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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