Structural Phase Separation and Enhanced Superconductivity in La <sub>1.875</sub> Ba <sub>0.125</sub> CuO <sub>4</sub> Under Uniaxial Strain

B Baizhi Gao (Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada) E Ehsan Nikbin (University of Toronto) G Graham Johnstone (Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada) Z Ze Shi (School of Physical Science and Technology, Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing, Inner Mongolia University , Hohhot 010021,) C Christopher Heath (Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada) N Narayan Appathurai B Beatriz Diaz Moreno (Canadian Light Source University of Saskatchewan Saskatoon Saskatchewan S7N 0X4 Canada) A Al Rahemtulla (Canadian Light Source University of Saskatchewan Saskatoon Saskatchewan S7N 0X4 Canada) G G. D. Gu J John M. Tranquada (Condensed Matter Physics and Materials Science Department Brookhaven National Laboratory New York 11973 USA) J Jane Y. Howe (University of Toronto) Y Young‐June Kim (Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada)

Abstract

Abstract Strain engineering has attracted significant attention in recent years due to its capability in tuning lattice and electronic structures of quantum materials. Using moderate uniaxial compressive strain, structural phase separation is induced in the low‐temperature phase of x = 1/8 (LBCO) single crystals. These structures are low temperature tetragonal (LTT), low temperature less orthorhombic (LTLO), and a plastically deformed nano‐domain structure (PDNS), comprised of few‐nanometer‐sized orthorhombic domains within an amorphous matrix. These three structures exhibit distinct superconducting behaviors. The volume fraction of the LTT structure is suppressed with increasing strain, while its superconducting transition temperature increases and broadens. The LTLO structure exhibits a sharp superconducting transition above 32 K, which increases up to ≈ 36 K at maximum strain. The PDNS phase exhibits a very broad superconducting transition and persists even after removing the strain. This study illustrates the sensitivity of superconductivity to the structure of the LBCO sample near its stripe instability.

Article Details

Volume / Issue Vol. 38, Issue 2
Published January 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (12)

B

Baizhi Gao

Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada

E

Ehsan Nikbin

University of Toronto

G

Graham Johnstone

Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada

Z

Ze Shi

School of Physical Science and Technology, Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing, Inner Mongolia University , Hohhot 010021,

C

Christopher Heath

Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada

N

Narayan Appathurai

B

Beatriz Diaz Moreno

Canadian Light Source University of Saskatchewan Saskatoon Saskatchewan S7N 0X4 Canada

A

Al Rahemtulla

Canadian Light Source University of Saskatchewan Saskatoon Saskatchewan S7N 0X4 Canada

G

G. D. Gu

J

John M. Tranquada

Condensed Matter Physics and Materials Science Department Brookhaven National Laboratory New York 11973 USA

J

Jane Y. Howe

University of Toronto

Y

Young‐June Kim

Department of Physics University of Toronto Toronto Ontario M5S 1A7 Canada