Non-collinear long-range magnetic ordering in HgCr2S4

The low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at T$_N\sim$22K with propagation vector \textbf{k}=(0,0,$\sim$0.18). On cooling below T$_N$, the propagation vector increases and saturates a...

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Main Authors: Chapon, L, Radaelli, P, Hor, Y, Telling, M, Mitchell, J
Format: Journal article
Published: 2006
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author Chapon, L
Radaelli, P
Hor, Y
Telling, M
Mitchell, J
author_facet Chapon, L
Radaelli, P
Hor, Y
Telling, M
Mitchell, J
author_sort Chapon, L
collection OXFORD
description The low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at T$_N\sim$22K with propagation vector \textbf{k}=(0,0,$\sim$0.18). On cooling below T$_N$, the propagation vector increases and saturates at the commensurate value \textbf{k}=(0,0,0.25). The magnetic structure below T$_N$ consists of ferromagnetic layers in the \textit{ab}-plane stacked in a spiral arrangement along the \textit{c}-axis. Symmetry analysis using corepresentations theory reveals a point group symmetry in the ordered magnetic phase of 422 (D$_4$), which is incompatible with macroscopic ferroelectricity. This finding indicates that the spontaneous electric polarization observed experimentally cannot be coupled to the magnetic order parameter.
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spelling oxford-uuid:bbd04dd1-438d-47ec-9ac4-0602ce787eb52022-03-27T05:19:45ZNon-collinear long-range magnetic ordering in HgCr2S4Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:bbd04dd1-438d-47ec-9ac4-0602ce787eb5Symplectic Elements at Oxford2006Chapon, LRadaelli, PHor, YTelling, MMitchell, JThe low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at T$_N\sim$22K with propagation vector \textbf{k}=(0,0,$\sim$0.18). On cooling below T$_N$, the propagation vector increases and saturates at the commensurate value \textbf{k}=(0,0,0.25). The magnetic structure below T$_N$ consists of ferromagnetic layers in the \textit{ab}-plane stacked in a spiral arrangement along the \textit{c}-axis. Symmetry analysis using corepresentations theory reveals a point group symmetry in the ordered magnetic phase of 422 (D$_4$), which is incompatible with macroscopic ferroelectricity. This finding indicates that the spontaneous electric polarization observed experimentally cannot be coupled to the magnetic order parameter.
spellingShingle Chapon, L
Radaelli, P
Hor, Y
Telling, M
Mitchell, J
Non-collinear long-range magnetic ordering in HgCr2S4
title Non-collinear long-range magnetic ordering in HgCr2S4
title_full Non-collinear long-range magnetic ordering in HgCr2S4
title_fullStr Non-collinear long-range magnetic ordering in HgCr2S4
title_full_unstemmed Non-collinear long-range magnetic ordering in HgCr2S4
title_short Non-collinear long-range magnetic ordering in HgCr2S4
title_sort non collinear long range magnetic ordering in hgcr2s4
work_keys_str_mv AT chaponl noncollinearlongrangemagneticorderinginhgcr2s4
AT radaellip noncollinearlongrangemagneticorderinginhgcr2s4
AT hory noncollinearlongrangemagneticorderinginhgcr2s4
AT tellingm noncollinearlongrangemagneticorderinginhgcr2s4
AT mitchellj noncollinearlongrangemagneticorderinginhgcr2s4