Particle-preserving fermionic shadows with mode-independent sample complexity
Abstract
We consider the problem of learning expectation values of particle-preserving operators with respect to an unknown $η$-particle $n$-mode fermionic state via classical shadows. Our main application is to estimating overlaps with arbitrary Slater determinant states: While it is known that such overlaps can, in the average case, be learnt to a fixed additive precision with a constant number of samples, the best-known worst case bound is $\mathcal{O}(\sqrt n \log n)$; here we improve this to $\mathc...
Description / Details
We consider the problem of learning expectation values of particle-preserving operators with respect to an unknown -particle -mode fermionic state via classical shadows. Our main application is to estimating overlaps with arbitrary Slater determinant states: While it is known that such overlaps can, in the average case, be learnt to a fixed additive precision with a constant number of samples, the best-known worst case bound is ; here we improve this to , achieving a mode-independent sample cost. Our procedure is also computationally efficient, requiring only classical post-processing which for a generic dense orbital runs in time . For the task of estimating the expectation value of a general particle-preserving quadratic fermionic observable , we prove a sample complexity bound of , where is the traceless component of ; the associated classical post-processing scales as . Finally, we discuss implementation of the required randomization: in a first-quantized encoding, approximate unitary designs give circuit depths polylogarithmic in the number of modes, contrasting with linear-depth requirements for nearest-neighbor second-quantized matchgate implementations. On the technical side, our proof reduces the extremal shadow variance to harmonic analysis on the AIII symmetric space and evaluates the resulting integral using techniques from the theories of Jacobi ensembles and orthogonal polynomials, in a calculation which may be of independent interest.
Source: arXiv:2606.27254v1 - http://arxiv.org/abs/2606.27254v1 PDF: https://arxiv.org/pdf/2606.27254v1 Original Link: http://arxiv.org/abs/2606.27254v1
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Jun 26, 2026
Quantum Computing
Quantum Physics
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