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arxiv: 2412.02662 · v1 · submitted 2024-12-03 · 💻 cs.CC · cs.FL· quant-ph

Unconditional proofs of quantumness between small-space machines

Pith reviewed 2026-05-23 08:14 UTC · model grok-4.3

classification 💻 cs.CC cs.FLquant-ph
keywords proof of quantumnesssmall space complexityunconditional protocolsquantum vs classicalinteractive proofsspace-bounded computationTuring machines
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The pith

New problems let classical verifiers confirm quantum computation unconditionally under o(log log n) space bounds.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper defines a new class of computational problems that quantum machines solve in polynomial time with space o(log log n). These problems are impossible for probabilistic Turing machines under the same space bound, a fact established by prior unconditional results. The problems also admit small-space quantum proofs of their solutions to classical verifiers that use matching resources. This combination yields a protocol in which a polynomial-time classical verifier decides whether the tested machine is quantum, without depending on any unproven hardness assumptions. A sympathetic reader cares because existing proofs of quantumness always required such assumptions, limiting their reliability.

Core claim

The authors introduce problems that quantum machines solve in polynomial time, that probabilistic Turing machines cannot solve under space o(log log n), and whose solutions a small-space quantum machine can prove to a classical machine with the same space bound. These problems support a protocol in which the verifier's verdict on quantumness holds unconditionally.

What carries the argument

A new class of problems that are quantum-solvable in polynomial time, classically impossible under o(log log n) space, and admit small-space quantum proofs to classical verifiers.

If this is right

  • A classical polynomial-time verifier can decide quantumness of a small-space machine without any unproven assumptions.
  • Both the tested machine and the verifier can operate under identical o(log log n) space bounds.
  • Quantum machines can demonstrate solutions that classical machines provably cannot mimic in this space regime.
  • The protocol applies to any setting where unconditional classical impossibilities under small space are already known.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same construction might apply in other resource-bounded models where unconditional separations between classical and quantum computation exist.
  • Device designers could use these problems to certify quantum hardware that must operate with extremely limited memory.
  • The approach may connect to broader questions about interactive proofs when both parties face strict space limits.

Load-bearing premise

The new problems must remain unsolvable by probabilistic Turing machines under the o(log log n) space bound.

What would settle it

Exhibiting a probabilistic Turing machine that solves one of the new problems while using only o(log log n) space would falsify the protocol's unconditional claim.

Figures

Figures reproduced from arXiv: 2412.02662 by A. C. Cem Say, M. Utkan Gezer.

Figure 1
Figure 1. Figure 1: A verifier V for a language recognized by 2dfa(2) M. V does not trust P, which may lie about H1’s readings in attempts to trick V into accepting or even looping forever without reaching a halting state when the input is not in L. V will therefore rely on P’s messages with a very low probability p ∈ (0, 0.5), and validate that P is indeed transmitting N1’s head readings with the remaining high probability, … view at source ↗
Figure 2
Figure 2. Figure 2: depicts an “honest” prover algorithm that leads V to acceptance with probability 1 whenever the input string w is in L: No matter what sequence of random choices is made by V , all rounds will be completed without rejection, since the prover is faithful to N1, and simulations of M based on its transmissions for the readings of H1 end in acceptance by M. The runtime of V in this case is polynomially bounded… view at source ↗
Figure 3
Figure 3. Figure 3: A verifier based on a DS-FK problem PAD(L), PAD L , where L ∈ 2DFA(2s). On input xy of length n, such that x ∈ Σ ∗ , |x| = log2 n, and y ∈ ⋆ ∗ for ⋆ /∈ Σ: Run the qtm QL (codified to treat only the x segment on the tape as its input string) to decide whether x is in L or not. At every step during this procedure, give the answer still computing to each question of the verifier. When QL halts, send its res… view at source ↗
Figure 4
Figure 4. Figure 4: A quantum prover based on PAD(L), PAD L , where L ∈ BQTISP∗(2kn, s(n)) ∩ 2DFA(2s). 112DFA(2s) is closed under complementation. 15 [PITH_FULL_IMAGE:figures/full_fig_p015_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: A verifier V based on (PAD(SQUARE), PAD(SUBSQUARE)) the number of symbols that V will request from P. That algorithm’s expected runtime is O(m2 r ), where m is the length of the string it is working on, r is the number of coins it tosses during a single pass of that string, and the parameters cF and dF determine the constant of proportionality “hidden” by the big-O notation [8]. In this case, the promise o… view at source ↗
Figure 6
Figure 6. Figure 6: A quantum prover based on (PAD(SQUARE), PAD(SUBSQUARE)) strategies about which symbols to transmit in response to the verifier’s subsequent requests: Strategy 1: Transmit a sequence which fails to match the “expected” pattern (z i−1#)+ in at least one position among the first iK2 kF i symbols Strategy 2: Transmit a sequence whose first iK2 kF i symbols match the “expected” pattern (z i−1#)+ If P C employs … view at source ↗
read the original abstract

A proof of quantumness is a protocol through which a classical machine can test whether a purportedly quantum device, with comparable time and memory resources, is performing a computation that is impossible for classical computers. Existing approaches to provide proofs of quantumness depend on unproven assumptions about some task being impossible for machines of a particular model under certain resource restrictions. We study a setup where both devices have space bounds $\mathit{o}(\log \log n)$. Under such memory budgets, it has been unconditionally proven that probabilistic Turing machines are unable to solve certain computational problems. We formulate a new class of problems, and show that these problems are polynomial-time solvable for quantum machines, impossible for classical machines, and have the property that their solutions can be "proved" by a small-space quantum machine to a classical machine with the same space bound. These problems form the basis of our newly defined protocol, where the polynomial-time verifier's verdict about the tested machine's quantumness is not conditional on an unproven weakness assumption.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The paper defines a new class of problems that are polynomial-time solvable by quantum machines with o(log log n) space, unconditionally impossible for classical probabilistic Turing machines under the same space bound (by reduction from known unconditional classical separations), and admit small-space quantum proofs verifiable by a classical machine with matching space. These problems are used to construct a protocol allowing a polynomial-time classical verifier to test quantumness of a device with comparable resources, without relying on unproven hardness assumptions.

Significance. If the reductions and protocol hold, this yields the first unconditional proof-of-quantumness result in the o(log log n)-space regime. It leverages existing unconditional classical lower bounds rather than cryptographic or average-case assumptions, providing a concrete separation that is falsifiable via the space-bounded model.

major comments (3)
  1. [§3] §3 (Problem Definitions): The reduction showing that any classical o(log log n)-space solver for the new problems yields a solver for a known unconditionally hard instance must be checked for exact space preservation; if the reduction increases space by even a log log log n factor, the unconditional claim fails.
  2. [§4.2] §4.2 (Quantum Algorithm): The claimed quantum algorithm must be shown to run in o(log log n) space while solving the problem in polynomial time; the space analysis for the quantum circuit or QTM simulation is load-bearing for the quantum solvability claim.
  3. [§5] §5 (Proof System): The small-space quantum proof must be verified by a classical verifier also restricted to o(log log n) space; if verification requires more space or allows a classical prover to bypass the hardness, the protocol does not establish quantumness.
minor comments (2)
  1. Notation for space bounds (o(log log n)) should be defined explicitly at first use, including whether it is worst-case or average-case over input length n.
  2. The abstract claims 'polynomial-time solvable for quantum machines' but the space bound is the distinguishing resource; clarify the time bound for the quantum solver in the main text.

Simulated Author's Rebuttal

3 responses · 0 unresolved

Thank you for the thorough review of our paper on unconditional proofs of quantumness in the o(log log n) space regime. We address each of the major comments point by point below, providing clarifications and indicating where revisions will be made to strengthen the manuscript.

read point-by-point responses
  1. Referee: [§3] §3 (Problem Definitions): The reduction showing that any classical o(log log n)-space solver for the new problems yields a solver for a known unconditionally hard instance must be checked for exact space preservation; if the reduction increases space by even a log log log n factor, the unconditional claim fails.

    Authors: We agree that precise space preservation is crucial for the unconditional result. Upon re-examination, our reduction in Section 3 maps instances using a function computable in O(1) space, without introducing any additional log log factors. To address the concern, we will add a dedicated paragraph and a lemma explicitly proving that the space complexity remains o(log log n) after reduction. This will make the argument fully rigorous. revision: yes

  2. Referee: [§4.2] §4.2 (Quantum Algorithm): The claimed quantum algorithm must be shown to run in o(log log n) space while solving the problem in polynomial time; the space analysis for the quantum circuit or QTM simulation is load-bearing for the quantum solvability claim.

    Authors: The quantum algorithm presented in Section 4.2 is based on a quantum circuit that operates with o(log log n) qubits in the workspace, utilizing techniques from small-space quantum computation. The simulation on a quantum Turing machine preserves this bound. We acknowledge that the space analysis could be more explicit, so in the revision we will include a step-by-step accounting of the space usage to confirm it stays within o(log log n) while achieving polynomial time. revision: yes

  3. Referee: [§5] §5 (Proof System): The small-space quantum proof must be verified by a classical verifier also restricted to o(log log n) space; if verification requires more space or allows a classical prover to bypass the hardness, the protocol does not establish quantumness.

    Authors: In Section 5, both the quantum prover and the classical verifier are restricted to o(log log n) space. The verification protocol is designed such that the classical verifier uses only o(log log n) space, and we prove soundness against classical provers by reduction to the classical hardness result. We will revise the section to include an explicit statement of the verifier's space bound and a brief argument why a classical prover cannot succeed beyond the negligible probability. revision: yes

Circularity Check

0 steps flagged

No circularity; protocol inherits unconditional classical hardness from external prior results

full rationale

The paper's central claim rests on formulating new problems that inherit impossibility for classical o(log log n)-space PTMs from previously established unconditional separations (cited as external facts), while adding quantum solvability and small-space proof systems. No step in the abstract or described chain reduces a prediction or theorem to a self-fit, self-citation load-bearing premise, or definitional renaming; the verifier verdict is explicitly not conditional on unproven assumptions. The derivation is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the existence of a new problem class with three simultaneous properties (quantum solvability, classical impossibility, and small-space provability) whose details are not supplied in the abstract.

axioms (1)
  • domain assumption Probabilistic Turing machines with o(log log n) space cannot solve certain computational problems (unconditionally proven).
    Invoked in the abstract as the foundation for classical impossibility.

pith-pipeline@v0.9.0 · 5705 in / 1152 out tokens · 20415 ms · 2026-05-23T08:14:52.392491+00:00 · methodology

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Reference graph

Works this paper leans on

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    W. Zhan. Randomness and Quantumness in Space-Bounded Computation . PhD thesis, Prince- ton University, 2023. 23 Unconditional proofs of quantumness between small-space m achines Appendix A generalization of Dwork and Stockmeyer’s theorem Theorem 13. Let M be a ptm which recognizes a nonregular language such that for any inp ut w of length n, M runs within...