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Record W2737368901 · doi:10.1103/physrevb.97.064502

Pseudogap temperature <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msup><mml:mi>T</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:math> of cuprate superconductors from the Nernst effect

2018· article· lv· W2737368901 on OpenAlexafffund
O. Cyr-Choinière, Ramzy Daou, F. Laliberté, Clément Collignon, S. Badoux, David LeBoeuf, J. Chang, B. J. Ramshaw, D. A. Bonn, W. N. Hardy, Ruixing Liang, Jiaqiang Yan, Jinguang Cheng, Jianshi Zhou, John B. Goodenough, Sunseng Pyon, T. Takayama, H. Takagi, N. Doiron-Leyraud, Louis Taillefer

Bibliographic record

VenuePhysical review. B./Physical review. B · 2018
Typearticle
Languagelv
FieldPhysics and Astronomy
TopicPhysics of Superconductivity and Magnetism
Canadian institutionsCanadian Institute for Advanced ResearchUniversity of British ColumbiaInstitut quantiqueUniversité de Sherbrooke
FundersFonds de recherche du Québec – Nature et technologiesNatural Sciences and Engineering Research Council of CanadaLaboratoire d’excellence Physique Atomes Lumière MatièreUniversité Paris-SudAgence Nationale de la RechercheUniversité Paris-SaclayCanada Foundation for InnovationJapan Society for the Promotion of ScienceCanadian Institute for Advanced ResearchLabexÉcole Supérieure de Physique et de Chimie Industrielles de la Ville de ParisSchweizerischer Nationalfonds zur Förderung der Wissenschaftlichen ForschungEuropean Research CouncilGordon and Betty Moore FoundationMinistry of Education, Culture, Sports, Science and TechnologyNational Science Foundation
KeywordsPseudogapCuprateCondensed matter physicsSuperconductivityPhysicsAngle-resolved photoemission spectroscopyPhase diagramDopingNernst effectPhase (matter)CrystallographyNernst equationElectronic structureChemistryQuantum mechanics

Abstract

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We use the Nernst effect to delineate the boundary of the pseudogap phase in the temperature-doping phase diagram of hole-doped cuprate superconductors. New data for the Nernst coefficient $\ensuremath{\nu}(T)$ of ${\mathrm{YBa}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{y}$ (YBCO), ${\mathrm{La}}_{1.8\ensuremath{-}x}{\mathrm{Eu}}_{0.2}{\mathrm{Sr}}_{x}{\mathrm{CuO}}_{4}$ (Eu-LSCO), and ${\mathrm{La}}_{1.6\ensuremath{-}x}{\mathrm{Nd}}_{0.4}{\mathrm{Sr}}_{x}{\mathrm{CuO}}_{4}$ (Nd-LSCO) are presented and compared with previously published data on YBCO, Eu-LSCO, Nd-LSCO, and ${\mathrm{La}}_{2\ensuremath{-}x}{\mathrm{Sr}}_{x}{\mathrm{CuO}}_{4}$ (LSCO). The temperature ${T}_{\ensuremath{\nu}}$ at which $\ensuremath{\nu}/T$ deviates from its high-temperature linear behavior is found to coincide with the temperature at which the resistivity $\ensuremath{\rho}(T)$ deviates from its linear-$T$ dependence, which we take as the definition of the pseudogap temperature ${T}^{★}$---in agreement with the temperature at which the antinodal spectral gap detected in angle-resolved photoemission spectroscopy (ARPES) opens. We track ${T}^{★}$ as a function of doping and find that it decreases linearly vs $p$ in all four materials, having the same value in the three LSCO-based cuprates, irrespective of their different crystal structures. At low $p,{T}^{★}$ is higher than the onset temperature of the various orders observed in underdoped cuprates, suggesting that these orders are secondary instabilities of the pseudogap phase. A linear extrapolation of ${T}^{★}(p)$ to $p=0$ yields ${T}^{★}(p\ensuremath{\rightarrow}0)\ensuremath{\simeq}{T}_{\mathrm{N}}$(0), the N\'eel temperature for the onset of antiferromagnetic order at $p=0$, suggesting that there is a link between pseudogap and antiferromagnetism. With increasing $p,{T}^{★}(p)$ extrapolates linearly to zero at $p\ensuremath{\simeq}{p}_{\mathrm{c}2}$, the critical doping below which superconductivity emerges at high doping, suggesting that the conditions which favor pseudogap formation also favor pairing. We also use the Nernst effect to investigate how far superconducting fluctuations extend above the critical temperature ${T}_{\mathrm{c}}$, as a function of doping, and find that a narrow fluctuation regime tracks ${T}_{\mathrm{c}}$, and not ${T}^{★}$. This confirms that the pseudogap phase is not a form of precursor superconductivity, and fluctuations in the phase of the superconducting order parameter are not what causes ${T}_{\mathrm{c}}$ to fall on the underdoped side of the ${T}_{\mathrm{c}}$ dome.

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame machine prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. The Gemma side is a direct model label for every work in the frame, read from the title-only record. The Codex side is a classifier learned from the 10,348 direct Codex labels and calibrated to design-weighted sample rates; fields without enough sample support carry no Codex call. Candidate is the union of the two sides; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels.

metaresearch head score (Codex)0.000
metaresearch head score (Gemma)0.001
Version: metacan-v3-hybrid-931329e0061cValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Observational · Consensus signal: none
GenreCandidate signal: Empirical · Consensus signal: none
Teacher disagreement score0.024
Threshold uncertainty score0.081

Distilled classifier scores by category (both heads)

CategoryCodexGemma
Metaresearch0.0000.001
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0000.000
Bibliometrics0.0010.000
Science and technology studies0.0000.000
Scholarly communication0.0010.001
Open science0.0010.000
Research integrity0.0000.001
Insufficient payload (model declined to judge)0.0240.007

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.018
GPT teacher head0.283
Teacher spread0.265 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one source (direct Gemma or distilled Codex), not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designObservational
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

Quick stats

Citations121
Published2018
Admission routes2
Has abstractyes

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Same venuePhysical review. B./Physical review. BSame topicPhysics of Superconductivity and MagnetismFrench-language works237,207