Changeset 6764 for trunk


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Timestamp:
03/07/05 15:16:49 (20 years ago)
Author:
hbartko
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  • trunk/MagicSoft/GC-Proposal/GC.tex

    r6762 r6764  
    105105\section{Introduction}
    106106
     107%<<<<<<< GC.tex
     108
     109%The Galactic Center (GC) region contains many unusual objects which may be responsible for the high energy processes generation gamma rays \cite{Aharonian2005,Atoyan2004,Horns2004}. The GC is rich in massive stellar clusters with up to 100 OB stars \cite{GC_environment}, immersed in a dense gas within the volume of 300 pc and the mass of $2.7 \cdot 10^7 M_{\odot}$, young supernova remnants e.g. G0.570-0.018 or Sgr A East, and nonthermal radio arcs. The dynamical center of the Milky Way is associated with the compact radio source Sgr A$^*$, which is believed to be a massive black hole \cite{GC_black_hole,Melia2001}. An overview of the sources in the GC region is given in figure \ref{fig:GC_sources}. Some data about the Galactic Center are summarized in table \ref{table:GC_properties}.
     110%=======
    107111The Galactic Center (GC) region contains many unusual objects which may be
    108112responsible for the high energy processes generating gamma rays
     
    110114clusters with up to 100 OB stars \cite{GC_environment}, immersed in a dense
    111115gas within a radius of 300 pc and the mass of $2.7 \cdot 10^7 M_{\odot}$,
    112 young supernova remnants e.g. G0.570-0.018 or Sgr A East, and nonthermal radio arcs. An overview of the sources in the GC region is given in figure \ref{fig:GC_sources}. Some data about the Galactic Center are summarized in table \ref{table:GC_properties}.
     116young supernova remnants e.g. G0.570-0.018 or Sgr A East, and nonthermal radio arcs. The dynamical center of the Milky Way is associated with the compact radio source Sgr A$^*$, which is believed to be a massive black hole \cite{GC_black_hole,Melia2001}. An overview of the sources in the GC region is given in figure \ref{fig:GC_sources}. Some data about the Galactic Center are summarized in table \ref{table:GC_properties}.
     117%>>>>>>> 1.15
    113118
    114119\begin{table}[h]{\normalsize\center
     
    196201\end{table}
    197202
     203
    198204\section{Scientific Case}
    199205
    200206
    201 High energy gamma rays can be produced in the GC in the non-thermal radio filaments by high-energy leptons which scatter background infrared photons from the nearby ionized clouds \cite{Pohl1997,Aharonian2005}, or by hadrons colliding with dense matter. These high energy hadrons can be accelerated by the massive black hole \cite{GC_black_hole}, associated with the Sgr A$^*$, supernovae or an energetic pulsar. Alternative mechanisms invoke the hypothetical annihilation of super-symmetric dark matter particles (for a review see \cite{jung96}) or curvature radiation of protons in the vicinity of the central super-massive black hole \cite{GC_black_hole,Melia2001}.
    202 
    203 
    204 In order to shed new light on the high energy phenomena in the GC region, and constrain the models mentioned above, new observations with high sensitivity, good spectra reconstruction and angular resolution are necessary.
    205 
    206 For the interpretation of the observed gamma flux the following observables are very important:
     207In the GC region high energy gamma rays can be produced in different sources:
     208
     209\begin{itemize}
     210\item{entire innermost 10 pc region (interaction between cosmic rays and the dense ambient gas)}
     211\item{non-thermal radio filaments  \cite{Pohl1997}}
     212\item{young SNR Sgr A East \cite{Fatuzzo2003}}
     213\item{in the compact radio source Sgr A*}
     214\item{central part of the dark matter halo.}
     215\end{itemize}
     216
     217It is quite possible that some of these potentioal gamma-ray production sites contribute comparably to the the observed TeV flux.
     218
     219
     220% in the non-thermal radio filaments by high-energy leptons which scatter background infrared photons from the nearby ionized clouds \cite{Pohl1997,Aharonian2005}, or by hadrons colliding with dense matter. These high energy hadrons can be accelerated by the massive black hole \cite{GC_black_hole}, associated with the Sgr A$^*$, supernovae or an energetic pulsar. Alternative mechanisms invoke the hypothetical annihilation of super-symmetric dark matter particles (for a review see \cite{jung96}) or curvature radiation of protons in the vicinity of the central super-massive black hole \cite{GC_black_hole,Melia2001}.
     221
     222
     223In order to shed new light on the high energy phenomena in the GC region, and constrain the emission mechanisms and sources, new observations with high sensitivity, good spectra reconstruction and angular resolution are necessary. For the interpretation of the observed gamma flux the following observables are very important:
    207224
    208225\begin{itemize}
    209226\item{source location, source extension}
    210227\item{time variability}
    211 \item{energy spectrum}
     228\item{energy spectrum.}
    212229\end{itemize}
    213230
     
    223240
    224241
    225 
    226 \subsection{Leptonic Models}
    227 
    228 
    229 \subsection{Hadronic Models}
     242\subsection{Emission from SgrA$^*$}
     243
     244
     245\cite{Aharonian2005,Atoyan2004}
     246
     247\subsubsection{Leptonic Models}
     248
     249
     250\subsubsection{Hadronic Models}
    230251
    231252
     
    233254
    234255
    235 \subsection{Dark Matter}
     256\subsection{Dark Matter Annihilation}
    236257
    237258
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