Author
Listed:
- KeYuan Ma
(Max Planck Institute for Chemical Physics of Solids)
- Igor Plokhikh
(PSI Center for Neutron and Muon Sciences CNM)
- Jennifer N. Graham
(PSI Center for Neutron and Muon Sciences CNM)
- Charles Mielke III
(PSI Center for Neutron and Muon Sciences CNM
Max Planck Institute for the Structure and Dynamics of Materials)
- Vahid Sazgari
(PSI Center for Neutron and Muon Sciences CNM)
- Hiroto Nakamura
(University of Tokyo, Kashiwa)
- Shams Sohel Islam
(PSI Center for Neutron and Muon Sciences CNM)
- Soohyeon Shin
(PSI Center for Neutron and Muon Sciences CNM)
- Petr Král
(PSI Center for Neutron and Muon Sciences CNM)
- Orion Gerguri
(PSI Center for Neutron and Muon Sciences CNM)
- Hubertus Luetkens
(PSI Center for Neutron and Muon Sciences CNM)
- Fabian O. Rohr
(University of Geneva)
- Jiaxin Yin
(Southern University of Science and Technology, Shenzhen)
- Ekaterina Pomjakushina
(PSI Center for Neutron and Muon Sciences CNM)
- Claudia Felser
(Max Planck Institute for Chemical Physics of Solids)
- Satoru Nakatsuji
(University of Tokyo)
- Björn Wehinger
(European Synchrotron Radiation Facility)
- Dariusz J. Gawryluk
(PSI Center for Neutron and Muon Sciences CNM)
- Sergey Medvedev
(Max Planck Institute for Chemical Physics of Solids)
- Zurab Guguchia
(PSI Center for Neutron and Muon Sciences CNM)
Abstract
The interplay between superconductivity and charge or spin order is a key focus in condensed matter physics, with kagome lattice systems providing unique insights. The kagome superconductor LaRu3Si2 (Tc ≃ 6.5 K) features a characteristic kagome band structure and a hierarchy of charge order transitions at Tco,I ≃ 400 K and Tco,II ≃ 80 K, along with an additional transition at T* ≃ 35 K associated with electronic and magnetic responses. Using magnetotransport under pressure up to 40 GPa, we find Tc peaks at 9 K (2 GPa)—the highest among kagome superconductors—remains nearly constant up to 12 GPa, and then decreases to 2 K at 40 GPa, forming a dome-shaped phase diagram. Similarly, both the resistivity anomaly at T* and the magnetoresistance exhibit a dome-shaped pressure dependence. Moreover, above 12 GPa, X-ray diffraction reveals that the charge order evolves from long-range to short-range, coinciding with the suppression of Tc. These observations indicate that superconductivity in LaRu3Si2 is closely linked to the charge-ordered state and the electronic responses at Tco,II and T*.
Suggested Citation
KeYuan Ma & Igor Plokhikh & Jennifer N. Graham & Charles Mielke III & Vahid Sazgari & Hiroto Nakamura & Shams Sohel Islam & Soohyeon Shin & Petr Král & Orion Gerguri & Hubertus Luetkens & Fabian O. Ro, 2025.
"Correlation between the dome-shaped superconducting phase diagram, charge order, and normal-state electronic properties in LaRu3Si2,"
Nature Communications, Nature, vol. 16(1), pages 1-9, December.
Handle:
RePEc:nat:natcom:v:16:y:2025:i:1:d:10.1038_s41467-025-61383-z
DOI: 10.1038/s41467-025-61383-z
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