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The two critical temperatures conundrum in La$_{1.83}$Sr$_{0.17}$CuO$_4$
by Abhisek Samanta, Itay Mangel, Amit Keren, Daniel P. Arovas, Assa Auerbach
This is not the latest submitted version.
Submission summary
| Authors (as registered SciPost users): | Assa Auerbach |
| Submission information | |
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| Preprint Link: | https://arxiv.org/abs/2308.15540v4 (pdf) |
| Date submitted: | Jan. 30, 2024, 12:23 p.m. |
| Submitted by: | Assa Auerbach |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approaches: | Theoretical, Experimental, Computational |
Abstract
The in-plane and out-of-plane superconducting stiffness of LSCO rings appear to vanish at different transition temperatures, which contradicts thermodynamical expectation. In addition, we observe a surprisingly strong dependence of the out-of-plane stiffness transition on sample width. With evidence from Monte Carlo simulations, this effect is explained by very small ratio $\alpha$ of interplane over intraplane superconducting stiffnesses. For three dimensional rings of millimeter dimensions, a crossover from layered three dimensional to quasi one dimensional behavior occurs at temperatures near the thermodynamic transition temperature $T_{\rm c}$, and the out of-plane stiffness appears to vanish below $T_{\rm c}$ by a temperature shift of order $\alpha L_a/\xi^\parallel$, where $L_a/\xi^\parallel$ is the sample's width over coherence length. Including the effects of layer-correlated disorder, the measured temperature shifts can be fit by $\alpha=4.1\times 10^{-5}$ near $T_{\rm c}$, which is significantly lower than its previously measured value near zero temperature.
Current status:
Reports on this Submission
Report #2 by Anonymous (Referee 2) on 2024-3-19 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2308.15540v4, delivered 2024-03-19, doi: 10.21468/SciPost.Report.8729
Strengths
2-in-depth modeling of obtained data according to established theory
Weaknesses
Report
Therefore, the paper should be published.
Requested changes
The paper is somewhat difficult to read. It has a rather simple, easy to convey experimental part that meets a lengthy theoretical treatment. The overall structure of the paper is somehow, at least, unusual. The Discussion and Summary is shorter than any other part of the paper, that has at least two striking typos 'crosover' and 'cold help'. There are more typos, even if one does not count those in the supplement. Here, in their own interest, the authors should use regular software to check on things.
Report #1 by Anonymous (Referee 1) on 2024-3-10 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2308.15540v4, delivered 2024-03-10, doi: 10.21468/SciPost.Report.8687
Strengths
- Innovative experimental method;
- Very deep theoretical analysis;
- Well-organised paper.
Weaknesses
- The experiments were performed on a small number of samples.
Report
Requested changes
Authors may optionally consider the following questions:
Can the authors exclude oxygen content variation during the ring-cutting process, especially at small ring sizes? How reproducible are the data shown in Fig.2 e,d? According to the authors, only two rings survived the size reduction procedure. Is there any valuable information from broken rings? Can the authors show other data?
The authors mentioned, "We note that the c-ring magnetizations exhibit a high-temperature tail of ≃ 0.5 K above the extrapolated transition at T¯c∥. This is attributed to layer-correlated inhomogeneity, as discussed in the Introduction and Appendix A." Why do inhomogeneities play a role only for the c-ring?
We Thank the Referee for the thoughtful Report and constructive questions. The Revised manuscript incorportaed the answers into the Introduction and Summary sections. The questions are answered in detail below.
Referee > Can the authors exclude oxygen content variation during the ring-cutting process, especially at small ring sizes?
Reply> We thank the Referee for raising this question.
We have applied exactly the same laser cutting or polishing process to both c-rings and a-rings. As shown in Figure 1, except for the narrowest c-ring sample (of dimensions 0.19/0.09), which we suspect has suffered a significant structural damage, all the other samples show very much the same Tc’s, and therefore no effect of the cutting and polishing process. If significant oxygen content was varied during the cutting process, the c-ring transition temperatures Tc^parallel would not stay constant as we cut and polished them.
In the a-rings, there is a definite systematic reduction in the apparent transition temperature, which we therefore associate with a finite size effect.
Referee> How reproducible are the data shown in Fig.2 e,d? According to the authors, only two rings survived the size reduction procedure. Is there any valuable information from broken rings? Can the authors show other data?
Reply> The data was reported for the a and c rings which survived the full sequential cutting procedure. The data for each width of the rings was totally reproducible. Broken rings bring no information to this experiment, since they do not close the persistent current loop, and have zero magnetization signal. The systematic finite size dependence of Tcperp is our main experimental discovery, which brought to light an interesting theoretical puzzle.
The experimental effort producing the data in Fig.2 e,d, was a sizeable fraction of a Ph.D. thesis: crystal growth, and sequences of cutting, polishing and measurements. We encourage other groups to perform similar measurements and find out if they obtain different results.
Referee> The authors mentioned, "We note that the c-ring magnetizations exhibit a high-temperature tail of ≃ 0.5 K above the extrapolated transition at Tcparallel. This is attributed to layer-correlated inhomogeneity, as discussed in the Introduction and Appendix A." Why do inhomogeneities play a role only for the c-ring?
Reply> Layer-correlated inhomogeneity affects the stiffness of both c and a rings, but in a different way, as explained in Appendix A and Figure 7.
The c-ring diamagnetization (whose persistent currents flow within the layers) is determined by the layer averaged in-plane stiffness, and therefore vanishes above the layer-averaged <Tcparallel>. The width of the high temperature tail indicates the width of the above-average in-plane stiffness distribution.
The a-ring’s magnetization is governed by layers with the smallest order parameters. Therefore it vanishes when the order parameters in these layers disappear, which happens at a lower temperature than <Tcparallel>. Therefore layer-correlated disorder can explain a difference between a and c ring Tc’s.
However, as discussed in the paper, for the magnitude of this shift, and more importantly, its functional dependence on the width La , the layer-correlated disorder is insufficient.
Author: Assa Auerbach on 2024-04-16 [id 4422]
(in reply to Report 2 on 2024-03-19)We thank the Referee for the constructive Report . The proposal to improve the discussions is well taken. We have followed the recommendation and extended the Introduction and Summary and Discussion Sections (1 and 7) in the resubmitted manuscript, which clarified the theoretical message. We have eliminated typos. We believe that the readability of the paper has been improved.