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pyrene_dimer/pyrene.tex
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pyrene_dimer/pyrene.tex
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%% ---------------
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\author{a}
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\affiliation[Universit\'e de Toulouse (UPS) and CNRS]{Laboratoire de Chimie et Physique Quantiques LCPQ/IRSAMC, Universit\'e de Toulouse (UPS) and CNRS, 118 Route de Narbonne, F-31062 Toulouse, France}
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\author{a}
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\affiliation[Universit\'e de Toulouse (UPS) and CNRS]{Laboratoire de Chimie et Physique Quantiques LCPQ/IRSAMC, Universit\'e de Toulouse (UPS) and CNRS, 118 Route de Narbonne, F-31062 Toulouse, France}
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\author{a}
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\affiliation[Universit\'e de Toulouse (UPS) and CNRS]{Laboratoire de Chimie et Physique Quantiques LCPQ/IRSAMC, Universit\'e de Toulouse (UPS) and CNRS, 118 Route de Narbonne, F-31062 Toulouse, France}
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\author{a}
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\affiliation[Universit\'e de Toulouse (UPS) and CNRS]{Laboratoire de Chimie et Physique Quantiques LCPQ/IRSAMC, Universit\'e de Toulouse (UPS) and CNRS, 118 Route de Narbonne, F-31062 Toulouse, France}
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\email{a}
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\phone{a}
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%% optional argument to \title.
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\title[An \textsf{achemso} demo]
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{pyrene dimer}
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%% supplied. These should be set up here, and will be printed after
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%% the title and author information, if needed.
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%\abbreviations{PES,ISM,COSAC,FT-IR,MRCI+Q,CCD,CCSD(T),RCCSD(T),UCCSD(T),MP2, MBPT, BSSE, ZPE, DFT, SCC-DFTB, CM3, MD, MDPT}
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\keywords{Molecular Dynamics, SCC-DFTB, Collision Induced Dissociation, Pyrene Dimer}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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%% The manuscript does not need to include \maketitle, which is
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%% executed automatically.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\begin{document}
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%% The "tocentry" environment can be used to create an entry for the
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%% graphical table of contents. It is given here as some journals
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%\begin{tocentry}
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\begin{abstract}
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\end{abstract}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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%% Start the main part of the manuscript here.
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\section{Introduction }
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\section{Computational Methods} \label{Comput_meth}
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\textbf{Exploration of the PES}
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\textbf{Dynamics Collision Simulations}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Results and Discussion} \label{resul_disc}
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\begin{figure}
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\includegraphics[width=0.8\linewidth]{figure/dissoci-Ar.eps}
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\centering
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\caption{The pyrene dimer dissociation percentage after collision with Ar at different collision energy levels.}
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\label{fig:dissoci-Ar}
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\end{figure}
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\begin{figure}
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\includegraphics[width=0.8\linewidth]{figure/distribute-prot-Ar.eps}
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\centering
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\caption{The ratio of the mean energy of the two pyrene and the global energy of the dimer after the collision of pyrene dimer with Ar at different collision energy levels.}
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\label{fig:distribute-prot-Ar}
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\end{figure}
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\begin{figure}
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\includegraphics[width=0.8\linewidth]{figure/distribute-Ar.eps}
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\centering
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\caption{The energy of Ar after collision with pyrene dimer at different collision energy levels.}
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\label{fig:distribute-Ar}
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\end{figure}
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\begin{figure}
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\includegraphics[width=0.8\linewidth]{figure/distribute-py.eps}
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\centering
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\caption{The global energy of the dimer (green line) and relative energy of the dimer (blue line) after collision with Ar at different collision energy levels.}
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\label{fig:distribute-py}
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\end{figure}
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\begin{table}
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\begin{center}
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\caption{The energy distribution after the collision of pyrene dimer with Ar at different collision energy. (E refers to the collision energy; E$_{dimer}$ refers to the the global energy of the pyrene dimer; E$_{Ar}$ refers to the energy of Ar; E$_{1}$ refers to the energy of one pyrene after collision; E$_{2}$ refers to the energy of the other pyrene; E$_{Re}$ refers to the relative energy of the pyrene dimer). All the energies are in eV.}
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\label{tab:table1}
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\begin{tabular}{c|c|c|c|c|c}
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\textbf{E} & \textbf{E$_{dimer}$} & \textbf{E$_{Ar}$} & \textbf{E$_{1}$} & \textbf{E$_{2}$} & \textbf{E$_{Re}$}\\
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\hline
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2.5 & 0.17 & 1.67 & 0.25 & 0.25 & 0.19\\
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5.0 & 0.29 & 3.56 & 0.40 & 0.41 & 0.39\\
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7.5 & 0.42 & 5.39 & 0.55 & 0.56 & 0.63\\
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10.0 & 0.53 & 7.29 & 0.71 & 0.71 & 0.81\\
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12.5 & 0.64 & 9.28 & 0.90 & 0.85 & 0.91\\
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15.0 & 0.73 & 11.2 & 1.01 & 1.03 & 1.06\\
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17.5 & 0.82 & 13.15 & 1.16 & 1.23 & 1.17\\
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20.0 & 0.88 & 15.15 & 1.38 & 1.30 & 1.29\\
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22.5 & 0.96 & 17.09 & 1.53 & 1.51 & 1.39\\
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25.0 & 1.03 & 19.12 & 1.63 & 1.69 & 1.47\\
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27.5 & 1.09 & 21.13 & 1.79 & 1.83 & 1.49\\
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30.0 & 1.16 & 23.03 & 2.17 & 1.97 & 1.55\\
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\end{tabular}
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\end{center}
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\end{table}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Conclusions} \label{Concl}
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\begin{acknowledgement}
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The authors acknowledge the supercomputing facility of CALMIP for generous allocation
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of computer resources (projects P1320 and P0059). The authors declare that there has
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been no significant financial support for this work.
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\end{acknowledgement}
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%\bibliographystyle{achemso}
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\bibliography{biblio}
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\end{document}
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