Update to v1.0
Changed: title. Added: comment in caption of Fig 1 on the dimensionless nature of all figures.
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\begin{document}
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\begin{document}
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\title{A fresh look at a simplified approach to the Bose gas}
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\title{A simplified approach to the repulsive Bose gas from low to high densities and its numerical accuracy}
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\author{Eric A. Carlen}
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\author{Eric A. Carlen}
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\affiliation{\it Department of Mathematics, Rutgers University}
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\affiliation{\it Department of Mathematics, Rutgers University}
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@ -483,6 +483,7 @@ For $\alpha=16$ this is even clearer, and one sees that the Medium Equation is m
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The energy as a function of density for the potential $e^{-|\mathbf x|}$ (top) and $16e^{-|\mathbf x|}$ (bottom).
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The energy as a function of density for the potential $e^{-|\mathbf x|}$ (top) and $16e^{-|\mathbf x|}$ (bottom).
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We compare the predictions of the Big, Medium and Simple Equations to a QMC simulation.
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We compare the predictions of the Big, Medium and Simple Equations to a QMC simulation.
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For comparison, we also plot the Lee-Huang-Yang (LHY) energy\-~(\ref{lhy}).
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For comparison, we also plot the Lee-Huang-Yang (LHY) energy\-~(\ref{lhy}).
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(All quantities plotted in this and the following figures are dimensionless.)
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}
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}
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\label{fig:energy}
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\label{fig:energy}
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\end{figure}
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\end{figure}
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@ -1,3 +1,11 @@
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v1.0:
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* Changed: title.
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* Added: comment in caption of Fig 1 on the dimensionless nature of all
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figures.
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v0.2:
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v0.2:
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* Added: Comparison of the energy for two different potentials that share
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* Added: Comparison of the energy for two different potentials that share
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