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  4. Nernst effect in the cuprate superconductor YBa_{2}Cu_{3}O_{y}: Broken rotational and translational symmetries
 
research article

Nernst effect in the cuprate superconductor YBa_{2}Cu_{3}O_{y}: Broken rotational and translational symmetries

Chang, Johan Juul  
•
Doiron-Leyraud, Nicolas
•
Laliberté, Francis
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2011
Physical Review B

The Nernst coefficient of the cuprate superconductor YBa2Cu 3Oy was recently shown to become strongly anisotropic within the basal plane when cooled below the pseudogap temperature T, revealing that the pseudogap phase breaks the fourfold rotational symmetry of the CuO 2 planes. Here we report on the evolution of this Nernst anisotropy at low temperature, once superconductivity is suppressed by a magnetic field. We find that the anisotropy drops rapidly below 80 K, to vanish in the T=0 limit. We show that this loss of anisotropy is due to the emergence of a small high-mobility electronlike pocket in the Fermi surface at low temperature, a reconstruction attributed to a low-temperature state that breaks the translational symmetry of the CuO2 planes. We discuss the sequence of broken symmetries-first rotational, then translational-in terms of an electronic nematic-to-smectic transition such as could arise when unidirectional spin or charge modulations order. We compare YBa2Cu 3Oy with iron-pnictide superconductors where the process of (unidirectional) antiferromagnetic ordering gives rises to the same sequence of broken symmetries. © 2011 American Physical Society.

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Type
research article
DOI
10.1103/PhysRevB.84.014507
Author(s)
Chang, Johan Juul  
•
Doiron-Leyraud, Nicolas
•
Laliberté, Francis
•
Daou, R.
•
Leboeuf, David
•
Ramshaw, B.
•
Liang, Ruixing
•
Bonn, D.
•
Hardy, W.
•
Proust, Cyril
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Date Issued

2011

Published in
Physical Review B
Volume

84

Issue

1

Article Number

014507

Editorial or Peer reviewed

NON-REVIEWED

Written at

EPFL

EPFL units
ICMP  
Available on Infoscience
November 8, 2012
Use this identifier to reference this record
https://infoscience.epfl.ch/handle/20.500.14299/86747
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