qml.import_operator¶
-
import_operator
(qubit_observable, format='openfermion', wires=None, tol=10000000000.0)[source]¶ Convert an external operator to a PennyLane operator.
We currently support OpenFermion operators: the function accepts most types of OpenFermion qubit operators, such as those corresponding to Pauli words and sums of Pauli words.
- Parameters
qubit_observable – external qubit operator that will be converted
format (str) – the format of the operator object to convert from
wires (Wires, list, tuple, dict) – Custom wire mapping used to convert the external qubit operator to a PennyLane operator. For types
Wires
/list/tuple, each item in the iterable represents a wire label for the corresponding qubit index. For type dict, only int-keyed dictionaries (for qubit-to-wire conversion) are accepted. IfNone
, the identity map (e.g.,0->0, 1->1, ...
) will be used.tol (float) – Tolerance in machine epsilon for the imaginary part of the coefficients in
qubit_observable
. Coefficients with imaginary part less than \((2.22 \cdot 10^{-16}) \cdot \text{tol}\) are considered to be real.
- Returns
PennyLane operator representing any operator expressed as linear combinations of Pauli words, e.g., \(\sum_{k=0}^{N-1} c_k O_k\)
- Return type
(Operator)
Example
>>> assert qml.operation.active_new_opmath() == True >>> h_pl = import_operator(h_of, format='openfermion') >>> print(h_pl) (-0.0548 * X(0 @ X(1) @ Y(2) @ Y(3))) + (0.14297 * Z(0 @ Z(1)))
If the new op-math is deactivated, a
Hamiltonian
is returned instead.>>> assert qml.operation.active_new_opmath() == False >>> from openfermion import QubitOperator >>> h_of = QubitOperator('X0 X1 Y2 Y3', -0.0548) + QubitOperator('Z0 Z1', 0.14297) >>> h_pl = import_operator(h_of, format='openfermion') >>> print(h_pl) (0.14297) [Z0 Z1] + (-0.0548) [X0 X1 Y2 Y3]