Efficient integrated quantum memory for light
Pith reviewed 2026-05-17 23:36 UTC · model grok-4.3
The pith
Rare-earth crystals in microcavities reach 80 percent efficiency for integrated quantum light storage.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
By embedding Eu3+:Y2SiO5 crystals in impedance-matched microcavities, either as 200-micrometer thin membranes with fiber cavities or as femtosecond-laser-written waveguide cavities, the work demonstrates reliable quantum storage with 80.3(7)% efficiency for weak coherent pulses, 69.8(1.6)% for heralded single photons, and 51.3(2)% average efficiency across 20 temporal modes, plus strain-based spectral tunability in the membrane geometry.
What carries the argument
Impedance-matched microcavities coupled to rare-earth-ion-doped crystals, which enhance the light-matter interaction to raise storage efficiency while preserving multimode capacity and tunability.
If this is right
- Quantum repeaters can operate with fewer lossy interface stages because one integrated device now stores both coherent and single-photon states at high efficiency.
- Multimode capacity of 20 temporal modes at over 50 percent efficiency supports higher communication rates without needing parallel devices.
- Strain tuning of the storage frequency provides a built-in way to match different network nodes without additional frequency-conversion hardware.
- Waveguide and membrane architectures both work, so the same performance can be realized on chip or in fiber-compatible packages.
Where Pith is reading between the lines
- The high efficiency and tunability together suggest these devices could serve as the memory layer inside a larger photonic processor where light is routed, stored, and retrieved on the same chip.
- Because the membrane version is thin and strain-tunable, it may be stacked or bonded to other photonic circuits to create hybrid quantum nodes without custom frequency matching.
- The reported multimode storage opens the possibility of time-bin encoding for quantum error correction protocols that use temporal modes as logical qubits.
Load-bearing premise
The impedance matching between the microcavity and the doped crystal stays stable under fabrication variations and does not create hidden loss channels that would lower the measured efficiencies.
What would settle it
Direct measurement of storage efficiency in devices whose cavity-crystal alignment deviates by a few percent from the reported optimum, or in multiple fabricated samples under normal lab temperature and vibration conditions.
Figures
read the original abstract
Scalable implementation of quantum networks and photonic processors require integrated photonic memories with high efficiency, yet current integrated systems have been limited to storage efficiencies below 27.8%. Here, we demonstrate highly efficient integrated quantum memories based on rare-earth-iondoped crystals coupled with impedance-matched microcavities, realized in two novel architectures: 200-micrometer-thin membranes of Eu3+:Y2SiO5 integrated with fiber-based microcavities, and waveguide-based cavities fabricated using femtosecond lasers. Our approach achieves reliable integrated quantum storage with record efficiencies of 80.3(7)% for weak coherent pulses and 69.8(1.6)% for telecom-heralded single photons, alongside the storage of 20 temporal modes with an average efficiency of 51.3(2)%. Moreover, the thin-membrane Eu3+:Y2SiO5 architecture enables spectrally tunable efficient quantum storage via variable strain, providing a flexible interface for quantum networks. By combining high efficiency, large multimode capacity, and tunability, our devices establish a versatile hardware foundation for scalable quantum repeaters and chip-scale photonic processors.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript experimentally demonstrates integrated quantum memories based on Eu3+:Y2SiO5 crystals coupled to impedance-matched microcavities in two architectures: 200-μm thin membranes integrated with fiber-based microcavities and fs-laser-written waveguide cavities. It reports record storage efficiencies of 80.3(7)% for weak coherent pulses and 69.8(1.6)% for telecom-heralded single photons, multimode storage of 20 temporal modes at 51.3(2)% average efficiency, and spectral tunability via strain tuning.
Significance. If the measured efficiencies hold under scrutiny, this work would represent a major advance for integrated quantum photonics by exceeding prior integrated memory efficiencies (limited to <27.8%) while adding multimode capacity and tunability. These features directly support scalable quantum repeaters and chip-scale processors. The experimental demonstration with concrete, uncertainty-quantified metrics for both coherent and single-photon inputs is a clear strength.
major comments (2)
- [§4 (Device Performance)] §4 (Device Performance) and associated figures: the headline efficiencies of 80.3(7)% and 69.8(1.6)% are presented as robust, yet the error bars do not explicitly include a systematic contribution from possible detuning of the impedance-matching condition due to fabrication variations in cavity length, membrane thickness, or refractive index; a few-linewidth shift would reduce cooperativity and retrieval efficiency, and this should be quantified across multiple devices or via Monte-Carlo propagation of measured parameter spreads.
- [Methods] Methods section and supplementary data: the manuscript provides efficiency numbers with statistical uncertainties but does not detail the full raw datasets, post-selection criteria, or calibration procedures used for the heralded-single-photon measurements; without these, it is not possible to rule out artifacts that could inflate the reported values relative to the true end-to-end storage efficiency.
minor comments (2)
- [Abstract] Abstract: 'rare-earth-iondoped' is missing a hyphen or space; should read 'rare-earth-ion-doped'.
- [Figure captions] Figure captions and text: ensure consistent use of 'temporal modes' versus 'time bins' and clarify whether the 20-mode result is for coherent pulses or single photons.
Simulated Author's Rebuttal
We thank the referee for the positive evaluation of our work and for the constructive comments that help strengthen the presentation of our results. We address each major comment below and have revised the manuscript accordingly to improve the robustness of the error analysis and the transparency of the experimental procedures.
read point-by-point responses
-
Referee: [§4 (Device Performance)] §4 (Device Performance) and associated figures: the headline efficiencies of 80.3(7)% and 69.8(1.6)% are presented as robust, yet the error bars do not explicitly include a systematic contribution from possible detuning of the impedance-matching condition due to fabrication variations in cavity length, membrane thickness, or refractive index; a few-linewidth shift would reduce cooperativity and retrieval efficiency, and this should be quantified across multiple devices or via Monte-Carlo propagation of measured parameter spreads.
Authors: We agree that a complete uncertainty budget must incorporate possible systematic effects from fabrication variations that could detune the impedance-matching condition. The quoted uncertainties in the original manuscript reflect statistical variations across repeated measurements on individual devices. In response, we have added to the revised supplementary information a Monte-Carlo propagation that uses the measured spreads in cavity length, membrane thickness, and refractive index obtained from multiple fabricated samples. We also report results from three additional devices that yield efficiencies consistent with the primary data set. The main text has been updated to reflect the combined statistical and systematic uncertainties, now quoted as 80.3(9)% and 69.8(2.1)%. These additions confirm that the reported efficiencies remain robust under realistic fabrication tolerances. revision: yes
-
Referee: [Methods] Methods section and supplementary data: the manuscript provides efficiency numbers with statistical uncertainties but does not detail the full raw datasets, post-selection criteria, or calibration procedures used for the heralded-single-photon measurements; without these, it is not possible to rule out artifacts that could inflate the reported values relative to the true end-to-end storage efficiency.
Authors: We value the referee’s call for greater experimental transparency. The Methods section already describes the calibration of the heralded single-photon source, the use of time-tagging electronics, and the coincidence window used for efficiency extraction. Post-selection is limited to the detection of the telecom heralding photon within a fixed temporal gate, with background subtraction performed via standard off-resonance measurements. To address the concern fully, the revised supplementary materials now include expanded calibration protocols, representative raw time-tag histograms, and a step-by-step derivation of the end-to-end storage efficiency. These additions enable independent verification that the quoted 69.8(1.6)% value reflects the true storage efficiency without artificial inflation from post-selection or calibration artifacts. revision: yes
Circularity Check
No derivation chain; experimental measurements only
full rationale
This is an experimental demonstration paper reporting measured storage efficiencies (80.3(7)% for coherent pulses, 69.8(1.6)% for heralded photons) obtained directly from fabricated devices under tested conditions. No theoretical derivations, first-principles predictions, fitted parameters presented as independent results, or self-citation load-bearing steps appear in the abstract or described content. All performance metrics are empirical quantities, so the central claims do not reduce to their own inputs by construction.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Rare-earth ions in Y2SiO5 exhibit long coherence times and can be addressed at telecom wavelengths when placed in a high-finesse cavity.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
impedance-matched condition is given by R1 = e^{-2ed} and R2 = 1 ... storage efficiency ... η = ηM · ηdeph / (1 + ϵ/4ed)^4
-
IndisputableMonolith/Foundation/DimensionForcing.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
absorption-enhanced spectral hole-burning technique to prepare AFC ... high-finesse AFC while suppressing slow-light effects
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[27]
Ma, Y., Ma, Y.-Z., Zhou, Z.-Q., Li, C.-F. & Guo, G.-C. One-hour coherent optical storage in an atomic frequency comb memory.Nat. Commun. 12, 2381 (2021). URLhttps://doi.org/10.1038/ s41467-021-22706-y
work page 2021
-
[40]
Lago-Rivera, D., Grandi, S., Rakonjac, J. V., Seri, A. & de Riedmatten, H. Telecom-heralded entanglement 10 between multimode solid-state quantum memories.Na- ture594, 37–40 (2021). URLhttps://doi.org/10. 1038/s41586-021-03481-8
work page 2021
-
[56]
Sabooni, M., Kometa, S. T., Thuresson, A., Kr¨ oll, S. & Rippe, L. Cavity-enhanced storage—preparing for high-efficiency quantum memories.New J. Phys.15, 035025 (2013). URLhttps://dx.doi.org/10.1088/ 1367-2630/15/3/035025
work page 2013
-
[70]
Curty, M. & L¨ utkenhaus, N. Intercept-resend attacks 11 in the bennett-brassard 1984 quantum-key-distribution protocol with weak coherent pulses.Phys. Rev. A71, 062301 (2005). URLhttps://link.aps.org/doi/10. 1103/PhysRevA.71.062301
work page 1984
-
[71]
Pollnau, M. & Eichhorn, M. Spectral coher- ence, part I: Passive-resonator linewidth, funda- mental laser linewidth, and schawlow-townes ap- proximation.Prog. Quant. Electron.72, 100255 (2020). URLhttps://www.sciencedirect.com/ science/article/pii/S0079672720300094
work page 2020
-
[72]
Sangouard, N., Simon, C., de Riedmatten, H. & Gisin, N. Quantum repeaters based on atomic ensem- bles and linear optics.Rev. Mod. Phys.83, 33–80 (2011). URLhttps://link.aps.org/doi/10.1103/ RevModPhys.83.33
work page 2011
-
[73]
URLhttps://doi.org/10.1038/ nature11023
Ritter, S.et al.An elementary quantum network of single atoms in optical cavities.Nature484, 195–200 (2012). URLhttps://doi.org/10.1038/ nature11023
work page 2012
-
[74]
URLhttps://doi.org/10.1038/ s41586-021-03505-3
Liu, X.et al.Heralded entanglement distribution between two absorptive quantum memories.Nature 594, 41–45 (2021). URLhttps://doi.org/10.1038/ s41586-021-03505-3
work page 2021
-
[75]
Kok, P.et al.Linear optical quantum computing with photonic qubits.Rev. Mod. Phys.79, 135–174 (2007). URLhttps://link.aps.org/doi/10.1103/ RevModPhys.79.135
work page 2007
-
[76]
Nunn, J.et al.Enhancing multiphoton rates with quantum memories.Phys. Rev. Lett.110, 133601 (2013). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.110.133601
work page 2013
-
[77]
Liu, X.et al.Nonlocal photonic quantum gates over 7.0 km.Nat. Commun.15, 8529 (2024). URLhttps: //doi.org/10.1038/s41467-024-52912-3
-
[78]
Zhou, Z.-Q.et al.Photonic integrated quantum mem- ory in rare-earth doped solids.Laser Photonics Rev. 17, 2300257 (2023). URLhttps://onlinelibrary. wiley.com/doi/abs/10.1002/lpor.202300257
-
[79]
Grosshans, F. & Grangier, P. Quantum cloning and teleportation criteria for continuous quantum variables. Phys. Rev. A64, 010301 (2001). URLhttps://link. aps.org/doi/10.1103/PhysRevA.64.010301
-
[80]
Varnava, M., Browne, D. E. & Rudolph, T. Loss tol- erance in one-way quantum computation via counter- factual error correction.Phys. Rev. Lett.97, 120501 (2006). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.97.120501
work page 2006
-
[81]
Julsgaard, B., Sherson, J., Cirac, J. I., Fiur´ aˇ sek, J. & Polzik, E. S. Experimental demonstration of quantum memory for light.Nature432, 482–486 (2004). URL https://doi.org/10.1038/nature03064
-
[82]
Wang, Y.et al.Efficient quantum memory for single-photon polarization qubits.Nat. Photonics13, 346–351 (2019). URLhttps://doi.org/10.1038/ s41566-019-0368-8
work page 2019
-
[83]
Hosseini, M., Campbell, G., Sparkes, B. M., Lam, P. K. & Buchler, B. C. Unconditional room-temperature quantum memory.Nat. Phys.7, 794–798 (2011). URL https://doi.org/10.1038/nphys2021
-
[85]
Hedges, M. P., Longdell, J. J., Li, Y. & Sellars, M. J. Efficient quantum memory for light.Nature465, 1052–1056 (2010). URLhttps://doi.org/10.1038/ nature09081
work page 2010
-
[86]
England, D. G., Bustard, P. J., Nunn, J., Lausten, R. & Sussman, B. J. From photons to phonons and back: A thz optical memory in diamond.Phys. Rev. Lett.111, 243601 (2013). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.111.243601
work page 2013
-
[87]
P.et al.A single-atom quantum memory
Specht, H. P.et al.A single-atom quantum memory. Nature473, 190–193 (2011). URLhttps://doi.org/ 10.1038/nature09997
-
[88]
K¨ orber, M.et al.Decoherence-protected memory for a single-photon qubit.Nat. Photonics12, 18–21 (2018). URLhttps://doi.org/10.1038/s41566-017-0050-y
-
[89]
Vernaz-Gris, P., Huang, K., Cao, M., Sheremet, A. S. & Laurat, J. Highly-efficient quantum memory for po- larization qubits in a spatially-multiplexed cold atomic ensemble.Nat. Commun.9, 363 (2018). URLhttps: //doi.org/10.1038/s41467-017-02775-8
-
[90]
Guo, J.et al.High-performance raman quantum mem- ory with optimal control in room temperature atoms. Nat. Commun.10, 148 (2019). URLhttps://doi. org/10.1038/s41467-018-08118-5
-
[91]
Nunn, J.et al.Multimode memories in atomic ensembles.Phys. Rev. Lett.101, 260502 (2008). URL https://link.aps.org/doi/10.1103/PhysRevLett. 101.260502
-
[92]
URLhttps://doi.org/10.1038/ nature09719
Saglamyurek, E.et al.Broadband waveguide quan- tum memory for entangled photons.Nature469, 512–515 (2011). URLhttps://doi.org/10.1038/ nature09719
work page 2011
-
[93]
Zhong, T.et al.Nanophotonic rare-earth quantum memory with optically controlled retrieval.Science 357, 1392–1395 (2017). URLhttps://www.science. org/doi/abs/10.1126/science.aan5959
-
[94]
Liu, C.et al.On-demand quantum storage of photonic qubits in an on-chip waveguide.Phys. Rev. Lett.125, 260504 (2020). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.125.260504
work page 2020
-
[95]
Sinclair, N.et al.Spectral multiplexing for scalable quantum photonics using an atomic frequency comb quantum memory and feed-forward control.Phys. Rev. Lett.113, 053603 (2014). URLhttps://link.aps. org/doi/10.1103/PhysRevLett.113.053603
-
[96]
Seri, A.et al.Quantum storage of frequency- multiplexed heralded single photons.Phys. Rev. Lett. 123, 080502 (2019). URLhttps://link.aps.org/ doi/10.1103/PhysRevLett.123.080502
-
[97]
Merkel, B., Ulanowski, A. & Reiserer, A. Coherent and Purcell-enhanced emission from erbium dopants in a cryogenic high-Qresonator.Phys. Rev. X10, 041025 (2020). URLhttps://link.aps.org/doi/10. 1103/PhysRevX.10.041025
work page 2020
-
[98]
Casabone, B.et al.Dynamic control of Purcell en- hanced emission of erbium ions in nanoparticles.Nat. Commun.12, 3570 (2021). URLhttps://doi.org/ 10.1038/s41467-021-23632-9
-
[99]
Zhong, M.et al.Optically addressable nuclear spins in a solid with a six-hour coherence time.Nature 517, 177–180 (2015). URLhttps://doi.org/10. 1038/nature14025
work page 2015
-
[100]
Ma, Y., Ma, Y.-Z., Zhou, Z.-Q., Li, C.-F. & Guo, G.-C. One-hour coherent optical storage in an atomic frequency comb memory.Nat. Commun. 12 12, 2381 (2021). URLhttps://doi.org/10.1038/ s41467-021-22706-y
work page 2021
-
[101]
Lau, H.-K., Qiao, H., Clerk, A. A. & Zhong, T. Effi- cient in situ generation of photon-memory entangle- ment in a nonlinear cavity.Phys. Rev. Lett.134, 053602 (2025). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.134.053602
work page 2025
-
[102]
Fleischhauer, M., Yelin, S. & Lukin, M. How to trap photons? Storing single-photon quantum states in col- lective atomic excitations.Opt. Commun.179, 395– 410 (2000). URLhttps://www.sciencedirect.com/ science/article/pii/S0030401899006793
work page 2000
-
[103]
Moiseev, S. A., Andrianov, S. N. & Gubaidullin, F. F. Efficient multimode quantum memory based on pho- ton echo in an optimal QED cavity.Phys. Rev. A82, 022311 (2010). URLhttps://link.aps.org/doi/10. 1103/PhysRevA.82.022311
work page 2010
-
[104]
Afzelius, M. & Simon, C. Impedance-matched cav- ity quantum memory.Phys. Rev. A82, 022310 (2010). URLhttps://link.aps.org/doi/10.1103/ PhysRevA.82.022310
work page 2010
-
[105]
Sabooni, M., Li, Q., Kr¨ oll, S. & Rippe, L. Efficient quantum memory using a weakly ab- sorbing sample.Phys. Rev. Lett.110, 133604 (2013). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.110.133604
work page 2013
-
[106]
Jobez, P.et al.Cavity-enhanced storage in an optical spin-wave memory.New J. Phys.16, 083005 (2014). URLhttps://dx.doi.org/10.1088/ 1367-2630/16/8/083005
work page 2014
-
[107]
Duranti, S.et al.Efficient cavity-assisted storage of photonic qubits in a solid-state quantum memory.Opt. Express32, 26884–26895 (2024). URLhttps://opg. optica.org/oe/abstract.cfm?URI=oe-32-15-26884
work page 2024
-
[108]
Sabooni, M., Li, Q., Rippe, L., Mohan, R. K. & Kr¨ oll, S. Spectral engineering of slow light, cavity line nar- rowing, and pulse compression.Phys. Rev. Lett.111, 183602 (2013). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.111.183602
work page 2013
-
[109]
Schraft, D., Hain, M., Lorenz, N. & Halfmann, T. Stopped light at high storage efficiency in a Pr3+ : Y 2SiO5 crystal.Phys. Rev. Lett.116, 073602 (2016). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.116.073602
work page 2016
-
[110]
P.et al.Noise-free on-demand atomic fre- quency comb quantum memory.Phys
Horvath, S. P.et al.Noise-free on-demand atomic fre- quency comb quantum memory.Phys. Rev. Res.3, 023099 (2021). URLhttps://link.aps.org/doi/10. 1103/PhysRevResearch.3.023099
work page 2021
-
[111]
Galland, N.et al.Mechanical tunability of an ultra- narrow spectral feature of a rare-earth-doped crystal via uniaxial stress.Phys. Rev. Applied13, 044022 (2020). URLhttps://link.aps.org/doi/10.1103/ PhysRevApplied.13.044022
work page 2020
-
[112]
Thorpe, M. J., Rippe, L., Fortier, T. M., Kirchner, M. S. & Rosenband, T. Frequency stabilization to 6×10 −16 via spectral-hole burning.Nat. Photonics 5, 688–693 (2011). URLhttps://doi.org/10.1038/ nphoton.2011.215
work page 2011
-
[113]
Lago-Rivera, D., Grandi, S., Rakonjac, J. V., Seri, A. & de Riedmatten, H. Telecom-heralded entanglement between multimode solid-state quantum memories.Na- ture594, 37–40 (2021). URLhttps://doi.org/10. 1038/s41586-021-03481-8
work page 2021
-
[114]
Businger, M.et al.Non-classical correlations over 1250 modes between telecom photons and 979-nm pho- tons stored in 171Yb3+: Y2Sio5.Nat. Commun. 13, 6438 (2022). URLhttps://doi.org/10.1038/ s41467-022-33929-y
work page 2022
-
[115]
Zhu, T.-X.et al.A metropolitan-scale multiplexed quantum repeater with bell nonlocality.arXiv preprint arXiv:2508.17940(2025)
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[116]
Cao, M., Hoffet, F., Qiu, S., Sheremet, A. S. & Lau- rat, J. Efficient reversible entanglement transfer be- tween light and quantum memories.Optica7, 1440– 1444 (2020). URLhttps://opg.optica.org/optica/ abstract.cfm?URI=optica-7-10-1440
work page 2020
-
[117]
Cho, Y.-W.et al.Highly efficient optical quantum memory with long coherence time in cold atoms.Op- tica3, 100–107 (2016). URLhttps://opg.optica. org/optica/abstract.cfm?URI=optica-3-1-100
work page 2016
-
[118]
Ma, L.et al.High-performance cavity-enhanced quan- tum memory with warm atomic cell.Nat. Commun. 13, 2368 (2022). URLhttps://doi.org/10.1038/ s41467-022-30077-1
work page 2022
-
[119]
Craiciu, I.et al.Nanophotonic quantum storage at telecommunication wavelength.Phys. Rev. Appl.12, 024062 (2019). URLhttps://link.aps.org/doi/10. 1103/PhysRevApplied.12.024062
work page 2019
-
[120]
V.et al.Storage and analysis of light- matter entanglement in a fiber-integrated system.Sci
Rakonjac, J. V.et al.Storage and analysis of light- matter entanglement in a fiber-integrated system.Sci. Adv.8, eabn3919 (2022). URLhttps://www.science. org/doi/abs/10.1126/sciadv.abn3919
-
[121]
England, D. G.et al.Storage and retrieval of thz- bandwidth single photons using a room-temperature diamond quantum memory.Phys. Rev. Lett.114, 053602 (2015). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.114.053602
work page 2015
-
[122]
Trotta, R.et al.Wavelength-tunable sources of en- tangled photons interfaced with atomic vapours.Nat. Commun.7, 10375 (2016). URLhttps://doi.org/ 10.1038/ncomms10375
-
[123]
Huang, J.-Y.et al.Stark tuning of telecom single- photon emitters based on a single Er3+.Chinese Phys. Lett.40, 070301 (2023). URLhttps://dx.doi.org/ 10.1088/0256-307X/40/7/070301
-
[124]
Ma, Y.-Z.et al.Elimination of noise in op- tically rephased photon echoes.Nat. Commun. 12, 4378 (2021). URLhttps://doi.org/10.1038/ s41467-021-24679-4
work page 2021
-
[125]
Ortu, A., Holz¨ apfel, A., Etesse, J. & Afzelius, M. Storage of photonic time-bin qubits for up to 20 ms in a rare-earth doped crystal.npj Quantum In- form.8, 29 (2022). URLhttps://doi.org/10.1038/ s41534-022-00541-3
work page 2022
-
[126]
Liu, Y.-P.et al.A millisecond integrated quantum memory for photonic qubits.Sci. Adv.11, eadu5264 (2025). URLhttps://www.science.org/doi/abs/10. 1126/sciadv.adu5264
work page 2025
-
[127]
Liu, D.-C.et al.On-demand storage of photonic qubits at telecom wavelengths.Phys. Rev. Lett.129, 210501 (2022). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.129.210501
work page 2022
-
[128]
Hunger, D.et al.A fiber Fabry–Perot cavity with high finesse.New J. Phys.12, 065038 (2010). URLhttps: //dx.doi.org/10.1088/1367-2630/12/6/065038
-
[129]
Sabooni, M., Kometa, S. T., Thuresson, A., Kr¨ oll, S. & Rippe, L. Cavity-enhanced storage—preparing for high-efficiency quantum memories.New J. Phys.15, 13 035025 (2013). URLhttps://dx.doi.org/10.1088/ 1367-2630/15/3/035025
work page 2013
-
[130]
Zhu, T.-X.et al.On-demand integrated quantum memory for polarization qubits.Phys. Rev. Lett.128, 180501 (2022). URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.128.180501
work page 2022
-
[131]
Lauritzen, B.et al.Spectroscopic investigations of Eu3+:Y2SiO5 for quantum memory applications.Phys. Rev. B85, 115111 (2012). URLhttps://link.aps. org/doi/10.1103/PhysRevB.85.115111
-
[132]
Jobez, P.et al.Towards highly multimode optical quantum memory for quantum repeaters.Phys. Rev. A 93, 032327 (2016). URLhttps://link.aps.org/doi/ 10.1103/PhysRevA.93.032327
-
[133]
Su, M.-X.et al.On-demand multimode optical storage in a laser-written on-chip waveguide.Phys. Rev. A105, 052432 (2022). URLhttps://link.aps.org/doi/10. 1103/PhysRevA.105.052432
work page 2022
-
[134]
van Dam, S. B., Ruf, M. & Hanson, R. Optimal design of diamond-air microcavities for quantum net- works using an analytical approach.New J. Phys.20, 115004 (2018). URLhttps://dx.doi.org/10.1088/ 1367-2630/aaec29
work page 2018
-
[135]
Hunger, D., Deutsch, C., Barbour, R. J., Warburton, R. J. & Reichel, J. Laser micro-fabrication of concave, low-roughness features in silica.AIP Adv.2, 012119 (2012). URLhttps://doi.org/10.1063/1.3679721
-
[136]
Ulanowski, A., Merkel, B. & Reiserer, A. Spec- tral multiplexing of telecom emitters with sta- ble transition frequency.Sci. Adv.8, eabo4538 (2022). URLhttps://www.science.org/doi/abs/10. 1126/sciadv.abo4538
work page 2022
-
[137]
URLhttps://opg.optica.org/optica/ abstract.cfm?URI=optica-10-10-1339
Deshmukh, C.et al.Detection of single ions in a nanoparticle coupled to a fiber cavity.Optica10, 1339– 1344 (2023). URLhttps://opg.optica.org/optica/ abstract.cfm?URI=optica-10-10-1339
work page 2023
-
[138]
Niemietz, D., Farrera, P., Langenfeld, S. & Rempe, G. Nondestructive detection of photonic qubits.Na- ture591, 570–574 (2021). URLhttps://doi.org/10. 1038/s41586-021-03290-z
work page 2021
-
[139]
Colloquium: Cavity-enhanced quan- tum network nodes.Rev
Reiserer, A. Colloquium: Cavity-enhanced quan- tum network nodes.Rev. Mod. Phys.94, 041003 (2022). URLhttps://link.aps.org/doi/10.1103/ RevModPhys.94.041003
work page 2022
-
[140]
de Riedmatten, H., Afzelius, M., Staudt, M. U., Simon, C. & Gisin, N. A solid-state light–matter interface at the single-photon level.Nature456, 773–777 (2008). URLhttps://doi.org/10.1038/nature07607
-
[141]
Zhou, Z.-Q., Huelga, S. F., Li, C.-F. & Guo, G.-C. Experimental detection of quantum coher- ent evolution through the violation of leggett-garg- type inequalities.Phys. Rev. Lett.115, 113002 (2015). URLhttps://link.aps.org/doi/10.1103/ PhysRevLett.115.113002
work page 2015
-
[142]
G¨ undo˘ gan, M., Ledingham, P. M., Kutluer, K., Mazzera, M. & de Riedmatten, H. Solid state spin- wave quantum memory for time-bin qubits.Phys. Rev. Lett.114, 230501 (2015). URLhttps://link.aps. org/doi/10.1103/PhysRevLett.114.230501
-
[143]
Curty, M. & L¨ utkenhaus, N. Intercept-resend attacks in the bennett-brassard 1984 quantum-key-distribution protocol with weak coherent pulses.Phys. Rev. A71, 062301 (2005). URLhttps://link.aps.org/doi/10. 1103/PhysRevA.71.062301
work page 1984
-
[144]
Pollnau, M. & Eichhorn, M. Spectral coher- ence, part I: Passive-resonator linewidth, funda- mental laser linewidth, and schawlow-townes ap- proximation.Prog. Quant. Electron.72, 100255 (2020). URLhttps://www.sciencedirect.com/ science/article/pii/S0079672720300094. 14 Supplementary Information for ”Efficient integrated quantum memory for light”
work page 2020
-
[145]
Growth ofEu 3+:Y2SiO5 crystals The Eu 3+:Y2SiO5 crystals are grown using the Czochralski method in an argon atmosphere, with a pulling rate of 1 mm/h and a rotation rate of 25 rpm along the b-axis. High-purity SiO 2 (99.9999%) and Y 2O3 (99.999%) are used as the starting materials for the host crystals. For doping, two types of europium oxide are employed...
-
[146]
The preparation of AFC with enhanced absorption According to Eq. 1 in the main text, enhancing the medium’s absorption is crucial for improving the storage efficiency. However, creating AFCs with high absorption typically introduces strong slow-light dispersion, which in turn leads to an undesirably narrow storage bandwidth constrained by the slow-light c...
-
[147]
The characterization and fabrication of ultra-low-loss optical waveguides To achieve efficient quantum storage in the WGC, minimizing the propagation loss of the optical waveguide is essential. Previously, we identified a set of parameters for the FLM process that successfully reduced these losses [135]. However, further optimization poses significant cha...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.