Source code for pennylane.labs.estimator_beta.ops.qubit.non_parametric_ops

# Copyright 2026 Xanadu Quantum Technologies Inc.

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r"""Resource operators for non parametric single qubit operations."""

import pennylane.labs.estimator_beta as qre
from pennylane.estimator.resource_operator import GateCount, resource_rep

# pylint: disable=arguments-differ, unused-argument


[docs] def hadamard_controlled_resource_decomp( num_ctrl_wires: int, num_zero_ctrl: int, target_resource_params: dict | None = None, ) -> list[GateCount | qre.Allocate | qre.Deallocate]: r"""Returns a list representing the resources for a controlled version of the :class:`~.pennylane.estimator.ops.qubit.non_parametric_ops.Hadamard` operator. Args: num_ctrl_wires (int): the number of qubits the operation is controlled on num_zero_ctrl (int): the number of control qubits, that are controlled when in the :math:`|0\rangle` state target_resource_params (dict | None): A dictionary containing the resource parameters of the target operator. Resources: For a single control wire, the cost is a single instance of ``CH``. Two additional ``X`` gates are used to flip the control qubit if it is zero-controlled. In the case where multiple controlled wires are provided, the resources are derived from the following identities: .. math:: \begin{align} \hat{H} &= \hat{R}_{y}(\frac{\pi}{4}) \cdot \hat{Z} \cdot \hat{R}_{y}(\frac{-\pi}{4}), \\ \hat{Z} &= \hat{H} \cdot \hat{X} \cdot \hat{H}. \end{align} Specifically, the resources are given by two ``RY`` gates, two ``Hadamard`` gates and a ``X`` gate. By replacing the ``X`` gate with ``MultiControlledX`` gate, we obtain a controlled-version of this identity. Decomposing the :math:`\hat{R}_y(\pm\frac{\pi}{4})` rotations into the Clifford+T basis and substituting yields: .. math:: \begin{align} \hat{H} &= (S H T H S^\dagger) \cdot \hat{Z} \cdot (S H T^\dagger H S^\dagger) \\ &= S H T \cdot (\hat{H} \hat{Z} \hat{H}) \cdot T^\dagger H S^\dagger \\ &= S H T \cdot \hat{X} \cdot T^\dagger H S^\dagger \end{align} The final resources are: 2 ``Hadamard``, 1 ``T``, 1 ``Adjoint(T)``, 1 ``S``, 1 ``Adjoint(S)``, and 1 ``MultiControlledX`` controlled on ``num_ctrl_wires``. Returns: list[:class:`~.estimator.resource_operator.GateCount`]: A list of ``GateCount`` objects, where each object represents a specific quantum gate and the number of times it appears in the decomposition. """ if num_ctrl_wires == 1: gate_lst = [GateCount(resource_rep(qre.CH))] if num_zero_ctrl: gate_lst.append(GateCount(resource_rep(qre.X), 2)) return gate_lst gate_lst = [] h = resource_rep(qre.Hadamard) mcx = resource_rep( qre.MultiControlledX, { "num_ctrl_wires": num_ctrl_wires, "num_zero_ctrl": num_zero_ctrl, }, ) gate_lst.append(qre.Allocate(1)) gate_lst.append(GateCount(h, 2)) gate_lst.append(GateCount(resource_rep(qre.T), 1)) gate_lst.append(GateCount(resource_rep(qre.Adjoint, {"base_cmpr_op": resource_rep(qre.T)}), 1)) gate_lst.append(GateCount(resource_rep(qre.S), 1)) gate_lst.append(GateCount(resource_rep(qre.Adjoint, {"base_cmpr_op": resource_rep(qre.S)}), 1)) gate_lst.append(GateCount(mcx, 2)) gate_lst.append(qre.Deallocate(1)) return gate_lst
[docs] def hadamard_toffoli_based_controlled_decomp( num_ctrl_wires: int, num_zero_ctrl: int, target_resource_params: dict | None = None, ) -> list[GateCount | qre.Allocate | qre.Deallocate]: r"""Returns a list representing the resources for a controlled version of the :class:`~.pennylane.estimator.ops.qubit.non_parametric_ops.Hadamard` operator. .. note:: This operation assumes a `catalytic T state <https://pennylane.ai/qml/demos/tutorial_magic_state_distillation>`_ is available. Users should ensure the cost of constructing such a state has been accounted for. Args: num_ctrl_wires (int): the number of qubits the operation is controlled on num_zero_ctrl (int): the number of control qubits, that are controlled when in the :math:`|0\rangle` state target_resource_params (dict | None): A dictionary containing the resource parameters of the target operator. Resources: The resources are derived from Figure 17 in `arXiv:2011.03494 <https://arxiv.org/pdf/2011.03494>`_. Returns: list[:class:`~.estimator.resource_operator.GateCount`]: A list of ``GateCount`` objects, where each object represents a specific quantum gate and the number of times it appears in the decomposition. """ gate_lst = [] if num_ctrl_wires > 1: gate_lst.append(qre.Allocate(1)) gate_lst.append(qre.Allocate(1)) h = resource_rep(qre.Hadamard) mcx = resource_rep( qre.MultiControlledX, { "num_ctrl_wires": num_ctrl_wires, "num_zero_ctrl": num_zero_ctrl, }, ) gate_lst.append(GateCount(h, 5)) gate_lst.append(GateCount(resource_rep(qre.S), 2)) gate_lst.append(GateCount(resource_rep(qre.Adjoint, {"base_cmpr_op": resource_rep(qre.S)}), 1)) gate_lst.append(GateCount(resource_rep(qre.Toffoli), 1)) gate_lst.append(GateCount(resource_rep(qre.CNOT), 5)) gate_lst.append(GateCount(resource_rep(qre.CZ), 1)) gate_lst.append(GateCount(resource_rep(qre.X), 4)) if num_ctrl_wires > 1: gate_lst.append(GateCount(mcx, 2)) gate_lst.append(qre.Deallocate(1)) gate_lst.append(qre.Deallocate(1)) return gate_lst