1. Quantum critical behavior of the hyperkagome magnet Mn_{3}CoSi
- Author
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Hiroki Yamauchi, Dita Puspita Sari, Yukio Yasui, Terutoshi Sakakura, Hiroyuki Kimura, Akiko Nakao, Takashi Ohhara, Takashi Honda, Katsuaki Kodama, Naoki Igawa, Kazutaka Ikeda, Kazuki Iida, Daichi Ueta, Tetsuya Yokoo, Matthias D. Frontzek, Songxue Chi, Jaime A. Fernandez-Baca, Kenji M. Kojima, Donald Arseneau, Gerald Morris, Bassam Hitti, Yipeng Cai, Adam Berlie, Isao Watanabe, Pai-Tse Hsu, Yu-Sheng Chen, Min Kai Lee, Amelia Elisabeth Hall, Geetha Balakrishnan, Lieh-Jeng Chang, and Shin-ichi Shamoto
- Subjects
Physics ,QC1-999 - Abstract
β-Mn-type family alloys Mn_{3}TX (T=Co, Rh, and Ir; X=Si and Ge) have a three-dimensional antiferromagnetic (AF) corner-shared triangular network, i.e., the hyperkagome lattice. The antiferromagnet Mn_{3}RhSi shows magnetic short-range order over a wide temperature range of approximately 500 K above the Néel temperature T_{N} of 190 K. In this family of compounds, as the lattice parameter decreases, the long-range magnetic ordering temperature decreases. Mn_{3}CoSi has the smallest lattice parameter and the lowest T_{N} in the family. The quantum critical point (QCP) from AF to the quantum paramagnetic state is expected near a cubic lattice parameter of 6.15 Å. Although the Néel temperature of Mn_{3}CoSi is only 140 K, the emergence of the quantum critical behavior in Mn_{3}CoSi is discussed. We study how the magnetic short-range order appears in Mn_{3}CoSi by using neutron scattering, μSR, and bulk characterization such as specific heat capacity. According to the results, the neutron scattering intensity of the magnetic short-range order in Mn_{3}CoSi does not change much at low temperatures from that of Mn_{3}RhSi, although the μSR short-range order temperature of Mn_{3}CoSi is largely suppressed to 240 K from that of Mn_{3}RhSi. Correspondingly, the volume fraction of the magnetic short-range order regions, as shown by the initial asymmetry drop ratio of μSR above T_{N}, also becomes small. Instead, the electronic-specific heat coefficient γ of Mn_{3}CoSi is the largest in this Mn_{3}TSi system, possibly due to the low-energy spin fluctuation near the quantum critical point.
- Published
- 2024
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