Linear Combination Of Unitaries

Functions:

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lcu

lcu(
coefficients: list[float],
unitaries: QCallableList,
block: QNum[Literal[‘max(ceiling(log(coefficients.len, 2)), 1)’]]
) -> None

[Qmod Classiq-library function] Implements a general linear combination of unitaries (LCU) procedure. The algorithm prepares a superposition over the unitaries according to the given coefficients, and then conditionally applies each unitary controlled by the block. The operation is of the form: $\sum_j \alpha_j U_j$ where $U_j$ is a unitary operation applied to data. Parameters:

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lcu_pauli

lcu_pauli(
operator: SparsePauliOp,
data: QArray[QBit, Literal[‘operator.num_qubits’]],
block: QNum[Literal[‘max(ceiling(log(operator.terms.len, 2)), 1)’]]
) -> None

[Qmod Classiq-library function] Applies a linear combination of unitaries (LCU) where each unitary is a Pauli term, represented as a tensor product of Pauli operators. The function prepares a superposition over the unitaries according to the given magnitudes and phases, and applies the corresponding Pauli operators conditionally. This is useful for implementing Hamiltonian terms of the form: $H=\sum_j \alpha_j P_j$ where $P_j$ is a tensor product of Pauli operators. The SELECT operator (_select_paulis) loads each data qubit’s Pauli column from the block index using gray-code uniformly-controlled RZ/RY rotations; the resulting per-term phases are folded into the coefficients so that the single phase table inside prepare_select corrects them together with the coefficient signs/phases. Parameters:

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prepare_select

prepare_select(
coefficients: list[float],
select: QCallable[QNum],
block: QNum[Literal[‘max(ceiling(log(coefficients.len, 2)), 1)’]]
) -> None

[Qmod Classiq-library function] Applies the ‘Prepare-Select’ scheme used for Linear Combination of Unitaries (LCU). Compared to the lcu function, here the Select operator should be provided directly, allowing to take advantage of some structure for the unitaries of the LCU. The select operator is defined by: $\mathrm\{SELECT\} = \sum_\{j=0\}^\{m-1\} |j\rangle\!\langle j|_\{block\} \otimes U_j$. Parameters: