Recognition: no theorem link
Insertion Correcting Capability for Quantum Deletion-Correcting Codes
Pith reviewed 2026-05-15 20:12 UTC · model grok-4.3
The pith
Quantum codes that correct t deletions also correct any combination of insertions and deletions adding up to t errors when their error spheres are disjoint.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Any quantum t-deletion-correcting code also corrects a total of t insertion and deletion errors when the error spheres of its code states remain disjoint. The quantum indel distance is defined to measure the minimum insertions plus deletions needed to map one state to another, and the paper shows that this distance determines the combined correcting capability for both error types.
What carries the argument
The quantum indel distance, which counts the fewest insertions and deletions required to change one quantum state into another.
If this is right
- Existing quantum deletion-correcting codes can be applied directly to channels that produce both insertions and deletions.
- Code construction efforts can concentrate on deletion correction alone and still obtain indel correction as a byproduct.
- The indel distance supplies a single metric that ranks quantum codes by their combined insertion-deletion performance.
- Bounds derived for deletion correction translate immediately to bounds on the total number of indel errors that can be corrected.
Where Pith is reading between the lines
- The result may allow quantum code designers to ignore insertion errors during initial construction and still obtain robustness against mixed indel noise.
- It raises the question of whether analogous extensions hold for other asymmetric error models such as deletions plus substitutions.
- Practical implementations could test small codes on hardware by injecting controlled numbers of insertions and deletions to verify the predicted capability.
Load-bearing premise
A quantum code is defined exactly by the requirement that the error spheres around its code states do not overlap.
What would settle it
An explicit quantum code that corrects every t-deletion pattern yet fails on at least one pattern consisting of k insertions and t-k deletions for some k between 0 and t.
read the original abstract
This paper proves that any quantum t-deletion-correcting codes also correct a total of t insertion and deletion errors under a certain condition. Here, this condition is that a set of quantum states is defined as a quantum error-correcting code if the error spheres of its states are disjoint, as classical coding theory. In addition, this paper proposes the quantum indel distance and describes insertion and deletion errors correcting capability of quantum codes by this distance.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proves that any quantum t-deletion-correcting code, defined via the condition that its states have disjoint t-deletion error spheres (as in classical coding theory), also corrects any combination of insertions and deletions whose total number is at most t. It further introduces the quantum indel distance as a metric to characterize the insertion-deletion correcting capability of such codes.
Significance. If the adopted disjoint-sphere definition is accepted as sufficient, the result directly transfers classical indel-correcting properties to the quantum setting without additional parameters, and the quantum indel distance supplies a new tool for code analysis. This could simplify constructions for quantum channels with length-changing errors, provided the definition aligns with standard quantum requirements.
major comments (1)
- [Abstract and definition of quantum codes] The central claim rests on defining a quantum code solely by disjoint t-deletion spheres (condition stated in the abstract). This definition is load-bearing, yet the manuscript does not verify that such codes satisfy the Knill-Laflamme condition <c_i|E_a^† E_b|c_j> = δ_ij λ_ab for the combined set of insertion and deletion operators (including those that change Hilbert-space dimension). A concrete check or counter-example discussion is required in the proof section.
minor comments (2)
- [Section introducing quantum indel distance] The quantum indel distance should be formally defined with an equation and compared to existing quantum distances (e.g., quantum Hamming distance) to clarify its contribution.
- Add at least one explicit low-dimensional example of a code satisfying the disjoint-sphere condition to illustrate the claimed indel correction.
Simulated Author's Rebuttal
We thank the referee for the careful review and constructive feedback on our manuscript. We address the major comment point by point below, clarifying our definition and strengthening the presentation as needed.
read point-by-point responses
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Referee: [Abstract and definition of quantum codes] The central claim rests on defining a quantum code solely by disjoint t-deletion spheres (condition stated in the abstract). This definition is load-bearing, yet the manuscript does not verify that such codes satisfy the Knill-Laflamme condition <c_i|E_a^† E_b|c_j> = δ_ij λ_ab for the combined set of insertion and deletion operators (including those that change Hilbert-space dimension). A concrete check or counter-example discussion is required in the proof section.
Authors: We thank the referee for highlighting this point. Our definition of a quantum t-deletion-correcting code is intentionally based on the disjointness of t-deletion error spheres (as in classical coding theory), which is stated explicitly in the abstract and formalized in Section II. This condition guarantees that distinct code states remain perfectly distinguishable after any sequence of at most t deletions. Theorem 1 then shows that the same disjoint-sphere property extends to any combination of insertions and deletions whose total count is at most t, because each such indel error maps the original codeword into a unique enlarged sphere. For the Knill-Laflamme condition, we note that standard KL applies to fixed-dimension errors; when operators change the Hilbert-space dimension, the condition must be adapted to the relevant subspaces. The disjoint-sphere assumption directly implies that post-error states belonging to different codewords have orthogonal supports, which enforces the off-diagonal vanishing <c_i | E† F | c_j> = 0 (i ≠ j) for any pair of indel operators E, F of total weight ≤ t. We will add a dedicated subsection in the proof of Theorem 1 that explicitly verifies this adapted orthogonality condition for the combined insertion-deletion operators and briefly discusses the dimension-changing case. revision: yes
Circularity Check
No circularity; proof follows directly from adopted disjoint-sphere definition
full rationale
The paper adopts the classical definition of error-correcting codes via disjoint error spheres and proves that any code satisfying this for t deletions also handles t total indels. This is a direct logical consequence of the sphere-disjointness property under the stated definition, with no reduction of the central claim to a fitted parameter, self-citation chain, or ansatz smuggled from prior work. The quantum indel distance is introduced as a descriptive measure based on the same framework. The derivation remains self-contained against the external benchmark of the disjoint-spheres condition and does not collapse by construction.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption A set of quantum states forms a quantum error-correcting code precisely when the error spheres of its codewords are disjoint.
invented entities (1)
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quantum indel distance
no independent evidence
Forward citations
Cited by 1 Pith paper
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Decoding Algorithm to Composite Errors Consisting of Deletions and Insertions for Quantum Deletion-Correcting Codes Based on Quantum Reed-Solomon Codes
A decoding algorithm is provided for composite deletion-insertion errors in quantum deletion-correcting codes based on quantum Reed-Solomon codes.
discussion (0)
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