From 1d62111c843740b89c80fd2f1dbd0a70925cf7a3 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 6 May 2020 20:06:06 -0400
Subject: Updated some citekeys.

---
 main.tex | 6 +++---
 1 file changed, 3 insertions(+), 3 deletions(-)

(limited to 'main.tex')

diff --git a/main.tex b/main.tex
index 3da57a9..374519e 100644
--- a/main.tex
+++ b/main.tex
@@ -286,7 +286,7 @@ to $f_\op$ with the identification $r\to\tilde r=r-b^2/2C^0_\X$.
 \end{figure}
 
 With the strain traced out, \eqref{eq:fo} describes the theory of a Lifshitz
-point at $\tilde r=c_\perp=0$.\cite{Lifshitz_1942a, Lifshitz_1942b} The
+point at $\tilde r=c_\perp=0$.\cite{Lifshitz_1942_OnI, Lifshitz_1942_OnII} The
 properties discussed in the remainder of this section can all be found in a
 standard text, e.g., in chapter 4 \S6.5  of Chaikin \&
 Lubensky.\cite{Chaikin_1995} For a one-component \op\ ($\Bog$ or $\Btg$) and
@@ -579,7 +579,7 @@ thermodynamic phase transition).
 Three dimensions is below the upper critical dimension $4\frac12$ of a
 one-component disordered-to-modulated transition, and so mean field theory
 should break down sufficiently close to the critical point due to fluctuations,
-at the Ginzburg temperature. \cite{Hornreich_1980, Ginzburg_1961} Magnetic
+at the Ginzburg temperature. \cite{Hornreich_1980, Ginzburg_1961_Some} Magnetic
 phase transitions tend to have a Ginzburg temperature of order one.  Our fit
 above gives $\xi_{\perp0}q_*=(D_\perp q_*^4/aT_c)^{1/4}\simeq2$, which combined
 with the speculation of $q_*\simeq\pi/a_3$ puts the bare correlation length
@@ -589,7 +589,7 @@ mean field exponent suggests that this region is outside the Ginzburg region,
 but an experiment may begin to see deviations from mean field behavior within
 approximately several Kelvin of the critical point. An ultrasound experiment
 with more precise temperature resolution near the critical point may be able to
-resolve a modified cusp exponent $\gamma\simeq1.31$,\cite{Guida_1998} since the
+resolve a modified cusp exponent $\gamma\simeq1.31$,\cite{Guida_1998_Critical} since the
 universality class of a uniaxial modulated one-component \op\ is $\mathrm
 O(2)$.\cite{Garel_1976} We should not expect any quantitative agreement between
 mean field theory and experiment in the low temperature phase since, by the
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