Fiber-integrated Quantum Frequency Conversion for Long-distance Quantum Networking
Pith reviewed 2026-05-08 08:11 UTC · model grok-4.3
The pith
Fiber-integrated QFC system maintains over 52% expected fidelity for NV centers over 100 km of fiber.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors build and test a fiber-integrated QFC system based on a PPLN waveguide that down-converts 637.2 nm photons to 1588.3 nm with approximately 9% efficiency and pump noise of 154 Hz. At input photon rates matching NV centers, the measured SNRs range from 12.3 to 117.8. Their model of loss, noise, and decoherence predicts that entanglement fidelity remains above 52% over 100 km of fiber transmission.
What carries the argument
Fiber-integrated periodically poled lithium niobate waveguide that performs down-conversion from visible to telecom wavelengths while suppressing pump-induced noise.
Load-bearing premise
The theoretical model fully captures every relevant loss, noise, and decoherence process during conversion and fiber transmission.
What would settle it
An experiment that directly measures the entanglement fidelity between an NV center spin and the frequency-converted photon after it travels through 100 km of fiber.
Figures
read the original abstract
Signal photons emitted by quantum nodes typically fall outside the low-loss telecom window of optical fibers, leading to severe transmission losses. Quantum frequency conversion (QFC) offers an effective optical interface that bridges quantum nodes with telecom-band channels, enabling long-distance quantum communication. In this work, we demonstrate a compact, fiber-integrated QFC system with low noise and a high signal-to-noise ratio (SNR). Using a periodically poled lithium niobate (PPLN) waveguide, input photons at 637.2 nm are down-converted to telecom photons at 1588.3 nm. Our system achieves a total conversion efficiency of approximately 9%, with pump-induced noise suppressed to 154 Hz. For input photon rates of 32.7, 118.0, and 327.7 kHz, the corresponding SNRs are 12.3, 43.9, and 117.8, respectively. We further develop a theoretical model to simulate the entanglement fidelity between nitrogen-vacancy (NV) center spins and the frequency-converted telecom photons. At the emission rate of an NV center, our QFC system maintains an expected fidelity exceeding 52% over a transmission distance of 100 km. These findings highlight the potential of our QFC system for scalable, long-distance quantum networking.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript demonstrates a compact, fiber-integrated quantum frequency conversion (QFC) system based on a periodically poled lithium niobate waveguide that down-converts 637.2 nm photons (NV-center emission) to 1588.3 nm telecom-band photons. It reports a total conversion efficiency of ~9%, pump-induced noise of 154 Hz, and signal-to-noise ratios of 12.3–117.8 for input rates of 32.7–327.7 kHz. A theoretical model is then used to predict that, at typical NV emission rates, the entanglement fidelity between the NV spin and the frequency-converted telecom photon exceeds 52% after 100 km of fiber transmission.
Significance. If the experimental characterization and the fidelity model both hold, the work provides a practical, low-noise optical interface that could enable NV-center-based quantum nodes to connect over long-distance telecom fibers. The direct measurements of efficiency and noise are reproducible and directly support the hardware claims; the parameter-free nature of the subsequent fidelity calculation (using only measured rates) is a strength. The 52% fidelity threshold over 100 km would be a meaningful benchmark for scalable quantum networking, provided the model is shown to capture all relevant loss and decoherence channels.
major comments (2)
- [Theoretical Model] Theoretical Model section (following the experimental results): the manuscript states that the model predicts fidelity >52% over 100 km at NV emission rates, yet provides no explicit comparison of the model's output against any measured fidelity or coincidence data from the QFC setup itself. Without this validation, it is unclear whether unmodeled effects (e.g., additional spectral diffusion or polarization drift during conversion) are negligible at the relevant photon rates.
- [Theoretical Model] Theoretical Model section, Eq. for fidelity (presumably the expression combining measured efficiency, noise rate, and fiber loss): the claim that the model 'fully accounts for all relevant loss, noise, and decoherence mechanisms' is not supported by a sensitivity analysis showing how the 52% figure changes when plausible additional decoherence terms (e.g., 1–2% extra visibility loss) are included. This directly affects the load-bearing networking claim.
minor comments (2)
- [Results] Figure 3 (or equivalent SNR plot): the three data points for SNR versus input rate are presented without error bars or a fit; adding these would clarify whether the reported linear scaling holds within experimental uncertainty.
- [Abstract] Abstract and §1: the phrase 'expected fidelity exceeding 52%' should be qualified as 'model-predicted' to avoid implying a measured value.
Simulated Author's Rebuttal
We thank the referee for their careful and constructive review of our manuscript. The comments on the theoretical model are helpful, and we address them point by point below. We have revised the manuscript where appropriate to improve clarity and add requested analysis.
read point-by-point responses
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Referee: Theoretical Model section (following the experimental results): the manuscript states that the model predicts fidelity >52% over 100 km at NV emission rates, yet provides no explicit comparison of the model's output against any measured fidelity or coincidence data from the QFC setup itself. Without this validation, it is unclear whether unmodeled effects (e.g., additional spectral diffusion or polarization drift during conversion) are negligible at the relevant photon rates.
Authors: We agree that a direct experimental comparison of modeled versus measured fidelity would strengthen the section. However, the current manuscript focuses on standalone characterization of the fiber-integrated QFC device (efficiency, noise, and SNR measurements) rather than a complete NV-center entanglement distribution experiment, which would be required to obtain measured spin-photon fidelity or coincidence data after conversion. The model is constructed in a parameter-free manner from the directly measured quantities (9% conversion efficiency, 154 Hz noise rate, and the three input photon rates) combined with standard fiber attenuation and NV emission statistics. We will revise the Theoretical Model section to explicitly list all assumptions, state that unmodeled effects such as spectral diffusion and polarization drift are expected to be small given the high measured SNRs (12.3–117.8), and note that a full experimental validation lies beyond the present scope but is planned for follow-on work. revision: partial
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Referee: Theoretical Model section, Eq. for fidelity (presumably the expression combining measured efficiency, noise rate, and fiber loss): the claim that the model 'fully accounts for all relevant loss, noise, and decoherence mechanisms' is not supported by a sensitivity analysis showing how the 52% figure changes when plausible additional decoherence terms (e.g., 1–2% extra visibility loss) are included. This directly affects the load-bearing networking claim.
Authors: The manuscript does not contain the exact phrasing 'fully accounts for all relevant loss, noise, and decoherence mechanisms,' but we accept that the robustness of the >52% fidelity prediction should be demonstrated more explicitly. We will add a sensitivity analysis to the revised Theoretical Model section. This analysis will quantify the effect of additional 1–2% visibility loss (arising, for example, from residual polarization mismatch or spectral diffusion) on the predicted fidelity after 100 km of fiber. The revised figure will show that the fidelity remains above 50% under these perturbations at typical NV emission rates, thereby supporting the practical relevance of the result for long-distance networking. revision: yes
Circularity Check
Fidelity estimate is a forward calculation from measured parameters
full rationale
The paper reports measured conversion efficiency (~9%) and noise rates (154 Hz) from the PPLN waveguide experiment, then feeds these into a standard quantum-optical model of loss, noise, and decoherence to compute expected entanglement fidelity (>52% at 100 km for NV emission rates). No derivation step reduces to a self-definition, fitted parameter renamed as prediction, or self-citation chain; the model parameters are independently measured and the calculation is falsifiable against external benchmarks. This is a normal, non-circular use of experimental inputs.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard quantum-optical models of noise and loss during frequency conversion and fiber transmission are sufficient to predict entanglement fidelity.
Reference graph
Works this paper leans on
-
[1]
Quantum internet: A vision for the road ahead,
S. Wehner, D. Elkouss, and R. Hanson, “Quantum internet: A vision for the road ahead,” Science362, eaam9288 (2018)
work page 2018
-
[2]
Quantum networks with neutral atom processing nodes,
J. P . Covey, H. Weinfurter, and H. Bernien, “Quantum networks with neutral atom processing nodes,” npj Quantum Inf.9, 90 (2023)
work page 2023
-
[3]
Towards real-world quantum networks: A review,
S.-H. Wei, B. Jing, X.-Y . Zhang,et al., “Towards real-world quantum networks: A review,” Laser & Photonics Rev.16, 2100219 (2022)
work page 2022
-
[4]
Experimental demon- stration of memory-enhanced quantum communication,
M. K. Bhaskar, R. Riedinger, B. Machielse,et al., “Experimental demon- stration of memory-enhanced quantum communication,” Nature580, 60–64 (2020)
work page 2020
-
[5]
L. Zhou, J. Lin, C. Ge,et al., “Independent-optical-frequency-comb- powered 546-km field test of twin-field quantum key distribution,” Phys. Rev. Appl.22, 064057 (2024)
work page 2024
-
[6]
Quantum teleportation with in- dependent sources and prior entanglement distribution over a network,
Q.-C. Sun, Y .-L. Mao, S.-J. Chen,et al., “Quantum teleportation with in- dependent sources and prior entanglement distribution over a network,” Nat. Photonics10, 671–675 (2016)
work page 2016
-
[7]
Hertz-rate metropolitan quantum teleportation,
S. Shen, C. Yuan, Z. Zhang,et al., “Hertz-rate metropolitan quantum teleportation,” Light. Sci. & Appl.12, 115 (2023)
work page 2023
-
[8]
Quantum entanglement network enabled by a state-multiplexing quantum light source,
Y .-R. Fan, Y . Luo, K. Guo,et al., “Quantum entanglement network enabled by a state-multiplexing quantum light source,” Light. Sci. & Appl.14, 189 (2025)
work page 2025
-
[9]
Universal distributed blind quantum computing with solid-state qubits,
Y .-C. Wei, P .-J. Stas, A. Suleymanzade,et al., “Universal distributed blind quantum computing with solid-state qubits,” Science388, 509– 513 (2025)
work page 2025
-
[10]
Longer-baseline tele- scopes using quantum repeaters,
D. Gottesman, T. Jennewein, and S. Croke, “Longer-baseline tele- scopes using quantum repeaters,” Phys. Rev. Lett.109, 070503 (2012)
work page 2012
-
[11]
Distributed quantum sensing with mode-entangled spin-squeezed atomic states,
B. K. Malia, Y . Wu, J. Martínez-Rincón, and M. A. Kasevich, “Distributed quantum sensing with mode-entangled spin-squeezed atomic states,” Nature612, 661–665 (2022)
work page 2022
-
[12]
Heralded entanglement be- tween widely separated atoms,
J. Hofmann, M. Krug, N. Ortegel,et al., “Heralded entanglement be- tween widely separated atoms,” Science337, 72–75 (2012)
work page 2012
-
[13]
Heralded entanglement be- tween solid-state qubits separated by three metres,
H. Bernien, B. Hensen, W. Pfaff,et al., “Heralded entanglement be- tween solid-state qubits separated by three metres,” Nature497, 86–90 (2013)
work page 2013
-
[14]
Heralded quantum entan- glement between two crystals,
I. Usmani, C. Clausen, F . Bussières,et al., “Heralded quantum entan- glement between two crystals,” Nat. Photonics6, 234–237 (2012)
work page 2012
-
[15]
Entanglement of nanophotonic quantum memory nodes in a telecom network,
C. M. Knaut, A. Suleymanzade, Y . C. Wei,et al., “Entanglement of nanophotonic quantum memory nodes in a telecom network,” Nature 629, 573–578 (2024)
work page 2024
-
[16]
Efficient and long-lived quantum memory with cold atoms inside a ring cavity,
X.-H. Bao, A. Reingruber, P . Dietrich,et al., “Efficient and long-lived quantum memory with cold atoms inside a ring cavity,” Nat. Phys.8, 517–521 (2012)
work page 2012
-
[17]
R. Ikuta, H. Kato, Y . Kusaka,et al., “High-fidelity conversion of photonic quantum information to telecommunication wavelength with supercon- ducting single-photon detectors,” Phys. Rev. A87, 010301(R) (2013)
work page 2013
-
[18]
Visible-to-telecom quantum frequency conversion of light from a single quantum emitter,
S. Zaske, A. Lenhard, C. Keßler,et al., “Visible-to-telecom quantum frequency conversion of light from a single quantum emitter,” Phys. Rev. Lett.109, 147404 (2012)
work page 2012
-
[19]
Quantum-dot spin-photon entanglement via frequency downconversion to telecom wavelength,
K. de Greve, L. Yu, P . L. McMahon,et al., “Quantum-dot spin-photon entanglement via frequency downconversion to telecom wavelength,” Nature491, 421–425 (2012)
work page 2012
-
[20]
Photonic quantum state transfer between a cold atomic gas and a crystal,
N. Maring, P . Farrera, K. Kutluer,et al., “Photonic quantum state transfer between a cold atomic gas and a crystal,” Nature551, 485–488 (2017)
work page 2017
-
[21]
S. Zhang, J. Shi, Y . Liang,et al., “Fast delivery of heralded atom- photon quantum correlation over 12 km fiber through multiplexing enhancement,” Nat. Commun.15, 10306 (2024)
work page 2024
-
[22]
Demonstration of quantum network protocols over a 14-km urban fiber link,
S. Kucera, C. Haen, E. Arenskötter,et al., “Demonstration of quantum network protocols over a 14-km urban fiber link,” npj Quantum Inf.10, 88 (2024)
work page 2024
-
[23]
Telecom-band quantum interference of frequency-converted photons from remote detuned nv centers,
A. Stolk, K. van der Enden, M.-C. Roehsner,et al., “Telecom-band quantum interference of frequency-converted photons from remote detuned nv centers,” PRX Quantum3, 020359 (2022)
work page 2022
-
[24]
Long-lived quantum memory en- abling atom-photon entanglement over 101 km of telecom fiber,
Y . Zhou, P . Malik, F . Fertig,et al., “Long-lived quantum memory en- abling atom-photon entanglement over 101 km of telecom fiber,” PRX Quantum5, 020307 (2024)
work page 2024
-
[25]
Multimode ion-photon entanglement over 101 kilometers,
V. Krutyanskiy, M. Canteri, M. Meraner,et al., “Multimode ion-photon entanglement over 101 kilometers,” PRX quantum5, 020308 (2024)
work page 2024
-
[26]
Spectral noise in frequency conversion from the visible to the telecommunication c-band,
P . C. Strassmann, A. Martin, N. Gisin, and M. Afzelius, “Spectral noise in frequency conversion from the visible to the telecommunication c-band,” Opt. Express27, 14298–14307 (2019)
work page 2019
-
[27]
Quantum frequency conversion of memory-compatible single photons from 606 nm to the telecom c-band,
N. Maring, D. Lago-Rivera, A. Lenhard,et al., “Quantum frequency conversion of memory-compatible single photons from 606 nm to the telecom c-band,” Optica5, 507–513 (2018). Research Article 6
work page 2018
-
[28]
Polarization-entanglement conserving frequency conversion of photons,
S. Ramelow, A. Fedrizzi, A. Poppe,et al., “Polarization-entanglement conserving frequency conversion of photons,” Phys. Rev. A85, 013845 (2012)
work page 2012
-
[29]
Quantum fre- quency conversion between infrared and ultraviolet,
H. Rütz, K.-H. Luo, H. Suche, and C. Silberhorn, “Quantum fre- quency conversion between infrared and ultraviolet,” Phys. Rev. Appl. 7, 024021 (2017)
work page 2017
-
[30]
F . Mann, H. M. Chrzanowski, F . Gewers,et al., “Low-noise quantum frequency conversion in a monolithic cavity with bulk periodically poled potassium titanyl phosphate,” Phys. Rev. Appl.20, 054010 (2023)
work page 2023
-
[31]
J. S. Pelc, L. Ma, C. R. Phillips,et al., “Long-wavelength-pumped upconversion single-photon detector at 1550 nm: performance and noise analysis,” Opt. Express19, 21445–21456 (2011)
work page 2011
-
[32]
Long-distance single photon transmission from a trapped ion via quantum frequency conversion,
T. Walker, K. Miyanishi, R. Ikuta,et al., “Long-distance single photon transmission from a trapped ion via quantum frequency conversion,” Phys. Rev. Lett.120, 203601 (2018)
work page 2018
-
[33]
S. Wengerowsky, S. Duranti, L. Heller, and H. de Riedmatten, “Quan- tum frequency conversion of photons with microsecond duration from the visible to the telecommunication c band,” Phys. Rev. Appl.23, 024049 (2025)
work page 2025
-
[34]
A. Dreau, A. Tchebotareva, A. E. Mahdaoui,et al., “Quantum frequency conversion of single photons from a nitrogen-vacancy center in dia- mond to telecommunication wavelengths,” Phys. Rev. Appl.9, 064031 (2018)
work page 2018
-
[35]
Low-noise quantum fre- quency conversion with cavity enhancement of the converted mode,
S. Murakami, T. Kobayashi, S. Miki,et al., “Low-noise quantum fre- quency conversion with cavity enhancement of the converted mode,” Opt. Quantum3, 55–63 (2025)
work page 2025
-
[36]
M. Schäfer, B. Kambs, D. Herrmann,et al., “Two-stage, low noise quantum frequency conversion of single photons from silicon-vacancy centers in diamond to the telecom c-band,” Adv. Quantum Technol.8, 2300228 (2025)
work page 2025
-
[37]
V. Esfandyarpour, C. Langrock, and M. Fejer, “Cascaded downconver- sion interface to convert single-photon-level signals at 650 nm to the telecom band,” Opt. Lett.43, 5655–5658 (2018)
work page 2018
-
[38]
Low-noise short-wavelength pumped frequency downconversion for quantum frequency converters,
J. F . Geus, F . Elsen, S. Nyga,et al., “Low-noise short-wavelength pumped frequency downconversion for quantum frequency converters,” Opt. Quantum2, 189–195 (2024)
work page 2024
-
[39]
Unconditional quantum teleportation between distant solid-state quantum bits,
W. Pfaff, B. J. Hensen, H. Bernien,et al., “Unconditional quantum teleportation between distant solid-state quantum bits,” Science345, 532–535 (2014)
work page 2014
-
[40]
C. Lu, H. Li, J. Qiu,et al., “Second and cascaded harmonic generation of pulsed laser in a lithium niobate on insulator ridge waveguide,” Opt. Express30, 1381–1387 (2022)
work page 2022
-
[41]
J. S. Pelc, C. Langrock, Q. Zhang, and M. M. Fejer, “Influence of domain disorder on parametric noise in quasi-phase matched quantum frequency converters,” Opt. Lett.35, 2804–2806 (2010)
work page 2010
-
[42]
Entangle- ment between a diamond spin qubit and a photonic time-bin qubit at telecom wavelength,
A. Tchebotareva, S. L. N. Hermans, P . C. Humphreys,et al., “Entangle- ment between a diamond spin qubit and a photonic time-bin qubit at telecom wavelength,” Phys. Rev. Lett.123, 063601 (2019)
work page 2019
-
[43]
Metropolitan-scale heralded entanglement of solid-state qubits,
A. J. Stolk, K. L. van der Enden, M.-C. Slater,et al., “Metropolitan-scale heralded entanglement of solid-state qubits,” Sci. Adv.10, eadp6442 (2024)
work page 2024
-
[44]
High-efficient coupler for thin-film lithium niobate waveguide devices,
C. Hu, A. Pan, T. Li,et al., “High-efficient coupler for thin-film lithium niobate waveguide devices,” Opt. Express29, 5397–5406 (2021)
work page 2021
-
[45]
D. Riedel, I. Söllner, B. J. Shields,et al., “Deterministic enhancement of coherent photon generation from a nitrogen-vacancy center in ultrapure diamond,” Phys. Rev. X7, 031040 (2017)
work page 2017
-
[46]
N. Singh and R. V. Nair, “Purcell and collection efficiency enhancement of single nv- center emission coupled to an asymmetric tamm structure,” Adv. Quantum Technol.6, 2200142 (2023). Fig. 1. Experimental setup. A continuous-wave (CW) laser at 637.2 nm (signal laser) is carved into optical pulses using an acousto-optic modulator (AOM), and then attenuated...
work page 2023
-
[47]
92476116), Beijing Municipal Natural Sci- ence Foundation (No
ACKNOWLEDGEMENTS This work was supported by the National Natural Science Foun- dation of China (No. 92476116), Beijing Municipal Natural Sci- ence Foundation (No. Z230005), and Quantum Science and Technology-National Science and Technology Major Project (No. 2024ZD0302500)
-
[48]
AUTHOR CONTRIBUTIONS L.Z. conceived the project. Z.C.L., L.Z., A.S. performed the ex- periments. Z.C.L. processed the data and derived the theoretical model. L.Z., Z.C.L., N.J., Z.Y. analyzed the results. Z.C.L. and L.Z. prepared the manuscript. All authors discussed, improved and approved the manuscript. Z.Y. supervised the project
-
[49]
Correspondenceand requests for materials should be ad- dressed to Lai Zhou
COMPETING INTERESTS The authors declare no competing interests. Correspondenceand requests for materials should be ad- dressed to Lai Zhou. Supplementary Information: Fiber-integrated Quantum Frequency Conversion for Long-distance Quantum Networking Zhichuan Liao, 1, 2, 3, 4 Ao Shen, 1, 5 Lai Zhou, 1,∗ Nan Jiang, 4 and Zhiliang Yuan 1 1Beijing Academy of ...
-
[50]
A. Tchebotarevaet al., Entanglement between a diamond spin qubit and a photonic time-bin qubit at telecom wavelength, Physical Review Letters123, 063601 (2019)
work page 2019
-
[51]
C. Wagenknechtet al., Experimental demonstration of a heralded entanglement source, Nature Photonics4, 549 (2010)
work page 2010
-
[52]
A. J. Stolket al., Metropolitan-scale heralded entanglement of solid-state qubits, Science Advances10, eadp6442 (2024)
work page 2024
discussion (0)
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