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arxiv: 1907.00425 · v1 · pith:Q3YVYOKYnew · submitted 2019-06-30 · ❄️ cond-mat.supr-con

Dissipative-regime measurements as a tool for confirming and characterizing near-room-temperature superconductivity

Pith reviewed 2026-05-25 12:09 UTC · model grok-4.3

classification ❄️ cond-mat.supr-con
keywords superconductivityroom temperature superconductivitydissipative transportmagnetoresistancethermopowerpair breakingvortexdetection
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The pith

Dissipative transport measurements on fast timescales confirm and characterize suspected near-room-temperature superconductivity

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

New materials suspected of near-room-temperature superconductivity often show only trace amounts of the superconducting phase. Standard confirmation via complete resistance drop to zero or Meissner expulsion may not occur if the percolation threshold is not met. The paper presents a set of fast-timescale dissipative transport measurements developed by the authors as an additional tool to detect and study these incomplete superconducting signatures through secondary behaviors like magnetoresistance transitions. A sympathetic reader would care because multiple independent methods strengthen claims of high-temperature superconductivity when signals are weak.

Core claim

The authors state that their unique fast-timescale and dissipative transport measurements provide another tool set for confirming and characterizing suspected superconductivity, especially useful when trace amounts are too weak to produce an observable Meissner effect or complete zero resistance.

What carries the argument

Fast-timescale dissipative transport measurements that examine pair-breaking and vortex motion in the dissipative regime

If this is right

  • These measurements detect superconductivity even when resistance does not reach zero due to incomplete percolation.
  • They characterize properties of suspected room-temperature superconductors using secondary indicators.
  • The methods add collaborative value alongside magnetoresistance, irreversibility, and thermopower data.
  • They aid the search for new superconducting materials near room temperature.

Where Pith is reading between the lines

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

  • Testing these measurements on established superconductors with diluted phases could confirm their reliability.
  • The approach might help resolve disputes over high-temperature superconductivity claims by providing orthogonal evidence.
  • Extending the techniques to other dissipative phenomena could broaden their use in materials characterization.

Load-bearing premise

The observed transitions in temperature dependence of magnetoresistance, magnetic irreversibility, or thermopower specifically indicate superconductivity rather than other physical processes

What would settle it

Demonstrating identical transitions in a non-superconducting control sample or absence of the signatures in a known small-volume superconductor would challenge the method's validity

Figures

Figures reproduced from arXiv: 1907.00425 by Charles L. Dean, Milind N. Kunchur.

Figure 1
Figure 1. Figure 1: FIG. 1: Progression of stages of dissipation, which alterna [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: (a) [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Some typical quasi-dc high-dissipation pulse wave [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: (a) Applied voltage plateau [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Current-voltage curves for an MgB [PITH_FULL_IMAGE:figures/full_fig_p005_6.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: (a) Resistive transitions measured at various value [PITH_FULL_IMAGE:figures/full_fig_p005_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7: The vortex core as a window to the normal state: Free [PITH_FULL_IMAGE:figures/full_fig_p006_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8: Detailed tests of the ideal free-flux-flow response [PITH_FULL_IMAGE:figures/full_fig_p006_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9: (a) The primitive curve for the hot-electron regime [PITH_FULL_IMAGE:figures/full_fig_p007_9.png] view at source ↗
read the original abstract

The search for new superconducting materials approaching room temperature benefits from having a variety of testing methodologies to confirm and characterize the presence of superconductivity. Often the first signatures of new superconducting species occur incompletely and in very small volume fractions. These trace amounts may be too weak to produce an observable Meissner effect and the resistance may not go completely to zero if the percolation threshold is not met. Under these conditions, secondary behavior--such as transitions or cross overs in the temperature dependence of magnetoresistance, magnetic irreversibility, or thermopower--are often used as indications for the presence of superconductivity. Our group has developed a rather unique set of fast-timescale and dissipative transport measurements that can provide another tool set for confirming and characterizing suspected superconductivity. Here we provide some background for these methods and elucidate their collaborative value in the search for new superconducting materials. Keywords: pairbreaking, pair-breaking, vortex, vortices, theory, tutorial, RTS, room-temperature superconductivity, superconductor, detection, characterization

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 advocates for fast-timescale dissipative transport measurements as an additional confirmatory tool for suspected superconductivity, particularly when Meissner effect or zero resistance are absent due to small volume fractions; it supplies background on these methods and notes their collaborative value with secondary indicators such as magnetoresistance or thermopower transitions.

Significance. If the methods can be shown to provide specific, unambiguous signatures of superconductivity, they would add a useful experimental approach to the search for near-room-temperature materials by detecting trace amounts that evade standard tests.

major comments (1)
  1. [Abstract] Abstract: the central claim that these measurements 'can provide another tool set for confirming and characterizing suspected superconductivity' is unsupported, as the text supplies no data, error analysis, models, or controls demonstrating that the dissipative signatures are specific to superconductivity rather than other processes (e.g., magnetic ordering or inhomogeneity).
minor comments (1)
  1. The keywords list 'theory, tutorial' but the manuscript contains neither derivations nor worked examples of the methods.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their constructive comments on our manuscript. Below we provide a point-by-point response to the major comment.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the central claim that these measurements 'can provide another tool set for confirming and characterizing suspected superconductivity' is unsupported, as the text supplies no data, error analysis, models, or controls demonstrating that the dissipative signatures are specific to superconductivity rather than other processes (e.g., magnetic ordering or inhomogeneity).

    Authors: This manuscript is a perspective article that outlines the background and potential utility of fast-timescale dissipative transport measurements for characterizing suspected superconductivity, particularly in cases where conventional signatures like the Meissner effect or zero resistance are absent due to small superconducting volume fractions. The detailed experimental data, error analyses, models, and controls that establish the specificity of these dissipative signatures to superconductivity (distinguishing them from other processes such as magnetic ordering or inhomogeneity) are provided in our group's prior publications, which are cited in the manuscript. We agree that the abstract could better clarify the scope of this work as a methods overview rather than a new experimental report. We have revised the abstract and added explicit references to the supporting prior studies in the revised manuscript. revision: partial

Circularity Check

0 steps flagged

No derivation chain or predictions present; paper is methodological advocacy

full rationale

The manuscript advocates for fast-timescale dissipative transport measurements as a confirmatory tool but contains no equations, derivations, fitted parameters, or claimed first-principles predictions. The abstract and described content present no load-bearing steps that reduce by construction to inputs, self-citations, or ansatzes. The central claim is a proposal about experimental utility rather than a derived result, making the paper self-contained against the circularity criteria with no steps to flag.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Only the abstract is available; the central methodological claim rests on the domain assumption that secondary transport signatures reliably indicate superconductivity.

axioms (1)
  • domain assumption Transitions or crossovers in magnetoresistance, magnetic irreversibility, or thermopower indicate the presence of superconductivity
    The abstract invokes these secondary behaviors as indications for superconductivity when primary signatures are absent.

pith-pipeline@v0.9.0 · 5708 in / 1295 out tokens · 40770 ms · 2026-05-25T12:09:48.012834+00:00 · methodology

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Reference graph

Works this paper leans on

36 extracted references · 36 canonical work pages

  1. [1]

    A. P. Drozdov, M. I. Eremets, I. A. Troyan, V. Kseno- fontov, and S. I. Shylin, Conventional superconductivity at 203 kelvin at high pressures in the sulfur hydride sys- tem, Nature 525, 73 (2015)

  2. [2]

    C. E. Precker, P. D. Esquinazi, A. Champi, J. Barzola- Quiquia, M. Zoraghi, S. Muinos-Landin, A. Setzer, W. Bohlmann, D. Spemann, J. Meijer, T. Muenster, O. Baehre, G. Kloess, and H. Beth, Identification of a possi- ble superconducting transition above room temperature in natural graphite crystals, New J. Phys. 18, 113041 (2016)

  3. [3]

    Blatter, M

    G. Blatter, M. V. Feigel’man, V. B. Mikhail, A. I. Larkin, and V. M. Valerii, Vortices in high-temperature supercon- ductors, Rev. Mod. Phys. 66, 1125 (1994)

  4. [4]

    M. N. Kunchur, Current induced pair breaking in Magne- sium Diboride, Topical Review in J. Phys.: Cond. Matter 16, R1183-R1204 (2004)

  5. [5]

    M. N. Kunchur, Novel transport behavior found in the dissipative regime of superconductors , Mod. Phys. Lett. B. 9, 399 (1995). 8

  6. [6]

    London, and H

    F. London, and H. London, The electromagnetic equa- tions of the supraconductor , Proc. R. Soc. A 149, 71 (1935)

  7. [7]

    Michael Tinkham, Introduction to Superconductivity, 2nd Edition, McGraw Hill, New York (1996)

  8. [8]

    P. D. Scholten, J. D. Lejeune, W. M. Saslow, and D. G. Naugle, Low-frequency electromagnetic response function for strong-coupling superconductors , Phys. Rev. B. 16, 1068 (1977)

  9. [9]

    I. F. Oppenheim, S. Frota-Pessoa, and M. Octavio, Time delay in the response of superconducting filaments to su- percritical current pulses, Phys. Rev. B. 25, 4495 (1982)

  10. [10]

    J. Y. Y. Lee and T. R. Lemberger, Penetration depth λ (T ) of Y1Ba2Cu3O7 films determined from the kinetic inductance, Appl. Phys. Lett. 62, 2419 (1993)

  11. [11]

    G. F. Saracila and M. N. Kunchur, Ballistic acceleration of a supercurrent in a superconductor , Phys. Rev. Lett. 102, 077001 (Feb. 20, 2009)

  12. [12]

    Goren, and E

    L. Goren, and E. Altmun, Quenching the superconduct- ing state of cuprate compounds with electric currents: A variational study , Phys. Rev. Lett. 104, 257002 (2010)

  13. [13]

    M. N. Kunchur, D. K. Christen, C. E. Klabunde, and J. M. Phillips, Pair-breaking effect of high current densities on the superconducting transition on YBa2Cu3O7 , Phys. Rev. Lett. 72, 752 (1994)

  14. [14]

    M. N. Kunchur, Sung-Ik Lee, and W. N. Kang, The pair- breaking critical current density of magnesium diboride , Phys. Rev. B. 68, 064516 (2003)

  15. [15]

    M. N. Kunchur, C. Dean, M. Liang, N. S. Moghaddam, A. Guarino, A. Nigro,G. Grimaldi, A. Leo, Depairing cur- rent density of Nd2-xCexCuO4-d superconducting films , Physica C 495, 66 (2013)

  16. [16]

    M. N. Kunchur, D. K. Christen, and J. M. Phillips, Ob- servation of free flux flow at high dissipation levels in YBa2Cu3O7 epitaxial films , Phys. Rev. Lett. 70, 998 (1993)

  17. [17]

    M. N. Kunchur, B. I. Ivlev, D. K. Christen, and J. M. Phillips, Metallic normal state of YBa2Cu3O7 , Phys. Rev. Lett. 84, 5204 (2000)

  18. [18]

    Liang, M

    M. Liang, M. N. Kunchur, J. Hua and Z. Xiao, Evaluat- ing free flux flow in low-pinning molybdenum-germanium superconducting films, Phys. Rev. B 82, 064502 (2010)

  19. [19]

    Ullah and A

    S. Ullah and A. T. Dorsey, Effect of fluctuations on the transport properties of type-II superconductors in a mag- netic field , Phys. Rev. B. 44, 262 (1991)

  20. [20]

    A. T. Dorsey, Vortex motion and the Hall effect in type- II superconductors: A time-dependent Ginzburg-Landau theory approach, Phys. Rev. B. 46, 8376 (1992)

  21. [21]

    A. I. Larkin and Yu. N. Ovchinnikov, in Nonequilibrium Superconductivity, edited by D. N. Langenberg and A. I. Larkin (Elsevier, Amsterdam, 1986), Chap. 11

  22. [22]

    A. I. Larkin and Yu. N. Ovchinnikov, Nonlinear conduc- tivity of superconductors in the mixed state , Zh. Eksp. Teor. Fiz. 68, 1915 (1975) [Sov. Phys. JETP 41, 960 (1976)]

  23. [23]

    M. N. Kunchur, Unstable flux flow due to heated electrons in superconducting films , Phys. Rev. Lett. 89, 137005 (2002)

  24. [24]

    Knight and M

    J.M. Knight and M. N. Kunchur, Energy relaxation at a hot-electron vortex instability , Phys. Rev. B 74, 64512 (2006)

  25. [25]

    L. E. Musienko, I. M. Dmitrenko, and V. G. Volotskaya, Nonlinear conductivity of thin films in the mixed state , Pis’ma Zh. Eksp. Teor. Fiz. 31, 603 (1980) [JETP Lett. 31, 567 (1980)]

  26. [26]

    Grimaldi, A

    G. Grimaldi, A. Leo, A. Nigro, S. Pace, and R. P. Huebener, Dynamic ordering and instability of the vortex lattice in Nb films exhibiting moderately strong pinning , Phys. Rev. B. 80, 144521 (2009)

  27. [27]

    M. N. Kunchur, B.I. Ivlev, and J. M. Knight, Steps in the negative-differential-conductivity regime of a super- conductor, Phys. Rev. Lett. 87, 177001 (2001)

  28. [28]

    M. N. Kunchur, B.I. Ivlev, and J. M. Knight, Shear frag- mentation of unstable flux flow , Phys. Rev. B 66, 060505 (2002)

  29. [29]

    V. R. Misko, S. Savel’ev, Alexander L. Rakhmanov, and Franco Nori, Negative differential resistivity in supercon- ductors with periodic arrays of pinning sites , Phys. Rev. B 75, 024509 (2007)

  30. [30]

    J. P. Carbotte, E. Schachlinger, and D. N. Basov, Cou- pling strength of charge carriers to spin fluctuations in high-temperature superconductors , Nature 401, 354 (1999)

  31. [31]

    J. J. Tu, C. C. Homes, G. D. Gu, D. N. Basov, and M. Strongin, Optical studies of charge dynamics in optimally doped Bi2Sr2CaCu2O8, Phys. Rev. B. 66, 144514 (2002)

  32. [32]

    M. N. Kunchur, D. K. Christen, C. E. Klabunde, and K. Salama, Exploring the dissipative regime of superconduc- tors for practical current-lead applications , Appl. Phys. Lett. 67, 848 (1995)

  33. [33]

    ⃗Aω ( ⃗r′)] R4 I(ω, ⃗R, T )d⃗r′, and I(ω, ⃗R, T ) is related to the electron-phonon spectral function α 2(ω )F (ω )

    In more detail [8], Lk ∝ I(0, 0, T ), where the superconductor’s electromagnetic response function I(ω, ⃗R, T ) is defined by ⃗j(⃗ r, ω) = e2N(0)vF 2π 2ℏc × ∫ ⃗R[ ⃗R. ⃗Aω ( ⃗r′)] R4 I(ω, ⃗R, T )d⃗r′, and I(ω, ⃗R, T ) is related to the electron-phonon spectral function α 2(ω )F (ω )

  34. [34]

    The normal-current component jn ≈ (nn/n )σ nE, which results from the electric field present during superfluid acceleration, is several orders of magnitude smaller than js at the frequencies of the experiment

  35. [35]

    This spectral function is defined as α 2F = V (2π )3ℏ2 ∫ d2k′ v′ F |Mk=k′|2δ(ω − cs|k − k′|), where Mk=k′ is the electron-phonon matrix element

  36. [36]

    Here fe(E, E ′) = f (Ek)[1− f (E′ k)] 1− f (Ek) ( 1 − ∆k∆k′ EkEk′ ) combines the coherence and occupation factors