes can be read and updated once the
Z2Symmetries
object has been constructed.参照
- [1]: Bravyi, S., et al, 「Tapering off qubits to simulate fermionic Hamiltonians」
- パラメータ:
symmetries (Iterable[Pauli]) – Object representing the list of $Z_2$ symmetries. These correspond to the generators of the symmetry group $langle tau_1, tau_2dots rangle>$.
sq_paulis (Iterable[Pauli]) – Object representing the list of single-qubit Pauli $sigma^x_{q(i)}$ anti-commuting with the symmetry $tau_i$ and commuting with all the other symmetries $tau_{jneq i}$. These operators are used to construct the unitary Clifford operators.
sq_list (Iterable[int]) – The list of indices $q(i)$ of the single-qubit Pauli operators used to build the Clifford operators.
tapering_values (Iterable[int] | None) – List of eigenvalues determining the symmetry sector for each symmetry.
tol (float) – Tolerance threshold for ignoring real and complex parts of a coefficient.
- 例外:
QiskitError – Invalid paulis. The lists of symmetries, single-qubit paulis support paulis and tapering values must be of equal length. This length is the number of applied symmetries and translates directly to the number of eliminated qubits.
Attributes
- cliffords#
Get clifford operators, built based on symmetries and single-qubit X.
- 戻り値:
A list of unitaries used to diagonalize the Hamiltonian.
- settings#
Return operator settings.
- sq_list#
Return sq list.
- sq_paulis#
Return sq paulis.
- symmetries#
Return symmetries.
Methods
- convert_clifford(operator)[ソース]#
This method operates the first part of the tapering. It converts the operator by composing it with the clifford unitaries defined in the current symmetry.
- パラメータ:
operator (SparsePauliOp) – The to-be-tapered operator.
- 戻り値:
SparsePauliOp
corresponding to the converted operator.- 戻り値の型:
- classmethod find_z2_symmetries(operator)[ソース]#
Finds Z2 Pauli-type symmetries of a
SparsePauliOp
.- 戻り値:
A
Z2Symmetries
instance.- 戻り値の型:
- taper(operator)[ソース]#
Taper an operator based on the z2_symmetries info and sector defined by tapering_values. Returns operator if the symmetry object is empty.
The tapering is a two-step algorithm which first converts the operator into a
SparsePauliOp
with same eigenvalues but where some qubits are only acted upon with the Pauli operators I or X. The number M of these redundant qubits is equal to the number M of identified symmetries.The second step of the reduction consists in replacing these qubits with the possible eigenvalues of the corresponding Pauli X, giving 2^M new operators with M less qubits. If an eigenvalue sector was previously identified for the solution, then this reduces to 1 new operator with M less qubits.
- パラメータ:
operator (SparsePauliOp) – The to-be-tapered operator.
- 戻り値:
[
SparsePauliOp
]; otherwise,SparsePauliOp
.- 戻り値の型:
If tapering_values is None
- taper_clifford(operator)[ソース]#
Operate the second part of the tapering. This function assumes that the input operators have already been transformed using
convert_clifford()
. The redundant qubits due to the symmetries are dropped and replaced by their two possible eigenvalues.- パラメータ:
operator (SparsePauliOp) – Partially tapered operator resulting from a call to
convert_clifford()
.- 戻り値:
[
SparsePauliOp
]; otherwise,SparsePauliOp
.- 戻り値の型:
If tapering_values is None