Pith. sign in

REVIEW 4 major objections 4 minor 42 references

Diversity in Coded TE-QKD Channels: Achieving Infinite Diversity out of Finite System Resources

T0 review · 4 major / 4 minor · reviewed 2026-08-08 · deepseek-v4-flash

Pith's one-line read This paper proves that coded time-entanglement QKD reconciliation can reach infinite diversity order — error probability decaying exponentially in signal-to-noise ratio — from a channel whose uncoded diversity is only 1/2.

desk verdict The algebraic-diversity condition is a genuine contribution, but the soft-decision theorem is not: the WLOG zero-codeword step ignores that Gray adjacency is not XOR-translation-invariant. read the letter →

arxiv 2608.05432 v1 pith:4PVIABZ6 submitted 2026-08-05 cs.IT math.ITquant-ph

classification cs.ITmath.ITquant-ph MSC 94B0594B3581P94 PACS 03.67.Dd
keywords time-entanglementquantumkeydistributioninformationreconciliationdiversityorderinfinitemaximalfinitesoft-decisiondecodingbounded-distanceGraylabeling
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

This paper establishes exactly when an error-correcting code used for information reconciliation in time-entanglement quantum key distribution (TE-QKD) makes the reconciliation error probability decay exponentially with signal-to-noise ratio, an infinite diversity order, even though the uncoded channel has diversity only 1/2 and the code is short. For hard-decision algebraic decoding, the condition is that the number of photons carrying one codeword does not exceed the decoder's correction radius. For soft-decision decoding, the condition is a new code property: no nonzero codeword can be formed entirely from single-bin jumps, which the paper calls MFD deficiency. A sympathetic reader should care because this converts a polynomial error decay into an exponential one, and soft decoding achieves this at twice the coding rate allowed by algebraic decoding. The paper argues this behavior has no counterpart in classical fading channels, where decoding can only multiply a finite diversity order by a finite factor.

What carries the argument

The load-bearing mechanism is the separation of TE-QKD detector errors into two asymptotic classes: single-bin jumps with probability Θ(γ^(−1/2)) and multi-bin jumps with probability O(e^(−γ/4)). A code attains infinite diversity when its decoder absorbs all configurations of single-bin jumps, leaving only exponentially rare multi-bin events. For soft-decision decoding, the central object is the maximal finite diversity (MFD) property, which records whether a non-zero codeword can be built entirely from labels that are single-bin neighbors of zero. The proof of Theorem 2 uses a demilitarized-zone (DMZ) cube of side Δ, with Δ ≥ 1/(1+√L), placed inside the correct codeword's decision region; leaving that cube costs a factor O(e^(−$Δ^{2}$ γ/4)), which is exponentially small. The same DMZ argument also shows that a full-MFD code has finite diversity, falling back to ω/2 for the offending weight ω.

What would settle it

Take the [6,3,3] shortened Hamming code on N = 8 bins (m = 3) and measure the soft-decision word error rate at SNR γ = 20, 25, and 30 dB: if the log-log slope keeps steepening rather than approaching a constant, the infinite-diversity claim is supported. A sharper test uses the same code with m = 2, where the paper's Table III shows an MFD(3,3) term, so the theory predicts finite diversity 3/2 and the slope should flatten near 1.5.

Watch

Extended reading notes

Core claim

The central claim is that infinite diversity in TE-QKD reconciliation occurs precisely when the code eliminates every dominant error pattern composed of single-bin jumps. Proposition 1 splits the uncoded channel errors into two regimes: a jump to a neighboring bin has probability Θ(γ^(−1/2)), while any jump of two or more bins has probability O(e^(−γ/4)). Theorem 1 proves that a bounded-distance algebraic decoder with correction radius t achieves infinite diversity if and only if L = n log2(q)/m ≤ t, where L is the number of photons per codeword. Theorem 2 proves that soft-decision decoding achieves infinite diversity if and only if the code is MFD deficient, meaning no non-zero codeword has a binary image whose Hamming weight ω is realized entirely by ω neighboring labels of zero; a sufficient condition is L < d_Hmin(C_b). The paper also derives Singleton-type rate bounds: algebraic decoding requires R_c ≤ 1 − 2 log2(q)/m, while soft decoding only requires R_c ≤ 1 − log2(q)/m. Examples with Golay, Reed–Solomon, BCH, and Reed–Muller codes confirm the predicted finite-to-infinite transitions.

Load-bearing premise

The argument depends on the high-SNR approximations to the per-photon likelihoods being accurate enough that a small cube of Bob's soft measurements, of fixed width around the bin boundary, lies entirely inside the correct codeword's decision region; if that cube is not fully inside, the exponential error bound does not follow.

Editorial extensions

If this is right

  • If the condition L ≤ t holds, bounded-distance algebraic reconciliation has error probability O(e^(−cγ)) instead of the polynomial decay typical of coded fading channels.
  • If the code is MFD deficient, soft-decision reconciliation has infinite diversity; conversely, a full-MFD code forces finite diversity ω/2 for some weight ω ≥ d_Hmin(C_b).
  • Soft reconciliation attains infinite diversity at rates up to R_c ≤ 1 − log2(q)/m, while algebraic reconciliation is limited to R_c ≤ 1 − 2 log2(q)/m, so the soft-decision rate penalty is half that of algebraic decoding.
  • Short codes such as the [24,12,8] Golay code and [6,3,3] shortened Hamming code reach infinite diversity under soft decoding at modest frame sizes (m = 3 or more coded bits per photon), while algebraic decoding needs larger frames.
  • The results imply a sudden, qualitative improvement in reconciliation error rate once the code parameters cross the threshold, an effect not observed in classical Rayleigh or Nakagami fading channels.

Reading between the lines

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

  • Editorial extension: If the infinite-diversity condition holds at modest SNR, TE-QKD implementations could tolerate larger detector jitter or use fewer bins per frame while still keeping reconciliation errors negligible; the paper states the exponential decay but does not quantify this operational trade-off.
  • Editorial extension: Because the MFD property depends on which labels are neighbors of zero, the claimed independence of the Gray-labeling version could be tested directly by comparing a standard and a centered Gray code on the same code; if the MFD classification changes, the labeling independence claim would need qualification.
  • Editorial extension: The same two-scale error structure—polynomial near-boundary events and exponential far-boundary events—may appear in other timing or quantization channels, suggesting that infinite diversity could be engineered wherever a decoder can absorb all low-order boundary-crossing error patterns.
  • Editorial extension: A practical verification would measure the frame error rate slope for an MFD-deficient code at multiple SNR values; if the slope continues to increase without flattening, the infinite-diversity prediction is confirmed, whereas saturation at a finite slope would indicate a missing dominant error event.
Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

4 major / 4 minor

Summary. The paper studies the diversity order of coded information reconciliation in time-entanglement QKD (TE-QKD). It derives high-SNR transition laws separating single-bin jumps (polynomial probability) from multi-bin jumps (exponential probability), and it formulates two main results: Theorem 1 gives a necessary and sufficient condition for infinite diversity under bounded-distance algebraic decoding in terms of the number of photons per codeword, while Theorem 2 claims that soft-decision decoding achieves infinite diversity if and only if the code is MFD deficient. The paper also presents rate bounds and simulation examples for Golay, Reed-Solomon, BCH, and Reed-Muller codes. The algebraic-decoding result is plausible, but the soft-decision characterization is not correct as stated.

Significance. If the main theorems were correct, the paper would report a striking phenomenon: a finite-diversity channel whose coded soft-decision decoder produces exponentially decaying error probability with finite-length codes. The split of the transition probabilities in Proposition 1 and the algebraic-decoding condition in Theorem 1 are useful and appear sound. However, the central soft-decision claim is false: the proof of Theorem 2 relies on an invalid reduction to the all-zero codeword, and an explicit counterexample shows an MFD-deficient code with finite diversity. The examples and tables based on Theorem 2 therefore do not validate the claimed theory.

major comments (4)
  1. [Section V-C, Theorem 2 sufficiency proof] The sufficiency proof of Theorem 2 is invalid because it assumes, 'without loss of generality and thanks to the code linearity,' that the transmitted word c_A is the all-zero word. Code linearity translates the set of competing codewords, but it does not translate the Gray-label adjacency relation: a single-bin jump from a nonzero label lands on a label that is Hamming-adjacent to that nonzero label, not necessarily to the zero label. Concretely, take m=3 with the standard reflected Gray code and the binary [6,2,2] code C=span(111111,010010). The nonzero codewords are 111111, 010010, and 101101; none uses only the zero-neighboring labels {001,100}, so C is MFD deficient by Definition 4. Yet if Alice transmits c_A=111111 and Bob's measured positions both fall in bin 6, the competing codeword 101101 has higher APP in each coordinate. This event consists of two single-bin jumps and has probability Θ(γ^{-1}), giving finite diversity at most 1. This directly contradicts Theorem 2 statement 1.
  2. [Theorem 2 proof, DMZ cube inclusion after Eq. (51)] Even in the zero-word case, the proof does not establish that the cube of side Δ lies entirely in the correct decision region. The derivation of Eq. (51) equates APP(c_A) and APP(c'_A) only at the single point y_ℓ = x_ℓ + 1 + Δ. The proof then asserts that this cube is included in the decision region of c_A without proving monotonicity of the APP ratio over the whole cube. This missing monotonicity argument is load-bearing for the claimed O(e^{-Δ²γ/4}) pairwise-error bound and hence for the sufficiency of MFD deficiency.
  3. [Lemma 6 necessary-condition proof] The necessity direction inherits the same translation problem. Lemma 6 constructs a finite-diversity lower-bound event using a full-MFD codeword whose labels are neighbors of zero, implicitly taking the transmitted word to be the all-zero word. For a nonzero transmitted word, the physical single-bin jumps are neighbors of the transmitted labels, not neighbors of zero. Thus the statement that full MFD implies finite diversity is not established for general transmissions. Both directions of the claimed equivalence in Theorem 2 are therefore unsupported.
  4. [Section III-B, Gray-labeling independence claim] The paper states that the results do not depend on the Gray-labeling version chosen. This is contradicted by Definition 3, which counts neighbors of the all-zero label; changing the Gray labeling changes the zero-neighboring set and can change the MFD status of a code. The RM(2,4) and RM(2,5) tables show different MFD distributions for different generator-matrix versions, illustrating the dependence. More fundamentally, a correct diversity condition must depend on the geometric adjacency of the transmitted labels, so the labeling-independence claim is not established.
minor comments (4)
  1. [Abstract and Introduction] The phrases 'shocking result' and 'never encountered in the literature' are overstated and are not appropriate for a technical claim that is not established by the proofs.
  2. [Section IV, around Lemma 3 and Proposition 1] The notation for exponential terms is inconsistent in a few places: for example, the text after Proposition 2 in [24] is quoted as O(e^{γ/4}), while the correct decaying form is O(e^{-γ/4}). Please harmonize the notation.
  3. [Table I and Table II] The layout of the Gray-code tables is garbled and should be redrawn so that the bin number, Gray label, and photon position are clearly aligned.
  4. [Lemma 5 proof, Eq. (48)] The proof says 'the calculus details are not shown' for the exact integration leading to Eq. (48). Since Lemma 5 is used in the main theorem, the intermediate steps should be included or a reference provided.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the infinite-diversity conditions are derived from the channel's high-SNR separation and the code's MFD property, not from fitted parameters or a self-citation chain.

full rationale

The paper's central claims are characterizations rather than disguised inputs. Theorem 1's condition L = n/m <= t follows from Proposition 1's separation of single-bin jumps (Theta(gamma^{-1/2})) from multi-bin jumps (O(e^{-gamma/4})), combined with the Gray-code fact that one single-bin jump flips one coded bit; no parameter is fitted to force the target conclusion. Theorem 2's MFD-deficiency condition is defined independently of the diversity result (Definitions 3-4, in terms of codewords, Gray labels, and the frame parameter m), and the proof attempts to show that the MAP decision region for a competing word is exponentially hard to enter unless the word is composed entirely of zero-neighboring labels; the characterization is therefore not a definitional identity, even though the proof's 'without loss of generality' reduction to the all-zero word is a correctness gap rather than a circular step. The paper does rely on the same authors' prior work [24] for the channel model, transition probabilities, and simplified APP expressions (13)-(14), but that is a published, parameter-free channel model and does not already contain the infinite-diversity theorem; it is a legitimate foundation rather than a smuggled conclusion. No fitted-input-called-prediction pattern, no uniqueness-imported-from-authors pattern, and no renaming of a known result as a new one are present. The skeptical counterexample to Theorem 2 is a substantive mathematical challenge to the validity of the WLOG/linearity step and to the Gray-label translation invariance, but a false or unproven step is not the same as circularity. Overall, the derivation chain is not equivalent to its inputs by construction.

Assumptions & free parameters 0 free parameters · 6 assumptions · 0 invented entities

The paper introduces the MFD property as a mathematical definition, not a new physical entity. The central claims rest on the Gaussian-jitter channel model, the Gray-labeling assumption, and the simplified APP expressions inherited from [24]. No parameters are fitted to data; the only free system parameters are the number of bins N and the noise variance sigma^2, which are physical inputs rather than tuning knobs.

assumptions (6)
  • domain assumption Detector jitter is modeled as independent additive Gaussian noise on both Alice's and Bob's measured photon positions (Eq. 1).
    This is the channel model taken from [24] and used throughout; the diversity conclusions depend on the Gaussian tails.
  • domain assumption The TE-QKD channel is memoryless, with independent photon-pair realizations and independent jitters across channel uses.
    Invoked in Section II to justify the product form of the APP expressions and the independence of per-photon error events.
  • domain assumption A Gray labeling of the time bins is used, so a single-bin jump flips exactly one bit in the m-bit label.
    This is the basis for the claim that t+1 single-bin jumps produce t+1 bit errors, which is central to Theorems 1 and 2.
  • domain assumption The simplified high-SNR APP expressions (13)-(14) from [24] are valid approximations for the soft-decision analysis.
    Used in the proofs of Lemma 6 and Theorem 2 to compare competing codewords; no proof of their uniformity at decision boundaries is given.
  • domain assumption At high SNR, the exact photon position U is uniform in [0,N[ and all bins are equiprobable given valid frames (Eqs. 55, 59).
    Adapted from [24] and used in Lemmas 1-4 to simplify the transition probability integrals.
  • domain assumption A t-bounded algebraic decoder corrects all error patterns of Hamming weight at most t and fails on patterns of weight greater than t.
    Standard definition of bounded-distance decoding, invoked in the proof of Theorem 1.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Diversity in Coded TE-QKD Channels: Achieving Infinite Diversity out of Finite System Resources." pith.science (2026). https://pith.science/paper/4PVIABZ6

@misc{pith2026260805432,
  author       = {Pith},
  title        = {Pith review of: Diversity in Coded TE-QKD Channels: Achieving Infinite Diversity out of Finite System Resources},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/4PVIABZ6}},
  note         = {Machine review of arXiv:2608.05432}
}
read the original abstract

We establish conditions and give proofs on how an error-correcting code can attain infinite diversity in a time-entanglement quantum key distribution (TE-QKD) reconciliation. The shocking result, never encountered in the literature on coding and communication theory, is that a decoder exhibits an infinite diversity order while the channel has finite diversity and the code has a relatively short finite length. This paper studies the diversity order of coded TE-QKD reconciliation, defined by the asymptotic slope of the error probability at high signal-to-noise ratio. For bounded-distance algebraic decoding, we derive a necessary and sufficient condition in terms of the number of photons per codeword and the decoding radius. For soft-decision decoding, we introduce the maximal finite diversity (MFD) property and prove that infinite diversity is achieved if and only if the code is MFD deficient. The infinite diversity in TE-QKD has no counterpart in classical fading channels, where decoding can only multiply a finite diversity order by a finite factor. Examples of short codes based on Golay, Reed-Solomon, Bose-Chaudhuri-Hocquenghem (BCH), and Reed-Muller codes validate the analysis and illustrate how the TE-QKD system parameters and the relatively short code parameters affect the achievable diversity for both hard and soft information reconciliation.

Figures

Figures reproduced from arXiv: 2608.05432 by the authors.

Figure 1
Figure 1. The frame structure on Alice’s side showing the photon position before and after detection jitter noise. X, ˜ Y˜ ∈ R, where Z1 and Z2 are independent identically distributed (i.i.d.) Gaussian noise with zero mean and variance σ 2 , denoted as N (0, σ2 ), modeling the detection jitter. The random variable U ∼ Unif([0, N[) is uniform in the real range [0, N[, N ∈ N, N ≥ 2. The variable U is the jitter-free photon posi… view at source ↗
Figure 2
Figure 2. Slepian table of the binary repetition [3, 1, 3]2 code (within the bold frame) and the syndrome on the left. In the first example of [PITH_FULL_IMAGE:figures/full_fig_p012_2.png] view at source ↗
Figure 3
Figure 3. Slepian table of the shortened Hamming code [6, 3, 3]2 (within the bold frame) and the syndrome on the left. mL = n log2 (q), assuming that the channel introduces no memory between the L photons, define the a posteriori probability as AP P(υ) = P(ˆcA = υ|Y = y) = Y L ℓ=1 P(ϕ(υℓ)|yℓ) = Y L ℓ=1 AP P(ϕ(υℓ)), υℓ ∈ F m 2 , υ ∈ F mL 2 . (12) For yˆℓ = j and ϕ(υℓ) = i ∈ ZN , the APP could be solved via Bayes rule from the … view at source ↗
Figures from the paper (13 more)
Figure 4
Figure 4. Figure 4: Hard-decision (algebraic) versus soft-decision of a binary shortened [30, 20, t = 2] BCH code, N = 8 bins per frame. 10-7 10-6 10-5 10-4 10-3 10-2 10-1 0 10 20 30 40 50 60 Peb [3,1,3] algebraic decoding Peb [3,1,3] soft decoding Slope of 1/SNR Slope of 1/SNR1.5 Probabi…
Figure 5
Figure 5. Figure 5: Hard-decision (algebraic) versus soft-decision of a 3-fold repetition binary [3, 1, 3] code, N = 8 bins per frame [PITH_FULL_IMAGE:figures/full_fig_p015_5.png]
Figure 6
Figure 6. Figure 6: Frame illustration for (a) Uˆ = i and (b) Uˆ = i − 1, while Xˆ = i and Yˆ = i + 1. Lemma 1. Consider the U − X − Y model where i ≤ X < i + 1 and i + 1 ≤ Y < i + 2. Thus, Xˆ = i and Yˆ = i + 1. Then, we have P(Yˆ = i + 1 | Xˆ = i) = 1 √πγ + O(e − γ 4 ) = Θ(γ −1/2 ). (17…
Figure 7
Figure 7. Figure 7: Hard-decision (algebraic) versus soft-decision of a [6, 3, 3]2 shortened binary Hamming code, N = 8 bins per frame. The fantastic performance of the [6, 3, 3, t = 1]2 in soft reconciliation is due to its infinite diversity, as we will prove in the sequel. It also impli…
Figure 8
Figure 8. Figure 8: Euclidean distances involved in the APP evaluation in (37) and (38). The APP per photon includes the squared Euclidean distances to the two borders of a bin. Binary labels are defined in Table I. For σ 2 ≪ 1, the soft reconciliation of cB will yield one of the two comp…
Figure 9
Figure 9. Figure 9: (a) Left: the decision boundary separating the region of cA (below) from the region of c ′ A (above). (b) Right: the demilitarized zone (hashed) defined by the square of side ∆. Lemma 5 (Demilitarized Zone (DMZ)). Assume that Alice’s detector measures the photon positi…
Figure 10
Figure 10. Figure 10: Representation of the two bins i and i + 1 with the demilitarized zone of width ∆. Proof: The demilitarized zone is illustrated by the red rectangle in [PITH_FULL_IMAGE:figures/full_fig_p032_10.png]
Figure 11
Figure 11. Figure 11: sketches cA and c ′ A with the full MF D(ω, ω) property. For simplicity, [PITH_FULL_IMAGE:figures/full_fig_p035_11.png]
Figure 12
Figure 12. Figure 12: Photon positions yℓ of Bob for bins 1 ≤ ℓ ≤ ω (left in (a)) and for bins ω < ℓ ≤ L (right in (b)). Then, by (13) and (14), we obtain AP P(cA) ∝ Yω ℓ=1 1 2  e − (yℓ−xˆℓ−1)2 2σ2 − e − (yℓ−xˆℓ ) 2 2σ2  · Y L ℓ=ω+1  1 − 1 2 e − (yℓ−xˆℓ ) 2 2σ2 − 1 2 e − (yℓ−xˆℓ−1)2 2σ2…
Figure 13
Figure 13. Figure 13: Alice’s word cA and a competing word c ′ A of weight ω, where the MFD(ω, L1) property is satisfied, L1 < ω, and the number of photons per word is L = L0 + L1 + L2 ≥ 1. • Consider the case where n log2 (q) is multiple of m, i.e., L = n log2 (q) m is integer, L ≥ 1, and…
Figure 14
Figure 14. Figure 14: Photon positions yℓ of Bob for bins 1 ≤ ℓ ≤ L1 (left in (a)) and for bins L1 < ℓ ≤ L1 +L2 (right in (b)). The competing word c ′ A makes the code MFD(ω, L1), where 0 ≤ L1 < ω, 0 < L2, and 0 < L1 + L2 ≤ ω. Bob’s photons positions for the L0 bins with identical labels h…
Figure 15
Figure 15. Figure 15: Hard reconciliation of TE-QKD via complete algebraic decoding of the extended binary [24, 12, 8]2 Golay code. N = 8, 16, 64, and 256 bins per frame, N = 2m, m coded bits per photon. Diversity follows the result of Theorem 1 and Table IV. 10−7 10−6 10−5 10−4 10−3 10−2 …
Figure 16
Figure 16. Figure 16: Soft reconciliation of TE-QKD via soft-decision decoding of the extended binary [24, 12, 8]2 Golay code. N = 4, 8, 16, and 64 bins per frame, N = 2m, m coded bits per photon. Diversity follows the result of Theorem 2 and Table IV [PITH_FULL_IMAGE:figures/full_fig_p04…

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

42 extracted references · 36 canonical work pages

  1. [1]

    Quantum cryptography: Public key distribution and coin tossing,

    C. H. Bennett and G. Brassard, “Quantum cryptography: Public key distribution and coin tossing,” Theoretical Computer Science , vol. 560, pp. 7–11, 2014

  2. [2]

    Quantum cryptography based on Bell’s theorem,

    A. K. Ekert, “Quantum cryptography based on Bell’s theorem,” Physical Review Letters , vol. 67, no. 6, pp. 661–663, Aug. 1991

  3. [3]

    Secure quantum key distribution with realistic devices,

    F. Xu, X. Ma, Q. Zhang, H.-K. Lo, and J.-W. Pan, “Secure quantum key distribution with realistic devices,” Reviews of Modern Physics , vol. 92, no. 2, p. 025002, May 2020. doi: 10.1103/RevModPhys.92.025002

  4. [4]

    Advances in quantum cryptography,

    S. Pirandola, U. L. Andersen, L. Banchi, M. Berta, D. Bunandar, R. Colbeck, D. Englund, T. Gehring, C. Lupo, C. Ottaviani, et al. , “Advances in quantum cryptography,” Advances in Optics and Photonics , vol. 12, no. 4, pp. 1012–1236, 2020

  5. [5]

    Secret key reconciliation using BCH code in quantum key distribution,

    W. Traisilanun, K. Sripimanwat, and O. Sangaroon, “Secret key reconciliation using BCH code in quantum key distribution,” in Proc. Int. Symp. Communications and Information Technologies (ISCIT) , Sydney, Australia, pp. 1482–1485, Oct. 2007

  6. [6]

    Efficient reconciliation protocol for discrete-variable quantum key distribution,

    D. Elkouss, A. Leverrier, R. Alléaume, and J. J. Boutros, “Efficient reconciliation protocol for discrete-variable quantum key distribution,” in Proc. IEEE International Symposium on Information Theory (ISIT) , pp. 1879–1883, 2009

  7. [7]

    High performance error correction for quantum key distribution using polar codes,

    P . Jouguet and S. Kunz-Jacques, “High performance error correction for quantum key distribution using polar codes,” Quantum Info. Comput., vol. 14, pp. 329–338, 2014

  8. [8]

    Improved reconciliation with polar codes in quantum key distribution,

    S. Lee, J. Park, and J. Heo, “Improved reconciliation with polar codes in quantum key distribution,” Quantum Info. Comput. , vol. 18, pp. 795–813, 2018

Show all 42 references
  1. [9]

    Blind Information Reconciliation With Polar Codes for Quantum Key Distribution,

    E. Kiktenko, A. O. Malyshev, and A. Fedorov, “Blind Information Reconciliation With Polar Codes for Quantum Key Distribution,” IEEE Communications Letters , vol. 25, no. 1, pp. 79–83, 2021, doi: 10.1109/LCOMM.2020.3021142

  2. [10]

    Asymmetric Adaptive LDPC-Based Information Reconciliation for Industrial Quantum Key Distribution,

    N. Borisov, I. Petrov, and A. Tayduganov, “Asymmetric Adaptive LDPC-Based Information Reconciliation for Industrial Quantum Key Distribution,” Entropy, vol. 25, 2022, doi: 10.3390/e25010031

  3. [11]

    Rateless Protograph LDPC Codes for Quantum Key Distribution,

    A. Tarable, R. Paganelli, and M. Ferrari, “Rateless Protograph LDPC Codes for Quantum Key Distribution,” IEEE Transactions on Quantum Engineering , vol. 5, pp. 1–11, 2024, doi: 10.1109/TQE.2024.3361810

  4. [12]

    Diversity and multiplexing in quantum MIMO channels,

    J. ur Rehman, L. Oleynik, S. Koudia, M. Bayraktar, and S. Chatzinotas, “Diversity and multiplexing in quantum MIMO channels,” EPJ Quantum Technology , vol. 12, no. 1, Art. no. 18, 2025

  5. [13]

    Free-space optical communication through atmospheric turbulence channels,

    X. Zhu and J. M. Kahn, “Free-space optical communication through atmospheric turbulence channels,” IEEE Trans. Commun. , vol. 50, no. 8, pp. 1293–1300, Aug. 2002, doi: 10.1109/tcomm.2002.800829

  6. [14]

    Fast adaptive optics for high-dimensional quantum communications in turbulent channels,

    L. Scarfe, F. Hufnagel, M. Ferrer-Garcia, A. D’Errico, K. Heshami, and E. Karimi, “Fast adaptive optics for high-dimensional quantum communications in turbulent channels,” Communications Physics , vol. 8, 2023,

  7. [15]

    Long-distance free- space measurement-device-independent quantum key distribution,

    Y . Cao, Y . Li, K.-X. Y ang, Y .-F. Jiang, S.-L. Li, X.-L. Hu, M. Abulizi, C.-L. Li, W. Zhang, Q.-C. Sun, W. Liu, X. Jiang, S. Liao, J.-G. Ren, H. Li, L. Y ou, Z. Wang, J. Yin, C.-Y . Lu, X.-B. Wang, Q. Zhang, C.-Z. Peng, and J.-W. Pan, “Long-distance free- space measurement-...

  8. [16]

    Atmospheric effects on continuous-variable quantum key distribution,

    S. Wang, P . Huang, T. Wang, and G. Zeng, “Atmospheric effects on continuous-variable quantum key distribution,” New J. Phys. , vol. 20, no. 8, Art. no. 083037, 2018, doi: 10.1088/1367-2630/aad9c4

  9. [17]

    Entanglement of Gaussian states and the applicability to quantum key distribution over fading channels,

    V . C. Usenko, B. Heim, C. Peuntinger, C. Wittmann, C. Marquardt, G. Leuchs, and R. Filip, “Entanglement of Gaussian states and the applicability to quantum key distribution over fading channels,” New J. Phys. , vol. 14, no. 9, Art. no. 093048, 2012

  10. [18]

    Quantum key distribution over combined atmospheric fading channels,

    N. Hosseinidehaj and R. Malaney, “Quantum key distribution over combined atmospheric fading channels,” in Proc. IEEE Int. Conf. Commun. (ICC) , London, U.K., Jun. 2015, pp. 7413–7419,

  11. [19]

    Limits and security of free-space quantum communications,

    S. Pirandola, “Limits and security of free-space quantum communications,” Phys. Rev. Research , vol. 3, no. 1, Art. no. 013279, 2021. 54

  12. [20]

    Spatial-mode diversity and multiplexing for continuous variables quantum communications,

    S. Koudia, L. Oleynik, J. Ur Rehman, and S. Chatzinotas, “Spatial-mode diversity and multiplexing for continuous variables quantum communications,” Communications Physics , vol. 8, no. 1, p. 351, 2025

  13. [21]

    Signal space diversity: A power- and bandwidth-efficient diversity technique for the Rayleigh fading channel,

    J. Boutros and E. Viterbo, “Signal space diversity: A power- and bandwidth-efficient diversity technique for the Rayleigh fading channel,” IEEE Transactions on Information Theory , vol. 44, no. 4, pp. 1453–1467, 1998

  14. [22]

    Coded diversity on block-fading channels,

    E. Malkamäki and H. Leib, “Coded diversity on block-fading channels,” IEEE Transactions on Information Theory , vol. 45, no. 2, pp. 771–781, 2002

  15. [23]

    Tse and P

    D. Tse and P . Viswanath, Fundamentals of Wireless Communication . Cambridge University Press, 2005

  16. [24]

    Time-Entanglement QKD: Secret Key Rates and Information Reconciliation Coding,

    J.J. Boutros and E. Soljanin, “Time-Entanglement QKD: Secret Key Rates and Information Reconciliation Coding,” IEEE Trans. on Comm., vol. 71, no. 12, pp. 7174-7188, Dec. 2023

  17. [25]

    QKD based on time-entangled photons and its key-rate promise,

    L. Dolecek and E. Soljanin, “QKD based on time-entangled photons and its key-rate promise,” IEEE BITS: The Information Theory Magazine, vol. 2, no. 3, pp. 39–48, 2023

  18. [26]

    Photon-efficient quantum key distribution using time–energy entanglement with high-dimensional encoding,

    T. Zhong, H. Zhou, R. D. Horansky, C. Lee, V . B. V erma, A. E. Lita, A. Restelli, J. C. Bienfang, R. P . Mirin, T. Gerrits, S. W. Nam, F. Marsili, M. D. Shaw, Z. Zhang, L. Wang, D. Englund, G. W. Wornell, J. H. Shapiro, and F. N. C. Wong, “Photon-efficient quantum key distribu...

  19. [27]

    Continuous-variable quantum key distribution with low-complexity information reconciliation,

    X. Wang, H. Wang, C. Zhou, Z. Chen, S. Y u, and H. Guo, “Continuous-variable quantum key distribution with low-complexity information reconciliation,” Opt. Express , vol. 30, no. 17, pp. 30455–30465, Aug. 2022, doi: 10.1364/OE.461665

  20. [28]

    Reconciliation Efficiency Impact on Discrete Modulated CV -QKD Systems Key Rates,

    M. Almeida, D. F. Pereira, M. Facão, A. N. Pinto, and N. Silva, “Reconciliation Efficiency Impact on Discrete Modulated CV -QKD Systems Key Rates,” J. Lightw. Technol., vol. 41, no. 18, pp. 6134–6141, Sept. 2023, doi: 10.1109/jlt.2023.3280076

  21. [29]

    El Gamal and Y

    A. El Gamal and Y . H. Kim, Network Information Theory . Cambridge University Press, 2011

  22. [30]

    Biglieri, Coding for Wireless Channels

    E. Biglieri, Coding for Wireless Channels . Springer, 2005

  23. [31]

    Low-Density Parity-Check Codes for Nonergodic Block-Fading Channels,

    J.J. Boutros, A. Guillén i Fàbregas, E. Biglieri, and G. Zémor, “Low-Density Parity-Check Codes for Nonergodic Block-Fading Channels,” IEEE Trans. on Inf. Theory , vol. 56, no. 9, pp. 4286-4300, Sept. 2010

  24. [32]

    Effective Diversity and Coding Gain over Fluid Antenna Channels,

    N. V ashakidze, J.J. Boutros, G.M. Kraidy, and I. Krikidis, “Effective Diversity and Coding Gain over Fluid Antenna Channels,” IEEE 25th Intern. Work. on Sig. Proc. Advances in Wireless Communications (SPAWC), Italy, Sept. 2024

  25. [33]

    Proakis and M

    J.G. Proakis and M. Salehi, Digital communications . McGraw-Hill, 5th edition, 2008

  26. [34]

    On performance analysis for signaling on correlated fading channels,

    V .V . V eeravalli, “On performance analysis for signaling on correlated fading channels,” IEEE Trans. Comm. , vol. 49, no. 11, pp. 1879- 1883, Nov. 2001

  27. [35]

    MacWilliams and N.J.A

    F.J. MacWilliams and N.J.A. Sloane, The Theory of Error-Correcting Codes . Amsterdam, The Netherlands: North-Holland, 1977

  28. [36]

    M. K. Simon, and M. S. Alouini Digital communication over fading channels, John Wiley & Sons , 2004

  29. [37]

    Performance of MRC Diversity Systems for the Detection of Signals with Nakagami Fading,

    E. Al-Hussaini and A.A.M. Al-Bassiouni, "Performance of MRC Diversity Systems for the Detection of Signals with Nakagami Fading," IEEE Trans. Commun , vol. COM-33, pp. 1315-1319, Dec. 1985

  30. [38]

    A class of binary signaling alphabets,

    D. Slepian, “A class of binary signaling alphabets,” Bell System Technical Journal , vol. 35, no. 1, pp. 203234, 1956

  31. [39]

    R. E. Blahut, Algebraic codes for data transmission . Cambridge University Press, 2003

  32. [40]

    Improved Decoding of ReedSolomon Codes and Algebraic Geometry Codes,

    V . Guruswami and M. Sudan, "Improved Decoding of ReedSolomon Codes and Algebraic Geometry Codes," IEEE Trans. Inform. Theory, vol. 45, no. 6, pp. 1757-1767, Sept. 1999

  33. [41]

    Turbo code Design for block fading channels,

    J.J. Boutros, E. Calvanese Strinati, and Guillén i Fàbregas, "Turbo code Design for block fading channels," Allertons Conference on Communication and Control , Illinois, Oct. 2004

  34. [42]

    Analysis of coding on non-ergodic block fading channels,

    J.J. Boutros, A. Guillén i Fàbregas, and E. Calvanese Strinati, "Analysis of coding on non-ergodic block fading channels," Allertons Conference on Communication and Control , Illinois, Sept. 2005

Pith tools

Reviewed August 8, 2026 · model on record in the stance chip above.