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$, the propagation vector increases and saturates a...
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Format: | Journal article |
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2006
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author | Chapon, L Radaelli, P Hor, Y Telling, M Mitchell, J |
author_facet | Chapon, L Radaelli, P Hor, Y Telling, M Mitchell, J |
author_sort | Chapon, L |
collection | OXFORD |
description | The low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at T$_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. |
first_indexed | 2024-03-07T03:34:26Z |
format | Journal article |
id | oxford-uuid:bbd04dd1-438d-47ec-9ac4-0602ce787eb5 |
institution | University of Oxford |
last_indexed | 2024-03-07T03:34:26Z |
publishDate | 2006 |
record_format | dspace |
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 |