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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-09-25 14:03:19 -0400 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2019-09-25 14:03:19 -0400 |
commit | 75b35bedad9a9b06caedf3083785ac3867b0567c (patch) | |
tree | db262a8f66ca52bd0be3f24cf2c9cc07a37ba4e8 /main.tex | |
parent | f2f4e6e51ace0412dc771b44b3bedac3cd425d55 (diff) | |
download | PRB_102_075129-75b35bedad9a9b06caedf3083785ac3867b0567c.tar.gz PRB_102_075129-75b35bedad9a9b06caedf3083785ac3867b0567c.tar.bz2 PRB_102_075129-75b35bedad9a9b06caedf3083785ac3867b0567c.zip |
Abstract reword.
Diffstat (limited to 'main.tex')
-rw-r--r-- | main.tex | 15 |
1 files changed, 8 insertions, 7 deletions
@@ -57,15 +57,16 @@ \date\today \begin{abstract} - We develop a phenomenological mean field theory for the elastic response of - \urusi\ through its hidden order transition. Several experimental features - are reproduced when the order parameter has $\Bog$ symmetry: the topology of - the temperature--pressure phase diagram, the response of the strain stiffness + We develop a phenomenological mean field theory for the strain in \urusi\ + through its hidden order transition. Several experimental features are + reproduced when the order parameter has $\Bog$ symmetry: the topology of the + temperature--pressure phase diagram, the response of the strain stiffness tensor above the hidden-order transition at zero pressure, and orthorhombic symmetry breaking in the high-pressure antiferromagnetic phase. In this - scenario, the hidden order is a version of the high-pressure - antiferromagnetic order modulated along the symmetry axis, and the triple - point joining those two phases with the paramagnetic phase is a Lifshitz point. + scenario, the hidden order is characterized by the order parameter in the + high-pressure antiferromagnetic phase modulated along the symmetry axis, and + the triple point joining those two phases with the paramagnetic phase is a + Lifshitz point. \end{abstract} \maketitle |