Abstract

We report thermopower measurements under hydrostatic pressure on the cuprate superconductor La$_{1.6-x}$Nd$_{0.4}$Sr$_x$CuO$_4$ (Nd-LSCO), at low-temperature in the normal state accessed by suppressing superconductivity with a magnetic field up to $H = 31$ T. Using a newly developed AC thermopower measurement technique suitable for high pressure and high field, we track the pressure evolution of the Seebeck coefficient $S$. At ambient pressure and low temperature, $S/T$ was recently found to suddenly increase in Nd-LSCO at the pseudogap critical doping $p^{\star} = 0.23$, consistent with a drop in carrier density $n$ from $n = 1 + p$ above $p^{\star}$ to $n = p$ below. Under a pressure of 2.0 GPa, we observe that this jump in $S/T$ is suppressed. This confirms a previous pressure study based on electrical resistivity and Hall effect which found $dp^{\star}/dP \simeq - 0.01$ holes/GPa, thereby reinforcing the interpretation that this effect is driven by the pressure-induced shift of the van Hove point. It implies that the pseudogap only exists when the Fermi surface is hole-like, which puts strong constraints on theories of the pseudogap phase. We also report thermopower measurements on Nd-LSCO and La$_{1.8-x}$Eu$_{0.2}$Sr$_x$CuO$_4$ in the charge density-wave phase near $p \sim 1/8$, which reveals a weakening of this phase under pressure.

Highlights

  • The pseudogap phase of cuprates is arguably one of their chief mysteries [1]

  • We report thermopower measurements under hydrostatic pressure on the cuprate superconductor La1.6−xNd0.4SrxCuO4 (Nd-LSCO), at low temperature in the normal state accessed by suppressing superconductivity with a magnetic field up to H = 31 T

  • We report thermopower measurements on Nd-LSCO and La1.8−xEu0.2SrxCuO4 in the charge density wave phase near p ∼ 1/8, which reveals a weakening of this phase under pressure

Read more

Summary

Introduction

The pseudogap phase of cuprates is arguably one of their chief mysteries [1]. Understanding the pseudogap phase of cuprates has been hindered in part by the fact that it does not exhibit a clear and well-defined symmetrybreaking phase transition at its characteristic temperature T. Upon crossing the pseudogap end point at doping p (where T vanishes) at low temperatures, recent measurements have revealed a clear and abrupt change in carrier density n, going from n = 1 + p above p to n = p below p [2]. P , the resistivity of Nd-LSCO [10] and LSCO [11] exhibits a purely linear temperature dependence at low T with a slope that reaches the Planckian limit [12], another signature of quantum criticality

Objectives
Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call