# qiskit.chemistry.transformations.FermionicTransformation¶

class FermionicTransformation(transformation=<FermionicTransformationType.FULL: 'full'>, qubit_mapping=<FermionicQubitMappingType.PARITY: 'parity'>, two_qubit_reduction=True, freeze_core=False, orbital_reduction=None, z2symmetry_reduction=None)[Quellcode]

A transformation from a fermionic problem, represented by a driver, to a qubit operator.

Parameter
• transformation (FermionicTransformationType) – full or particle_hole

• qubit_mapping (FermionicQubitMappingType) – ‚jordan_wigner‘, ‚parity‘ or ‚bravyi_kitaev‘

• two_qubit_reduction (bool) – Whether two qubit reduction should be used, when parity mapping only

• freeze_core (bool) – Whether to freeze core orbitals when possible

• orbital_reduction (Optional[List[int]]) – Orbital list to be frozen or removed

• z2symmetry_reduction (Union[str, List[int], None]) – If z2 symmetry reduction should be applied to resulting qubit operators that are computed. For each symmetry detected the operator will be split in two where each requires one qubit less for computation. So for example 3 symmetries will split in the original operator into 8 new operators each requiring 3 less qubits. Now only one of these operators will have the ground state and be the correct symmetry sector needed for the ground state. Setting ‚auto‘ will use an automatic computation of the correct sector. If from other experiments, with the z2symmetry logic, the sector is known, then the tapering values of that sector can be provided (a list of int of values -1, and 1). The default is None meaning no symmetry reduction is done. Note that dipole and other operators such as spin, num particles etc are also symmetry reduced according to the symmetries found in the main operator if this operator commutes with the main operator symmetry. If it does not then the operator will be discarded since no meaningful measurement can take place.

Verursacht

QiskitChemistryError – Invalid symmetry reduction

__init__(transformation=<FermionicTransformationType.FULL: 'full'>, qubit_mapping=<FermionicQubitMappingType.PARITY: 'parity'>, two_qubit_reduction=True, freeze_core=False, orbital_reduction=None, z2symmetry_reduction=None)[Quellcode]
Parameter
• transformation (FermionicTransformationType) – full or particle_hole

• qubit_mapping (FermionicQubitMappingType) – ‚jordan_wigner‘, ‚parity‘ or ‚bravyi_kitaev‘

• two_qubit_reduction (bool) – Whether two qubit reduction should be used, when parity mapping only

• freeze_core (bool) – Whether to freeze core orbitals when possible

• orbital_reduction (Optional[List[int]]) – Orbital list to be frozen or removed

• z2symmetry_reduction (Union[str, List[int], None]) – If z2 symmetry reduction should be applied to resulting qubit operators that are computed. For each symmetry detected the operator will be split in two where each requires one qubit less for computation. So for example 3 symmetries will split in the original operator into 8 new operators each requiring 3 less qubits. Now only one of these operators will have the ground state and be the correct symmetry sector needed for the ground state. Setting ‚auto‘ will use an automatic computation of the correct sector. If from other experiments, with the z2symmetry logic, the sector is known, then the tapering values of that sector can be provided (a list of int of values -1, and 1). The default is None meaning no symmetry reduction is done. Note that dipole and other operators such as spin, num particles etc are also symmetry reduced according to the symmetries found in the main operator if this operator commutes with the main operator symmetry. If it does not then the operator will be discarded since no meaningful measurement can take place.

Verursacht

QiskitChemistryError – Invalid symmetry reduction

Methods

 __init__([transformation, qubit_mapping, …]) type transformation FermionicTransformationType build_hopping_operators([excitations]) Builds the product of raising and lowering operators (basic excitation operators) Returns a default filter criterion method to filter the eigenvalues computed by the eigen solver. interpret(raw_result) Interprets an EigenstateResult in the context of this transformation. transform(driver[, aux_operators]) Transformation from the driver to a qubit operator.

Attributes

 commutation_rule Getter of the commutation rule molecule_info Getter of the molecule information. qubit_mapping Getter of the qubit mapping. untapered_qubit_op Getter for the untapered qubit operator
build_hopping_operators(excitations='sd')[Quellcode]

Builds the product of raising and lowering operators (basic excitation operators)

Parameter

excitations (Union[str, List[List[int]]]) – The excitations to be included in the eom pseudo-eigenvalue problem. If a string (‚s‘, ‚d‘ or ‚sd‘) then all excitations of the given type will be used. Otherwise a list of custom excitations can directly be provided.

Rückgabetyp

Tuple[Dict[str, WeightedPauliOperator], Dict[str, List[bool]], Dict[str, List[Any]]]

Rückgabe

A tuple containing the hopping operators, the types of commutativities and the excitation indices.

property commutation_rule

Getter of the commutation rule

Rückgabetyp

bool

get_default_filter_criterion()[Quellcode]

In the fermionic case the default filter ensures that the number of particles is being preserved.

Rückgabetyp

Optional[Callable[[Union[List, ndarray], float, Optional[List[float]]], bool]]

interpret(raw_result)[Quellcode]

Interprets an EigenstateResult in the context of this transformation.

Parameter

raw_result (Union[EigenstateResult, EigensolverResult, MinimumEigensolverResult]) – an eigenstate result object.

Rückgabetyp

ElectronicStructureResult

Rückgabe

An electronic structure result.

property molecule_info

Getter of the molecule information.

Rückgabetyp

Dict[str, Any]

property qubit_mapping

Getter of the qubit mapping.

Rückgabetyp

str

transform(driver, aux_operators=None)[Quellcode]

Transformation from the driver to a qubit operator.

Parameter
• driver (BaseDriver) – A driver encoding the molecule information.

• aux_operators (Optional[List[FermionicOperator]]) – Additional auxiliary FermionicOperator instances to evaluate.

Rückgabetyp

Tuple[OperatorBase, List[OperatorBase]]

Rückgabe

A qubit operator and a dictionary of auxiliary operators.

property untapered_qubit_op

Getter for the untapered qubit operator