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authorJaron Kent-Dobias <jaron@kent-dobias.com>2017-07-27 13:24:44 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2017-07-27 13:24:44 -0400
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@@ -374,7 +374,7 @@ correction appears to match data quite well.
\end{figure}
Abrupt phase transitions, such as the jump in magnetization in the Ising
-model below $T_c$, are known to imply essential singularities in the free
+model below $T_\c$, are known to imply essential singularities in the free
energy that are usually thought to be unobservable in practice. We have
argued that this essential singularity controls the universal scaling
behavior near continuous phase transitions, and have derived an explicit
@@ -384,7 +384,7 @@ for the Ising model in a field, and showed that incorporating our singularity
into the scaling function gives good convergence to the simulations in \twodee.
Our results should allow improved high-precision functional forms for the free
-energy~\cite{CaselleXXX}, and should have implications for the scaling
+energy~\cite{caselle.2001.critical}, and should have implications for the scaling
of correlation functions~\cite{YJXXX,XXX}. Our methods might be generalized
to predict similar singularities in systems where nucleation and metastability
are proximate to continuous phase transitions, such as 2D superfluid