LinearPauliRotations#
- class qiskit.circuit.library.LinearPauliRotations(num_state_qubits=None, slope=1, offset=0, basis='Y', name='LinRot')[ソース]#
ベースクラス:
FunctionalPauliRotations
Linearly-controlled X, Y or Z rotation.
For a register of state qubits \(|x\rangle\), a target qubit \(|0\rangle\) and the basis
'Y'
this circuit acts as:q_0: ─────────────────────────■───────── ... ────────────────────── │ . │ q_(n-1): ─────────────────────────┼───────── ... ───────────■────────── ┌────────────┐ ┌───────┴───────┐ ┌─────────┴─────────┐ q_n: ─┤ RY(offset) ├──┤ RY(2^0 slope) ├ ... ┤ RY(2^(n-1) slope) ├ └────────────┘ └───────────────┘ └───────────────────┘
This can for example be used to approximate linear functions, with \(a =\)
slope
\(/2\) and \(b =\)offset
\(/2\) and the basis'Y'
:\[|x\rangle |0\rangle \mapsto \cos(ax + b)|x\rangle|0\rangle + \sin(ax + b)|x\rangle |1\rangle\]Since for small arguments \(\sin(x) \approx x\) this operator can be used to approximate linear functions.
Create a new linear rotation circuit.
- パラメータ:
num_state_qubits (int | None) – The number of qubits representing the state \(|x\rangle\).
slope (float) – The slope of the controlled rotation.
offset (float) – The offset of the controlled rotation.
basis (str) – The type of Pauli rotation (『X』, 『Y』, 『Z』).
name (str) – The name of the circuit object.
Attributes
- ancillas#
Returns a list of ancilla bits in the order that the registers were added.
- basis#
The kind of Pauli rotation to be used.
Set the basis to 『X』, 『Y』 or 『Z』 for controlled-X, -Y, or -Z rotations respectively.
- 戻り値:
The kind of Pauli rotation used in controlled rotation.
- calibrations#
Return calibration dictionary.
The custom pulse definition of a given gate is of the form
{'gate_name': {(qubits, params): schedule}}
- clbits#
Returns a list of classical bits in the order that the registers were added.
- data#
- extension_lib = 'include "qelib1.inc";'#
- global_phase#
Return the global phase of the circuit in radians.
- header = 'OPENQASM 2.0;'#
- instances = 187#
- layout#
Return any associated layout information about the circuit
This attribute contains an optional
TranspileLayout
object. This is typically set on the output fromtranspile()
orPassManager.run()
to retain information about the permutations caused on the input circuit by transpilation.There are two types of permutations caused by the
transpile()
function, an initial layout which permutes the qubits based on the selected physical qubits on theTarget
, and a final layout which is an output permutation caused bySwapGate
s inserted during routing.
- metadata#
The user provided metadata associated with the circuit.
The metadata for the circuit is a user provided
dict
of metadata for the circuit. It will not be used to influence the execution or operation of the circuit, but it is expected to be passed between all transforms of the circuit (ie transpilation) and that providers will associate any circuit metadata with the results it returns from execution of that circuit.
- num_ancilla_qubits#
The minimum number of ancilla qubits in the circuit.
- 戻り値:
The minimal number of ancillas required.
- num_ancillas#
Return the number of ancilla qubits.
- num_clbits#
Return number of classical bits.
- num_parameters#
- num_qubits#
Return number of qubits.
- num_state_qubits#
The number of state qubits representing the state \(|x\rangle\).
- 戻り値:
The number of state qubits.
- offset#
The angle of the single qubit offset rotation on the target qubit.
Before applying the controlled rotations, a single rotation of angle
offset
is applied to the target qubit.- 戻り値:
The offset angle.
- op_start_times#
Return a list of operation start times.
This attribute is enabled once one of scheduling analysis passes runs on the quantum circuit.
- 戻り値:
List of integers representing instruction start times. The index corresponds to the index of instruction in
QuantumCircuit.data
.- 例外:
AttributeError – When circuit is not scheduled.
- parameters#
- prefix = 'circuit'#
- qregs: list[QuantumRegister]#
A list of the quantum registers associated with the circuit.
- qubits#
Returns a list of quantum bits in the order that the registers were added.
- slope#
The multiplicative factor in the rotation angle of the controlled rotations.
The rotation angles are
slope * 2^0
,slope * 2^1
, … ,slope * 2^(n-1)
wheren
is the number of state qubits.- 戻り値:
The rotation angle common in all controlled rotations.