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stateQIP = statePSPACE

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arxiv 2301.07730 v2 pith:NWEK4MT2 submitted 2023-01-18 quant-ph cs.CC

classification quant-phcs.CC
keywords quantumcomplexitystatepspacestateqipstatetechniquesclassclasses
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Complexity theory traditionally studies the hardness of solving classical computational problems. In the quantum setting, it is also natural to consider a different notion of complexity, namely the complexity of physically preparing a certain quantum state. We study the relation between two such state complexity classes: statePSPACE, which contains states that can be generated by space-uniform polynomial-space quantum circuits, and stateQIP, which contains states that a polynomial-time quantum verifier can generate by interacting with an all-powerful untrusted quantum prover. The latter class was recently introduced by Rosenthal and Yuen (ITCS 2022), who proved that statePSPACE $\subseteq$ stateQIP. Our main result is the reverse inclusion, stateQIP $\subseteq$ statePSPACE, thereby establishing equality of the two classes and providing a natural state-complexity analogue to the celebrated QIP = PSPACE theorem of Jain, et al. (J. ACM 2011). To prove this, we develop a polynomial-space quantum algorithm for solving a large class of exponentially large "PSPACE-computable" semidefinite programs (SDPs), which also prepares an optimiser encoded in a quantum state. Our SDP solver relies on recent block-encoding techniques from quantum algorithms, demonstrating that these techniques are also useful for complexity theory. Using similar techniques, we also show that optimal prover strategies for general quantum interactive protocols can be implemented in quantum polynomial space. We prove this by studying an algorithmic version of Uhlmann's theorem and establishing an upper bound on the complexity of implementing Uhlmann transformations.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. The Keyl-Werner algorithm is not optimal for spectrum estimation

    quant-ph 2026-07 accept novelty 8.0 of 10

    Spectrum estimation of a d-dimensional quantum state is possible with o(d²) copies—specifically O(d² (log log d / log d)²)—beating Keyl–Werner and full tomography.

  2. Optimal fidelity estimation when one state is pure via algorithmic Uhlmann transform

    quant-ph 2026-08 accept novelty 6.0 of 10

    When at least one of two quantum states is pure, the Uhlmann fidelity can be estimated with Θ(1/ε) queries and Θ(1/ε²) samples without knowing which state is pure, matching the optimal lower bounds.

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