Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7

© 2015 American Physical Society. ©2015 American Physical Society. au. Magnetic properties of the S=12 antiferromagnet α-Cu2V2O7 have been studied using magnetization, quantum Monte Carlo (QMC) simulations, and neutron diffraction. Magnetic susceptibility shows a broad peak at ∼50K followed by an ab...

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Main Authors: G. Gitgeatpong, Y. Zhao, M. Avdeev, R. O. Piltz, T. J. Sato, K. Matan
Other Authors: Mahidol University
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Published: 2018
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Online Access:https://repository.li.mahidol.ac.th/handle/123456789/36188
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spelling th-mahidol.361882018-11-23T17:23:06Z Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7 G. Gitgeatpong Y. Zhao M. Avdeev R. O. Piltz T. J. Sato K. Matan Mahidol University ThEP University of Maryland NIST Center for Neutron Research Australian Nuclear Science and Technology Organisation Tohoku University Materials Science © 2015 American Physical Society. ©2015 American Physical Society. au. Magnetic properties of the S=12 antiferromagnet α-Cu2V2O7 have been studied using magnetization, quantum Monte Carlo (QMC) simulations, and neutron diffraction. Magnetic susceptibility shows a broad peak at ∼50K followed by an abrupt increase indicative of a phase transition to a magnetically ordered state at TN=33.4(1) K. Above TN, a fit to the Curie-Weiss law gives a Curie-Weiss temperature of Θ=-73(1) K suggesting the dominant antiferromagnetic coupling. The result of the QMC calculations on the helical-honeycomb spin network with two antiferromagnetic exchange interactions J1 and J2 provides a better fit to the susceptibility than the previously proposed spin-chain model. Two sets of the coupling parameters J1:J2=1:0.45 with J1=5.79(1) meV and 0.65:1 with J2=6.31(1) meV yield equally good fits down to ∼TN. Below TN, weak ferromagnetism due to spin canting is observed. The canting is caused by the Dzyaloshinskii-Moriya interaction with an estimated bc-plane component Dp≃0.14J1. Neutron diffraction reveals that the S=12Cu2+ spins antiferromagnetically align in the Fd′d′2 magnetic space group. The ordered moment of 0.93(9) μB is predominantly along the crystallographic a axis. 2018-11-23T10:23:06Z 2018-11-23T10:23:06Z 2015-07-23 Article Physical Review B - Condensed Matter and Materials Physics. Vol.92, No.2 (2015) 10.1103/PhysRevB.92.024423 1550235X 10980121 2-s2.0-84938936919 https://repository.li.mahidol.ac.th/handle/123456789/36188 Mahidol University SCOPUS https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84938936919&origin=inward
institution Mahidol University
building Mahidol University Library
continent Asia
country Thailand
Thailand
content_provider Mahidol University Library
collection Mahidol University Institutional Repository
topic Materials Science
spellingShingle Materials Science
G. Gitgeatpong
Y. Zhao
M. Avdeev
R. O. Piltz
T. J. Sato
K. Matan
Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
description © 2015 American Physical Society. ©2015 American Physical Society. au. Magnetic properties of the S=12 antiferromagnet α-Cu2V2O7 have been studied using magnetization, quantum Monte Carlo (QMC) simulations, and neutron diffraction. Magnetic susceptibility shows a broad peak at ∼50K followed by an abrupt increase indicative of a phase transition to a magnetically ordered state at TN=33.4(1) K. Above TN, a fit to the Curie-Weiss law gives a Curie-Weiss temperature of Θ=-73(1) K suggesting the dominant antiferromagnetic coupling. The result of the QMC calculations on the helical-honeycomb spin network with two antiferromagnetic exchange interactions J1 and J2 provides a better fit to the susceptibility than the previously proposed spin-chain model. Two sets of the coupling parameters J1:J2=1:0.45 with J1=5.79(1) meV and 0.65:1 with J2=6.31(1) meV yield equally good fits down to ∼TN. Below TN, weak ferromagnetism due to spin canting is observed. The canting is caused by the Dzyaloshinskii-Moriya interaction with an estimated bc-plane component Dp≃0.14J1. Neutron diffraction reveals that the S=12Cu2+ spins antiferromagnetically align in the Fd′d′2 magnetic space group. The ordered moment of 0.93(9) μB is predominantly along the crystallographic a axis.
author2 Mahidol University
author_facet Mahidol University
G. Gitgeatpong
Y. Zhao
M. Avdeev
R. O. Piltz
T. J. Sato
K. Matan
format Article
author G. Gitgeatpong
Y. Zhao
M. Avdeev
R. O. Piltz
T. J. Sato
K. Matan
author_sort G. Gitgeatpong
title Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
title_short Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
title_full Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
title_fullStr Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
title_full_unstemmed Magnetic structure and Dzyaloshinskii-Moriya interaction in the S= 12 helical-honeycomb antiferromagnet α-Cu2 V2 O7
title_sort magnetic structure and dzyaloshinskii-moriya interaction in the s= 12 helical-honeycomb antiferromagnet α-cu2 v2 o7
publishDate 2018
url https://repository.li.mahidol.ac.th/handle/123456789/36188
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