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arxiv: 2606.10306 · v1 · pith:XR4BPE4M · submitted 2026-06-09 · quant-ph

Reconfigurable MDI-QKD and BB84 over 20 km optical channels via EOM-tailored weak coherent states

Jaesung Lim , Yonggi Jo , Nam Hun Park , Zaeill Kim , Yong Sup Ihn This is my paper

Reviewed by Pith2026-06-27 13:19 UTCgrok-4.3pith:XR4BPE4Mopen to challenge →

classification quant-ph
keywords MDI-QKDBB84weak coherent statesreconfigurable quantum key distributionHong-Ou-Mandel interferenceoptical fiber channelselectro-optic modulation
0
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The pith

A shared continuous-wave laser and one half-wave plate rotation let the same optical hardware run either MDI-QKD or BB84 over 20 km fiber channels.

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

The paper establishes that two mutually phase-randomized weak coherent states generated via electro-optic modulation and etalon filtering from one laser source can support measurement-device-independent quantum key distribution over 20 km channels, with the identical setup switched to standard BB84 by rotating a single half-wave plate 22.5 degrees in one arm. Channel indistinguishability is shown through time-resolved Hong-Ou-Mandel interference that approaches the classical limit of 0.5. A sympathetic reader would care because this removes the need for separate hardware for each protocol, cutting redundancy in quantum networks that must adapt to changing conditions.

Core claim

The central claim is that the transmitted states enable partial Bell-state measurement for MDI-QKD, while the system reconfigures directly for BB84 polarization encoding by the half-wave plate adjustment, all while preserving the same optical hardware and maintaining sufficient indistinguishability after 20 km transmission as verified by the reported interference visibility.

What carries the argument

EOM-tailored weak coherent states from a shared CW laser with etalon sideband filtering, combined with partial Bell-state measurement and half-wave plate rotation for protocol switching.

If this is right

  • MDI-QKD proceeds directly from the partial Bell-state measurement on the transmitted states.
  • BB84 operates on the same hardware after the 22.5-degree half-wave plate rotation without other changes.
  • Hardware redundancy drops because one module handles both protocols.
  • Operational flexibility increases for dynamic network environments.
  • EOM-based frequency engineering from a shared laser provides a practical route to scalable quantum communication.

Where Pith is reading between the lines

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

  • Networks could switch protocols on demand by remote control of the half-wave plate without physical hardware swaps.
  • The approach might extend to additional protocols if similar minimal adjustments preserve state indistinguishability.
  • Longer-distance tests would check whether the reported visibility holds over fibers beyond 20 km.
  • Integration with existing fiber infrastructure becomes simpler if the shared-laser source can serve multiple nodes.

Load-bearing premise

The two phase-randomized weak coherent states remain sufficiently indistinguishable after 20 km fiber transmission for secure partial Bell-state measurement to function.

What would settle it

A measured Hong-Ou-Mandel visibility that falls below 0.5 after 20 km transmission in a manner that prevents extraction of a positive secret key rate in the MDI-QKD configuration.

Figures

Figures reproduced from arXiv: 2606.10306 by Jaesung Lim, Nam Hun Park, Yonggi Jo, Yong Sup Ihn, Zaeill Kim.

Figure 1
Figure 1. Figure 1: FIG. 1. Experimental setup and spectral characterization of the reconfigurable QKD platform. (a) Schematic of the optical [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Experimental verification of phase randomization and two-photon indistinguishability. (a,b) First-order interference [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Evaluation of QKD performance in the MDI-QKD and BB84 operation modes. (a,b) Normalized single-photon count [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
read the original abstract

Measurement-device-independent quantum key distribution (MDI-QKD) is designed to eliminate detector side-channel vulnerabilities. However, its practical deployment remains experimentally demanding because it requires two-photon interference (TPI) between mutually phase-randomized optical states. In this study, we demonstrate a reconfigurable platform that supports both polarization encoded MDI-QKD and BB84 measurements utilizing the same optical hardware over 20 km optical fiber channels. Two mutually phase-randomized weak coherent states (WCSs) are generated from a shared continuous-wave (CW) laser via electro-optic phase modulation and subsequent etalon-based first-order sideband filtering. Channel indistinguishability is verified through Hong-Ou-Mandel (HOM) interference, combining time-resolved coincidence measurements and polarization mismatch scans, confirming a high degree of indistinguishability that robustly approaches the classical upper limit of 0.5 for WCSs. The transmitted states go through partial Bell-state measurement (BSM) to implement MDI-QKD. Here, the sytem can be directly reconfigured for BB84 simply by rotatinga single half-wave plate (HWP) by 22.5 degree in one arm of the module. This seamless reconfiguration drastically reduces hardware redundancy and enhances operational flexibility in dynamic network environments. These results indicate that EOM-based frequency engineering using a shared CW laser offers a highly practical route toward scalable and reconfigurable quantum communication systems.

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 / 3 minor

Summary. The manuscript demonstrates a reconfigurable optical platform supporting both polarization-encoded MDI-QKD and BB84 over 20 km fiber channels with the same hardware. Mutually phase-randomized weak coherent states are generated from a shared CW laser via EOM phase modulation and etalon sideband filtering; channel indistinguishability is verified via HOM interference (time-resolved coincidences and polarization scans) yielding visibility approaching the classical WCS limit of 0.5; partial BSM implements MDI-QKD; reconfiguration to BB84 occurs by rotating one HWP by 22.5°.

Significance. If the post-fiber indistinguishability and reconfiguration function as described, the work offers a practical route to flexible quantum networks by eliminating protocol-specific hardware duplication. The single-laser EOM+etalon method for consistent phase-randomized WCS generation is a technical strength that could reduce complexity in dynamic environments.

major comments (2)
  1. [Abstract] Abstract: the central claim of successful MDI-QKD after 20 km requires that the reported HOM visibility (approaching 0.5) suffices for positive key rate under a security proof, yet no measured visibility value with error bars, no quantum bit error rate, and no secret key rate are provided; without these the support for secure partial BSM cannot be assessed.
  2. [Abstract] Abstract: fiber-induced effects (differential polarization rotation, timing jitter, residual phase correlations) are not shown to be fully captured by the single HOM metric; if these degrade two-photon interference below the threshold needed for the MDI-QKD security analysis, the reconfiguration claim (which presupposes both modes function) does not hold.
minor comments (3)
  1. [Abstract] Abstract: 'sytem' is a typo for 'system'.
  2. [Abstract] Abstract: 'rotatinga' is missing a space; should read 'rotating a'.
  3. [Abstract] Abstract: '22.5 degree' should be '22.5 degrees'.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed review and constructive feedback on our manuscript. We address each major comment below, focusing on clarifying the scope of our demonstration and revising the abstract accordingly.

read point-by-point responses

  1. Referee: [Abstract] Abstract: the central claim of successful MDI-QKD after 20 km requires that the reported HOM visibility (approaching 0.5) suffices for positive key rate under a security proof, yet no measured visibility value with error bars, no quantum bit error rate, and no secret key rate are provided; without these the support for secure partial BSM cannot be assessed.

    Authors: We agree that the abstract phrasing implies a full MDI-QKD implementation with positive key rate, which is not supported by the presented data. Our work demonstrates a reconfigurable hardware platform capable of generating mutually phase-randomized WCSs, verifies post-fiber indistinguishability via HOM, and performs partial BSM, but does not include QBER measurements or secret key rate extraction. The HOM visibility value with error bars appears in the main text (HOM interference section). We will revise the abstract to state that the platform supports MDI-QKD via partial BSM on transmitted states with verified indistinguishability, without claiming a complete key distribution experiment. revision: yes

  2. Referee: [Abstract] Abstract: fiber-induced effects (differential polarization rotation, timing jitter, residual phase correlations) are not shown to be fully captured by the single HOM metric; if these degrade two-photon interference below the threshold needed for the MDI-QKD security analysis, the reconfiguration claim (which presupposes both modes function) does not hold.

    Authors: The time-resolved coincidence and polarization-scan HOM measurements are performed after the 20 km fiber transmission, so the reported visibility already incorporates fiber-induced effects on the two-photon interference. We will add explicit wording in the revised abstract and/or methods to clarify this. The BB84 reconfiguration is a separate hardware adjustment (single HWP rotation) that operates independently of the MDI-QKD interference threshold; we will ensure the abstract does not overstate interdependence between the two modes. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental demonstration with direct measurements

full rationale

The paper reports an experimental implementation of reconfigurable MDI-QKD and BB84 over 20 km fiber using EOM-generated phase-randomized WCS, with indistinguishability verified directly via time-resolved HOM coincidence measurements and polarization scans yielding visibility approaching 0.5. No derivation chain, equations, or fitted parameters are presented that reduce to inputs by construction; the central claims rest on hardware reconfiguration (HWP rotation) and measured performance metrics rather than any self-definitional, fitted-prediction, or self-citation load-bearing step. The work is self-contained against external benchmarks of experimental quantum optics.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Central claim rests on experimental generation and transmission of phase-randomized WCS with sufficient indistinguishability; no free parameters, axioms, or invented entities are introduced beyond standard quantum optics assumptions.

axioms (1)
  • standard math Quantum mechanics and linear optics govern the interference and measurement outcomes
    Invoked implicitly throughout the description of HOM interference and partial BSM

pith-pipeline@v0.9.1-grok · 5803 in / 1219 out tokens · 27999 ms · 2026-06-27T13:19:32.508223+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

21 extracted references · 1 canonical work pages · 1 internal anchor

  1. [1]

    Measurement of subpicosecond time intervals between two photons by interference,

    C. K. Hong, Z. Y. Ou, and L. Mandel, “Measurement of subpicosecond time intervals between two photons by interference,”Phys. Rev. Lett.59, 2044–2046 (1987)

    2044

  2. [2]

    Two-photon inter- ference: the Hong–Ou–Mandel effect,

    F. Bouchard, A. Sit, Y. Zhang, R. Fickler, F. M. Miatto, Y. Yao, F. Sciarrino, and E. Karimi, “Two-photon inter- ference: the Hong–Ou–Mandel effect,”Rep. Prog. Phys. 84, 012402 (2021)

    2021

  3. [3]

    Time- resolved two-photon quantum interference,

    T. Legero, T. Wilk, A. Kuhn, and G. Rempe, “Time- resolved two-photon quantum interference,”Appl. Phys. B77, 797–802 (2003)

    2003

  4. [4]

    Condi- tions for two-photon interference with coherent pulses,

    Y.-S. Kim, O. Slattery, P. S. Kuo, and X. Tang, “Condi- tions for two-photon interference with coherent pulses,” Phys. Rev. A87, 063843 (2013)

    2013

  5. [5]

    Two- photon interference with continuous-wave multi-mode co- herent light,

    Y.-S. Kim, O. Slattery, P. S. Kuo, and X. Tang, “Two- photon interference with continuous-wave multi-mode co- herent light,”Opt. Express22, 3611–3620 (2014)

    2014

  6. [6]

    Spectral char- acterization of weak coherent state sources based on two- photon interference,

    T. Ferreira da Silva, G. C. do Amaral, D. Vitoreti, G. P. Tempor˜ ao, and J. P. von der Weid, “Spectral char- acterization of weak coherent state sources based on two- photon interference,”J. Opt. Soc. Am. B32, 545–549 (2015)

    2015

  7. [7]

    Experimental study of Hong– Ou–Mandel interference using independent phase ran- domized weak coherent states,

    E. Moschandreou, J. I. Garcia, B. J. Rollick, B. Qi, R. Pooser, and G. Siopsis, “Experimental study of Hong– Ou–Mandel interference using independent phase ran- domized weak coherent states,”J. Lightwave Technol. 36, 3752–3759 (2018)

    2018

  8. [8]

    Hong–Ou– Mandel interference of two independent continuous-wave coherent photons,

    H. Kim, D. Kim, J. Park, and H. S. Moon, “Hong–Ou– Mandel interference of two independent continuous-wave coherent photons,”Photon. Res.8, 1491–1495 (2020)

    2020

  9. [9]

    Time-resolved two- photon interference of weak coherent pulses,

    H. Kim, O. Kwon, and H. S. Moon, “Time-resolved two- photon interference of weak coherent pulses,”Appl. Phys. Lett.118, 244001 (2021)

    2021

  10. [10]

    Se- cure quantum key distribution with realistic devices,

    F. Xu, X. Ma, Q. Zhang, H.-K. Lo, and J.-W. Pan, “Se- cure quantum key distribution with realistic devices,” Rev. Mod. Phys.92, 025002 (2020)

    2020

  11. [11]

    Measurement-device- independent quantum key distribution,

    H.-K. Lo, M. Curty, and B. Qi, “Measurement-device- independent quantum key distribution,”Phys. Rev. Lett. 108, 130503 (2012)

    2012

  12. [12]

    Hacking commercial quantum cryp- tography systems by tailored bright illumination,

    L. Lydersenet al., “Hacking commercial quantum cryp- tography systems by tailored bright illumination,”Nat. Photonics4, 686–689 (2010)

    2010

  13. [13]

    Full-field implementation of a perfect eavesdropper on a quantum cryptography sys- tem,

    I. Gerhardt, Q. Liu, A. Lamas-Linares, J. Skaar, C. Kurt- siefer, and V. Makarov, “Full-field implementation of a perfect eavesdropper on a quantum cryptography sys- tem,”Nat. Commun.2, 349 (2011)

    2011

  14. [14]

    Device-independent security of quan- tum cryptography against collective attacks,

    A. Ac´ ın, N. Brunner, N. Gisin, S. Massar, S. Pironio, and V. Scarani, “Device-independent security of quan- tum cryptography against collective attacks,”Phys. Rev. Lett.98, 230501 (2007)

    2007

  15. [15]

    Real-world two-photon interference and proof-of-principle quantum key distribution immune to detector attacks,

    A. Rubenok, J. A. Slater, P. Chan, I. Lucio-Martinez, and W. Tittel, “Real-world two-photon interference and proof-of-principle quantum key distribution immune to detector attacks,”Phys. Rev. Lett.111, 130501 (2013)

    2013

  16. [16]

    Experimental measurement-device- independent quantum key distribution,

    Y. Liuet al., “Experimental measurement-device- independent quantum key distribution,”Phys. Rev. Lett. 111, 130502 (2013)

    2013

  17. [17]

    Experimental demonstration of polarization encoding measurement-device-independent quantum key distribu- tion,

    Z. Tang, Z. Liao, F. Xu, B. Qi, L. Qian, and H.-K. Lo, “Experimental demonstration of polarization encoding measurement-device-independent quantum key distribu- tion,”Phys. Rev. Lett.112, 190503 (2014)

    2014

  18. [18]

    Measurement-device-independent quantum key distribution over untrustful metropolitan network,

    Y.-L. Tanget al., “Measurement-device-independent quantum key distribution over untrustful metropolitan network,”Phys. Rev. X6, 011024 (2016)

    2016

  19. [19]

    Free-space reconfigurable quantum key distribution network

    B. Qi, H.-K. Lo, C. C. W. Lim, G. Siopsis, E. A. Chi- tambar, R. Pooser, P. G. Evans, and W. Grice, “Free- space reconfigurable quantum key distribution network,” in2015 IEEE International Conference on Space Op- tical Systems and Applications (ICSOS)(IEEE, 2015), arXiv:1510.04891

    work page internal anchor Pith review Pith/arXiv arXiv 2015

  20. [20]

    Measurement-device-independent quantum key distribution for nonstandalone networks,

    G.-J. Fan-Yuanet al., “Measurement-device-independent quantum key distribution for nonstandalone networks,” Photon. Res.9, 1881–1891 (2021)

    2021

  21. [21]

    Precise tuning of single-photon frequency using an optical single sideband modulator,

    H. P. Lo and H. Takesue, “Precise tuning of single-photon frequency using an optical single sideband modulator,” Optica4, 919–923 (2017)

    2017