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arxiv: 2604.12313 · v1 · submitted 2026-04-14 · ❄️ cond-mat.supr-con · cond-mat.mes-hall· physics.app-ph

Nanoscale electrothermal-switch superconducting diode for electrically programmable superconducting circuits

Pith reviewed 2026-05-10 15:30 UTC · model grok-4.3

classification ❄️ cond-mat.supr-con cond-mat.mes-hallphysics.app-ph
keywords superconducting diodeelectrothermal switchnanowirenonreciprocal transportvortex dynamicsprogrammable circuitsrectificationgate control
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The pith

A gate-controlled nanoscale hotspot in a superconducting nanowire creates an electrically tunable diode enabling programmable rectification circuits.

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

The paper demonstrates a superconducting diode where a small gate current generates a local hotspot that breaks inversion symmetry and produces directional current flow. This creates two regimes of nonreciprocal transport, one tied to the superconducting-to-normal transition and the other to vortex motion, both arising from the same process. The diode reaches efficiencies of 42 percent and 60 percent and can be turned on, off, or reversed in polarity using only electrical signals. If the mechanism holds, it provides a way to build superconducting circuits whose rectification functions can be reconfigured on demand without magnetic fields or other external controls.

Core claim

We demonstrate an electrothermal-switch superconducting diode in which a gate-controlled nanoscale hotspot dynamically breaks inversion symmetry in a superconducting nanowire. This mechanism gives rise to two coexisting nonreciprocal transport regimes—one associated with a nonreciprocal superconducting-to-normal transition and the other with ratchet-like vortex dynamics—both originating from the same electrothermal-switch process. The diode exhibits efficiencies up to 42% and 60% for the two regimes, respectively, and can be electrically switched on, off, or reversed in polarity in situ by applying a small gate current. These capabilities enable programmable superconducting circuits that can

What carries the argument

Gate-controlled nanoscale hotspot that dynamically breaks inversion symmetry through the electrothermal-switch process in the superconducting nanowire, producing nonreciprocal transport in two regimes.

Load-bearing premise

The observed nonreciprocal transport originates specifically from the electrothermal-switch process that dynamically breaks inversion symmetry rather than from fabrication artifacts or other unaccounted mechanisms.

What would settle it

Fabricating control devices that cannot form the gate-controlled hotspot or measuring identical nonreciprocal behavior when the hotspot is deliberately suppressed would show that the electrothermal-switch is not the cause.

read the original abstract

Superconducting diodes enable dissipationless directional transport, yet achieving electrical tunability and scalability remains a major challenge for circuit-level integration. Here, we demonstrate an electrothermal-switch superconducting diode in which a gate-controlled nanoscale hotspot dynamically breaks inversion symmetry in a superconducting nanowire. This mechanism gives rise to two coexisting nonreciprocal transport regimes-one associated with a nonreciprocal superconducting-to-normal transition and the other with ratchet-like vortex dynamics-both originating from the same electrothermal-switch process. The diode exhibits efficiencies up to 42% and 60% for the two regimes, respectively, and can be electrically switched on, off, or reversed in polarity in situ by applying a small gate current. These capabilities enable programmable superconducting circuits that realize electrically reconfigurable full-wave and half-wave rectification. The lithography-compatible design, high performance, and gate-controlled functionality establish a scalable platform for programmable superconducting electronics and hybrid quantum systems.

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 reports the experimental demonstration of an electrothermal-switch superconducting diode in a superconducting nanowire. A gate-controlled nanoscale hotspot is used to dynamically break inversion symmetry, producing two coexisting nonreciprocal transport regimes (one tied to a nonreciprocal superconducting-to-normal transition and the other to ratchet-like vortex dynamics) with efficiencies up to 42% and 60%, respectively. The device can be electrically switched on, off, or polarity-reversed in situ by a small gate current, enabling programmable superconducting circuits that realize reconfigurable full-wave and half-wave rectification.

Significance. If the central attribution to the dynamic electrothermal mechanism holds and the reported efficiencies and switching are robust, this provides a lithography-compatible, scalable platform for electrically programmable superconducting electronics. The dual-regime operation and in-situ gate control would be valuable for circuit-level integration and hybrid quantum systems.

major comments (1)
  1. [Abstract] The headline claim that the observed nonreciprocity (including the 42% and 60% efficiencies and in-situ polarity reversal) originates specifically from the gate-induced nanoscale hotspot dynamically breaking inversion symmetry is load-bearing but insufficiently secured. The manuscript provides no quantitative metrology (e.g., SEM uniformity data) or symmetric control-device measurements to bound static fabrication asymmetries, vortex pinning gradients, or residual flux as alternative sources; without these, the mechanism attribution cannot be isolated from fabrication artifacts.
minor comments (1)
  1. Device dimensions, material (e.g., NbN), gate-current values, and full error-bar/statistical details of the efficiency measurements should be stated explicitly in the main text rather than deferred entirely to supplementary material.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their thorough review and valuable feedback on our manuscript. We address the major comment point by point below and outline the revisions we will make to strengthen the claims regarding the mechanism.

read point-by-point responses
  1. Referee: [Abstract] The headline claim that the observed nonreciprocity (including the 42% and 60% efficiencies and in-situ polarity reversal) originates specifically from the gate-induced nanoscale hotspot dynamically breaking inversion symmetry is load-bearing but insufficiently secured. The manuscript provides no quantitative metrology (e.g., SEM uniformity data) or symmetric control-device measurements to bound static fabrication asymmetries, vortex pinning gradients, or residual flux as alternative sources; without these, the mechanism attribution cannot be isolated from fabrication artifacts.

    Authors: We acknowledge the importance of rigorously excluding static fabrication artifacts to confirm the dynamic electrothermal mechanism. The key evidence supporting the dynamic origin is the in-situ electrical programmability: the diode can be turned on, off, or have its polarity reversed by applying a small gate current. This tunability would not be possible if the nonreciprocity arose from fixed static asymmetries due to fabrication imperfections, vortex pinning gradients, or residual flux, as those are not gate-dependent. The gate current specifically induces the nanoscale hotspot that dynamically breaks the inversion symmetry. To further secure this attribution, we will add quantitative SEM uniformity data in the revised manuscript to characterize the nanowire uniformity and bound potential fabrication asymmetries. While we do not have dedicated symmetric control devices in the current dataset, the gate-controlled switching acts as a built-in control demonstrating the dynamic control. We will also discuss the exclusion of residual flux effects more explicitly in the text. These additions will strengthen the manuscript without altering the core conclusions. revision: partial

Circularity Check

0 steps flagged

No circularity: experimental measurements with no derivational reduction

full rationale

The paper is an experimental report on a fabricated superconducting nanowire device. Reported efficiencies (42% and 60%) are direct measurements of nonreciprocal transport under gate bias; no equations, ansatzes, or fitted parameters are presented that redefine or predict these values from themselves. No self-citation chains are invoked to justify uniqueness theorems or load-bearing premises. The central claim (electrothermal symmetry breaking) is an interpretive attribution of observed data rather than a closed mathematical derivation. This is the expected outcome for a measurement-focused manuscript.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

No explicit free parameters, axioms, or invented entities are identifiable from the abstract; the central claims rest on experimental observation of the electrothermal mechanism.

pith-pipeline@v0.9.0 · 5524 in / 1031 out tokens · 53761 ms · 2026-05-10T15:30:56.051833+00:00 · methodology

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Reference graph

Works this paper leans on

60 extracted references · 60 canonical work pages · 1 internal anchor

  1. [1]

    Nadeem, M., Fuhrer, M. S. & Wang, X. The superconducting diode effect. Nature Reviews Physics 5, 558-577 (2023)

  2. [2]

    Ando, F. et al. Observation of superconducting diode effect. Nature 584, 373-376 (2020)

  3. [3]

    Wan, Z. et al. Unconventional superconductivity in chiral molecule -TaS2 hybrid superlattices. Nature 632, 69-74 (2024)

  4. [4]

    Castellani, M. et al. A superconducting full -wave bridge rectifier. Nature Electronics 8, 417- 425 (2025)

  5. [5]

    Lyu, Y. -Y. et al. Superconducting diode effect via conformal -mapped nanoholes. Nature Communications 12, 2703 (2021)

  6. [6]

    Ingla-Aynés, J. et al. Efficient superconducting diodes and rectifiers for quantum circuitry. Nature Electronics 8, 411-416 (2025)

  7. [7]

    Baumgartner, C. et al. Supercurrent rectification and magnetochiral effects in symmetric Josephson junctions. Nature Nanotechnology 17, 39-44 (2021)

  8. [8]

    & Krasnov, V

    Golod, T. & Krasnov, V. M. Demonstration of a supe rconducting diode -with-memory, operational at zero magnetic field with switchable nonreciprocity. Nature Communications 13, 3658 (2022)

  9. [9]

    Narita, H. et al. Field-free superconducting diode effect in noncentrosymmetric superconductor/ferromagnet multilayers. Nature Nanotechnology 17, 823-828 (2022)

  10. [10]

    Hou, Y. S. et al. Ubiquitous Superconducting Diode Effect in Superconductor Thin Films. Physical Review Letters 131, 094002 (2023)

  11. [11]

    Trahms, M. et al. Diode effect in Josephson junctions with a single magnetic atom. Nature 615, 628-633 (2023)

  12. [12]

    Jeon, K. -R. et al. Zero-field polarity -reversible Josephson supercurrent diodes enabled by a proximity-magnetized Pt barrier. Nature Materials 21, 1008-1013 (2022)

  13. [13]

    Li, J. et al. Field ‐ Free Superconducting D iode Enabled by Geometric Asymmetry and Perpendicular Magnetization. Advanced Materials, e11414 (2025)

  14. [14]

    Turini, B. et al. Josephson Diode Effect in High- Mobility InSb Nanoflags. Nano Letters 22, 8502-8508 (2022)

  15. [15]

    Pal, B. et al. Josephson diode effect from Cooper pair momentum in a topological semimetal. Nature Physics 18, 1228-1233 (2022)

  16. [16]

    Wu, H. et al. The field-free Josephson diode in a van der Waals heterostructure. Nature 604, 653-656 (2022)

  17. [17]

    Bauriedl, L. et al. Supercurrent diode effect and magnetochiral anisotropy in few -layer NbSe2. Nature Communications 13, 4266 (2022)

  18. [18]

    Chen, P. et al. Edelstein Effect Induced Superconducting Diode Effect in Inversion Symmetry Breaking MoTe2 Josephson Junctions. Advanced Functional Materials 34, 2311229 (2023)

  19. [19]

    Qi, S. et al. High-temperature field -free superconducting diode effect in high- Tc cuprates. Nature Communications 16 (2025)

  20. [20]

    Díez-Mérida, J. et al. Symmetry-broken Josephson junctions and superconducting diodes i n magic-angle twisted bilayer graphene. Nature Communications 14, 2396 (2023)

  21. [21]

    Ghosh, S. et al. High-temperature Josephson diode. Nature Materials 23, 612-618 (2024). 15

  22. [22]

    Zhao, S. Y. F. et al. Time-reversal symmetry breaking superconductivity between t wisted cuprate superconductors. Science 382, 1422-1427 (2023)

  23. [23]

    Lin, J.-X. et al. Zero-field superconducting diode effect in small -twist-angle trilayer graphene. Nature Physics 18, 1221-1227 (2022)

  24. [24]

    Wang, H. et al. Quantum superconducting diode effect with perfect efficiency above liquid- nitrogen temperature. Nature Physics (2025)

  25. [25]

    Qin, F. et al. Superconductivity in a chiral nanotube. Nature Communications 8, 14465 (2017)

  26. [26]

    Le, T. et al. Superconducting diode effect and interference patterns in kagome CsV3Sb5. Nature 630, 64-69 (2024)

  27. [27]

    Gupta, M. et al. Gate-tunable superconducting diode effect in a three-terminal Josephson device. Nature Communications 14, 3078 (2023)

  28. [28]

    Ciaccia, C. et al. Gate-tunable Josephson diode in proximitized InAs supercurrent interferometers. Physical Review Research 5, 033131 (2023)

  29. [29]

    Valentini, M. et al. Parity-conserving Cooper-pair transport and ideal superconducting diode in planar germanium. Nature Communications 15, 169 (2024)

  30. [30]

    Reinhardt, S. et al. Link between supercurrent diode and anomalous Josephson effect re vealed by gate-controlled interferometry. Nature Communications 15, 4413 (2024)

  31. [31]

    Mazur, G. P. et al. Gate-tunable Josephson diode. Physical Review Applied 22, 054034 (2024)

  32. [32]

    Shin, J. et al. Electric Control of Polarity in Spin -Orbit Josephson Diode . arXiv:2409.17820 (2024). <https://ui.adsabs.harvard.edu/abs/2024arXiv240917820S>

  33. [33]

    Yan, S. L. et al. Gate Tunable Josephson Diode Effect in Josephson Junctions Made from InAs Nanosheets. Advanced Functional Materials 35, 2503401 (2025)

  34. [34]

    & Nagaosa, N

    Lu, B., Ikegaya, S., Burset, P., Tanaka, Y. & Nagaosa, N. Tunable Josephson Diode Effect on the Surface of Topological Insulators. Physical Review Letters 131, 096001 (2023)

  35. [35]

    Xiong, J. L. et al. Electrical switching of Ising -superconducting nonreciprocity for quantum neuronal transistor. Nature Communications 15, 4953 (2024)

  36. [36]

    McCaughan, A. N. & Berggren, K. K. A Superconducting- Nanowire Three- Terminal Electrothermal Device. Nano Letters 14, 5748-5753 (2014)

  37. [37]

    Huang, Y. -H. et al. Splitter trees of superconducting nanowire cryotrons for large fan -out. Applied Physics Letters 122, 092601 (2023)

  38. [38]

    McCaughan, A. N. et al. A superconducting thermal switch with ultrahigh impedance for interfacing superconductors to semiconductors. Nature Electronics 2, 451-456 (2019)

  39. [39]

    N., Dane, A

    Zhao, Q.-Y., McCaughan, A. N., Dane, A. E., Berggren, K. K. & Ortlepp, T. A nanocryotron comparator can connect single -flux-quantum circuits to conventional electronics. Superconductor Science and Technology 30, 044002 (2017)

  40. [40]

    Tanaka, M. et al. Josephson-CMOS Hybrid Memory With Nanocryotrons. IEEE Transactions on Applied Superconductivity 27, 1-4 (2017)

  41. [41]

    Buzzi, A. et al. A nanocryotron memory and logic family. Applied Physics Letters 122, 142601 (2023)

  42. [42]

    Zheng, K. et al. Characterize the switching performance of a superconducting nanowire cryotron for reading superconducting nanowire single photon detectors. Scientific Reports 9, 16345 (2019). 16

  43. [43]

    Baghdadi, R. et al. Multilayered Heater Nanocryotron: A Superconducting -Nanowire-Based Thermal Switch. Physical Review Applied 14, 054011 (2020)

  44. [44]

    Strambini, E. et al. Superconducting spintronic tunnel diode. Nature Communications 13, 2431 (2022)

  45. [45]

    Schneider, M. et al. SuperMind: a survey of the potential of superconducting electronics for neuromorphic computing. Superconductor Science and Technology 35, 053001 (2022)

  46. [46]

    & Livingston, J

    Bean, C. & Livingston, J. Surface barrier in type -II superconductors. Physical Review Letters 12, 14 (1964). 1 Supplementary information for Nanoscale electrothermal-switch superconducting diode for electrically programmable superconducting circuits Tianyu Li1,2,#, Jiong Li3,#, Chong Li1,4,#, Peiyuan Huang1,5, Nuo-Zhou Yang1,2, Wuyue Xu1,2, Wen-Cheng Yue...

  47. [47]

    As the gate current is increased (enhance Joule heating), both I c+ and Ic- are progressively suppressed (Fig

    Further explanation of a spatial thermal gradient that breaks inversion symmetry We conducted experiments using different gating currents which modifies the Joule heating of the hotspots (Figure S7). As the gate current is increased (enhance Joule heating), both I c+ and Ic- are progressively suppressed (Fig. S7a) with a monotonic decrease in diode effici...

  48. [48]

    The influence of magnetic fields on the device Figure S8a presents the I–V characteristics measured at zero magnetic field and zero gate current at various temperatures below the superconducting transition temperature (2–7 K). In this case, the positive and negative critical currents are nearly identical, indicating negligible nonreciprocity in the absenc...

  49. [49]

    i) Fully superconducting interval (Green)

    The states of each diode in the full-wave rectifier We use the bridge circuit in Figure S11 a as an example and provide a detailed breakdown of the operational status of each diode during different temporal intervals, as illustrated in Figure S11 and summarized in Table 1. i) Fully superconducting interval (Green). When the input sinusoidal signal is in t...

  50. [50]

    As shown in Figure S13, the degree of nonreciprocity gradually diminishes with increasing gate current amplitude

    Dependence on gate current amplitude To elucidate the origin of the nonreciprocal transport, we examined the effect of gate current magnitude on the diode behavior. As shown in Figure S13, the degree of nonreciprocity gradually diminishes with increasing gate current amplitude. This trend can be attributed to the enhanced electrothermal homogenization ind...

  51. [51]

    The magnetic- field- dependent critical currents were measured over a temperature range of 2 K to 7.5 K (Figure S14)

    Temperature dependence of nonreciprocal transport We next investigated the temperature dependence of the SDE. The magnetic- field- dependent critical currents were measured over a temperature range of 2 K to 7.5 K (Figure S14). The results show that the device exhibits clear nonreciprocity of the critical current (± Ic) below its superconducting transitio...

  52. [52]

    The results reveal a gradual reduction in the maximum efficiency as temperature rises

    Maximum diode efficiency at different temperatures To provide a quantitative overview, the maximum diode efficiencies obtained at different temperatures are summarized in Fig ure S 17. The results reveal a gradual reduction in the maximum efficiency as temperature rises. This correlated evolution of diode efficiency further supports the thermally driven o...

  53. [53]

    This asymmetry arises from the presence of the gate current, which slightly offsets the effective bias current

    Correction for asymmetry in normal-state resistance A minor discrepancy was observed between the normal -state resistances measured directly under positive and negative current biases (Figure S 18a). This asymmetry arises from the presence of the gate current, which slightly offsets the effective bias current. If the current in the positive direction is d...

  54. [54]

    The bandwidth limitation and switching speed of the electrothermal -switch superconducting diode From the practical measurement perspective, the present rectification demonstrations at 100 Hz are limited by our cryogenic measurement setup rather than by the intrinsic device physics. In our current low -temperature system, each measurement line uses enamel...

  55. [55]

    The energy and dissipation characteristics of the device (1) Steady-state gate power. In our device, the steady -state gate power required to maintain the electrothermal hotspot is approximately 42 nW, estimated from the applied gate current and voltage across the gate lead. Most prior reports on electrically tunable superconducting diodes [Nat. Nanotechn...

  56. [56]

    Ginzburg, V . L. & Landau, L. D. On superconductivity and superfluidity: a scientific autobiography 113-137 (Springer, 2009)

  57. [57]

    & Adams, C

    Winiecki, T. & Adams, C. S. A Fast Semi -Implicit Finite -Difference Method for the TDGL Equations. J. Comput. Phys. 179, 127-139 (2002)

  58. [58]

    Y ., Peeters, F

    V odolazov, D. Y ., Peeters, F. M., Morelle, M. & Moshchalkov, V . V . Masking effect of heat dissipation on the current-voltage characteristics of a mesoscopic superconducting sample with leads. Phys. Rev. B 71, 184502 (2005)

  59. [59]

    Lyu, Y .-Y. et al. Superconducting diode effect via conformal-mapped nanoholes. Nat. Commun. 12, 2703 (2021)

  60. [60]

    S, A. et al. Superconducting properties of Nb, NbN, and MoN thin films grown on topological insulator Bi 1.95Sb0.05Se3: a comparative study. Superconductor Science and Technology 35, 094002 (2022)