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REVIEW 3 major objections 3 minor 44 references

Demonstration of an optical microwave rectification by a superconducting diode with near 100% efficiency

T0 review · 3 major / 3 minor · reviewed 2026-08-05 · deepseek-v4-flash

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Pith's one-line read A tuned niobium Josephson junction acts as a near-perfect diode and rectifies 75 GHz microwaves without a threshold.

desk verdict Solid near-perfect dc diode data, but the optical rectification claim is overreaching and rests on an unverified shunting mechanism. read the letter →

arxiv 2508.21696 v1 pith:UJ3ZIERJ submitted 2025-08-29 cond-mat.supr-con physics.app-ph

Razmik A. Hovhannisyan , Amirreza Lotfian , Taras Golod , Vladimir M. Krasnov This is my paper · ORCID
classification cond-mat.supr-conphysics.app-ph PACS 74.50.+r85.25.Cp85.25.-j
keywords superconductingdiodeJosephsonjunctionself-fieldeffectnonreciprocalcriticalcurrentmicrowaverectificationopticalniobiumTHzsignalprocessing
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

This paper tries to show that a simple planar Josephson junction made from ordinary niobium can act as a nearly ideal superconducting diode, and that it can rectify wireless microwave radiation, not just a wired current. The authors achieve this by tuning the device so that the magnetic self-field produced by an asymmetric bias exactly compensates one flux quantum, and by keeping the junction short enough that its critical current truly vanishes at the first field minimum. The result is a diode with nonreciprocity greater than 1000 and efficiency greater than 99.8 percent. The new result is threshold-free rectification of 75 GHz microwave radiation, which the authors attribute to the low input resistance of the current source shunting one side of the microwave antenna and creating the required impedance asymmetry. If it holds, this would give superconducting electronics a missing building block: an efficient, switchable diode for high-frequency wireless signal processing and passive signal routing.

What carries the argument

The self-field effect in a four-terminal planar Josephson junction: an asymmetric bias injects current at one edge, creating a self-field flux Φ_sf = L_sf I_c0 that tilts the field-dependent critical-current pattern. The optimization conditions are Eq. (1), Φ_sf = Φ0, which places the central maximum opposite the first minimum, and Eq. (2), Lx < 4λJ, the short-junction limit required for a true zero of Ic at one flux quantum. In the optical case, the load-bearing element is the dual role of the low-resistance current source: it sets the current-flow asymmetry for transport, and it shunts one side of the millimeter-scale microwave antenna, creating the impedance asymmetry that makes the junct

What would settle it

Disconnect the current source from one side of the device, or replace it with a high-impedance termination, while keeping the 75 GHz beam fixed: if the shunting interpretation is correct, the rectified dc voltage should drop dramatically or vanish; if substantial rectification persists, another mechanism is at work. Sweeping the source impedance continuously and checking that the polarity flips when connections move from left to right electrodes would further settle the matter.

Watch

Extended reading notes

Core claim

Deliberately optimized planar Nb Josephson junctions satisfy two conditions: L_sf I_c0 = Φ0, aligning the central Ic maximum with the opposite first minimum, and Lx < 4λJ, the short-junction limit where Ic genuinely vanishes at that minimum. The optimized device carries about 100 μA of critical current in one direction and none (<0.1 μA) in the other, yielding A > 1000 and η > 99.8%. The paper then reports, for what it states is the first time, optical rectification: 75 GHz microwaves yield a threshold-free dc voltage that tracks the transport signal. The mechanism is distinct: the low input resistance of the current source shunts one side of the millimeter-scale antenna, creating the microw

Load-bearing premise

The optical rectification claim depends on the assumption that the low input resistance of the current source shunts one side of the microwave antenna and thereby creates the impedance asymmetry; no control experiment varies that impedance to rule out other sources of rectification such as bolometric or thermoelectric response.

Editorial extensions

If this is right

  • A near-perfect superconducting diode removes the threshold power problem, so weak microwave signals can be rectified and detected at arbitrarily low power.
  • The tuning recipe, if it scales, should work at higher frequencies up to the sub-THz gap limit of niobium, directly serving upper microwave and lower terahertz wireless bands.
  • Polarity can be switched by changing the magnetic field or by flipping which electrodes carry the bias, enabling reconfigurable signal routing.
  • In superconducting digital circuits, such diodes could function as passive switches that block current leakage across interconnections, a role currently missing.
  • Transport and optical rectification being driven by different asymmetries means the device can be optimized separately for wired and wireless operation.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the paper's shunting explanation is right, the device is not an intrinsically free-space optical diode: a practical wireless receiver would need an integrated low-impedance shunt or an asymmetric antenna on-chip to reproduce the asymmetry without the measurement current source.
  • The close but non-identical magnetic-field dependence of transport versus optical rectification could be used as a diagnostic to map how the microwave current distribution differs from the transport current path.
  • A natural next test is to sweep the current-source output impedance, or disconnect it entirely, while measuring the 75 GHz rectified voltage; a monotonic dependence would confirm the shunting mechanism and quantify the impedance asymmetry.
  • Combining this near-ideal rectifier with the vortex-controlled polarity switching described in an earlier work could yield a zero-field, memory-enabled rectifier for wireless signal processing.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 3 minor

Summary. The manuscript reports Nb planar Josephson junctions with multi-terminal asymmetric electrodes whose self-field produces critical-current nonreciprocity. By tuning the junction length to Lx = 3λJ and the temperature so that the self-flux satisfies Φsf = Φ0, the authors achieve A > 1000 and η > 99.8% in transport, with complete suppression of Ic in one direction within a 0.1 μA resolution. They then measure a rectified dc voltage under 75 GHz irradiation, observe threshold-free behavior, and interpret this as optical microwave rectification enabled by the low input resistance of the current source shunting one side of the MW antenna. The paper claims the first demonstration of the optical diode effect in such junctions.

Significance. If the optical claim holds, the work would show that simple Nb Josephson junctions can act as near-ideal rectifying elements for both transport currents and wireless upper-microwave signals, with clear relevance to superconducting digital circuits and sub-THz communication. The transport demonstration is convincing, the design rules in Eqs. (1) and (2) are useful, and the numerical sine-Gordon fit provides quantitative support for the short-junction regime. However, the distinctive novelty—optical microwave rectification—currently rests on an untested shunting mechanism and lacks a measured conversion efficiency, so the near-100% efficiency claim in the title goes beyond what the data establish.

major comments (3)
  1. [Optical rectification, Fig. 2(f) and following paragraph] The proposed mechanism for optical rectification is asserted but not verified. The paragraph after Fig. 2(f) states that the low input resistance of the current source shunts one side of the MW antenna, creating the impedance asymmetry, but no measurement of the source impedance, antenna impedance, or control experiment is presented. A bolometric/thermoelectric response or direct MW coupling to the junction nonlinearity could produce a similar field-dependent dc voltage. Since the optical effect is the central novelty, this missing control is load-bearing. Please add a control experiment (e.g., varying the current-source impedance, adding a known shunt, or disconnecting the source) and report the relevant impedances.
  2. [Title, Abstract, and Conclusion] The 'near 100% efficiency' claim is not supported for optical rectification. The value η > 99.8% is defined through the transport critical currents, not through conversion of 75 GHz radiation into dc power. Fig. 2(f) shows only a rectified voltage versus MW power with no absolute power calibration, absorbed-power estimate, or conversion efficiency. Either measure the optical conversion efficiency or rephrase the claim to 'near-unity transport nonreciprocity with threshold-free optical detection'.
  3. [Fig. 2(e) comparison of transport and optical field dependence] The transport and optical field dependencies are described as 'qualitatively similar but not identical,' but the origin of the difference is not discussed. If the shunting mechanism is correct, the difference presumably reflects the frequency-dependent impedance asymmetry; if it is not, the difference could indicate a different rectification path. Quantifying this comparison (e.g., normalizing the two curves and testing whether the same nanotesla-scale features appear) would strengthen the interpretation.
minor comments (3)
  1. [Page 3, V/W bands] Typo: 'boarder' should be 'border'.
  2. [Fig. 2(e) and (f)] Please specify the lock-in chopper frequency, time constant, and the MW power units used in the bottom panel of Fig. 2(e); the current axis and field axis are clear, but the optical power scale is not defined.
  3. [Methods, sine-Gordon equation] The numerical fit for Lx = 3λJ would be easier to evaluate if the damping parameter α and the junction length in normalized units were stated explicitly, along with the fit's sensitivity to λJ.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: the diode optimization follows from sine-Gordon design rules and is verified by direct transport and optical measurements; the main weaknesses are evidential, not circular.

full rationale

The paper's derivation chain is self-contained. Eqs. (1) and (2) are design conditions derived from the sine-Gordon model and standard Josephson-junction properties, not fitted to the headline result. The 'perfect diode' claim rests on direct lock-in measurements of Ic (Fig. 2d) giving A > 1000, not on a fit or on a self-citation. The optical rectification data (Fig. 2e,f) are independent measurements of rectified dc voltage versus magnetic field and MW power; the threshold-free behavior is observed directly. The numerical fit of Ic(H) to Lx = 3λJ is used only to confirm the short-junction regime, and the subsequent alignment of central maxima with opposing minima is a measured outcome, not an input. Self-citations to [12,20] provide prior physical mechanism and device concepts, but the present paper includes its own sine-Gordon modeling and new experimental data, so they are not load-bearing circular steps. The main concerns are not circularity: the shunting of the MW antenna by the low-resistance current source is stated without a control experiment, and the 'near 100% efficiency' in the title is inferred from transport efficiency rather than measured optically. These are correctness/evidential risks, not circular reductions.

Assumptions & free parameters 1 free parameters · 5 assumptions · 0 invented entities

The central claim rests on standard sine-Gordon theory and a geometric scaling rule, neither invented for this paper. The most fragile load is the ad hoc shunting assumption for optical rectification, which is not tested. No new physical entities are introduced.

free parameters (1)
  • Lx/lambda_J (junction length over Josephson penetration depth) = 3
    Obtained from the numerical sine-Gordon fit to Ic(H) in Fig. 2(a) at 6.5 K; used to claim short-junction limit Eq. (2) and alignment of maxima with minima Eq. (1).
assumptions (5)
  • standard math Sine-Gordon model describes the planar JJ with self-field boundary conditions.
    Used in Methods to compute Ic(H) and to justify design rules; the fit is shown in Fig. 2(a).
  • standard math In the short-junction limit (Lx < 4 lambda_J) the critical current vanishes at one flux quantum.
    Eq. (2) and the claim that perfect cancellation is possible rely on Owen-Scalapino short-junction theory [44].
  • domain assumption The self-field inductance scales as Lsf proportional to Lx/Wz and is dominated by notch geometry and kinetic inductance.
    Used to design D2 with narrow electrodes; no direct measurement of Lsf is presented.
  • ad hoc to paper The optical rectification is caused by the low input resistance of the current source shunting one side of the MW antenna.
    Stated in the paragraph after Fig. 2(f); no control experiment is provided.
  • domain assumption The Golay cell calibration and quasi-optical path deliver a known relative MW power to the diode.
    Underlies Fig. 2(e,f) and the threshold-free conclusion; absolute power at the junction is not reported.

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Cite this review

Pith. "Pith review of Demonstration of an optical microwave rectification by a superconducting diode with near 100% efficiency." pith.science (2026). https://pith.science/paper/UJ3ZIERJ

@misc{pith2026250821696,
  author       = {Pith},
  title        = {Pith review of: Demonstration of an optical microwave rectification by a superconducting diode with near 100% efficiency},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/UJ3ZIERJ}},
  note         = {Machine review of arXiv:2508.21696}
}
read the original abstract

Superconducting electronics offer significant advantages in speed and power efficiency for next-generation computing and communication systems. However, their practical deployment is limited by the absence of simple, efficient, and scalable superconducting counterparts to key semiconductor components. In this work, we investigate diodes based on planar Josephson junctions fabricated from a conventional niobium superconductor. The nonreciprocity in these diodes arises from the self-field effect induced by the geometrical asymmetry of the junction. By deliberate tuning of the junction parameters, we achieved effectively infinite nonreciprocity (within experimental resolution), characterized by a complete suppression of the superconducting critical current in one direction while maintaining a significant current in the opposite direction. The key novelty of this work lies in the demonstration of the optical diode effect. We observed threshold-free rectification of 75 GHz microwave radiation, indicating that these diodes exhibit near-ideal optical nonreciprocity. Our results open new avenues for ultrafast superconducting electronics and lay the groundwork for wireless sub-THz signal processing.

Figures

Figures reproduced from arXiv: 2508.21696 by the authors.

Figure 1
Figure 1. (d) shows calculated Ic(H) patterns for the three bias configurations sketched in the insets. The field is normalized by the flux quantization field, H0. It can be seen that symmetric biasing (olive) leads to reciprocal Ic(H). Asymmetric biasing from one edge leads to the appearance of a self-field, which tilts the Ic(H) patterns and causes nonreciprocity at finite fields [12, 20, 30]. The sign of self-field depends… view at source ↗
Figure 2
Figure 2. (d). The offset-free Ohmic behavior indicates that there is no critical current within our experimental res￾olution (∼ 0.1 µA). Thus, conscious optimization led to the realization of a perfect (within resolution) diode with A > 1000 (100 µA/0.1 µA), and η > 99.8%. Signal processing is one of the primary applications of diodes. The top panel in [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗

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Works this paper leans on

44 extracted references · 40 canonical work pages

  1. [1]

    IEEE Comm

    Chafii, M., Bariah, L., Muhaidat, S., and Debbah, M., Twelve Scientific Challenges for 6G: Rethinking the Foundations of Communications Theory. IEEE Comm. Surv. & Tut.25, 868-904 (2023)

    work page 2023

  2. [2]

    Six Crit- ical Challenges for 6G Wireless Systems: A Summary and Some Solutions

    Tataria, H., Shafi, M., Dohler, M., and Sun, S. Six Crit- ical Challenges for 6G Wireless Systems: A Summary and Some Solutions. IEEE Veh. Techn. Mag.17, 16-26 (2022)

    work page 2022

  3. [3]

    & Van Duzer, T

    Ortlepp, T. & Van Duzer, T. Access time and power dissipation of a model 256-bit single flux quantum RAM. IEEE Trans. Appl. Supercond.24, 1300307 (2014)

    2014

  4. [4]

    and Semenov, V.K

    Likharev, K.K. and Semenov, V.K. RSFQ logic/memory family: A new Josephson-junction technology for sub- terahertz-clock-frequency digital systems. IEEE Trans. Appl. Supercond.1, 3-28 (1991)

    work page 1991

  5. [5]

    & Johnson, L.M

    Tolpygo, S.K., Bolkhovsky, V., Rastogi, R., Zarr, S., Day, A.L., Golden, E., Weir, T.J., Wynn, A. & Johnson, L.M. Advanced fabrication processes for superconductor electronics: current status and new developments. IEEE Trans. Appl. Supercond.29, 1102513 (2019)

    work page 2019

  6. [6]

    F., Vernik, I

    Kirichenko, A. F., Vernik, I. V., Kamkar, M. Y., Walter, J., Miller, M., Albu, L. R. & Mukhanov, O. A. ERSFQ 8-Bit Parallel Arithmetic Logic Unit. IEEE Trans. Appl. Supercond. 29, 1302407 (2019)

    work page 2019

  7. [7]

    A., Bum- ble, B., Le Duc, H

    Karpov, A., Miller, D., Rice, F., Stern, J. A., Bum- ble, B., Le Duc, H. D., and Zmuidzinas, J. Low Noise 1 THz–1.4 THz Mixers Using Nb/Al-AlN/NbTiN SIS Junctions. IEEE Trans. Appl. Supercond.17, 343 (2007)

    work page 2007

  8. [8]

    V., Khudchenko, A

    Tretyakov, I. V., Khudchenko, A. V., Rudakov, K. I., Ivashentseva, I. V., Kaurova, N. S., Voronov, B. M., Kir- sanova, M. S., Larchenkova, T. I., Goltsman, G. N., Bary- shev, A. M., Hesper, R., Khan, F. V., Zhukova, E. S., Chekushkin, A. M., Melentev, A. V., Zhivetev, K. V., Terentiev, A. V., and Koshelets, V. P. Development of Mixers for the High-Resolut...

    work page 2025

Show all 44 references
  1. [9]

    Y., Yuan, J., Kinev, N., Li, M

    An, D. Y., Yuan, J., Kinev, N., Li, M. Y., Huang, Y., Ji, M., Zhang, H., Sun, Z.L., Kang, L., Jin, B. B., Chen, J., Li, J., Gross, B., Ishii, A., Hirata, K., Hatano, T., Koshelets, V.P., Koelle, D., Kleiner, R., Wang, H. B., Xu, W. W., and Wu. P. H. Terahertz emission and dete...

    2013

  2. [10]

    Josephson emission with frequency span 1-11 THz from small Bi2Sr2CaCu2O8+δ mesa structures

    Borodianskyi, E.A., & Krasnov, V.M. Josephson emission with frequency span 1-11 THz from small Bi2Sr2CaCu2O8+δ mesa structures. Nat. Com. 8, 1742 (2017)

    2017

  3. [11]

    Miyamoto, M., Kobayashi, R., Kuwano, G., Tsuji- moto, M., & Kakeya, I

    M. Miyamoto, M., Kobayashi, R., Kuwano, G., Tsuji- moto, M., & Kakeya, I. Wide-band frequency modula- tion of a terahertz intrinsic Josephson junction emitter of a cuprate superconductor. Nat. Photon. 18, 267 (2024)

    2024

  4. [12]

    & Pedersen, N.F

    Krasnov, V.M., Oboznov, V.A. & Pedersen, N.F. Fluxon dynamics in long Josephson junctions in the presence of a temperature gradient or spatial nonuniformity. Phys. Rev. B 55, 14486 1997

    1997

  5. [13]

    & Ono, T

    Ando, F., Miyasaka, Y., Li, T., Ishizuka, J., Arakawa, T., Shiota, Y., Moriyama, T., Yanase, Y. & Ono, T. 5 Observation of superconducting diode effect. Nature 584, 373 (2020)

    2020

  6. [14]

    & Yanase, Y

    Nagaosa, N. & Yanase, Y. Nonreciprocal Transport and Optical Phenomena in Quantum Materials. Ann. Rev. Cond. Mat. Phys.15, 63-83 (2024)

    2024

  7. [15]

    The supercon- ducting diode effect

    Nadeem, M., Fuhrer, M.S., & Wang, X.L. The supercon- ducting diode effect. Nat. Rev. Phys.5, 558-577 (2023)

    2023

  8. [16]

    Banerjee, S., & Scheurer, M.S., Altermagnetic supercon- ducting diode effect. Phys. Rev. B.110, 024503 (2024)

    2024

  9. [17]

    & Li, J.I.A

    Lin, J.X., Siriviboon, P., Scammell, H.D., Liu, S., Rhodes, D., Watanabe, K., Taniguchi, T., Hone, J., Scheurer, M.S. & Li, J.I.A. Zero-field superconducting diode effect in small-twist-angle trilayer graphene. Nat. Phys. 18, 1221-1227 (2022)

    2022

  10. [18]

    & Ali, M.N

    Wu, H., Wang, Y., Xu, Y., Sivakumar, P.K., Pasco, C., Filippozzi, U., Parkin, S.S., Zeng, Y.J., McQueen, T. & Ali, M.N. The field-free Josephson diode in a van der Waals heterostructure. Nature 604, 653 (2022)

    2022

  11. [19]

    Fabian, J

    Baumgartner, C., Fuchs, L., Costa, A., Reinhardt, S., Gronin, S., Gardner, G.C., Lindemann, T., Manfra, M.J., Faria Junior, P.E., Kochan, D. Fabian, J. Paradiso N. & Strunk C. Supercurrent rectification and magnetochi- ral effects in symmetric Josephson junctions. Nat. Nan- ot...

    2022

  12. [20]

    and Krasnov, V.M

    Golod, T. and Krasnov, V.M. Demonstration of a super- conducting diode-with-memory, operational at zero mag- netic field with switchable nonreciprocity.Nat. Commun. 13, 3658 (2022)

    2022

  13. [21]

    Zhao, S. Y. F., Cui, X., Volkov, P.A., Yoo, H., Lee, S., Gardener, J.A., Akey, A.J., Engelke, R., Ronen, Y., Zhong, R., Gu, G., Plugge, S., Tummuru, T., Kim, M., Franz, M., Pixley, J.H., Poccia, N., and Kim, P. Time-reversal symmetry breaking superconductivity be- tween twiste...

    2023

  14. [22]

    & Pribiag, V.S

    Gupta, M., Graziano, G.V., Pendharkar, M., Dong, J.T., Dempsey, C.P., Palmstrom, C. & Pribiag, V.S. Gate- tunable superconducting diode effect in a three-terminal Josephson device. Nat. Com. 14, 3078 (2023)

    2023

  15. [23]

    & Finkelstein, G., Nonreciprocal Supercurrents in a Field- Free Graphene Josephson Triode

    Chiles, J., Arnault, E.G., Chen, C.C., Larson, T.F., Zhao, L., Watanabe, K., Taniguchi, T., Amet, F. & Finkelstein, G., Nonreciprocal Supercurrents in a Field- Free Graphene Josephson Triode. Nano Lett. 23, 5257 (2023)

    2023

  16. [24]

    Efficiency of diode effect in asymmetric inline long Josephson junc- tions

    Guarcello, C., Pagano, S., & Filatrella, G. Efficiency of diode effect in asymmetric inline long Josephson junc- tions. Appl. Phys. Lett.124, 162601 (2024)

    2024

  17. [25]

    F., Mahendru, B., Tamir, I., Bogdanoff, N., Peters, O., Reecht, G., Winkel- mann, C.B., von Oppen, F., and Franke, K.J

    Trahms, M., Melischek, L., Steiner, J. F., Mahendru, B., Tamir, I., Bogdanoff, N., Peters, O., Reecht, G., Winkel- mann, C.B., von Oppen, F., and Franke, K.J. Diode ef- fect in Josephson junctions with a single magnetic atom. Nature 615, 628–633 (2023)

    2023

  18. [26]

    Diamagnetic mechanism of critical cur- rent non-reciprocity in multilayered superconductors

    Sundaresh, A., V¨ ayrynen, J., Lyanda-Geller, Y., & Rokhinson, L.P. Diamagnetic mechanism of critical cur- rent non-reciprocity in multilayered superconductors. Nat. Com. 14, 1628 (2023)

    2023

  19. [27]

    & Deshmukh, M.M

    Ghosh, S., Patil, V., Basu, A., Kuldeep, Dutta, A., Jan- gade, D.A., Kulkarni, R., Thamizhavel, A., Steiner, J.F., von Oppen, F. & Deshmukh, M.M. High-temperature Josephson diode. Nat. Mat. 23, 612 (2024)

    2024

  20. [28]

    Cuoco, M

    Margineda, D., Crippa, A., Strambini, E., Borgongino, L., Paghi, A., de Simoni, G., Sorba, L., Fukaya, Y., Mer- caldo, M.T., Ortix, C. Cuoco, M. & Giazotto, F. Back- action supercurrent rectifiers. Com. Phys. 8, 16 (2025)

    2025

  21. [29]

    Qi, S., Ge, J., Ji, C., Ai, Y., Ma, G., Wang, Z., Cui, Z., Liu, Y., Wang Z., & Wang J., High-temperature field-free superconducting diode effect in high- Tc cuprates. Nat. Com. 16, 531 (2025)

    2025

  22. [30]

    Schmid, A

    C. Schmid, A. Jozani, R. Kleiner, D. Koelle, & E. Goldobin, YBa 2Cu3O7 Josephson diode fabricated by focused-helium-ion-beam irradiation. Phys. Rev. Appl. 24, 014041 (2025)

    2025

  23. [31]

    & Ono, T

    Narita, H., Ishizuka, J., Kawarazaki, R., Kan, D., Sh- iota, Y., Moriyama, T., Shimakawa, Y., Ognev, A.V., Samardak, A.S., Yanase, Y. & Ono, T. Field-free super- conducting diode effect in noncentrosymmetric supercon- ductor/ferromagnet multilayers. Nat. Nanotechn.17(8), 823-8...

    2022

  24. [32]

    Direct observa- tion of a superconducting vortex diode

    Gutfreund, A., Matsuki, H., Plastovets, V., Noah A., Gorzawski, L., Fridman, N., Yang, G., Buzdin, A., Millo, O., Robinson, J.W.A., and Anahory, Y. Direct observa- tion of a superconducting vortex diode. Nat. Com. 14, 1630 (2023)

    2023

  25. [33]

    Virtanen, P., Heikkla T.T

    Strambini, E., Spies, M., Ligato, N., Ili´ c, S., Rouco, M., Gonz´ alez-Orellana, C., Ilyn, M., Rogero, C., Bergeret, F.S., Moodera, J.S. Virtanen, P., Heikkla T.T. & Gia- zotto F. Superconducting spintronic tunnel diode. Nat. Com., 13, 2431 (2022)

    2022

  26. [34]

    & Peng, X., Non- reciprocal superconducting NbSe2 antenna

    Zhang, E., Xu, X., Zou, Y.C., Ai, L., Dong, X., Huang, C., Leng, P., Liu, S., Zhang, Y., Jia, Z. & Peng, X., Non- reciprocal superconducting NbSe2 antenna. Nat. Comm., 11, 5634 (2020)

    2020

  27. [35]

    & Moodera, J.S

    Ingla-Ayn´ es, J., Hou, Y., Wang, S., Chu, E.D., Mukhanov, O.A., Wei, P. & Moodera, J.S. Highly Ef- ficient Superconducting Diodes and Rectifiers for Quan- tum Circuitry. arXiv:2406.12012

    arXiv

  28. [36]

    & Gulian, A

    Chahid, S., Teknowijoyo, S., Mowgood, I. & Gulian, A. High-frequency diode effect in superconducting Nb 3Sn microbridges. Phys. Rev. B, 107, 054506 (2023)

    2023

  29. [37]

    & Berggren, K.K

    Castellani, M., Medeiros, O., Buzzi, A., Foster, R.A., Colangelo, M. & Berggren, K.K. A superconduct- ing full-wave bridge rectifier. Nat. Electron. (2025). https://doi.org/10.1038/s41928-025-01376-4

    2025 doi

  30. [38]

    Europhys

    Weiss, S., Koelle, D., M¨ uller, J., Gross, R., & Barthel, K, Ratchet effect in dc SQUIDs. Europhys. Lett.51, 499 (2000)

    2000

  31. [39]

    & Vicent, J.L

    Villegas, J.E., Savel’ev, S., Nori, F., Gonzalez, E.M., An- guita, J.V., Garcia, R. & Vicent, J.L. A superconducting reversible rectifier that controls the motion of magnetic flux quanta. Science 302, 1188 (2003)

    2003

  32. [40]

    C., Van de Vondel, J., Morelle, M

    de Souza Silva, C. C., Van de Vondel, J., Morelle, M. & Moshchalkov, V. V. Controlled multiple reversals of a ratchet effect. Nature 440, 651 (2006)

    2006

  33. [41]

    & Saitoh, E

    Lustikova, J., Shiomi, Y., Yokoi, N., Kabeya, N., Kimura, N., Ienaga, K., Kaneko, S.I., Okuma, S., Takahashi, S. & Saitoh, E. Vortex rectenna powered by environmental fluctuations. Nat. Commun. 10, 1038 (2018)

    2018

  34. [42]

    & Koelle, D

    Beck, M., Goldobin, E., Neuhaus, M., Siegel, M., Kleiner, R. & Koelle, D. High-efficiency deterministic Josephson vortex ratchet. Phys. Rev. Lett.95, 090603 (2005)

    2005

  35. [43]

    V. M. Krasnov, A distributed active patch antenna model of a Josephson oscillator. Beilstein J. Nanotechnol. 14, 151 (2023)

    2023

  36. [44]

    Owen C. S. & Scalapino D. J. Vortex Structure and Criti- cal Currents in Josephson Junctions. Phys. Rev.164, 538 (1967). 6 METHODS Device fabrication. The diodes were fabricated from a single thin (70 nm) niobium film, deposited by DC magnetron sputtering. The electrodes were ...

    1967

Pith tools

Reviewed August 5, 2026 · model on record in the stance chip above.