changed the figure caption

2 files changed, 6 insertions, 5 deletions

diff --git a/hidden_order.bib b/hidden_order.bib
index 436345a..05136cb 100644
--- a/hidden_order.bib
+++ b/hidden_order.bib
@@ -416,7 +416,7 @@ Raman spectroscopy is used to uncover an unusual ordering in the low-temperature
   abstract = {Recent experiments on URu2Si2URu2Si2 show that the low-pressure hidden order is nonmagnetic but it breaks time reversal invariance. Restricting our attention to local order parameters of 5f25f2 shells, we find that the best candidate for hidden order is staggered order of either Tz{$\beta$}T{$\beta$}z or TxyzTxyz octupoles. Group theoretical arguments for the effect of symmetry-lowering perturbations (magnetic field, mechanical stress) predict behavior in good overall agreement with observations. We illustrate our general arguments on the example of a five-state crystal field model which differs in several details from models discussed in the literature. The general appearance of the mean field phase diagram agrees with the experimental results. In particular, we find that (a) at zero magnetic field, there is a first-order phase boundary between octupolar order and large-moment antiferromagnetism with increasing hydrostatic pressure; (b) arbitrarily weak uniaxial pressure induces staggered magnetic moments in the octupolar phase; and (c) a new phase with different symmetry appears at large magnetic fields.},
   number = {5},
   journal = {Physical Review B},
-  doi = {10/dx7d23},
+  doi = {10.1103/physrevb.71.054415},
   author = {Kiss, Annam{\'a}ria and Fazekas, Patrik},
   month = feb,
   year = {2005},
diff --git a/main.tex b/main.tex
index 2017904..a194abd 100644
--- a/main.tex
+++ b/main.tex
@@ -247,10 +247,11 @@ diagrams for this model are shown in Figure \ref{fig:phases}.
   \includegraphics[width=0.51\columnwidth]{phases_scalar}\hspace{-1.5em}
   \includegraphics[width=0.51\columnwidth]{phases_vector}
   \caption{
-    Schematic phase diagrams for this model. Solid lines denote continuous
-    transitions, while dashed lines indicated abrupt transitions. (a) The
-    phases for a scalar ($\Bog$ or $\Btg$). (b) The phases for a vector
-    ($\Eg$).
+    Phase diagrams for (a) \urusi\ from experiments (neglecting the
+    superconducting phase) \cite{hassinger_temperature-pressure_2008} (b) mean
+    field theory of a scalar ($\Bog$ or $\Btg$) Lifshitz point (c) mean field
+    theory of a vector ($\Eg$) Lifshitz point. Solid lines denote continuous
+    transitions, while dashed lines denote abrupt transitions.
   }
   \label{fig:phases}
 \end{figure}