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A Simple and Efficient Joint Measurement Strategy for Estimating Fermionic Observables and Hamiltonians

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arxiv 2402.19230 v3 pith:FFXQTGQW submitted 2024-02-29 quant-ph math-phmath.MP

classification quant-phmath-phmath.MP
keywords fermionicmathcalmeasurementclassicalepsilonhamiltoniansmajoranascheme
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abstract

We propose a simple scheme to estimate fermionic observables and Hamiltonians relevant in quantum chemistry and correlated fermionic systems. Our approach is based on implementing a measurement that jointly measures noisy versions of any product of two or four Majorana operators in an $N$ mode fermionic system. To realize our measurement we use: (i) a randomization over a set of unitaries that realize products of Majorana fermion operators; (ii) a unitary, sampled at random from a constant-size set of suitably chosen fermionic Gaussian unitaries; (iii) a measurement of fermionic occupation numbers; (iv) suitable post-processing. Our scheme can estimate expectation values of all quadratic and quartic Majorana monomials to $\epsilon$ precision using $\mathcal{O}(N \log(N)/\epsilon^2)$ and $\mathcal{O}(N^2 \log(N)/\epsilon^2)$ measurement rounds respectively, matching the performance offered by fermionic classical shadows. In certain settings, such as a rectangular lattice of qubits which encode an $N$ mode fermionic system via the Jordan-Wigner transformation, our scheme can be implemented in circuit depth $\mathcal{O}(N^{1/2})$ with $\mathcal{O}(N^{3/2})$ two-qubit gates, offering an improvement over fermionic and matchgate classical shadows that require depth $\mathcal{O}(N)$ and $\mathcal{O}(N^2)$ two-qubit gates. By benchmarking our method on exemplary molecular Hamiltonians and observing performances comparable to fermionic classical shadows, we demonstrate a novel, competitive alternative to existing strategies.

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  1. Pretty-good simulation of all quantum measurements by projective measurements

    quant-ph 2025-01 accept novelty 8.0 of 10

    Every POVM on C^d becomes projectively simulable after depolarizing with dimension-independent visibility c = 0.02, and can be simulated with postselection probability 1/8 using only a single auxiliary qubit.

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