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Designing the stripe-ordered cuprate phase diagram through uniaxial-stress.
Guguchia, Z; Das, D; Simutis, G; Adachi, T; Küspert, J; Kitajima, N; Elender, M; Grinenko, V; Ivashko, O; Zimmermann, M V; Müller, M; Mielke, C; Hotz, F; Mudry, C; Baines, C; Bartkowiak, M; Shiroka, T; Koike, Y; Amato, A; Hicks, C W; Gu, G D; Tranquada, J M; Klauss, H-H; Chang, J J; Janoschek, M; Luetkens, H.
Afiliação
  • Guguchia Z; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Das D; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Simutis G; Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen, Switzerland.
  • Adachi T; Department of Engineering and Applied Sciences, Sophia University, Tokyo 102-8554, Japan.
  • Küspert J; Physik-Institut, Universität Zürich, CH-8057 Zürich, Switzerland.
  • Kitajima N; Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan.
  • Elender M; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Grinenko V; Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Pudong, 201210 Shanghai, China.
  • Ivashko O; Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany.
  • Zimmermann MV; Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany.
  • Müller M; Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Mielke C; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Hotz F; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Mudry C; Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Baines C; Institut de Physique, École Polytechnique Fédérale de Lausanne, Lausanne CH-1015, Switzerland.
  • Bartkowiak M; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Shiroka T; Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen, Switzerland.
  • Koike Y; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Amato A; Laboratorium für Festkörperphysik, ETH Zürich, CH-8093 Zürich, Switzerland.
  • Hicks CW; Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan.
  • Gu GD; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Tranquada JM; Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany.
  • Klauss HH; School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, United Kingdom.
  • Chang JJ; Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Upton, NY 11973.
  • Janoschek M; Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Upton, NY 11973.
  • Luetkens H; Institute for Solid State and Materials Physics, Technische Universitat Dresden, D-01069 Dresden, Germany.
Proc Natl Acad Sci U S A ; 121(1): e2303423120, 2024 Jan 02.
Article em En | MEDLINE | ID: mdl-38150501
ABSTRACT
The ability to efficiently control charge and spin in the cuprate high-temperature superconductors is crucial for fundamental research and underpins technological development. Here, we explore the tunability of magnetism, superconductivity, and crystal structure in the stripe phase of the cuprate La[Formula see text]Ba[Formula see text]CuO[Formula see text], with [Formula see text] = 0.115 and 0.135, by employing temperature-dependent (down to 400 mK) muon-spin rotation and AC susceptibility, as well as X-ray scattering experiments under compressive uniaxial stress in the CuO[Formula see text] plane. A sixfold increase of the three-dimensional (3D) superconducting critical temperature [Formula see text] and a full recovery of the 3D phase coherence is observed in both samples with the application of extremely low uniaxial stress of [Formula see text]0.1 GPa. This finding demonstrates the removal of the well-known 1/8-anomaly of cuprates by uniaxial stress. On the other hand, the spin-stripe order temperature as well as the magnetic fraction at 400 mK show only a modest decrease under stress. Moreover, the onset temperatures of 3D superconductivity and spin-stripe order are very similar in the large stress regime. However, strain produces an inhomogeneous suppression of the spin-stripe order at elevated temperatures. Namely, a substantial decrease of the magnetic volume fraction and a full suppression of the low-temperature tetragonal structure is found under stress, which is a necessary condition for the development of the 3D superconducting phase with optimal [Formula see text]. Our results evidence a remarkable cooperation between the long-range static spin-stripe order and the underlying crystalline order with the three-dimensional fully coherent superconductivity. Overall, these results suggest that the stripe- and the SC order may have a common physical mechanism.
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Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2024 Tipo de documento: Article