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author | bradramshaw undefined <bradramshaw@cornell.edu> | 2020-06-26 14:16:17 +0000 |
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committer | overleaf <overleaf@localhost> | 2020-07-03 10:23:52 +0000 |
commit | b7100d954aac955ae7131a0b59beeef8b380dbe4 (patch) | |
tree | 9a6774051bf957afc1b91a07f592c03445413b30 /main.tex | |
parent | 3137e4478621446dc9592688f4ec342459bc4749 (diff) | |
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-rw-r--r-- | main.tex | 4 |
1 files changed, 2 insertions, 2 deletions
@@ -140,11 +140,11 @@ under pressure.\cite{Choi_2018} Above 0.13--0.5 $\GPa$ (depending on temperature), \urusi\ undergoes a $\Bog$ nematic distortion, which might be related to the anomalous softening of the $\Bog$ elastic modulus $(C_{11}-C_{12})/2$ that occurs over a broad temperature range at zero -pressure.\cite{Wolf_1994, Kuwahara_1997} Motivated by these results---which +pressure.\cite{Wolf_1994, Kuwahara_1997,yanagisawa2012gamma3} Motivated by these results---which hint at a $\Bog$ strain susceptibility associated with the \ho\ state---we construct a phenomenological mean field theory for an arbitrary \op\ coupled to strain, and then determine the effect of its phase transitions on the elastic -response in different symmetry channels. +response in different symmetry channels. We find that only one \op\ representation reproduces the anomalous $\Bog$ elastic modulus, which softens in a Curie--Weiss-like manner from room |