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Ideal charge-density-wave order in the high-field state of superconducting YBCO.
Jang, H; Lee, W-S; Nojiri, H; Matsuzawa, S; Yasumura, H; Nie, L; Maharaj, A V; Gerber, S; Liu, Y-J; Mehta, A; Bonn, D A; Liang, R; Hardy, W N; Burns, C A; Islam, Z; Song, S; Hastings, J; Devereaux, T P; Shen, Z-X; Kivelson, S A; Kao, C-C; Zhu, D; Lee, J-S.
Afiliação
  • Jang H; Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Lee WS; Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory and Stanford University, Menlo Park, CA 94025.
  • Nojiri H; Institute for Materials Research, Tohoku University, Katahira 2-1-1, Sendai 980-8577, Japan.
  • Matsuzawa S; Institute for Materials Research, Tohoku University, Katahira 2-1-1, Sendai 980-8577, Japan.
  • Yasumura H; Institute for Materials Research, Tohoku University, Katahira 2-1-1, Sendai 980-8577, Japan.
  • Nie L; Geballe Laboratory for Advanced Materials, Departments of Physics and Applied Physics, Stanford University, Stanford, CA 94305.
  • Maharaj AV; Geballe Laboratory for Advanced Materials, Departments of Physics and Applied Physics, Stanford University, Stanford, CA 94305.
  • Gerber S; SwissFEL, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Liu YJ; Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Mehta A; Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Bonn DA; Department of Physics & Astronomy, University of British Columbia, Vancouver, BC, Canada V6T 1Z1.
  • Liang R; Canadian Institute for Advanced Research, Toronto, ON, Canada M5G 1Z8.
  • Hardy WN; Department of Physics & Astronomy, University of British Columbia, Vancouver, BC, Canada V6T 1Z1.
  • Burns CA; Canadian Institute for Advanced Research, Toronto, ON, Canada M5G 1Z8.
  • Islam Z; Department of Physics & Astronomy, University of British Columbia, Vancouver, BC, Canada V6T 1Z1.
  • Song S; Canadian Institute for Advanced Research, Toronto, ON, Canada M5G 1Z8.
  • Hastings J; Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Devereaux TP; Department of Physics, Western Michigan University, Kalamazoo, MI 49008.
  • Shen ZX; The Advanced Photon Source, Argonne National Laboratory, Argonne, IL 60439.
  • Kivelson SA; Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Kao CC; Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025.
  • Zhu D; Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory and Stanford University, Menlo Park, CA 94025.
  • Lee JS; Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory and Stanford University, Menlo Park, CA 94025.
Proc Natl Acad Sci U S A ; 113(51): 14645-14650, 2016 12 20.
Article em En | MEDLINE | ID: mdl-27930313
ABSTRACT
The existence of charge-density-wave (CDW) correlations in cuprate superconductors has now been established. However, the nature of the CDW ground state has remained uncertain because disorder and the presence of superconductivity typically limit the CDW correlation lengths to only a dozen unit cells or less. Here we explore the field-induced 3D CDW correlations in extremely pure detwinned crystals of YBa2Cu3O2 (YBCO) ortho-II and ortho-VIII at magnetic fields in excess of the resistive upper critical field ([Formula see text]) where superconductivity is heavily suppressed. We observe that the 3D CDW is unidirectional and possesses a long in-plane correlation length as well as significant correlations between neighboring CuO2 planes. It is significant that we observe only a single sharply defined transition at a critical field proportional to [Formula see text], given that the field range used in this investigation overlaps with other high-field experiments including quantum oscillation measurements. The correlation volume is at least two to three orders of magnitude larger than that of the zero-field CDW. This is by far the largest CDW correlation volume observed in any cuprate crystal and so is presumably representative of the high-field ground state of an "ideal" disorder-free cuprate.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article