TY - JOUR
T1 - Transport signatures of the pseudogap critical point in the cuprate superconductor
AU - Lizaire, M.
AU - Legros, A.
AU - Gourgout, A.
AU - Benhabib, S.
AU - Badoux, S.
AU - Laliberté, F.
AU - Boulanger, M. E.
AU - Ataei, A.
AU - Grissonnanche, G.
AU - LeBoeuf, D.
AU - Licciardello, S.
AU - Wiedmann, S.
AU - Ono, S.
AU - Raffy, H.
AU - Kawasaki, S.
AU - Zheng, G. Q.
AU - Doiron-Leyraud, N.
AU - Proust, C.
AU - Taillefer, L.
N1 - Funding Information:
Canadian Institute for Advanced Research Natural Sciences and Engineering Research Council of Canada Fonds de Recherche du Qu?bec - Nature et Technologies Canada Foundation for Innovation Canada Research Chairs Agence Nationale de la Recherche Canada First Research Excellence Fund Gordon and Betty Moore Foundation
Funding Information:
L.T. acknowledges support from the Canadian Institute for Advanced Research (CIFAR) as a CIFAR Fellow, and funding from the Natural Sciences and Engineering Research Council of Canada (NSERC; PIN:123817), the Fonds de Recherche du Québec—Nature et Technologies (FRQNT), the Canada Foundation for Innovation (CFI), and a Canada Research Chair. C.P. acknowledges support from the EUR grant NanoX No. -17-EURE-0009 and from the ANR grant NEPTUN No. ANR-19-CE30-0019-01. This research was undertaken thanks in part to funding from the Canada First Research Excellence Fund. Part of this work was funded by the Gordon and Betty Moore Foundation's EPiQS Initiative (Grant GBMF5306 to L.T.). This work was supported by HFML-RU/NWO-I and LNCMI-CNRS, members of the European Magnetic Field Laboratory (EMFL).
Publisher Copyright:
© 2021 American Physical Society
PY - 2021/7/1
Y1 - 2021/7/1
N2 - Five transport coefficients of the cuprate superconductor were measured in the normal state down to low temperature, reached by applying a magnetic field (up to 66 T) large enough to suppress superconductivity. The electrical resistivity, Hall coefficient, thermal conductivity, Seebeck coefficient, and thermal Hall conductivity were measured in two overdoped single crystals, with La concentration ( K) and ( K). The samples have dopings very close to the critical doping where the pseudogap phase ends. The resistivity displays a linear dependence on temperature whose slope is consistent with Planckian dissipation. The Hall number decreases with reduced , consistent with a drop in carrier density from above to below . This drop in is concomitant with a sharp drop in the density of states inferred from prior NMR Knight shift measurements. The thermal conductivity satisfies the Wiedemann-Franz law, showing that the pseudogap phase at is a metal whose fermionic excitations carry heat and charge as do conventional electrons. The Seebeck coefficient diverges logarithmically at low temperature, a signature of quantum criticality. The thermal Hall conductivity becomes negative at low temperature, showing that phonons are chiral in the pseudogap phase. Given the observation of these same properties in other, very different cuprates, our study provides strong evidence for the universality of these five signatures of the pseudogap phase and its critical point.
AB - Five transport coefficients of the cuprate superconductor were measured in the normal state down to low temperature, reached by applying a magnetic field (up to 66 T) large enough to suppress superconductivity. The electrical resistivity, Hall coefficient, thermal conductivity, Seebeck coefficient, and thermal Hall conductivity were measured in two overdoped single crystals, with La concentration ( K) and ( K). The samples have dopings very close to the critical doping where the pseudogap phase ends. The resistivity displays a linear dependence on temperature whose slope is consistent with Planckian dissipation. The Hall number decreases with reduced , consistent with a drop in carrier density from above to below . This drop in is concomitant with a sharp drop in the density of states inferred from prior NMR Knight shift measurements. The thermal conductivity satisfies the Wiedemann-Franz law, showing that the pseudogap phase at is a metal whose fermionic excitations carry heat and charge as do conventional electrons. The Seebeck coefficient diverges logarithmically at low temperature, a signature of quantum criticality. The thermal Hall conductivity becomes negative at low temperature, showing that phonons are chiral in the pseudogap phase. Given the observation of these same properties in other, very different cuprates, our study provides strong evidence for the universality of these five signatures of the pseudogap phase and its critical point.
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U2 - 10.1103/PhysRevB.104.014515
DO - 10.1103/PhysRevB.104.014515
M3 - Article
AN - SCOPUS:85111643364
SN - 2469-9950
VL - 104
JO - Physical Review B
JF - Physical Review B
IS - 1
M1 - 014515
ER -