Magnetic structures and quadratic magnetoelectric effect in LiNiPO\(_4\) beyond 30T

Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO\(_4\) up to 25T and 42T, respectively. By combining these results with magnetometry and electric polarization measurements under pulsed fields, the magnetic and magnetoelectric phas...

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Published inarXiv.org
Main Authors Fogh, Ellen, Kihara, Takumi, Toft-Petersen, Rasmus, Bartkowiak, Maciej, Narumi, Yasuo, Prokhnenko, Oleksandr, Miyake, Atsushi, Tokunaga, Masashi, Oikawa, Kenichi, Sørensen, Michael Korning, Dyrnum, Julia Cathrine, Grimmer, Hans, Nojiri, Hiroyuki, Niels Bech Christensen
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Published Ithaca Cornell University Library, arXiv.org 03.10.2019
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Abstract Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO\(_4\) up to 25T and 42T, respectively. By combining these results with magnetometry and electric polarization measurements under pulsed fields, the magnetic and magnetoelectric phases are investigated up to 56T applied along the easy \(c\)-axis. In addition to the already known transitions at lower fields, three new ones are reported at 37.6, 39.4 and 54T. Ordering vectors are identified with \({\bf Q}_{\mathrm{VI}}\) = (0, 1/3, 0) in the interval 37.6--39.4T and \({\bf Q}_{\mathrm{VII}}\) = (0, 0, 0) in the interval 39.4-54T. A quadratic magnetoelectric effect is discovered in the \({\bf Q}_{\mathrm{VII}}\) = (0, 0, 0) phase and the field-dependence of the induced electric polarization is described using a simple mean-field model. The observed magnetic structure and magnetoelectric tensor elements point to a change in the lattice symmetry in this phase. We speculate on the possible physical mechanism responsible for the magnetoelectric effect in LiNiPO4.
AbstractList Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO\(_4\) up to 25T and 42T, respectively. By combining these results with magnetometry and electric polarization measurements under pulsed fields, the magnetic and magnetoelectric phases are investigated up to 56T applied along the easy \(c\)-axis. In addition to the already known transitions at lower fields, three new ones are reported at 37.6, 39.4 and 54T. Ordering vectors are identified with \({\bf Q}_{\mathrm{VI}}\) = (0, 1/3, 0) in the interval 37.6--39.4T and \({\bf Q}_{\mathrm{VII}}\) = (0, 0, 0) in the interval 39.4-54T. A quadratic magnetoelectric effect is discovered in the \({\bf Q}_{\mathrm{VII}}\) = (0, 0, 0) phase and the field-dependence of the induced electric polarization is described using a simple mean-field model. The observed magnetic structure and magnetoelectric tensor elements point to a change in the lattice symmetry in this phase. We speculate on the possible physical mechanism responsible for the magnetoelectric effect in LiNiPO4.
Author Fogh, Ellen
Grimmer, Hans
Kihara, Takumi
Bartkowiak, Maciej
Dyrnum, Julia Cathrine
Miyake, Atsushi
Niels Bech Christensen
Prokhnenko, Oleksandr
Toft-Petersen, Rasmus
Oikawa, Kenichi
Narumi, Yasuo
Nojiri, Hiroyuki
Sørensen, Michael Korning
Tokunaga, Masashi
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Snippet Neutron diffraction with static and pulsed magnetic fields is used to directly probe the magnetic structures in LiNiPO\(_4\) up to 25T and 42T, respectively....
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SubjectTerms Dependence
Electric polarization
Magnetic measurement
Magnetic structure
Neutron diffraction
Tensors
Title Magnetic structures and quadratic magnetoelectric effect in LiNiPO\(_4\) beyond 30T
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