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This research establishes the exact minimum statistical cost for learning many-body correlations using classical shadows with entangling measurements, proving optimality over both Clifford and general unitary groups for small system sizes. The findings refine theoretical bounds on measurement efficiency, confirming that specific Pauli rotation circuits achieve the asymptotic optimum previously conjectured by Wu et al. These results provide a rigorous foundation for optimizing quantum sensing and tomography protocols in near-term devices.
Exact Clifford Optimality for Two-Sided Locally Randomized Classical Shadows
arXiv:2610.04621v1 Announce Type: new Abstract: Entangling measurements can reduce the statistical cost of learning many-body correlations. We study Pauli strings with full support on a specified $k$-qubit region using classical shadows with two independent, uniformly random product single-qubit Clifford layers around a controllable unitary acting on that region, followed by computational-basis readout. In this architecture, we prove that a circuit $U_*$ of two collective Pauli rotations attains the exact minimum squared shadow norm over all Clifford choices of the controllable unitary for every $k\geq1$, namely $C_k^{\rm opt}=4\cdot 9^k/(3\cdot 5^k+3^k-6)$ for odd $k$ and $C_k^{\rm opt}=4\cdot 9^k/(3\cdot 5^k-3^k+2)$ for even $k$. The asymptotic optimum $(4/3)\cdot(9/5)^k$ establishes Wu et al.'s exponential base as optimal and improves their prefactor from $2$ to $4/3$. For $1\leq k\leq6$, exact rational certificates prove that the same optimum holds over the entire unitary group $\mathrm U(2^k)$, including all non-Clifford unitaries, within the same measurement architecture. These finite-size results motivate the conjecture that $U_*$ is optimal over all unitaries for arbitrary $k$ within this architecture.
Abstract:Entangling measurements can reduce the statistical cost of learning many-body correlations. We study Pauli strings with full support on a specified $k$-qubit region using classical shadows with two independent, uniformly random product single-qubit Clifford layers around a controllable unitary acting on that region, followed by computational-basis readout. In this architecture, we prove that a circuit $U_*$ of two collective Pauli rotations attains the exact minimum squared shadow norm over all Clifford choices of the controllable unitary for every $k\geq1$, namely $C_k^{\rm opt}=4\cdot 9^k/(3\cdot 5^k+3^k-6)$ for odd $k$ and $C_k^{\rm opt}=4\cdot 9^k/(3\cdot 5^k-3^k+2)$ for even $k$. The asymptotic optimum $(4/3)\cdot(9/5)^k$ establishes Wu et al.'s exponential base as optimal and improves their prefactor from $2$ to $4/3$. For $1\leq k\leq6$, exact rational certificates prove that the same optimum holds over the entire unitary group $\mathrm U(2^k)$, including all non-Clifford unitaries, within the same measurement architecture. These finite-size results motivate the conjecture that $U_*$ is optimal over all unitaries for arbitrary $k$ within this architecture.
arXiv:2610.04621 [quant-ph]
(or arXiv:2610.04621v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2610.04621 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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