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Spin dynamics in the pseudogap state of a high-temperature superconductor

Authors :
Chengtian Lin
Stéphane Pailhès
Vladimir Hinkov
Christopher D. Frost
D. P. Chen
Bernhard Keimer
Philippe Bourges
Alexandre Ivanov
Yvan Sidis
Toby Perring
LLB - Nouvelles frontières dans les matériaux quantiques (NFMQ)
Laboratoire Léon Brillouin (LLB - UMR 12)
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Centre National de la Recherche Scientifique (CNRS)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Centre National de la Recherche Scientifique (CNRS)-Université Paris-Saclay
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)
Source :
Nature Physics, Nature Physics, Nature Publishing Group, 2007, 3 (11), pp.780-785. ⟨10.1038/nphys720⟩, Nature Physics, 2007, 3 (11), pp.780-785. ⟨10.1038/nphys720⟩
Publication Year :
2008
Publisher :
arXiv, 2008.

Abstract

The pseudogap is one of the most pervasive phenomena of high temperature superconductors. It is attributed either to incoherent Cooper pairing setting in above the superconducting transition temperature Tc, or to a hidden order parameter competing with superconductivity. Here we use inelastic neutron scattering from underdoped YBa(2)Cu(3)O(6.6) to show that the dispersion relations of spin excitations in the superconducting and pseudogap states are qualitatively different. Specifically, the extensively studied "hour glass" shape of the magnetic dispersions in the superconducting state is no longer discernible in the pseudogap state and we observe an unusual "vertical" dispersion with pronounced in-plane anisotropy. The differences between superconducting and pseudogap states are thus more profound than generally believed, suggesting a competition between these two states. Whereas the high-energy excitations are common to both states and obey the symmetry of the copper oxide square lattice, the low-energy excitations in the pseudogap state may be indicative of collective fluctuations towards a state with broken orientational symmetry predicted in theoretical work.<br />Comment: 6 pages, 8 figures, contains supplementary information. Some data from V. Hinkov et al., arXiv:cond-mat/0601048, is included

Details

ISSN :
17452473 and 14764636
Database :
OpenAIRE
Journal :
Nature Physics, Nature Physics, Nature Publishing Group, 2007, 3 (11), pp.780-785. ⟨10.1038/nphys720⟩, Nature Physics, 2007, 3 (11), pp.780-785. ⟨10.1038/nphys720⟩
Accession number :
edsair.doi.dedup.....f56b54b7afa00329e8a0def30ea0155b
Full Text :
https://doi.org/10.48550/arxiv.0806.4134