Volume 80, Issue 5 pp. 393-400
research papers

Magnetic structure of the noncentrosymmetric magnet Sr2MnSi2O7 through irreducible representation and magnetic space group analyses

Y. Nambu

Corresponding Author

Y. Nambu

Tohoku University, Institute for Materials Research, Sendai, 980-8577 Japan

Tohoku University, Organization for Advanced Studies, Sendai, 980-8577 Japan

Japan Science and Technology Agency, FOREST, Saitama, 332-0012 Japan

Y. Nambu, e-mail: [email protected]Search for more papers by this author
M. Kawamata

M. Kawamata

Tohoku University, Department of Physics, Sendai, 980-8578 Japan

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X. Pang

X. Pang

Tohoku University, Department of Physics, Sendai, 980-8578 Japan

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H. Murakawa

H. Murakawa

Osaka University, Department of Physics, Osaka, 560-0043 Japan

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M. Avdeev

M. Avdeev

Australian Nuclear Science and Technology Organisation, Kirrawee DC, NSW 2232 Australia

University of Sydney, School of Chemistry, Sydney, 2006 Australia

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H. Kimura

H. Kimura

Tohoku University, Institute of Multidisciplinary Research for Advanced Materials, Sendai, 980-8577 Japan

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H. Masuda

H. Masuda

Tohoku University, Institute for Materials Research, Sendai, 980-8577 Japan

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N. Hanasaki

N. Hanasaki

Osaka University, Department of Physics, Osaka, 560-0043 Japan

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Y. Onose

Y. Onose

Tohoku University, Institute for Materials Research, Sendai, 980-8577 Japan

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First published: 25 September 2024

Abstract

Magnetic structures of the noncentrosymmetric magnet Sr2MnSi2O7 were examined through neutron diffraction for powder and single-crystalline samples, as well as magnetometry measurements. All allowed magnetic structures for space group P421m with the magnetic wavevector qm = (0, 0, ½) were refined via irreducible representation and magnetic space group analyses. The compound was refined to have in-plane magnetic moments within the magnetic space group Cmc21.1′c (No. 36.177) under zero field, which can be altered to P212121.1′c (No. 19.28) above μ0H = 0.067 (5) T to align induced weak-ferromagnetic components within one layer on the ab plane. All refined parameters are provided following the recent framework based upon the magnetic space group, which better conveys when exchanging crystallographic information for commensurate magnetic structures.

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