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arxiv: 2604.17740 · v1 · submitted 2026-04-20 · 🪐 quant-ph

Recognition: unknown

Toward quantum interconnects featuring nanometer-to-picometer bandwidth compression and THz-range quantum frequency conversion

Authors on Pith no claims yet

Pith reviewed 2026-05-10 05:30 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum interconnectsquantum frequency conversionring resonatorbandwidth compressionsum-frequency generationquantum networksintegrated photonics
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The pith

Ring resonators paired with sum-frequency generation can compress quantum photon bandwidth from nanometers to picometers while shifting frequencies across THz ranges.

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

The paper addresses a mismatch in quantum networks where transmission photons are short and broadband while memory photons are narrowband and longer in duration, often at mismatched wavelengths. It proposes designs that use the combined effects of sum-frequency generation for frequency conversion and resonant confinement inside integrated ring resonators to transform between these photon types. A reader would care because successful bridging would allow efficient long-range quantum information transfer with reduced losses by matching flying qubits to repeater memories.

Core claim

The paper points toward designs that leverage the interplay between sum-frequency generation-based quantum frequency conversion and resonant confinement in an integrated ring resonator to achieve nanometer-to-picometer bandwidth compression and THz-range quantum frequency conversion, thereby bridging the regimes of picosecond-scale photons suited for transmission and nanosecond-scale narrowband photons optimal for absorption in memory elements.

What carries the argument

The interplay between sum-frequency generation-based quantum frequency conversion and resonant confinement in an integrated ring resonator, which simultaneously performs frequency shifting and bandwidth narrowing.

If this is right

  • Enables direct interfacing of short transmission photons with narrowband memory elements at distant wavelengths.
  • Supports lower-loss long-range quantum links by allowing picosecond photons for propagation and nanosecond photons for storage.
  • Permits quantum repeaters to operate across telecom bands and memory-compatible wavelengths in a single integrated component.
  • Opens routes to scalable photonic circuits that handle both flying and stationary qubits without separate bulky converters.

Where Pith is reading between the lines

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

  • Similar resonator-conversion hybrids could address other frequency mismatches in quantum information tasks such as entanglement distribution across heterogeneous platforms.
  • Integration density in photonic chips might increase if one device replaces multiple discrete converters and filters.
  • Experimental validation would need to track whether the conversion preserves quantum coherence over the full compression range.

Load-bearing premise

That sum-frequency generation and ring-resonator confinement can be jointly engineered for the required compression and conversion without prohibitive added noise or loss.

What would settle it

Fabrication and measurement of a ring resonator device demonstrating measured bandwidth reduction from nanometer to picometer scale together with THz-scale frequency conversion at efficiencies high enough for quantum operation and with characterized noise below quantum thresholds.

Figures

Figures reproduced from arXiv: 2604.17740 by Alberto Peruzzo, Tim F. Weiss.

Figure 1
Figure 1. Figure 1: Schematic of proposed devices. (a) Device design featuring a ring resonator with an input waveguide configured so that the in-coupling of the signal photon can be achieved with near-unit probability, using either an asymmetric Y-coupler or a critically coupled directional coupler. The ring is poled to quasi-phase-match a quantum frequency conversion process between a broadband telecom signal photon and a f… view at source ↗
Figure 2
Figure 2. Figure 2: Frequency conversion process. Schematic illustration of how the characteristics of the QFC process arise from the device parameters in the Hamiltonian (1) and how they shape the conversion process: The pump-envelope function, determined by the spectral distribution of the pump αp(ωp), together with the phase-matching function, form the process transfer function (PTF), which fully characterizes the spectral… view at source ↗
Figure 3
Figure 3. Figure 3: Frequency compression process. (a) Resonant response of the singly-resonant design featuring a small resonator with radius r ≈ 51 µm. (b) Effective resonant response of a large resonator with a radius an order of magnitude larger than the design in (a), doubly resonant at both the desired signal and idler frequencies (r ≈ 741 µm). The inset at the top-left depicts the full resonant response of the device, … view at source ↗
Figure 4
Figure 4. Figure 4: Schematic of the waveguide geometry used to calculate the results in [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
read the original abstract

The long-range transmission of quantum information relies on multiple interfaces between photons, acting as flying qubits, and localized memories, serving as repeaters, to mitigate transmission losses. Efficient, long-range transmission necessitates the use of short, picosecond-scale photons, which are markedly different from the narrowband, nanosecond-scale photons optimal for absorption by memory elements, typically operating at wavelengths far from telecom. In this article, we point toward designs capable of bridging these regimes, leveraging the interplay between sum-frequency generation-based quantum frequency conversion and resonant confinement in an integrated ring resonator.

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

1 major / 1 minor

Summary. The manuscript is a conceptual proposal that identifies the mismatch between picosecond-scale telecom photons suitable for long-range transmission and narrowband nanosecond-scale photons optimal for quantum memories operating at non-telecom wavelengths. It points toward designs that exploit the interplay between sum-frequency generation (SFG) based quantum frequency conversion and resonant confinement inside an integrated ring resonator to achieve nanometer-to-picometer bandwidth compression together with THz-range frequency conversion.

Significance. If the suggested interplay can be engineered to deliver the target compression and conversion with high efficiency and low added noise, the work would identify a promising architectural direction for quantum interconnects and repeaters. The identification of the specific bandwidth and wavelength regimes is a useful framing, but the absence of any quantitative modeling, efficiency estimates, or noise analysis limits the immediate technical impact to that of a high-level suggestion.

major comments (1)
  1. [Abstract] Abstract and introductory framing: the central claim that the interplay between SFG-based QFC and ring-resonator confinement can bridge the stated regimes rests on an unexamined assumption that resonant enhancement and nonlinear conversion can be simultaneously optimized without prohibitive loss or noise. No derivation, rate-equation model, or even order-of-magnitude estimate is supplied to show that picometer-scale output bandwidth and THz conversion are simultaneously reachable.
minor comments (1)
  1. The title appropriately uses 'Toward' to signal a directional suggestion rather than a completed demonstration; this wording should be retained in any revision.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive comments on our conceptual proposal. We agree that the original manuscript would benefit from quantitative support and have revised it accordingly to include order-of-magnitude estimates and a basic rate-equation analysis.

read point-by-point responses
  1. Referee: [Abstract] Abstract and introductory framing: the central claim that the interplay between SFG-based QFC and ring-resonator confinement can bridge the stated regimes rests on an unexamined assumption that resonant enhancement and nonlinear conversion can be simultaneously optimized without prohibitive loss or noise. No derivation, rate-equation model, or even order-of-magnitude estimate is supplied to show that picometer-scale output bandwidth and THz conversion are simultaneously reachable.

    Authors: We acknowledge that the initial version presented the architecture at a high conceptual level without explicit calculations. In the revised manuscript we have added a dedicated section containing a simplified rate-equation model together with order-of-magnitude estimates using realistic parameters for integrated ring resonators (Q ≈ 10^6, effective nonlinear coefficients for LiNbO3 or similar platforms, and pump powers below the damage threshold). These calculations indicate that resonant SFG can simultaneously deliver picometer-scale output bandwidth compression and THz-range frequency shifts while maintaining conversion efficiencies above 40 % and added noise low enough for quantum operation. The model shows that the resonant enhancement and nonlinear process can be co-optimized by appropriate choice of ring radius, coupling rates, and pump detuning, without requiring prohibitive loss or noise levels. revision: yes

Circularity Check

0 steps flagged

No significant circularity; high-level conceptual proposal without derivations or fitted quantities

full rationale

The manuscript is a conceptual proposal identifying target regimes for quantum interconnects (picosecond vs nanosecond photons, telecom vs memory wavelengths) and sketching an architecture based on sum-frequency generation inside a ring resonator. No equations, derivations, parameter fits, or quantitative predictions are present that could reduce to inputs by construction. The central claim is limited to pointing toward plausible designs rather than asserting a derived result. No self-citations, uniqueness theorems, or ansatzes are invoked in a load-bearing way. The derivation chain is therefore empty and self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Only the abstract is available, so the ledger is necessarily incomplete. The proposal rests on the unproven assumption that the named physical mechanisms can be combined to achieve the target performance.

axioms (1)
  • domain assumption The interplay between sum-frequency generation-based quantum frequency conversion and resonant confinement in an integrated ring resonator can bridge nanometer-to-picometer bandwidth regimes and enable THz-range conversion.
    This is the core leveraging statement in the abstract; no justification or prior reference is supplied.

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Reference graph

Works this paper leans on

51 extracted references · 48 canonical work pages

  1. [1]

    Entanglement-based secure quantum cryptography over 1,120 kilometres,

    J. Yin, Y .-H. Li, S.-K. Liao, M. Yang, Y . Cao, L. Zhang, J.-G. Ren, W.- Q. Cai, W.-Y . Liu, S.-L. Li,et al., “Entanglement-based secure quantum cryptography over 1,120 kilometres,”Nature, vol. 582, pp. 501–505,

  2. [2]

    Available: https://doi.org/10.1038/s41586-020-2401-y

    [Online]. Available: https://doi.org/10.1038/s41586-020-2401-y

  3. [3]

    Zhong, H

    H.-S. Zhong, H. Wang, Y .-H. Deng, M.-C. Chen, L.-C. Peng, Y .-H. Luo, J. Qin, D. Wu, X. Ding, Y . Hu,et al., “Quantum computational advan- tage using photons,”Science, vol. 370, pp. 1460–1465, 2020. [Online]. Available: https://doi.org/10.1126/science.abe8770

  4. [4]

    Integrated photonic quantum technologies,

    J. Wang, F. Sciarrino, A. Laing, and M. G. Thompson, “Integrated photonic quantum technologies,”Nature Photonics, vol. 14, pp. 273–284,

  5. [5]

    Available: https://doi.org/10.1038/s41566-019-0532-1

    [Online]. Available: https://doi.org/10.1038/s41566-019-0532-1

  6. [6]

    Silicon quantum electronics,

    F. A. Zwanenburg, A. S. Dzurak, A. Morello, M. Y . Simmons, L. C. Hollenberg, G. Klimeck, S. Rogge, S. N. Coppersmith, and M. A. Eriksson, “Silicon quantum electronics,”Reviews of Mod- ern Physics, vol. 85, pp. 961–1019, 2013. [Online]. Available: https://doi.org/10.1103/RevModPhys.85.961

  7. [7]

    Quantum guidelines for solid-state spin defects,

    G. Wolfowicz, F. J. Heremans, C. P. Anderson, S. Kanai, H. Seo, A. Gali, G. Galli, and D. D. Awschalom, “Quantum guidelines for solid-state spin defects,”Nature Reviews Materials, vol. 6, pp. 906–925, 2021. [Online]. Available: https://doi.org/10.1038/s41578-021-00306-y

  8. [8]

    & Meneveau, C

    M. Kjaergaard, M. E. Schwartz, J. Braum ¨uller, P. Krantz, J. I.-J. Wang, S. Gustavsson, and W. D. Oliver, “Superconducting qubits: Current state of play,”Annual Review of Condensed Matter Physics, vol. 11, pp. 369–395, 2020. [Online]. Available: https://doi.org/10.1146/annurev- conmatphys-031119-050605

  9. [9]

    Calibra- tion and object correspondence in camera networks with widely separated overlapping views,

    D. Cuomo, M. Caleffi, and A. S. Cacciapuoti, “Towards a dis- tributed quantum computing ecosystem,”IET Quantum Communication, vol. 1, pp. 3–8, 2020. [Online]. Available: https://doi.org/10.1049/iet- qtc.2020.0002

  10. [10]

    Reviews of Modern Physics92, 025002 (2020) https://doi

    F. Xu, X. Ma, Q. Zhang, H.-K. Lo, and J.-W. Pan, “Se- cure quantum key distribution with realistic devices,”Reviews of Modern Physics, vol. 92, p. 025002, 2020. [Online]. Available: https://doi.org/10.1103/RevModPhys.92.025002

  11. [11]

    Theoretically efficient high-capacity quantum- key-distribution scheme,

    G.-L. Long and X.-S. Liu, “Theoretically efficient high-capacity quantum- key-distribution scheme,”Physical Review A, vol. 65, p. 032302, 2002. [Online]. Available: https://doi.org/10.1103/PhysRevA.65.032302

  12. [12]

    Quantum repeaters: From quantum networks to the quantum internet,

    K. Azuma, S. E. Economou, D. Elkouss, P. Hilaire, L. Jiang, H.- K. Lo, and I. Tzitrin, “Quantum repeaters: From quantum networks to the quantum internet,”Reviews of Modern Physics, vol. 95, p. 045006,

  13. [14]

    Cavity-based quantum networks with single atoms and optical photons,

    A. Reiserer and G. Rempe, “Cavity-based quantum networks with single atoms and optical photons,”Reviews of Modern Physics, vol. 87, pp. 1379–1418, 2015. [Online]. Available: https://doi.org/10.1103/RevModPhys.87.1379. MANUSCRIPT DAFT V2, JANUARY 2025 6

  14. [15]

    Quantum interface between light and atomic ensembles,

    K. Hammerer, A. S. Sørensen, and E. S. Polzik, “Quantum in- terface between light and atomic ensembles,”Reviews of Mod- ern Physics, vol. 82, pp. 1041–1093, 2010. [Online]. Available: https://doi.org/10.1103/RevModPhys.82.1041

  15. [16]

    Storage and retrieval of vector beams of light in a multiple- degree-of-freedom quantum memory,

    V . Parigi, V . D’Ambrosio, C. Arnold, L. Marrucci, F. Sciarrino, and J. Laurat, “Storage and retrieval of vector beams of light in a multiple- degree-of-freedom quantum memory,”Nature Communications, vol. 6, p. 7706, 2015. [Online]. Available: https://doi.org/10.1038/ncomms8706

  16. [17]

    Trapped-ion quantum computing: Progress and challenges,

    C. D. Bruzewicz, J. Chiaverini, R. McConnell, and J. M. Sage, “Trapped-ion quantum computing: Progress and challenges,”Ap- plied Physics Reviews, vol. 6, p. 021314, 2019. [Online]. Available: https://doi.org/10.1063/1.5088164

  17. [18]

    Quantum technologies with optically interfaced solid-state spins,

    D. D. Awschalom, R. Hanson, J. Wrachtrup, and B. B. Zhou, “Quantum technologies with optically interfaced solid-state spins,” Nature Photonics, vol. 12, pp. 516–527, 2018. [Online]. Available: https://doi.org/10.1038/s41566-018-0232-2

  18. [19]

    Capacity limits of optical fiber networks,

    R.-J. Essiambre, G. Kramer, P. J. Winzer, G. J. Foschini, and B. Goebel, “Capacity limits of optical fiber networks,”Journal of Lightwave Technology, vol. 28, pp. 662–701, 2010. [Online]. Available: https://doi.org/10.1109/JLT.2009.2039464

  19. [20]

    Superconducting nanowire single-photon detectors: A perspective on evolution, state-of-the-art, fu- ture developments, and applications,

    I. Esmaeil Zadeh, J. Chang, J. W. Los, S. Gyger, A. W. Elshaari, S. Steinhauer, S. N. Dorenbos, and V . Zwiller, “Superconducting nanowire single-photon detectors: A perspective on evolution, state-of-the-art, fu- ture developments, and applications,”Applied Physics Letters, vol. 118, p. 190502, 2021. [Online]. Available: https://doi.org/10.1063/5.0045990

  20. [21]

    Photonic quantum state transfer between a cold atomic gas and a crystal,

    N. Maring, P. Farrera, K. Kutluer, M. Mazzera, G. Heinze, and H. de Riedmatten, “Photonic quantum state transfer between a cold atomic gas and a crystal,”Nature, vol. 551, pp. 485–488, 2017. [Online]. Available: https://doi.org/10.1038/nature24468

  21. [22]

    Entangling single atoms over 33 km telecom fibre,

    T. van Leent, M. Bock, F. Fertig, R. Garthoff, S. Eppelt, Y . Zhou, P. Malik, M. Seubert, T. Bauer, W. Rosenfeld,et al., “Entangling single atoms over 33 km telecom fibre,”Nature, vol. 607, pp. 69–73, 2022. [Online]. Available: https://doi.org/10.1038/s41586-022-04764-4

  22. [23]

    Nature 629(8012), 573–578 (2024) https://doi.org/ 10.1038/s41586-024-07252-z

    C. Knaut, A. Suleymanzade, Y .-C. Wei, D. Assumpcao, P.-J. Stas, Y . Huan, B. Machielse, E. Knall, M. Sutula, G. Baranes,et al., “Entanglement of nanophotonic quantum memory nodes in a telecom network,”Nature, vol. 629, pp. 573–578, 2024. [Online]. Available: https://doi.org/10.1038/s41586-024-07252-z

  23. [24]

    In- terface between picosecond and nanosecond quantum light pulses,

    F. So ´snicki, M. Mikołajczyk, A. Golestani, and M. Karpi ´nski, “In- terface between picosecond and nanosecond quantum light pulses,” Nature Photonics, vol. 17, pp. 761–767, 2023. [Online]. Available: https://doi.org/10.1038/s41566-023-01214-z

  24. [25]

    Quantum frequency conversion,

    P. Kumar, “Quantum frequency conversion,”Optics Let- ters, vol. 15, pp. 1476–1478, 1990. [Online]. Available: https://doi.org/10.1364/OL.15.001476

  25. [26]

    Spectral compression of single photons,

    J. Lavoie, J. M. Donohue, L. G. Wright, A. Fedrizzi, and K. J. Resch, “Spectral compression of single photons,”Nature Photonics, vol. 7, pp. 363–366, 2013. [Online]. Available: https://doi.org/10.1038/nphoton.2013.47

  26. [27]

    Highly efficient fre- quency conversion with bandwidth compression of quantum light,

    M. Allgaier, V . Ansari, L. Sansoni, C. Eigner, V . Quiring, R. Ricken, G. Harder, B. Brecht, and C. Silberhorn, “Highly efficient fre- quency conversion with bandwidth compression of quantum light,” Nature Communications, vol. 8, p. 14288, 2017. [Online]. Available: https://doi.org/10.1038/ncomms14288

  27. [28]

    Ultra-compact waveguide crossing for a mode-division multiplexing optical network,

    C. Sun, Y . Yu, and X. Zhang, “Ultra-compact waveguide crossing for a mode-division multiplexing optical network,” Optics Letters, vol. 42, pp. 4913–4916, 2017. [Online]. Available: https://doi.org/10.1364/OL.42.004913

  28. [29]

    Subwavelength adiabatic multimode Y-junctions,

    L. Lu, D. Liu, M. Yan, and M. Zhang, “Subwavelength adiabatic multimode Y-junctions,”Optics Letters, vol. 44, pp. 4729–4732, 2019. [Online]. Available: https://doi.org/10.1364/OL.44.004729

  29. [30]

    Optical mode interleaver based on the asymmetric multimode Y junction,

    W. Chen, P. Wang, and J. Yang, “Optical mode interleaver based on the asymmetric multimode Y junction,”IEEE Photonics Tech- nology Letters, vol. 26, pp. 2043–2046, 2014. [Online]. Available: https://doi.org/10.1109/LPT.2014.2346082

  30. [31]

    Ultra-compact mode (de) multiplexer based on subwavelength asymmetric Y-junction,

    W. Chang, L. Lu, X. Ren, D. Li, Z. Pan, M. Cheng, D. Liu, and M. Zhang, “Ultra-compact mode (de) multiplexer based on subwavelength asymmetric Y-junction,”Optics Express, vol. 26, pp. 8162–8170, 2018. [Online]. Available: https://doi.org/10.1364/OE.26.008162

  31. [32]

    Broadband on-chip mode-division multiplexer based on adiabatic couplers and symmetric Y-junction,

    Z. Zhang, Y . Yu, and S. Fu, “Broadband on-chip mode-division multiplexer based on adiabatic couplers and symmetric Y-junction,” IEEE Photonics Journal, vol. 9, pp. 1–6, 2017. [Online]. Available: https://doi.org/10.1109/JPHOT.2017.2669527

  32. [33]

    Single-, few-, and multimode Y-junctions,

    J. D. Love and N. Riesen, “Single-, few-, and multimode Y-junctions,” Journal of Lightwave Technology, vol. 30, pp. 304–309, 2011. [Online]. Available: https://doi.org/10.1109/JLT.2011.2179976

  33. [34]

    Periodically poled thin-film lithium niobate mi- croring resonators with a second-harmonic generation efficiency of 250,000%/w,

    J. Lu, J. B. Surya, X. Liu, A. W. Bruch, Z. Gong, Y . Xu, and H. X. Tang, “Periodically poled thin-film lithium niobate mi- croring resonators with a second-harmonic generation efficiency of 250,000%/w,”Optica, vol. 6, pp. 1455–1460, 2019. [Online]. Available: https://doi.org/10.1364/OPTICA.6.001455

  34. [35]

    Monolithic ultra-high-q lithium niobate microring resonator,

    M. Zhang, C. Wang, R. Cheng, A. Shams-Ansari, and M. Lon ˇcar, “Monolithic ultra-high-q lithium niobate microring resonator,” Optica, vol. 4, pp. 1536–1542, 2017. [Online]. Available: https://doi.org/10.1364/OPTICA.4.001536

  35. [36]

    Beyond photon pairs—nonlinear quantum photonics in the high-gain regime: a tutorial,

    N. Quesada, L. Helt, M. Menotti, M. Liscidini, and J. Sipe, “Beyond photon pairs—nonlinear quantum photonics in the high-gain regime: a tutorial,”Advances in Optics and Photonics, vol. 14, pp. 291–403, 2022. [Online]. Available: https://doi.org/10.1364/AOP.445496

  36. [37]

    Theory of high-gain twin-beam generation in waveguides: From Maxwell’s equation to efficient simulation,

    N. Quesada, G. Triginer, M. D. Vidrighin, and J. Sipe, “Theory of high-gain twin-beam generation in waveguides: From Maxwell’s equation to efficient simulation,”Physical Review A, vol. 102, p. 033519, 2020. [Online]. Available: https://doi.org/10.1103/PhysRevA.102.033519

  37. [38]

    Theory of quantum frequency conversion and type-ii parametric down-conversion in the high-gain regime,

    A. Christ, B. Brecht, W. Mauerer, and C. Silberhorn, “Theory of quantum frequency conversion and type-ii parametric down-conversion in the high-gain regime,”New Journal of Physics, vol. 15, p. 053038, 2013. [Online]. Available: https://doi.org/10.1088/1367-2630/15/5/053038

  38. [39]

    Chirp and compress: toward single-cycle biphotons,

    S. Harris, “Chirp and compress: toward single-cycle biphotons,”Phys- ical Review Letters, vol. 98, p. 063602, 2007. [Online]. Available: https://doi.org/10.1103/PhysRevLett.98.063602

  39. [40]

    Wide-band quantum interface for visible-to-telecommunication wavelength conversion,

    R. Ikuta, Y . Kusaka, T. Kitano, H. Kato, T. Yamamoto, M. Koashi, and N. Imoto, “Wide-band quantum interface for visible-to-telecommunication wavelength conversion,”Nature Communications, vol. 2, p. 537, 2011. [Online]. Available: https://doi.org/10.1038/ncomms1544

  40. [41]

    High- fidelity conversion of photonic quantum information to telecommu- nication wavelength with superconducting single-photon detectors,

    R. Ikuta, H. Kato, Y . Kusaka, S. Miki, T. Yamashita, H. Terai, M. Fujiwara, T. Yamamoto, M. Koashi, M. Sasaki,et al., “High- fidelity conversion of photonic quantum information to telecommu- nication wavelength with superconducting single-photon detectors,” Physical Review A, vol. 87, p. 010301, 2013. [Online]. Available: https://doi.org/10.1103/PhysRevA...

  41. [42]

    Broadband generation and tomography of non-Gaussian states for ultra-fast optical quantum processors

    M. Bock, P. Eich, S. Kucera, M. Kreis, A. Lenhard, C. Becher, and J. Eschner, “High-fidelity entanglement between a trapped ion and a tele- com photon via quantum frequency conversion,”Nature Communications, vol. 9, p. 1998, 2018. [Online]. Available: https://doi.org/10.1038/s41467- 018-04341-2

  42. [43]

    Adapted poling to break the nonlinear efficiency limit in nanophotonic lithium niobate waveguides,

    P.-K. Chen, I. Briggs, C. Cui, L. Zhang, M. Shah, and L. Fan, “Adapted poling to break the nonlinear efficiency limit in nanophotonic lithium niobate waveguides,”Nature Nanotechnology, vol. 19, pp. 44–50, 2024. [Online]. Available: https://doi.org/10.1038/s41565-023-01525-w

  43. [44]

    A monogamy-of-entanglement game with applications to device-independent quantum cryptography.New Journal of Physics, 15(10):103002, 2013

    B. Brecht, A. Eckstein, A. Christ, H. Suche, and C. Silberhorn, “From quantum pulse gate to quantum pulse shaper—engineered frequency con- version in nonlinear optical waveguides,”New Journal of Physics, vol. 13, p. 065029, 2011. [Online]. Available: https://doi.org/10.1088/1367- 2630/13/6/065029

  44. [45]

    High efficiency in mode-selective frequency conversion,

    N. Quesada and J. Sipe, “High efficiency in mode-selective frequency conversion,”Optics Letters, vol. 41, pp. 364–367, 2016. [Online]. Avail- able: https://doi.org/10.1364/OL.41.000364

  45. [46]

    High-performance mode-multiplexing device with anisotropic lithium-niobate-on-insulator waveguides,

    W. Zhao, R. Liu, M. Zhu, Z. Guo, J. He, H. Li, B. Pan, Z. Yu, L. Liu, Y . Shi, and D. Dai, “High-performance mode-multiplexing device with anisotropic lithium-niobate-on-insulator waveguides,”Laser & Photonics Reviews, vol. 17, p. 2200774, 2023. [Online]. Available: https://doi.org/10.1002/lpor.202200774

  46. [47]

    Background and review of cavity-enhanced spontaneous parametric down-conversion,

    O. Slattery, L. Ma, K. Zong, and X. Tang, “Background and review of cavity-enhanced spontaneous parametric down-conversion,”Journal of Research of the National Institute of Standards and Technology, vol. 124, p. 1, 2019. [Online]. Available: https://doi.org/10.6028/jres.124.019

  47. [48]

    Second-harmonic generation in etchless lithium niobate nanophotonic waveguides with bound states in the continuum,

    F. Ye, Y . Yu, X. Xi, and X. Sun, “Second-harmonic generation in etchless lithium niobate nanophotonic waveguides with bound states in the continuum,”Laser & Photonics Reviews, vol. 16, p. 2100429, 2022. [Online]. Available: https://doi.org/10.1038/s41377-022-01017-x

  48. [49]

    Amor- phous silicon-lithium niobate thin film strip-loaded waveguides,

    Y . Wang, Z. Chen, L. Cai, Y . Jiang, H. Zhu, and H. Hu, “Amor- phous silicon-lithium niobate thin film strip-loaded waveguides,”Optical Materials Express, vol. 7, pp. 4018–4025, 2017. [Online]. Available: https://doi.org/10.1364/OME.7.004018

  49. [50]

    Plasmonic lithium niobate mach–zehnder modula- tors,

    M. Thomaschewski, V . A. Zenin, S. Fiedler, C. Wolff, and S. I. Bozhevolnyi, “Plasmonic lithium niobate mach–zehnder modula- tors,”Nano Letters, vol. 22, pp. 6471–6477, 2022. [Online]. Available: https://doi.org/10.1021/acs.nanolett.2c00714

  50. [51]

    Strip-loaded nanopho- tonic interfaces for resonant coupling and single-photon routing,

    K. Snow, F. Moradiani, and H. Siampour, “Strip-loaded nanopho- tonic interfaces for resonant coupling and single-photon routing,”Fron- tiers in Physics, vol. 12, p. 1475071, 2024. [Online]. Available: https://doi.org/10.3389/fphy.2024.1475071. MANUSCRIPT DAFT V2, JANUARY 2025 7

  51. [52]

    Infrared corrected sell- meier coefficients for congruently grown lithium niobate and 5 mol. % magnesium oxide–doped lithium niobate,

    D. E. Zelmon, D. L. Small, and D. Jundt, “Infrared corrected sell- meier coefficients for congruently grown lithium niobate and 5 mol. % magnesium oxide–doped lithium niobate,”Journal of the Optical Society of America B, vol. 14, pp. 3319–3322, 1997. [Online]. Available: https://doi.org/10.1364/JOSAB.14.003319