modifications in Sec. 1
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@ -164,7 +164,7 @@ One could then exploit the structure of these Riemann surfaces to develop method
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\begin{wrapfigure}{r}{0.5\textwidth}
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\centering
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\includegraphics[width=\linewidth]{TopologyEP.pdf}
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\caption{A generic EP with the square root branch point topology. A loop around the EP interconvert the states.}
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\caption{A generic EP with the square-root branch point topology. A loop around the EP interconvert the states.}
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\label{fig:TopologyEP}
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\end{wrapfigure}
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By analytically continuing the electronic energy $E(\lambda)$ in the complex domain (where $\lambda$ is a coupling parameter), the ground and excited states of a molecule can be smoothly connected.
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