| Literature DB >> 30760922 |
B Michon1,2,3, C Girod1,2,3, S Badoux2, J Kačmarčík4, Q Ma5, M Dragomir6, H A Dabkowska6, B D Gaulin5,6,7, J-S Zhou8, S Pyon9, T Takayama9, H Takagi9, S Verret2, N Doiron-Leyraud2, C Marcenat10, L Taillefer11,12, T Klein13,14.
Abstract
The three central phenomena of cuprate (copper oxide) superconductors are linked by a common doping level p*-at which the enigmatic pseudogap phase ends and the resistivity exhibits an anomalous linear dependence on temperature, and around which the superconducting phase forms a dome-shaped area in the phase diagram1. However, the fundamental nature of p* remains unclear, in particular regarding whether it marks a true quantum phase transition. Here we measure the specific heat C of the cuprates Eu-LSCO and Nd-LSCO at low temperature in magnetic fields large enough to suppress superconductivity, over a wide doping range2 that includes p*. As a function of doping, we find that Cel/T is strongly peaked at p* (where Cel is the electronic contribution to C) and exhibits a log(1/T) dependence as temperature T tends to zero. These are the classic thermodynamic signatures of a quantum critical point3-5, as observed in heavy-fermion6 and iron-based7 superconductors at the point where their antiferromagnetic phase comes to an end. We conclude that the pseudogap phase of cuprates ends at a quantum critical point, the associated fluctuations of which are probably involved in d-wave pairing and the anomalous scattering of charge carriers.Entities:
Year: 2019 PMID: 30760922 DOI: 10.1038/s41586-019-0932-x
Source DB: PubMed Journal: Nature ISSN: 0028-0836 Impact factor: 49.962