Coexisting Multiple Charge Orders and Magnetism in the Kagome Superconductor LaRu <sub>3</sub> Si <sub>2</sub>
Abstract
Abstract The Kagome lattice has emerged as a promising platform for hosting unconventional chiral charge orders at high temperatures. In the context of the correlated Kagome superconductor LaRu 3 Si 2 , a room‐temperature charge‐ordered state with a propagation vector of (, 0, 0) is previously reported. However, understanding the interplay between this charge order and superconductivity, particularly with respect to time‐reversal‐symmetry breaking, remains elusive. In this study, we employ single‐crystal X‐ray diffraction, magnetotransport measurements, muon‐spin rotation experiments, and first‐principles calculations to investigate charge order and its electronic and magnetic responses in LaRu 3 Si 2 across a wide temperature range, down to the superconducting state. These findings reveal the appearance of a charge order with a propagation vector of (, 0, 0) below T co, 2 ≃ 80 K, which coexists with the previously identified room temperature primary charge order (, 0, 0). The primary charge‐ordered state exhibits zero magnetoresistance. In contrast, the appearance of the secondary charge order at T co, 2 is accompanied by a notable magnetoresistance response and a pronounced temperature‐dependent Hall effect, which experiences a sign reversal, switching from positive to negative below T * ≃ 35 K. Intriguingly, a significant enhancement is observed in the internal field width sensed by the muon ensemble below T * ≃ 35 K. Moreover, the muon spin relaxation rate exhibits a substantial increase upon the application of an external magnetic field below T co, 2 ≃ 80 K. These results highlight the coexistence of two distinct types of charge order and magnetism in LaRu 3 Si 2 within the correlated Kagome lattice, along with superconductivity. This study sheds light on the intricate electronic and magnetic phenomena occurring in Kagome superconductors, providing valuable insights into their unique properties and potential applications.
Article Details
Authors (27)
C. Mielke
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
V. Sazgari
I. Plokhikh
Mingsheng Yi
Wuhan National High Magnetic Field Center and School of Physics Huazhong University of Science and Technology Wuhan 430074 China
S. Shin
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
H. Nakamura
Institute for Solid State Physics (ISSP) University of Tokyo Chiba Japan
J.N. Graham
PSI Center for Neutron and Muon Sciences CNM Paul Scherrer Institut Switzerland
J. Küspert
Physik‐Institut Universität Zürich Winterthurerstrasse 190 Zürich CH‐8057 Switzerland
I. Biało
G. Garbarino
European Synchrotron Radiation Facility 71 Avenue des Martyrs Grenoble 38000 France
D. Das
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
M. Medarde
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
M. Bartkowiak
J.‐X. Yin
Department of Physics Southern University of Science and Technology Shenzhen Guangdong 518055 China
S.S. Islam
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
R. Khasanov
H. Luetkens
M.Z. Hasan
Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7) Department of Physics Princeton University Princeton New Jersey 08544 USA
E. Pomjakushina
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
M. H. Fischer
Physik‐Institut Universität Zürich Winterthurerstrasse 190 Zürich CH‐8057 Switzerland
J. Chang
School of Physical Science and Technology, Northwestern Polytechnical University , Xi’an 710072,
T. Neupert
Physik‐Institut Universität Zürich Winterthurerstrasse 190 Zürich CH‐8057 Switzerland
S. Nakatsuji
Institute for Solid State Physics (ISSP) University of Tokyo Chiba Japan
B. Wehinger
European Synchrotron Radiation Facility 9 , 71, avenue des Martyrs, CS 40220, 38043 Grenoble Cedex 9,
Gang Xu
D.J. Gawryluk
PSI Center for Neutron and Muon Sciences CNM Villigen PSI 5232 Switzerland
Z. Guguchia