Magnetic excitation in the hyperkagome antiferromagnet <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Mn</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:mi>RhSi</mml:mi></mml:mrow></mml:math>

In a paramagnetic state of a hyperkagome lattice antiferromagnet <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:msub><a:mi>Mn</a:mi><a:mn>3</a:mn></a:msub><a:mi>RhSi</a:mi></a:mrow></a:math>, magnetic diffuse scattering by magnetic short-range order is observed over a wide temperature range of approximately 500 K above the Néel temperature of 190 K. We have studied the magnetic excitation with a single crystal in a wide energy range from 0.3 to 140 meV by inelastic neutron scattering, where the prominent inelastic neutron-scattering signal is observed at <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mrow><b:mi mathvariant="bold">Q</b:mi><b:mo>=</b:mo><b:mo>(</b:mo><b:mn>2</b:mn><b:mo>,</b:mo><b:mn>0</b:mn><b:mo>,</b:mo><b:mn>0</b:mn><b:mo>)</b:mo></b:mrow></b:math>. The inelastic scattering intensity integrated for two of twelve magnon modes leads to a localized magnetic moment of about 5 <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:msub><d:mi>μ</d:mi><d:mi mathvariant="normal">B</d:mi></d:msub></d:math> per Mn site, although the long-range ordered magnetic moment is only 2.61 <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>μ</f:mi><f:mi mathvariant="normal">B</f:mi></f:msub></f:math> at 4 K. The result suggests that a large part of the magnetic moment does not order in <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msub><h:mi>Mn</h:mi><h:mn>3</h:mn></h:msub><h:mi>RhSi</h:mi></h:mrow></h:math>, possibly due to the geometrical spin frustration of the hyperkagome lattice. Published by the American Physical Society 2024

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Journal
Physical Review Research
Published
2024-09-16
DOI
https://doi.org/10.1103/physrevresearch.6.033303
Primary Topic
Advanced Condensed Matter Physics
Type
article
Field-Weighted Citation Impact
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Magnetic excitation in the hyperkagome antiferromagnet <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Mn</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:mi>RhSi</mml:mi></mml:mrow></mml:math>

G. Balakrishnan, Shin‐ichi Shamoto, A. E. Hall, Yu‐Sheng Chen et al.
Physical Review Research
Advanced Condensed Matter Physics
article

Magnetic excitation in the hyperkagome antiferromagnet <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Mn</mml:mi><mml:mn>3</mml:mn></mml:msub><mml:mi>RhSi</mml:mi></mml:mrow></mml:math>

G. Balakrishnan, Shin‐ichi Shamoto, A. E. Hall, Yu‐Sheng Chen, Min Kai Lee, Koji Kaneko, Kazuki Iida, Hiroki Yamauchi, L. J. Chang, Kazuhiko Ikeuchi, Shin-ichiro Yano, Pai-Tse Hsu
article en

Abstract

In a paramagnetic state of a hyperkagome lattice antiferromagnet <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:msub><a:mi>Mn</a:mi><a:mn>3</a:mn></a:msub><a:mi>RhSi</a:mi></a:mrow></a:math>, magnetic diffuse scattering by magnetic short-range order is observed over a wide temperature range of approximately 500 K above the Néel temperature of 190 K. We have studied the magnetic excitation with a single crystal in a wide energy range from 0.3 to 140 meV by inelastic neutron scattering, where the prominent inelastic neutron-scattering signal is observed at <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mrow><b:mi mathvariant="bold">Q</b:mi><b:mo>=</b:mo><b:mo>(</b:mo><b:mn>2</b:mn><b:mo>,</b:mo><b:mn>0</b:mn><b:mo>,</b:mo><b:mn>0</b:mn><b:mo>)</b:mo></b:mrow></b:math>. The inelastic scattering intensity integrated for two of twelve magnon modes leads to a localized magnetic moment of about 5 <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:msub><d:mi>μ</d:mi><d:mi mathvariant="normal">B</d:mi></d:msub></d:math> per Mn site, although the long-range ordered magnetic moment is only 2.61 <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>μ</f:mi><f:mi mathvariant="normal">B</f:mi></f:msub></f:math> at 4 K. The result suggests that a large part of the magnetic moment does not order in <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msub><h:mi>Mn</h:mi><h:mn>3</h:mn></h:msub><h:mi>RhSi</h:mi></h:mrow></h:math>, possibly due to the geometrical spin frustration of the hyperkagome lattice. Published by the American Physical Society 2024

Physical Review ResearchVol. 6(3)
Japan Atomic Energy Agency (JP), High Energy Accelerator Research Organization (JP), University of Warwick (GB), National Synchrotron Radiation Research Center (TW), Comprehensive Research Organization for Science and Society (JP), Advanced Science Research Center (JP), Institute of Materials Structure Science (JP), Academia Sinica (TW), National Cheng Kung University (TW)
Japan Proton Accelerator Research Complex, University of Warwick, Engineering and Physical Sciences Research Council, Japan Society for the Promotion of Science
Affordable and clean energy
Openalex Percentile: Top 91%
Advanced Condensed Matter Physics
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