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arxiv: 2607.02444 · v1 · pith:7YJ3UH5Lnew · submitted 2026-07-02 · 🪐 quant-ph · cs.CC· cs.DS· cs.IT· cs.LG· math.IT

Optimal Stabilizer Testing and Learning with Limited Quantum Memory

Pith reviewed 2026-07-03 11:38 UTC · model grok-4.3

classification 🪐 quant-ph cs.CCcs.DScs.ITcs.LGmath.IT
keywords stabilizer statesquantum memorysample complexitystate testingstate learninghidden shift problempurity testing
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The pith

With only k qubits of coherent memory, testing n-qubit stabilizer states requires Θ(n-k) samples.

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

The paper determines the sample complexities of testing and learning stabilizer states when an algorithm may retain only k qubits of coherent quantum memory between measurements on successive copies. Testing requires Θ(n-k) copies, with the upper bound obtained by reduction to the hidden shift problem and the lower bound obtained via a combinatorial argument on average-case likelihood ratios. Learning requires Θ(n²/k) copies in the non-adaptive setting. These bounds show that the separation between constant-copy testing and linear-copy learning disappears under memory limits, and that even near-full memory (k = 0.99n) precludes constant-copy testing.

Core claim

In the k-qubit memory model the sample complexity of testing stabilizer states is Θ(n-k) and the sample complexity of learning them non-adaptively is Θ(n²/k). The testing upper bound follows from a connection to the hidden shift problem; the lower bound follows from a novel combinatorial approach to average-case likelihood ratio bounds that uses the stochastic orthogonal group. Consequently even with k = 0.99n memory a constant-copy tester does not exist, and when k = cn for constant c < 1 both tasks require Θ(n) copies.

What carries the argument

The k-qubit coherent memory model, in which the algorithm receives copies sequentially but may retain only k qubits coherently between measurements.

If this is right

  • Even with 99 percent of full memory, stabilizer testing cannot be performed with a constant number of copies.
  • When memory is a constant fraction cn of the system size, testing and learning have identical Θ(n) sample complexity.
  • Purity testing requires exponentially many copies even when memory may remain fully coherent throughout the protocol.

Where Pith is reading between the lines

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

  • The same memory-dependent separation may appear in testing other structured quantum states if analogous combinatorial lower-bound techniques apply.
  • The non-adaptive learning bound leaves open whether adaptive algorithms could achieve lower sample complexity with the same memory limit.
  • The framework suggests memory size rather than adaptivity alone is the dominant resource separating testing from learning for stabilizer states.

Load-bearing premise

The combinatorial argument that produces average-case likelihood ratio bounds via the stochastic orthogonal group holds and yields the stated lower bound on testing.

What would settle it

An explicit protocol that tests n-qubit stabilizer states with o(n-k) copies while using only k qubits of coherent memory between measurements would falsify the lower bound.

Figures

Figures reproduced from arXiv: 2607.02444 by Louis Schatzki, Srinivasan Arunachalam.

Figure 1
Figure 1. Figure 1: Protocol using k-qubits of memory and single-copy measurements. In each round a new copy of an input state ρ is loaded. There is also a coherent memory register of k-qubits. The operations in each round act on the memory and the input at that step. The channels applied may depend classically upon the prior observations. 1.1 Main results Our main result is to settle both of these questions. Even with 0.99n … view at source ↗
Figure 2
Figure 2. Figure 2: Sample complexity of learning and testing stabilizer states with limited quantum memory. [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Partially contracting a swap operation. By contracting the first register of SWAP [PITH_FULL_IMAGE:figures/full_fig_p009_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Partial Bell sampling using a quantum memory. Part of the input state [PITH_FULL_IMAGE:figures/full_fig_p017_4.png] view at source ↗
read the original abstract

We study stabilizer state testing and learning with limited coherent quantum memory. Here an algorithm sequentially receives copies of an unknown $n$-qubit state, but may keep only $k$ qubits of coherent quantum memory between measurements. With unrestricted memory, seminal work of Gross, Nezami and Walter showed how to test $n$-qubit stabilizer states using $6$ copies, which is dimension independent, unlike the learning complexity of $\Theta(n)$. We show that this testing-vs-learning separation is lost under memory constraints. More concretely we show that (1) The sample complexity of testing stabilizer states in the $k$-qubit memory framework is $\Theta(n-k)$. Our upper bound goes via a novel connection to the hidden shift problem and the lower bound is proven using a novel approach to average case bounds on likelihood ratios via combinatorics of the stochastic orthogonal group. (2) The sample complexity of learning stabilizer states with $k$ qubits of memory, in the non-adaptive framework, is $\Theta(n^2/k)$. As a further application of our techniques, we prove an exponential lower bound for purity testing even when the memory may be left coherent throughout the protocol. Our main results identify coherent quantum memory as the resource enabling the usual separation between stabilizer testing and learning. In particular, even with $k=0.99n$ qubits of memory, there is no constant-copy stabilizer tester; furthermore for $k=cn$ qubits of memory (for $0< c < 1$), stabilizer testing is as hard as learning, with both requiring $\Theta(n)$ copies.

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

2 major / 2 minor

Summary. The manuscript claims to determine the sample complexities for testing and learning n-qubit stabilizer states when the algorithm has access to only k qubits of coherent quantum memory. Specifically, testing requires Θ(n - k) copies, with the upper bound derived from a connection to the hidden shift problem and the lower bound from a new combinatorial approach to bounding likelihood ratios using the stochastic orthogonal group. Learning requires Θ(n² / k) copies in the non-adaptive setting. The results highlight that coherent quantum memory is the key resource separating testing from learning complexities, as even with k = 0.99n, constant-copy testing is impossible, and for k = cn with c < 1, testing matches learning in requiring Θ(n) copies. An exponential lower bound for purity testing with coherent memory is also provided.

Significance. If the bounds hold, this work significantly advances understanding of quantum resources in property testing and learning by showing how memory constraints eliminate the constant-sample testing advantage for stabilizers established by Gross, Nezami and Walter. The hidden-shift connection for the upper bound and the new combinatorial technique for the lower bound are notable. The results have implications for quantum algorithm design under realistic memory limits and provide tight optimal bounds.

major comments (2)
  1. [Lower bound for stabilizer testing (combinatorial argument via stochastic orthogonal group)] The Θ(n-k) lower bound for testing (central to the claim that coherent memory enables the testing-learning separation and that k=0.99n yields no constant-copy tester) is established via the novel average-case likelihood-ratio bound from combinatorics on the stochastic orthogonal group. This argument is load-bearing; the manuscript should expand the key measure estimates on distinguishable elements (as described in the abstract) to allow independent verification, since no machine-checked proof or prior reference is indicated.
  2. [Learning lower bound (non-adaptive framework)] The non-adaptive learning lower bound of Ω(n²/k) should be checked for consistency with the testing result: if the testing lower bound technique applies directly, it must be shown why it does not yield a stronger learning lower bound that would alter the claimed separation for k=cn.
minor comments (2)
  1. [Abstract] The abstract introduces the stochastic orthogonal group without a brief inline definition or pointer to the relevant section; adding this would improve accessibility for readers unfamiliar with the combinatorial tool.
  2. [Introduction] Notation for memory parameter k and dimension n should be consistently introduced with a short reminder in the introduction before the main theorems.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive comments, which help clarify the presentation of our results on stabilizer testing and learning under memory constraints. We address the major comments below.

read point-by-point responses
  1. Referee: [Lower bound for stabilizer testing (combinatorial argument via stochastic orthogonal group)] The Θ(n-k) lower bound for testing (central to the claim that coherent memory enables the testing-learning separation and that k=0.99n yields no constant-copy tester) is established via the novel average-case likelihood-ratio bound from combinatorics on the stochastic orthogonal group. This argument is load-bearing; the manuscript should expand the key measure estimates on distinguishable elements (as described in the abstract) to allow independent verification, since no machine-checked proof or prior reference is indicated.

    Authors: We agree that the combinatorial argument via the stochastic orthogonal group is central to the Θ(n-k) testing lower bound. In the revised manuscript, we will expand the relevant section to include additional intermediate steps and details on the measure estimates for distinguishable elements, facilitating independent verification of the average-case likelihood ratio bounds. revision: yes

  2. Referee: [Learning lower bound (non-adaptive framework)] The non-adaptive learning lower bound of Ω(n²/k) should be checked for consistency with the testing result: if the testing lower bound technique applies directly, it must be shown why it does not yield a stronger learning lower bound that would alter the claimed separation for k=cn.

    Authors: The testing lower bound technique is tailored to the decision problem of distinguishing whether an unknown state is a stabilizer or Ω(1)-far from every stabilizer; it does not directly apply to the search problem of learning (i.e., outputting a description of the unknown stabilizer). Our Ω(n²/k) non-adaptive learning lower bound is obtained via a separate information-theoretic argument that counts the number of possible n-qubit stabilizers and accounts for the k-qubit memory bottleneck. For k = cn with c < 1 the two bounds coincide at Θ(n), preserving the claimed absence of a testing-learning separation under linear memory constraints. We will add a short clarifying paragraph making this distinction explicit. revision: partial

Circularity Check

0 steps flagged

No circularity; testing and learning bounds derived from independent combinatorial arguments and hidden-shift reduction

full rationale

The paper's central claims rest on an upper bound obtained by reducing stabilizer testing to the hidden-shift problem and a lower bound obtained via a new average-case likelihood-ratio analysis on the stochastic orthogonal group. Neither step is shown to reduce to a prior result by the paper's own equations, self-definition, or self-citation chain; the combinatorial argument is explicitly presented as novel and is not justified by any cited prior work of the authors. The learning bound is likewise obtained by direct non-adaptive analysis. No fitted parameter is relabeled as a prediction, and no uniqueness theorem is imported from the authors' earlier papers. The derivation chain is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Based on abstract only; no explicit free parameters, axioms, or invented entities identified in the provided text.

pith-pipeline@v0.9.1-grok · 5833 in / 1133 out tokens · 33579 ms · 2026-07-03T11:38:25.427755+00:00 · methodology

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