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arXiv:2509.01945

Quantum Statistical Witness Indistinguishability

Shafik Nassar, Ramachandran, Ronak

Published Sep 2, 2025• 0 citations
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Abstract

Statistical witness indistinguishability is a relaxation of statistical zero-knowledge which guarantees that the transcript of an interactive proof reveals no information about which valid witness the prover used to generate it. In this paper we define and initiate the study of QSWI, the class of problems with quantum statistically witness indistinguishable proofs. Using inherently quantum techniques from Kobayashi (TCC 2008), we prove that any problem with an honest-verifier quantum statistically witness indistinguishable proof has a 3-message public-coin malicious-verifier quantum statistically witness indistinguishable proof. There is no known analogue of this result for classical statistical witness indistinguishability. As a corollary, our result implies SWI is contained in QSWI. Additionally, we extend the work of Bitansky et al. (STOC 2023) to show that quantum batch proofs imply quantum statistically witness indistinguishable proofs with inverse-polynomial witness indistinguishability error.

DOI
10.48550/arxiv.2509.01945

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Statistical witness indistinguishability is a relaxation of statistical zero-knowledge which guarantees that the transcript of an interactive proof reveals no information about which valid witness the prover used to generate it. In this paper we define and initiate the study of QSWI, the class of problems with quantum statistically witness indistinguishable proofs. Using inherently quantum techniques from Kobayashi (TCC 2008), we prove that any problem with an honest-verifier quantum statistically witness indistinguishable proof has a 3-message public-coin malicious-verifier quantum statistically witness indistinguishable proof. There is no known analogue of this result for classical statistical witness indistinguishability. As a corollary, our result implies SWI is contained in QSWI. Additionally, we extend the work of Bitansky et al. (STOC 2023) to show that quantum batch proofs imply quantum statistically witness indistinguishable proofs with inverse-polynomial witness indistinguishability error.
In this paper we propose a definition for (honest verifier) quantum statistical zero-knowledge interactive proof systems and study the resulting complexity class, which we denote QSZK/sub HV/. We prove several facts regarding this class, including: the following problem is a complete promise problem for QSZKHV: given instructions for preparing two mixed quantum states, are the states close together or far apart in the trace norm metric? This problem is a quantum generalization of the complete promise problem of Sahai and Vadhan (1997) for (classical) statistical zero-knowledge; QSZK/sub HV/ is closed under complement; QSZK/sub HV//spl sube/PSPACE. (At present it is not known if arbitrary quantum interactive proof systems can be simulated in PSPACE even for one-round proof systems); any polynomial-round honest verifier quantum statistical zero-knowledge proof system can be simulated by a two-message (i.e., one-round) honest verifier quantum statistical zero-knowledge proof system. Similarly, any polynomial-round honest verifier quantum statistical zero-knowledge proof system can be simulated by a three-message public-coin honest verifier quantum statistical zero-knowledge proof system. These facts establish close connections between classical statistical zero-knowledge and our definition for quantum statistical zero-knowledge, and give some insight regarding the effect of this zero-knowledge restriction on quantum interactive proof systems. The relationship between our definition and possible definitions of general (i.e., not necessarily honest) quantum statistical zero-knowledge are also discussed.
Quantum information and computation provide a fascinating twist on the notion of proofs in computational complexity theory. For instance, one may consider a quantum computational analogue of the complexity class NP, known as QMA, in which a quantum state plays the role of a proof (also called a certificate or witness), and is checked by a polynomial-time quantum computation. For some problems, the fact that a quantum proof state could be a superposition over exponentially many classical states appears to offer computational advantages over classical proof strings. In the interactive proof system setting, one may consider a verifier and one or more provers that exchange and process quantum information rather than classical information during an interaction for a given input string, giving rise to quantum complexity classes such as QIP, QSZK, and QMIP* that represent natural quantum analogues of IP, SZK, and MIP. While quantum interactive proof systems inherit some properties from their classical counterparts, they also possess distinct and uniquely quantum features that lead to an interesting landscape of complexity classes based on variants of this model. In this survey we provide an overview of many of the known results concerning quantum proofs, computational models based on this concept, and properties of the complexity classes they define. In particular, we discuss non-interactive proofs and the complexity class QMA, single-prover quantum interactive proof systems and the complexity class QIP, statistical zero-knowledge quantum interactive proof systems and the complexity class QSZK, and multiprover interactive proof systems and the complexity classes QMIP, QMIP*, and MIP*.
Interactive proof systems with a laconic prover, studied by Goldreich, Vadhan, and Wigderson (CC, 2002), capture problems verifiable with logarithmic prover communication in the classical setting. For two-message quantum analogs, even a single-bit prover response contains quantum statistical zero-knowledge (QSZK\sf QSZKQSZK), introduced by Watrous (FOCS 2002). However, restricting the verifier's question to classical public coins collapses the corresponding class to BQP\sf BQPBQP, as shown by Beigi, Shor, and Watrous (ToC, 2011). We further study two-message quantum interactive proof systems with a laconic prover. To this end, we introduce the class QIPℓ-bit(2){\sf QIP}_{\ell\text{-}{\rm bit}}(2)QIPℓ-bit​(2), where ℓ\ellℓ is the length of the prover's response, and establish: 1. A natural complete characterization of QIPℓ-bit(2){\sf QIP}_{\ell\text{-}{\rm bit}}(2)QIPℓ-bit​(2) by Multi-State Distinguishability. In particular, Quantum State Distinguishability (QSD) is QIPbit{\sf QIP}_{\rm bit}QIPbit​-complete. Since QSD is QSZK\sf QSZKQSZK-hard, our result places QIPℓ-bit(2){\sf QIP}_{\ell\text{-}{\rm bit}}(2)QIPℓ-bit​(2), for ℓ≥2\ell\geq 2ℓ≥2, in a landscape "just above" QSZK\sf QSZKQSZK. 2. Easy regimes for QIPℓ-bit(2){\sf QIP}_{\ell\text{-}{\rm bit}}(2)QIPℓ-bit​(2) collapsing to QSZK\sf QSZKQSZK. We prove that QSD[a,b][a,b][a,b] (and thus QIPbit[a,b]{\sf QIP}_{\rm bit}[a,b]QIPbit​[a,b]) is in QSZK\sf QSZKQSZK when a(n)−b(n)≥1/O(log⁡n)a(n)-b(n)\geq 1/O(\log n)a(n)−b(n)≥1/O(logn), and combine this with an answer compression from QIPℓ-bit[2,c,s]{\sf QIP}_{\ell\text{-}{\rm bit}}[2,c,s]QIPℓ-bit​[2,c,s] to QIPbit{\sf QIP}_{\rm bit}QIPbit​ to obtain another easy regime when 2c>(1+2ℓ/2)s2c>(1+2^{\ell/2})s2c>(1+2ℓ/2)s. Remarkably, our improved polarization applies to SD and SZK\sf SZKSZK, resolving an open problem in Sahai and Vadhan (JACM, 2003). 3. Quantum public coins also make the interaction useless: qc-QAM[O(log⁡n)]{\sf qc}\text{-}{\sf QAM}[O(\sqrt{\log{n}})]qc-QAM[O(logn​)] with constant gap is in BQP\sf BQPBQP, where qc-QAM[ℓ]{\sf qc}\text{-}{\sf QAM}[\ell]qc-QAM[ℓ] is a subclass of QIPℓ-bit(2){\sf QIP}_{\ell\text{-}{\rm bit}}(2)QIPℓ-bit​(2) in which the verifier's question is exactly halves of EPR pairs.
The development of quantum computers has urged the cryptographic community to prepare cryptographic primitives for the eventual arrival of the post‐quantum world. To this end, the authors study the witness indistinguishability (WI) and witness hiding (WH) of proof systems against quantum adversaries. They give formal definitions of quantum WI (QWI) and quantum WH (QWH), present proof systems satisfying these definitions, and specify a condition under which QWI implies QWH. Regarding the non‐interactive proof systems, they prove that, even if a common reference string is used to generate polynomially many non‐interactive proofs, the QWI is still preserved, while quantum zero‐knowledge has no such beneficial property. To show the strength of QWI, they present two applications of them. First, they prove that the construction proposed by Feige et al . that transforms any non‐interactive bounded zero‐knowledge proof system to a general one is also feasible against quantum adversaries. Second, they construct a quantum‐secure signature scheme in the CRS model, which is existentially unforgeable against quantum adversaries and remains secure even if a common random string is used to sign polynomially many messages.
With the rapid development of quantum computers, proofs of quantumness have recently become an interesting research direction. However, in current schemes for proofs of quantumness, quantum provers face the risk of being maliciously exploited by classical verifiers. Through malicious strategies in interaction with quantum provers, classical verifiers could solve some instances of hard problems that arise from the specific scheme in use. This is due to the lack of formalization that prevents malicious verifiers from extracting useful information in proofs of quantumness. To address this issue, we formalize zero-knowledge proofs of quantumness. Intuitively, the zero-knowledge property necessitates that the information gained by the classical verifier from interactions with the quantum prover should not surpass what can be simulated using a simulated classical prover interacting with the same verifier. As a result, the new zero-knowledge notion can prevent a malicious verifier from exploiting quantum advantage. We find that the classical zero-knowledge proof is sufficient to compile some existing proofs of quantumness schemes into zero-knowledge proofs of quantumness schemes. It appears to be more general to require zero-knowledge proof on the verifier side instead of the prover side. This helps to regulate the verifier's behavior from malicious to be honest-but-curious. As a result, both parties will play not only one role in the proofs of quantumness but also the dual role in the classical zero-knowledge proof. Specifically, Shor's factoring-based scheme and the learning with errors-based scheme in [Brakerski et al., FOCS, 2018] can be transformed into zero-knowledge proofs of quantumness by requiring an extractable non-interactive zero-knowledge argument on the verifier side. Zero-knowledge proofs of quantumness can thus be viewed as an enhanced security notion for proofs of quantumness.
The complexity class Quantum Statistical Zero-Knowledge (QSZK\mathsf{QSZK}QSZK), introduced by Watrous (FOCS 2002) and later refined in Watrous (SICOMP, 2009), has the best known upper bound QIP(2)∩co-QIP(2)\mathsf{QIP(2)} \cap \text{co-}\mathsf{QIP(2)}QIP(2)∩co-QIP(2), which was simplified following the inclusion QIP(2)⊆PSPACE\mathsf{QIP(2)} \subseteq \mathsf{PSPACE}QIP(2)⊆PSPACE established in Jain, Upadhyay, and Watrous (FOCS 2009). Here, QIP(2)\mathsf{QIP(2)}QIP(2) denotes the class of promise problems that admit two-message quantum interactive proof systems in which the honest prover is typically computationally unbounded, and co-QIP(2)\text{co-}\mathsf{QIP(2)}co-QIP(2) denotes the complement of QIP(2)\mathsf{QIP(2)}QIP(2). We slightly improve this upper bound to QIP(2)∩co-QIP(2)\mathsf{QIP(2)} \cap \text{co-}\mathsf{QIP(2)}QIP(2)∩co-QIP(2) with a quantum linear-space honest prover. Specifically, the honest prover uses space linear in the size of the transcript of the original QSZK\mathsf{QSZK}QSZK proof system. A similar improvement also applies to the upper bound for the non-interactive variant NIQSZK\mathsf{NIQSZK}NIQSZK. Our main techniques are algorithmic versions of the Holevo-Helstrom measurement and the Uhlmann transform, both implementable in quantum linear space, implying polynomial-time complexity in the state dimension, using the recent space-efficient quantum singular value transformation of Le Gall, Liu, and Wang (CC, to appear).