pith. sign in

arxiv: 2604.15971 · v1 · submitted 2026-04-17 · 🪐 quant-ph · cond-mat.mes-hall

A Modular Cryogenic Link for Microwave Quantum Communication Over Distances of Tens of Meters

Josua D. Sch\"ar , Simon Storz , Paul Magnard , Philipp Kurpiers , Janis L\"utolf , Melvin Gehrig , Jean-Claude Besse , Anatoly Kulikov
show 1 more author
Andreas Wallraff
This is my paper

Pith reviewed 2026-05-10 08:03 UTC · model grok-4.3

classification 🪐 quant-ph cond-mat.mes-hall
keywords cryogenic linkmicrowave quantum communicationsuperconducting circuitsquantum networksdilution refrigeratorsthermal modelmodular designBell test
0
0 comments X

The pith

A modular cryogenic microwave link connects superconducting circuits over 30 meters at temperatures below 50 mK.

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

This paper demonstrates a hardware solution for linking superconducting quantum devices at microwave frequencies across distances of 5 to 30 meters while maintaining the millikelvin temperatures needed for quantum operations. The authors build and test a modular system that spans separate dilution refrigerators using a quantum communication channel, supported by a thermal model to guide material selection and heat-load suppression. Achieving stable operating conditions in the longest configuration would allow quantum information to be exchanged between spatially separated processors, enabling distributed algorithms and non-local tests with superconducting circuits.

Core claim

The assembled 30-meter-long system achieves operating temperatures of below 50 mK after a cooldown time of about six and a half days. This modular cryogenic link connects two superconducting circuit systems located in individual dilution refrigerators through a quantum communication channel, enabling the exchange of quantum information between spatially separated parties.

What carries the argument

The modular cryogenic link: a chain of coaxial cables and thermal anchoring stages whose design is optimized by a thermal model that evaluates heat transfer from room temperature to the cold stage while preserving microwave signal fidelity.

If this is right

  • Enables execution of distributed quantum computing and communication algorithms across separate dilution refrigerators.
  • Introduces the resource of non-locality to superconducting-circuit experiments, certifiable by a loophole-free Bell test.
  • Supports local-area networks of quantum information processing units operating at microwave frequencies.

Where Pith is reading between the lines

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

  • The same modular approach could be scaled to connect more than two refrigerators or to longer distances provided heat loads stay within the dilution-refrigerator budget.
  • Comparable links might be adapted for other cryogenic platforms if their thermal and signal requirements can be matched by analogous cable and anchoring designs.
  • Performing an actual quantum-state transfer or entanglement-swapping protocol over the link would directly test whether the achieved temperature and noise levels suffice for quantum communication.

Load-bearing premise

The thermal model correctly predicts heat transfer rates and the chosen materials and modular construction suppress room-temperature heat loads without introducing unacceptable noise or loss in the microwave channel.

What would settle it

After a 6.5-day cooldown of the 30-meter assembly, record the base temperature at the far end; if it remains above 50 mK or if microwave transmission shows excess loss or added noise that prevents quantum-coherent operation, the performance claim is falsified.

Figures

Figures reproduced from arXiv: 2604.15971 by Anatoly Kulikov, Andreas Wallraff, Janis L\"utolf, Jean-Claude Besse, Josua D. Sch\"ar, Melvin Gehrig, Paul Magnard, Philipp Kurpiers, Simon Storz.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) Longitudinal cross-section of a schematic representation (left half) and a 3D model (right half) of a 30 m cryogenic [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. (a) Photograph of an adapter module connected to [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Steady-state temperature distribution of the (a) 5-m-long, (b) 10-m-long and (c) 30-m-long cryogenic link. The [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Lowest (solid dots) and highest (open dots) tem [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (a) Front view of the cooling unit installed at the center of the 30 m link, used to actively cool the 50K and 4K [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. (a) Schematic representation of heat transfer from [PITH_FULL_IMAGE:figures/full_fig_p013_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. (a) Scheme of the experimental setup used to characterize heat transfer in the link and braid modules. (b) 4K [PITH_FULL_IMAGE:figures/full_fig_p014_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. (a) Cross-sectional CAD drawings of the 50K (left) [PITH_FULL_IMAGE:figures/full_fig_p016_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. (a) Photograph of a typical experimental setup used [PITH_FULL_IMAGE:figures/full_fig_p017_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. (a) Simulated heat load of a post on the 50K stage [PITH_FULL_IMAGE:figures/full_fig_p018_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11. (a) Perspective view, and (b), cross-section of a [PITH_FULL_IMAGE:figures/full_fig_p019_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: FIG. 12. (a) Schematic illustrating the location of tempera [PITH_FULL_IMAGE:figures/full_fig_p021_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: FIG. 13. (a) A schematic of the 30-meter-long link with [PITH_FULL_IMAGE:figures/full_fig_p022_13.png] view at source ↗
read the original abstract

Quantum technologies promise a radically new way to solve classically intractable computing problems. Superconducting circuits as a platform are at the forefront of this field. The cryogenic operation temperatures of superconducting circuits however impose challenges for the further scaling to many connected quantum information processing units into a local area or global network. In this work, we present a hardware solution for connecting quantum devices operating at microwave frequencies into local area networks, which enable the exchange of quantum information between spatially separated parties. Specifically, we demonstrate a modular system spanning distances of 5, 10 and 30 meters operated at cryogenic temperatures and connecting two superconducting circuit systems, located in individual dilution refrigerators, through a quantum communication channel. We develop a thermal model to evaluate the heat transfer processes in the setup, optimize the design and select appropriate materials for its construction. The assembled 30-meter-long system achieves operating temperatures of below 50 mK after a cooldown time of about six and a half days. This link enables the execution of distributed quantum computing and communication algorithms. It also adds the resource of non-locality, certified by a loophole-free Bell test, to the field of quantum science and technology with superconducting circuits.

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

0 major / 2 minor

Summary. The manuscript presents the design, thermal modeling, construction, and experimental testing of a modular cryogenic microwave link that connects two dilution refrigerators over distances of 5, 10, and 30 meters. The central experimental result is that the fully assembled 30 m system reaches operating temperatures below 50 mK after a cooldown time of approximately 6.5 days, enabling potential quantum communication between spatially separated superconducting circuits.

Significance. If the reported temperature performance and thermal isolation hold under operational conditions, this work supplies a concrete hardware platform for distributed quantum computing and communication with superconducting circuits. The modular architecture and empirical cooldown data constitute a practical engineering advance that adds the resource of non-locality to the superconducting platform.

minor comments (2)
  1. [Abstract] Abstract: the claim that the link 'enables the execution of distributed quantum computing and communication algorithms' would be strengthened by a brief quantitative statement of expected channel loss, added noise, or error rates, even if these are estimates derived from the thermal model.
  2. [Results / Experimental section] The manuscript would benefit from an explicit table or figure summarizing the measured heat loads, cooldown curve, and final base temperature together with the corresponding model predictions for direct comparison.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of our manuscript and for recommending acceptance. We appreciate the recognition that the modular cryogenic link provides a practical hardware platform for distributed quantum computing and communication with superconducting circuits, along with the value placed on the empirical cooldown data and thermal isolation performance.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper reports an experimental hardware demonstration in which a 30-meter modular cryogenic link is assembled and measured to reach operating temperatures below 50 mK after a six-and-a-half-day cooldown. A thermal model is developed and referenced only for prior design optimization and material selection; the central claim rests on direct empirical temperature data from the completed system rather than on any model-derived prediction or fitted parameter. No self-definitional equations, fitted inputs relabeled as predictions, load-bearing self-citations, uniqueness theorems, or ansatzes smuggled via citation appear in the derivation chain. The result is therefore self-contained as a measured outcome and receives the default non-circularity score.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The demonstration rests on established cryogenic engineering and heat-transfer physics without introducing new entities or many fitted parameters beyond standard material selection.

axioms (1)
  • standard math Standard heat conduction, radiation, and convection laws govern the thermal behavior of the link at cryogenic temperatures.
    Invoked to build the thermal model that guides material choice and predicts cooldown time.

pith-pipeline@v0.9.0 · 5545 in / 1098 out tokens · 26982 ms · 2026-05-10T08:03:39.867575+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

88 extracted references · 88 canonical work pages

  1. [1]

    1.5 2.0 .5 1 1.5 T (K)still BT heat load, BT ( /uni03BCW ) ∝T 3.3 P (d) (a) (b) (c) FIG. 10. (a) Simulated heat load of a post on the 50K stage vstemperature of the vacuum can, based on finite elements method. Simulations for (b) 4K, (c) still and (d) base stage, see panel in (a) for the legend. The solid lines are fits to a power law dependence between t...

    work page 2000

  2. [2]

    H. J. Kimble, Nature453, 1023 (2008)

    work page 2008

  3. [3]

    Wehner, D

    S. Wehner, D. Elkouss, and R. Hanson, Science362, eaam9288 (2018)

    work page 2018

  4. [4]

    D. P. DiVincenzo, Fortschritte der Physik48, 771 (2000)

    work page 2000

  5. [5]

    Krantz, M

    P. Krantz, M. Kjaergaard, F. Yan, T. P. Orlando, S. Gus- tavsson, and W. D. Oliver, Applied Physics Reviews6, 021318 (2019)

    work page 2019

  6. [6]

    Kumar, A

    A. Kumar, A. Suleymanzade, M. Stone, L. Taneja, A. Anferov, D. I. Schuster, and J. Simon, Nature615, 614 (2023)

    work page 2023

  7. [7]

    B. M. Brubaker, J. M. Kindem, M. D. Urmey, S. Mittal, R. D. Delaney, P. S. Burns, M. R. Vissers, K. W. Lehnert, and C. A. Regal, Phys. Rev. X12, 021062 (2022)

    work page 2022

  8. [8]

    Stockill, M

    R. Stockill, M. Forsch, F. Hijazi, G. Beaudoin, K. Pantzas, I. Sagnes, R. Braive, and S. Gr¨ oblacher, Nature Communications13, 6583 (2022)

    work page 2022

  9. [9]

    Forsch, R

    M. Forsch, R. Stockill, A. Wallucks, I. Marinkovi´ c, C. G¨ artner, R. A. Norte, F. van Otten, A. Fiore, K. Srini- vasan, and S. Gr¨ oblacher, Nature Physics (2019)

    work page 2019

  10. [10]

    Hease, A

    W. Hease, A. Rueda, R. Sahu, M. Wulf, G. Arnold, H. G. Schwefel, and J. M. Fink, PRX Quantum1, 020315 (2020)

    work page 2020

  11. [11]

    Mirhosseini, A

    M. Mirhosseini, A. Sipahigil, M. Kalaee, and O. Painter, Nature588, 599 (2020)

    work page 2020

  12. [12]

    Tu, K.-Y

    H.-T. Tu, K.-Y. Liao, Z.-X. Zhang, X.-H. Liu, S.-Y. Zheng, S.-Z. Yang, X.-D. Zhang, H. Yan, and S.-L. Zhu, Nat. Photonics , 1 (2022)

    work page 2022

  13. [13]

    C.-H. Wang, F. Li, and L. Jiang, Nature Communica- tions13, 6698 (2022)

    work page 2022

  14. [14]

    Wallraff, D

    A. Wallraff, D. I. Schuster, A. Blais, L. Frunzio, R.-S. Huang, J. Majer, S. Kumar, S. M. Girvin, and R. J. Schoelkopf, Nature431, 162 (2004)

    work page 2004

  15. [15]

    Wenner, Y

    J. Wenner, Y. Yin, Y. Chen, R. Barends, B. Chiaro, E. Jeffrey, J. Kelly, A. Megrant, J. Mutus, C. Neill, P. O ´Malley, P. Roushan, D. Sank, A. Vainsencher, T. White, A. N. Korotkov, A. Cleland, and J. M. Mar- tinis, Phys. Rev. Lett.112, 210501 (2014)

    work page 2014

  16. [16]

    Pechal, L

    M. Pechal, L. Huthmacher, C. Eichler, S. Zeytino˘ glu, A. A. Abdumalikov Jr., S. Berger, A. Wallraff, and S. Filipp, Phys. Rev. X4, 041010 (2014)

    work page 2014

  17. [17]

    Pfaff, C

    W. Pfaff, C. J. Axline, L. D. Burkhart, U. Vool, P. Rein- hold, L. Frunzio, L. Jiang, M. H. Devoret, and R. J. Schoelkopf, Nat. Phys. (2017), 10.1038/nphys4143

    work page doi:10.1038/nphys4143 2017

  18. [18]

    Ilves, S

    J. Ilves, S. Kono, Y. Sunada, S. Yamazaki, M. Kim, K. Koshino, and Y. Nakamura, npj Quantum Informa- tion6, 34 (2020)

    work page 2020

  19. [19]

    Besse, K

    J.-C. Besse, K. Reuer, M. C. Collodo, A. Wulff, L. Wernli, A. Copetudo, D. Malz, P. Magnard, A. Akin, M. Gabu- reac, G. J. Norris, J. I. Cirac, A. Wallraff, and C. Eichler, Nat. Commun.11, 4877 (2020)

    work page 2020

  20. [20]

    Kurpiers, M

    P. Kurpiers, M. Pechal, B. Royer, P. Magnard, T. Walter, J. Heinsoo, Y. Salath´ e, A. Akin, S. Storz, J.-C. Besse, S. Gasparinetti, A. Blais, and A. Wallraff, Phys. Rev. Appl.12, 044067 (2019)

    work page 2019

  21. [21]

    Axline, L

    C. Axline, L. Burkhart, W. Pfaff, M. Zhang, K. Chou, 23 P. Campagne-Ibarcq, P. Reinhold, L. Frunzio, S. M. Girvin, L. Jiang, M. H. Devoret, and R. J. Schoelkopf, Nature Physics14, 705 (2018)

    work page 2018

  22. [22]

    Zhong, H.-S

    Y. Zhong, H.-S. Chang, A. Bienfait, E. Dumur, M.-H. Chou, C. R. Conner, J. Grebel, R. G. Povey, H. Yan, D. I. Schuster, and A. N. Cleland, Nature590, 571 (2021)

    work page 2021

  23. [23]

    Leung, Y

    N. Leung, Y. Lu, S. Chakram, R. K. Naik, N. Earnest, R. Ma, K. Jacobs, A. N. Cleland, and D. I. Schuster, npj Quantum Information5, 18 (2019)

    work page 2019

  24. [24]

    Y. P. Zhong, H.-S. Chang, K. J. Satzinger, M.-H. Chou, A. Bienfait, C. R. Conner, E. Dumur, J. Grebel, G. A. Peairs, R. G. Povey, D. I. Schuster, and A. N. Cleland, Nature Physics (2019)

    work page 2019

  25. [25]

    L. D. Burkhart, J. D. Teoh, Y. Zhang, C. J. Ax- line, L. Frunzio, M. Devoret, L. Jiang, S. Girvin, and R. Schoelkopf, PRX Quantum2, 030321 (2021)

    work page 2021

  26. [26]

    Kurpiers, T

    P. Kurpiers, T. Walter, P. Magnard, Y. Salathe, and A. Wallraff, EPJ Quantum Technology4, 8 (2017)

    work page 2017

  27. [27]

    Xiang, M

    Z.-L. Xiang, M. Zhang, L. Jiang, and P. Rabl, Physical Review X7, 011035 (2017)

    work page 2017

  28. [28]

    M. J. A. Schuetz, B. Vermersch, G. Kirchmair, L. M. K. Vandersypen, J. I. Cirac, M. D. Lukin, and P. Zoller, Phys. Rev. B99, 241302 (2019)

    work page 2019

  29. [29]

    Magnard, S

    P. Magnard, S. Storz, P. Kurpiers, J. Sch¨ ar, F. Marxer, J. L¨ utolf, T. Walter, J.-C. Besse, M. Gabureac, K. Reuer, A. Akin, B. Royer, A. Blais, and A. Wallraff, Phys. Rev. Lett.125, 260502 (2020)

    work page 2020

  30. [30]

    Storz, J

    S. Storz, J. Sch¨ ar, A. Kulikov, P. Magnard, P. Kurpiers, J. L¨ utolf, T. Walter, A. Copetudo, K. Reuer, A. Akin, J.- C. Besse, M. Gabureac, G. J. Norris, A. Rosario, F. Mar- tin, J. Martinez, W. Amaya, M. W. Mitchell, C. Abel- lan, J.-D. Bancal, N. Sangouard, B. Royer, A. Blais, and A. Wallraff, Nature617, 265 (2023)

    work page 2023

  31. [31]

    Storz, A

    S. Storz, A. Kulikov, J. D. Sch¨ ar, V. Barizien, X. Val- carce, F. Berterotti` ere, N. Sangouard, J.-D. Bancal, and A. Wallraff, Phys. Rev. Lett.135, 030801 (2025)

    work page 2025

  32. [32]

    Kulikov, S

    A. Kulikov, S. Storz, J. D. Sch¨ ar, M. Sandfuchs, R. Wolf, F. Berterotti` ere, C. Hellings, R. Renner, and A. Wallraff, arXiv:2412.17931 (2024)

    work page arXiv 2024

  33. [33]

    Alduino, F

    C. Alduino, F. Alessandria, M. Balata, D. Biare, M. Bi- assoni, C. Bucci, A. Caminata, L. Canonica, L. Cap- pelli, G. Ceruti, A. Chiarini, N. Chott, M. Clemenza, S. Copello, A. Corsi, O. Cremonesi, A. D’Addabbo, S. Dell’Oro, L. Di Paolo, M. Di Vacri, A. Drobizhev, M. Faverzani, E. Ferri, M. Franceschi, R. Gaigher, L. Gladstone, P. Gorla, M. Guetti, L. Ioa...

    work page 2019

  34. [34]

    M. I. Hollister, D. A. Bauer, R. C. Dhuley, P. Lukens, L. D. Martin, M. K. Ruschman, R. L. Schmitt, and G. L. Tatkowski, IOP Conference Series: Materials Science and Engineering278, 012118 (2017)

    work page 2017

  35. [35]

    Pobell,Matter and Methods at Low Temperatures (Springer, 3rd edition, 2006)

    F. Pobell,Matter and Methods at Low Temperatures (Springer, 3rd edition, 2006)

    work page 2006

  36. [36]

    Electronic industries alliance standards,

    “Electronic industries alliance standards,” The inner di- mensions, operating frequency range, and performance characteristics of rectangular waveguides are pecified in the standards RS-261-B

    work page

  37. [37]

    W. K. Yam, M. Renger, S. Gandorfer, F. Fesquet, M. Handschuh, K. E. Honasoge, F. Kronowetter, Y. No- jiri, M. Partanen, M. Pfeiffer, H. van der Vliet, A. J. Matthews, J. Govenius, R. N. Jabdaraghi, M. Prunnila, A. Marx, F. Deppe, R. Gross, and K. G. Fedorov, npj Quantum Information11, 87 (2025)

    work page 2025

  38. [38]

    J. H. Lienhard, IV and J. H. Lienhard, V,A Heat Trans- fer Textbook, 5th ed. (Dover Publications, Mineola, NY, 2019)

    work page 2019

  39. [39]

    M. A. Bramson,Infrared Radiation(Springer, New York, NY, 1968) pp. 533–552

    work page 1968

  40. [40]

    Parma, CAS - CERN Accelerator School: Course on Superconductivity for Accelerators (2014), 10.5170/CERN-2014-005.353

    V. Parma, CAS - CERN Accelerator School: Course on Superconductivity for Accelerators (2014), 10.5170/CERN-2014-005.353

    work page doi:10.5170/cern-2014-005.353 2014

  41. [41]

    W. A. Marlow,Design of Multilayer Insulation for the Multipurpose Hydrogen Test Bed, Tech. Rep. (NASA, 2011)

    work page 2011

  42. [42]

    The working principle of MLI is based on radiation bal- ance. One reflective foil between the vacuum can and the 50 K shield will be irradiated from the vacuum can with some powerPheating up the foil so that its radiated power is in balance with the irradiation. Hence powerP/2 is emitted on each side, and inserting the foil reduces the radiation heat load...

    work page

  43. [43]

    Kang, inMicrosatellites as Research Tools, COSPAR Colloquia Series, Vol

    C.-S. Kang, inMicrosatellites as Research Tools, COSPAR Colloquia Series, Vol. 10, edited by F.-B. Hsiao (Pergamon, 1999) pp. 175–179

    work page 1999

  44. [44]

    Q. Shu, R. Fast, and H. Hart, Cryogenics26, 671 (1986)

    work page 1986

  45. [45]

    W. L. Johnson and J. E. Fesmire, inCryogenic Engineer- ing Conference / Cryogenic Society of America(NASA, Kennedy Space Center, Cocoa Beach, FL, 2009) (ac- cessed: 12.08.2025)

    work page 2009

  46. [46]

    M. M. Finckenor and D. Dooling,Multilayer Insulation Material Guidelines, Technical Publication NASA/TP- 1999-209263 (NASA Marshall Space Flight Center / D2 Associates, Huntsville, AL, United States, 1999) (ac- cessed: 12.08.2025)

    work page 1999

  47. [47]

    Accura bluestone (sla),

    3D Systems, “Accura bluestone (sla),” (accessed: 10.02.2025)

    work page 2025

  48. [48]

    A. L. Woodcraft, Cryogenics45, 626 (2005)

    work page 2005

  49. [49]

    German copper association: Kupferschl¨ ussel 1.0 (visited on 06.06.2024)

    work page 2024

  50. [50]

    F. R. Fickett, Journal of Physics F: Metal Physics12, 1753 (1982)

    work page 1982

  51. [51]

    Kurpiers,Quantum Networks with Superconducting Circuits, Ph.D

    P. Kurpiers,Quantum Networks with Superconducting Circuits, Ph.D. thesis, ETH Zurich (2019)

    work page 2019

  52. [52]

    L. J. Salerno and P. Kittel,Thermal Contact Conduc- tance, Tech. Rep. (NASA, 1997)

    work page 1997

  53. [53]

    Material prop- erties of 6061-t6 aluminum (UNS A96061),

    NIST Material Measurement Laborator, “Material prop- erties of 6061-t6 aluminum (UNS A96061),” (accessed: 06.06.2024)

    work page 2024

  54. [54]

    C. B. Satterthwaite, Phys. Rev.125, 873 (1962)

    work page 1962

  55. [55]

    Magnard,Meter-scale Microwave Quantum Networks for Superconducting Circuits, Ph.D

    P. Magnard,Meter-scale Microwave Quantum Networks for Superconducting Circuits, Ph.D. thesis, ETH Zurich (2021)

    work page 2021

  56. [56]

    L. W. McKeen,Permeability properties of plastics and elastomers, fourth edition ed., PDL Plastics Design Li- brary (Elsevier, Amsterdam, 2017)

    work page 2017

  57. [57]

    The digital vacuum technology book,

    Pfeiffer Vacuum GmbH, “The digital vacuum technology book,” (accessed: 23.04.2024)

    work page 2024

  58. [58]

    D. M. Pozar,Microwave Engineering, 4th Edition (In- ternational Adaptation)., 4th ed. (John Wiley & Sons, Incorporated, New York, 2021). 24

    work page 2021

  59. [59]

    Storz,Non-local Physics with Superconducting Cir- cuits, Ph.D

    S. Storz,Non-local Physics with Superconducting Cir- cuits, Ph.D. thesis, ETH Zurich (2023)

    work page 2023

  60. [60]

    X. Y. Jin, A. Kamal, A. P. Sears, T. Gudmundsen, D. Hover, J. Miloshi, R. Slattery, F. Yan, J. Yoder, T. P. Orlando, S. Gustavsson, and W. D. Oliver, Phys. Rev. Lett.114, 240501 (2015)

    work page 2015

  61. [61]

    Kulikov, R

    A. Kulikov, R. Navarathna, and A. Fedorov, Phys. Rev. Lett.124, 240501 (2020)

    work page 2020

  62. [62]

    Magnard, P

    P. Magnard, P. Kurpiers, B. Royer, T. Walter, J.-C. Besse, S. Gasparinetti, M. Pechal, J. Heinsoo, S. Storz, A. Blais, and A. Wallraff, Phys. Rev. Lett.121, 060502 (2018)

    work page 2018

  63. [63]

    Vermersch, P.-O

    B. Vermersch, P.-O. Guimond, H. Pichler, and P. Zoller, Phys. Rev. Lett.118, 133601 (2017)

    work page 2017

  64. [64]

    Rosenblum, W

    S. Rosenblum, W. Steyert, and F. Fickett, Cryogenics 17, 645 (1977)

    work page 1977

  65. [65]

    G. F. Pe˜ nas, R. Puebla, T. Ramos, P. Rabl, and J. J. Garc´ ıa-Ripoll, Phys. Rev. Applied17, 054038 (2022)

    work page 2022

  66. [66]

    Vazirani and T

    U. Vazirani and T. Vidick, Phys. Rev. Lett.113, 140501 (2014)

    work page 2014

  67. [67]

    Pironio, A

    S. Pironio, A. Ac´ ın, S. Massar, A. B. de la Giroday, D. N. Matsukevich, P. Maunz, S. Olmschenk, D. Hayes, L. Luo, T. A. Manning, and C. Monroe, Nature464, 1021 (2010)

    work page 2010

  68. [68]

    Kessler and R

    M. Kessler and R. Arnon-Friedman, IEEE Journal on Selected Areas in Information Theory1, 568 (2020)

    work page 2020

  69. [69]

    ˇSupi´ c, D

    I. ˇSupi´ c, D. Cavalcanti, and J. Bowles, Quantum5, 418 (2021)

    work page 2021

  70. [70]

    Bowles, I

    J. Bowles, I. ˇSupi´ c, D. Cavalcanti, and A. Ac´ ın, Phys. Rev. Lett.121, 180503 (2018)

    work page 2018

  71. [71]

    F. Dinc, L. E. Hayward, and A. M. Bra´ nczyk, Phys. Rev. Res.2, 043149 (2020)

    work page 2020

  72. [72]

    Dinc and A

    F. Dinc and A. M. Branczyk, Phys. Rev. Research1, 032042 (2019)

    work page 2019

  73. [73]

    Calaj´ o, Y.-L

    G. Calaj´ o, Y.-L. L. Fang, H. U. Baranger, and F. Cic- carello, Phys. Rev. Lett.122, 073601 (2019)

    work page 2019

  74. [74]

    K.-H. K. Wolfgang Thomala,Schraubenverbindungen (Springer Berlin, Heidelberg, 2007)

    work page 2007

  75. [75]

    Bossard: Approximate values for metric coarse threads VDI 2230) (visited on 02.11.2023)

    work page 2023

  76. [76]

    The new rapid prototyping ma- chine at the cern polymer lab,

    P. Fessia, S. Clement, R. Fornasiere, E.and Gauthier, M. Goncalves Lopes, S. Izquierdo Bermudez, L. . Lam- bert, A. Cherif, A. Gerardin, S. Langeslag, S. M. Mar- cuzzi, and M. Brugger, “The new rapid prototyping ma- chine at the cern polymer lab,” (2013)

    work page 2013

  77. [77]

    Apiezon n grease,

    M&I materials, “Apiezon n grease,” (accessed: 14.02.2025)

    work page 2025

  78. [78]

    An exper- imental study of heat transfer in multilayer insulation systems from room temperature to 77 k,

    Q. S. Shu, R. W. Fast, and H. L. Hart, “An exper- imental study of heat transfer in multilayer insulation systems from room temperature to 77 k,” inAdvances in Cryogenic Engineering: Volume 31, edited by R. W. Fast (Springer US, Boston, MA, 1986) pp. 455–463

    work page 1986

  79. [79]

    Icec19 proceeding: Performance characterization of perfo- rated multilayer insulation blankets,

    J. Fesmire, S. Augustynowicz, and C. Darve, “Icec19 proceeding: Performance characterization of perfo- rated multilayer insulation blankets,” (2002), (accessed: 20.02.2025)

    work page 2002

  80. [80]

    Heine,Werkstoffpr¨ ufung : Ermittlung von Werkstof- feigenschaften(Hanser, M¨ unchen, 2011)

    B. Heine,Werkstoffpr¨ ufung : Ermittlung von Werkstof- feigenschaften(Hanser, M¨ unchen, 2011)

    work page 2011

Showing first 80 references.