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Logical information localisation in stabiliser codes via single-qubit measurements

Quantum Physics · Submitted 30 Sep 2026 · 56 references

Pith's verdict: Proves an exact localisation threshold at p=1/2 for the planar surface code with a clean percolation-plus-disjointness argument, and ships two algorithms that genuinely beat the prior state of the art.

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arXiv ID2609.39980 (version 1)
Pith IDQLHNTKWB, Pith's permanent record of this paper and its review
CitationHemant Sharma, Jelena Mackeprang, Jonas Helsen. "Logical information localisation in stabiliser codes via single-qubit measurements." arXiv:2609.39980 (2026). https://pith.science/paper/QLHNTKWB
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Referee report
The paper

The paper claims

The planar surface code can still deliver its logical qubit when up to half its qubits are lost, and fails beyond that.

The reading

The paper asks a practical question: when qubits in a stabiliser code are lost one by one, can the code's logical qubit still be extracted by measuring the surviving qubits one at a time? It answers yes for the planar surface code, with an exact dividing line at a loss probability p = 1/2. Below that line the logical information can be concentrated onto a constant number of physical qubits, with success probability converging to one as the code grows; above it no such localisation survives. The proof works by combining two existing ideas — bond percolation on the square lattice and the disjointness of stabiliser codes — and the paper also provides two practical algorithms that reproduce the threshold numerically and run much faster than earlier methods.

What carries the argument

The central object is the g-SPF pair, a pair of logical operators X and Z that avoid all lost qubits and anti-commute qubit-wise on at most g qubits; measuring them qubit-wise localises the logical information onto those g qubits. The proof chain runs through four steps: edge-disjoint open paths in the lattice survive as disjoint logical representatives after loss (percolation, Lemma 9 cited from Grimmett); Harris' inequality joins the left-to-right and top-to-bottom path events; Corollary 11 converts the number of edge-disjoint open paths into a lower bound on the disjointness of surviving X and Z representatives; and Lemma 2, a variant of the scrubbing lemma from Ref. [30], bounds the minimum support intersection by n divided by the product of the two disjointnesses. Since the number of qubit-wise anti-commutations satisfies α(X, Z) ≤ |supp(X) ∩ supp(Z)|, a constant bound on the intersection yields a constant-g pair.

Extended reading notes

Core claim

Theorem 1: for the family of planar surface codes under i.i.d. qubit loss, there is an exact localisation threshold at p = 1/2. For every p < 1/2 there exists a strictly positive constant g = g(p) such that the probability of finding a g-SPF pair converges to one as the code size grows, where a g-SPF pair is a pair of logical X and Z representatives with no support on lost qubits that anti-commute qubit-wise on at most g qubits. For every p > 1/2 the g-SPF success rate converges to zero for any constant g. Practically, this means that below 1/2 loss a sufficiently large surface code allows a readout of the logical qubit by one round of single-qubit measurements that concentrate the information onto O(1) physical qubits. The authors stress that this localisation threshold coincides with the known erasure threshold even though localisation and erasure decoding are not obviously the same task.

Load-bearing premise

The lower-bound half of Theorem 1 rests on the percolation concentration statement that for every p < 1/2 the number of edge-disjoint open left-to-right paths in the Λ × (Λ−1) lattice is at least β(Λ−1) with probability exponentially close to one; if that bound failed for some p < 1/2, the whole chain from percolation to a constant-g pair would collapse.

Editorial extensions

If this is right

  • For any loss rate below 1/2, a sufficiently large planar surface code lets one read out the logical qubit onto O(1) physical qubits by single-qubit measurements, with probability converging to one.
  • For any loss rate above 1/2, no constant-size localisation set survives, so p = 1/2 is a sharp cutoff rather than a soft crossover.
  • The localisation threshold equals the standard erasure threshold even though localisation and erasure decoding are distinct tasks, suggesting the erasure threshold governs more than mere survival of the logical qubit.
  • The exact D-LoFi and heuristic H-LoFi algorithms reproduce this threshold numerically and extend analyses to surface codes of distance 9 (81 qubits) and graph codes of 51 qubits, well beyond earlier limits.
  • Because g = 1 already shows threshold behaviour numerically, the attainable localisation set may in fact be a single qubit for all p < 1/2, a stronger statement than the theorem proves.
  • Relaxing a pre-designated target qubit to an arbitrary one measurably raises the success rate, so flexible target choice is strictly better than fixing a target in advance.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The proof uses support intersection as a proxy for qubit-wise anti-commutation, which is a loose bound: two operators with large overlapping supports can still anti-commute on very few qubits. A commutation-aware notion of disjointness could sharpen the constant g, plausibly down to g = 1, which the numerics already suggest.
  • Because every stabiliser code is local-Clifford equivalent to a graph code, the localisation threshold plausibly transfers to graph-code versions of the surface code, making the result relevant to photonic fusion and teleportation schemes that express codes as graphs.
  • The exact coincidence of the localisation threshold with the erasure threshold is a hint that, in this setting, localisation via g-SPF may be equivalent to erasure decodability; if that equivalence held broadly, it would give a clean necessary-and-sufficient characterisation of post-loss localisation by LOCC.
  • The upper-bound half of the theorem is inherited from the exactness of the erasure threshold, so the genuinely new content is the lower-bound half; a failure of either the percolation concentration bound or the disjointness argument would collapse the threshold claim at p = 1/2.
Original abstract

Stabiliser path finding (SPF) has previously been introduced as a method to localise logical information in a stabiliser code undergoing loss onto a single pre-specified target qubit, using only one round of single-qubit measurements. When working with limited resources and flying qubits, this fast read-out of logical information is a helpful tool for fault-tolerant communication. In this work, we provide a broad analytical and computational study of localisation via SPF. We introduce $g$-SPF, where the task is to localise the logical information onto a set of at most $g$ unspecified target qubits. Through analytical arguments based on percolation theory and the disjointness of stabiliser codes, we prove that for i.i.d. qubit loss with probability $p<1/2$ and sufficiently large planar surface codes, localisation via $g$-SPF for constant $g$ succeeds with a probability converging to one, which establishes a localisation threshold. Furthermore, we propose and implement two algorithms to solve SPF. The first is exact and formulates SPF as an integer linear program, whereas the second is heuristic and formulates SPF as a decoding problem. We validate both algorithms by numerically reproducing the localisation threshold for the surface code and demonstrate that the heuristic algorithm is considerably faster. Our work significantly reduces the time required to solve SPF compared to current state-of-the-art algorithms, allowing us to study localisation in substantially larger stabiliser codes than previously considered in the literature. Together, these theoretical and computational results open the door to various applications, such as fault-tolerant teleportation and efficient logical fusion.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-10-01: 1 request, 7,713 input tokens.

What the abstract itself states, as probabilities: claims first 0.09 · states limitation 0.22 · human participants 0.01 · controlled comparison 0.16 · randomized assignment 0.02 · states quantitative result 0.96 · compares with prior results 0.88 · mentions code or data availability 0.03.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

Stabiliser path finding (SPF) has previously been introduced as a method to localise logical information in a stabiliser code undergoing loss onto a single pre-specified target qubit, using only one round of single-qubit measurements. When working with limited resources and flying qubits, this fast read-out of logical information is a helpful tool for fault-tolerant communication. In this work, we provide a broad analytical and computational study of localisation via SPF. We introduce $g$-SPF, where the task is to localise the logical information onto a set of at most $g$ unspecified target qubits. Through analytical arguments based on percolation theory and the disjointness of stabiliser codes, we prove that for i.i.d. qubit loss with probability $p<1/2$ and sufficiently large planar surface codes, localisation via $g$-SPF for constant $g$ succeeds with a probability converging to one, which establishes a localisation threshold. Furthermore, we propose and implement two algorithms to solve SPF. The first is exact and formulates SPF as an integer linear program, whereas the second is heuristic and formulates SPF as a decoding problem. We validate both algorithms by numerically reproducing the localisation threshold for the surface code and demonstrate that the heuristic algorithm is considerably faster. Our work significantly reduces the time required to solve SPF compared to current state-of-the-art algorithms, allowing us to study localisation in substantially larger stabiliser codes than previously considered in the literature. Together, these theoretical and computational results open the door to various applications, such as fault-tolerant teleportation and efficient logical fusion.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Stabiliser path finding (SPF) has previously been introduced as a method to localise logical information in a stabiliser code undergoing loss onto a single pre-specified target qubit, using only one round of single-qubit measurements. background 1.00 0.05 0.04 asserted 1.00
s1 When working with limited resources and flying qubits, this fast read-out of logical information is a helpful tool for fault-tolerant communication. background 0.86 0.06 0.03 asserted 0.87
s2 In this work, we provide a broad analytical and computational study of localisation via SPF. contribution 1.00 0.91 0.04 asserted 0.88
s3 We introduce $g$-SPF, where the task is to localise the logical information onto a set of at most $g$ unspecified target qubits. contribution 0.97 0.94 0.08 asserted 0.97
s4 Through analytical arguments based on percolation theory and the disjointness of stabiliser codes, we prove that for i.i.d. qubit loss with probability $p<1/2$ and sufficiently large planar surface codes, localisation via $g$-SPF for constant $g$ succeeds with a probability converging to one, which establishes a localisation threshold. result 0.99 0.94 0.70 asserted 1.00
s5 Furthermore, we propose and implement two algorithms to solve SPF. contribution 0.51 0.95 0.04 asserted 1.00
s6 The first is exact and formulates SPF as an integer linear program, whereas the second is heuristic and formulates SPF as a decoding problem. method 0.93 0.94 0.03 asserted 1.00
s7 We validate both algorithms by numerically reproducing the localisation threshold for the surface code and demonstrate that the heuristic algorithm is considerably faster. result 0.97 0.97 0.11 asserted 1.00
s8 Our work significantly reduces the time required to solve SPF compared to current state-of-the-art algorithms, allowing us to study localisation in substantially larger stabiliser codes than previously considered in the literature. result 0.53 0.94 0.13 asserted 1.00
s9 Together, these theoretical and computational results open the door to various applications, such as fault-tolerant teleportation and efficient logical fusion. interpretation 0.85 0.43 0.22 asserted 0.58

What kind of paper the classifier reports this is: method or tool 0.74 · evidence from proof or derivation 0.79.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. Success rate at which a g-SPF pair is found for the rotated surface code (see for example Ref. [32]) and g = 1. For every loss probability p we Monte Carlo sample at least 5000 loss configurations and estimate the success rate of g-SPF. code after loss. Note that the tableau representation is the natural representation of stabiliser codes and does not require any particular structure of the code, allowing us to analyse stabiliser codes beyond graph codes. We numerically reproduce threshold behaviour similar to what was predicted by Theorem 1 using our algorithms D-LoFi and H-LoFi in
Figure 2. In (a) we plot the average runtime of D-LoFi and H-LoFi with increasing code distance for a fixed
Figure 3. We plot the runtime comparison of D-LoFi with the algorithm from Ref. [
Figure 4. The triangular graph and the crazy graph (
Figure 5. The planar surface code on a square lattice with
Figure 6. g-SPF threshold, where g = 1, for the rotated surface code. For every loss probability we sample at least 5000 loss configurations according to an i.i.d. loss probability distribution and estimate the success rate according to Eqn. (57). The standard error of the mean is too small to be visible in the figure and has been omitted for that reason. We compare the runtime of D-LoFi and H-LoFi in
Figure 7. Here, we benchmark the runtimes and minimisation performance of D-LoFi and H-LoFi. We plot the
Figure 8. Threshold behaviour comparison of graph codes in the presence of loss. We sample 2000 loss configu
Figure 9. Here, we plot the runtime comparison of D-LoFi with the algorithm from Ref. [
Figure 10. Here, we compare the success rate of the D-LoFi algorithm for Target-SPF and

Figures reproduced from arXiv:2609.39980 by the authors.

References

Discussion

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