Designing the stripe-ordered cuprate phase diagram through uniaxial-stress.

cuprate high-temperature superconductor muon-spin rotation stripe order superconductivity uniaxial stress

Journal

Proceedings of the National Academy of Sciences of the United States of America
ISSN: 1091-6490
Titre abrégé: Proc Natl Acad Sci U S A
Pays: United States
ID NLM: 7505876

Informations de publication

Date de publication:
02 Jan 2024
Historique:
medline: 27 12 2023
pubmed: 27 12 2023
entrez: 27 12 2023
Statut: ppublish

Résumé

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.

Identifiants

pubmed: 38150501
doi: 10.1073/pnas.2303423120
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

e2303423120

Déclaration de conflit d'intérêts

Competing interests statement:The authors declare no competing interest.

Auteurs

Z Guguchia (Z)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

D Das (D)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

G Simutis (G)

Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen, Switzerland.

T Adachi (T)

Department of Engineering and Applied Sciences, Sophia University, Tokyo 102-8554, Japan.

J Küspert (J)

Physik-Institut, Universität Zürich, CH-8057 Zürich, Switzerland.

N Kitajima (N)

Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan.

M Elender (M)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

V Grinenko (V)

Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Pudong, 201210 Shanghai, China.

O Ivashko (O)

Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany.

M V Zimmermann (MV)

Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany.

M Müller (M)

Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

C Mielke (C)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

F Hotz (F)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

C Mudry (C)

Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
Institut de Physique, École Polytechnique Fédérale de Lausanne, Lausanne CH-1015, Switzerland.

C Baines (C)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

M Bartkowiak (M)

Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen, Switzerland.

T Shiroka (T)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
Laboratorium für Festkörperphysik, ETH Zürich, CH-8093 Zürich, Switzerland.

Y Koike (Y)

Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan.

A Amato (A)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

C W Hicks (CW)

Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany.
School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, United Kingdom.

G D Gu (GD)

Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Upton, NY 11973.

J M Tranquada (JM)

Condensed Matter Physics and Materials Science Division, Brookhaven National Laboratory, Upton, NY 11973.

H-H Klauss (HH)

Institute for Solid State and Materials Physics, Technische Universitat Dresden, D-01069 Dresden, Germany.

J J Chang (JJ)

Physik-Institut, Universität Zürich, CH-8057 Zürich, Switzerland.

M Janoschek (M)

Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen, Switzerland.
Physik-Institut, Universität Zürich, CH-8057 Zürich, Switzerland.

H Luetkens (H)

Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.

Classifications MeSH