PiecewisePolynomialPauliRotations¶
- class PiecewisePolynomialPauliRotations(num_state_qubits=None, breakpoints=None, coeffs=None, basis='Y', name='pw_poly')[código fonte]¶
Bases:
FunctionalPauliRotations
Piecewise-polynomially-controlled Pauli rotations.
This class implements a piecewise polynomial (not necessarily continuous) function, \(f(x)\), on qubit amplitudes, which is defined through breakpoints and coefficients as follows. Suppose the breakpoints \((x_0, ..., x_J)\) are a subset of \([0, 2^n-1]\), where \(n\) is the number of state qubits. Further on, denote the corresponding coefficients by \([a_{j,1},...,a_{j,d}]\), where \(d\) is the highest degree among all polynomials.
Then \(f(x)\) is defined as:
\[\begin{split}f(x) = \begin{cases} 0, x < x_0 \\ \sum_{i=0}^{i=d}a_{j,i}/2 x^i, x_j \leq x < x_{j+1} \end{cases}\end{split}\]where if given the same number of breakpoints as polynomials, we implicitly assume \(x_{J+1} = 2^n\).
Nota
Note the \(1/2\) factor in the coefficients of \(f(x)\), this is consistent with Qiskit’s Pauli rotations.
Examples
>>> from qiskit import QuantumCircuit >>> from qiskit.circuit.library.arithmetic.piecewise_polynomial_pauli_rotations import\ ... PiecewisePolynomialPauliRotations >>> qubits, breakpoints, coeffs = (2, [0, 2], [[0, -1.2],[-1, 1, 3]]) >>> poly_r = PiecewisePolynomialPauliRotations(num_state_qubits=qubits, ...breakpoints=breakpoints, coeffs=coeffs) >>> >>> qc = QuantumCircuit(poly_r.num_qubits) >>> qc.h(list(range(qubits))); >>> qc.append(poly_r.to_instruction(), list(range(qc.num_qubits))); >>> qc.draw() ┌───┐┌──────────┐ q_0: ┤ H ├┤0 ├ ├───┤│ │ q_1: ┤ H ├┤1 ├ └───┘│ │ q_2: ─────┤2 ├ │ pw_poly │ q_3: ─────┤3 ├ │ │ q_4: ─────┤4 ├ │ │ q_5: ─────┤5 ├ └──────────┘
References
- [1]: Haener, T., Roetteler, M., & Svore, K. M. (2018).
Optimizing Quantum Circuits for Arithmetic. arXiv:1805.12445
- [2]: Carrera Vazquez, A., Hiptmair, R., & Woerner, S. (2022).
Enhancing the Quantum Linear Systems Algorithm using Richardson Extrapolation. ACM Transactions on Quantum Computing 3, 1, Article 2
- Parâmetros
num_state_qubits (Optional[int]) – The number of qubits representing the state.
breakpoints (Optional[List[int]]) – The breakpoints to define the piecewise-linear function. Defaults to
[0]
.coeffs (Optional[List[List[float]]]) – The coefficients of the polynomials for different segments of the
x (piecewise-linear function. coeffs[j][i] is the coefficient of the i-th power of) –
polynomial. (for the j-th) – Defaults to linear:
[[1]]
.basis (str) – The type of Pauli rotation (
'X'
,'Y'
,'Z'
).name (str) – The name of the circuit.
Methods Defined Here
Classically evaluate the piecewise polynomial rotation.
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.
- Retorno
The kind of Pauli rotation used in controlled rotation.
- breakpoints¶
The breakpoints of the piecewise polynomial function.
The function is polynomial in the intervals
[point_i, point_{i+1}]
where the last point implicitly is2**(num_state_qubits + 1)
.- Retorno
The list of breakpoints.
- 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.
- coeffs¶
The coefficients of the polynomials.
- Retorno
The polynomial coefficients per interval as nested lists.
- contains_zero_breakpoint¶
Whether 0 is the first breakpoint.
- Retorno
True, if 0 is the first breakpoint, otherwise False.
- data¶
- extension_lib = 'include "qelib1.inc";'¶
- global_phase¶
Return the global phase of the circuit in radians.
- header = 'OPENQASM 2.0;'¶
- instances = 315¶
- layout¶
Return any associated layout information anout 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.
- mapped_coeffs¶
The coefficients mapped to the internal representation, since we only compare x>=breakpoint.
- Retorno
The mapped coefficients.
- 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.
- Retorno
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 \(|x\rangle\).
- Retorno
The number of state qubits.
- 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.
- Retorno
List of integers representing instruction start times. The index corresponds to the index of instruction in
QuantumCircuit.data
.- Levanta
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.