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author | jaron-overleaf <jaron-overleaf@kent-dobias.com> | 2019-11-05 17:01:54 +0000 |
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committer | overleaf <overleaf@localhost> | 2019-11-05 20:28:05 +0000 |
commit | 465e900315f97fd2e69cb933ea5c4d7c09f7e1ca (patch) | |
tree | 0bf5e387f3e19079f1100943a9d60a5a2cdf3f2a /main.tex | |
parent | de09cbeb5d1af65b68035f7b4a78daf195a36553 (diff) | |
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@@ -439,7 +439,7 @@ where $\eta$ has a large nonzero value and higher powers in the free energy become important. The data in the high-temperature phase can be fit to the theory \eqref{eq:elastic.susceptibility}, with a linear background modulus $C^0_\Bog$ and $\tilde r-\tilde r_c=a(T-T_c)$, and the result is shown in -Figure \ref{fig:fit}. The data and theory appear quantitatively consistent in +Figure \ref{fig:data}. The data and theory appear quantitatively consistent in the high temperature phase, suggesting that \ho\ can be described as a $\Bog$-nematic phase that is modulated at finite $q$ along the $c-$axis. |