Ian Jauslin
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authorIan Jauslin <ian@jauslin.org>2021-03-24 18:37:22 -0400
committerIan Jauslin <ian@jauslin.org>2021-03-24 18:37:22 -0400
commita7c23d52429f0729157480d58c2d5a7220446022 (patch)
tree2a7a71027272c4fe44901cf2624cf82c515dedc5
parent6a019dc4f91c3db3731193aa0351444462b44a24 (diff)
Update to v1.0HEADv1.0master
Changed: title. Added: comment in caption of Fig 1 on the dimensionless nature of all figures.
-rw-r--r--Carlen_Holzmann_Jauslin_Lieb_2020.tex3
-rw-r--r--Changelog8
2 files changed, 10 insertions, 1 deletions
diff --git a/Carlen_Holzmann_Jauslin_Lieb_2020.tex b/Carlen_Holzmann_Jauslin_Lieb_2020.tex
index 67398df..93b8791 100644
--- a/Carlen_Holzmann_Jauslin_Lieb_2020.tex
+++ b/Carlen_Holzmann_Jauslin_Lieb_2020.tex
@@ -15,7 +15,7 @@
\begin{document}
-\title{A fresh look at a simplified approach to the Bose gas}
+\title{A simplified approach to the repulsive Bose gas from low to high densities and its numerical accuracy}
\author{Eric A. Carlen}
\affiliation{\it Department of Mathematics, Rutgers University}
@@ -483,6 +483,7 @@ For $\alpha=16$ this is even clearer, and one sees that the Medium Equation is m
The energy as a function of density for the potential $e^{-|\mathbf x|}$ (top) and $16e^{-|\mathbf x|}$ (bottom).
We compare the predictions of the Big, Medium and Simple Equations to a QMC simulation.
For comparison, we also plot the Lee-Huang-Yang (LHY) energy\-~(\ref{lhy}).
+ (All quantities plotted in this and the following figures are dimensionless.)
}
\label{fig:energy}
\end{figure}
diff --git a/Changelog b/Changelog
index ab62ec5..5b9b61c 100644
--- a/Changelog
+++ b/Changelog
@@ -1,3 +1,11 @@
+v1.0:
+
+ * Changed: title.
+
+ * Added: comment in caption of Fig 1 on the dimensionless nature of all
+ figures.
+
+
v0.2:
* Added: Comparison of the energy for two different potentials that share