| 1 | \section{Introduction}
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| 2 | The MAGIC telescope has been designed especially light with a special focus on
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| 3 | being able to react fastly to GRB alerts from the satellites.
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| 4 | In \cite{design} and~\cite{PETRY},
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| 5 | the objective was set to turn the telescope to the burst position in 10-30~s
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| 6 | in order to have a fair chance of detecting a burst with the MAGIC telescope.
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| 7 | The current possible value is 20 sec. for full turn-around
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| 8 | %FIXME
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| 9 | {\it \bf THIS HAS TO BE CHECKED FROM THOMAS B. !!}
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| 10 | \par
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| 11 | Several attempts have been made in the past to observe GRBs at energies
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| 12 | from the GeV range upwards each indicating some excess over background but
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| 13 | without stringent evidence. The only secured detection was performed by EGRET
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| 14 | which detected seven GRBs emitting high energy photons in the
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| 15 | 100~MeV to 18~GeV range~\cite{EGRET}. There have been
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| 16 | results suggesting gamma rays beyond the GeV range from the TIBET array~\cite{TIBET} and
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| 17 | from HEGRA-AIROBICC~\cite{HEGRA}. Evidence for TeV emission of one burst was claimed by
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| 18 | the MILAGRITO experiment~\cite{MILAGRO}. Recently, the GRAND array has reported some
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| 19 | excess of observed muons during seven BATSE bursts~\cite{GRAND}. In this context, note
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| 20 | especially a recent publication from the TASC detector on \eg~\cite{TASC},
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| 21 | finding a high-energy spectral
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| 22 | component presumably due to ultra-relativistic acceleration of hadrons and
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| 23 | producing a spectral index of $-1$ with no cut-off up to the detector limit (200 MeV).
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| 24 | \par
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| 25 | The nowadays most widely accepted model for gamma emission from GRB suggests a bursts
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| 26 | environment involving collisions of an ultra-relativistic e$^+$-e$^-$
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| 27 | plasma fireball~\cite{PAZCYNSKI,GOODMAN,SARI}. These fireballs may produce
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| 28 | low-energy gamma rays either by ``internal'' collisions of multiple
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| 29 | shocks~\cite{XU,REES} or by ``external'' collisions of a single shock
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| 30 | with the ambient circum burst medium (CBM)~\cite{MESZAROS94}.
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| 31 | \par
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| 32 | In many publications,
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| 33 | the possibility that more energetic gamma-rays come along with the (low-energy) gamma-ray
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| 34 | burst, have been explored.
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| 35 | Proton-synchrotron emission~\cite{TOTANI} have
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| 36 | been suggested as well as photo-pion production~\cite{WAXMAN,BAHCALL,BOETTCHER}
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| 37 | and inverse-Comption
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| 38 | scattering in the burst environment~\cite{MESZAROS93,CHIANG,PILLA,ZHANG}.
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| 39 | Long-term high-energy gamma emission from accelerated protons in forward-shock
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| 40 | has been predicted in~\cite{LI}.
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| 41 | Even considering pure electron-synchrotron radiation predicts measurable GeV emission for a
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| 42 | significant fraction of GRBs~\cite{ZHANG}.
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| 43 | Implications of the observation of a high-energy gamma-ray component on
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| 44 | distance scale, energy production in the GRB and distinction between internal and
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| 45 | external shock models have been treated in~\cite{HARTMANN,MANNHEIM,SALOMON,PRIMACK}.
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| 46 | \par
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| 47 | \ldots {\bf MORE ELABORATE TREATMENT OF HE-EMISSION: WHICH MODELS, WHAT TIME DIFFERENCE TO
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| 48 | GRB, TIME DEVELOPMENT, EXPECTED FLUXES, SPECTRA } \ldots
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| 49 | \par
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| 50 | \ldots {\bf UPDATE CURRENT PAPERS} \ldots
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| 51 | \par
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| 52 | \par
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| 53 | \ldots {\bf MORE DETAILED DESCRIPTION OF GEV-EMISSION MODELS }\ldots
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| 54 | \par
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| 55 | \par
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| 56 | \ldots {\bf SATOKO AND MARKUS GARCZ.}\ldots
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| 57 | \par
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| 58 | In the year 2005, three satellites will produce GRB alerts: The \he
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| 59 | satellite, launched in October 2000, the \ig satellite, launched October 2002 and the
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| 60 | \sw satellite, launched in October, 2004 and expected to be fully operational in March, 2005.
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| 61 | \par
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| 62 | Concerning estimates about the MAGIC observability of GRBs, a very detailed study
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| 63 | of GRB spectra obtained from the third and fourth \ba catalogue has been made
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| 64 | in~\cite{ICRC,NICOLA}. The spectra were extrapolated to \ma energies with a simple continuation
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| 65 | of the observed high-energy power law behaviour and the calculated fluxes compared
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| 66 | with \ma sensitivities. Setting conservative cuts on observation times and significances,
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| 67 | and assuming an energy threshold of 15~GeV, a GRB detection rate of $0.5--2$ per year
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| 68 | was obtained for an assumed observation delay of 15~sec. and the \sw GRB trigger rate ($\sim 100/year$).
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| 69 |
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| 70 | \subsection{Observing XRFs}
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| 71 |
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| 72 | {\ldots \it \bf CAN BE MAYBE GO INTO A SEPARATE PROPOSAL \ldots \\}
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| 73 |
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| 74 | \subsection{Observing SGRs}
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| 75 |
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| 76 | {\ldots \it \bf CAN BE MAYBE GO INTO A SEPARATE PROPOSAL \ldots \\}
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| 77 |
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