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| 1 | \section{Timing considerations}
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| 2 |
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| 3 | {\ldots \it \bf HAS TO BE UPDATED AND COMPLETED!! \ldots \\}
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| 4 | {\it Here, all possible models should go in with reasonning why certain time
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| 5 | or flux estimates are proposed. We have now only estimates on extrapolations
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| 6 | of the \eg power-laws. Maybe we should include: IC (in many possible combinations),
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| 7 | hadronic emission models (see~\cite{TASC}), Cannonball model. }
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| 8 | \par
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| 9 |
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| 10 | The EGRET~\cite{EGRET} instrument on the CGRO
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| 11 | has detected GeV emission of GRB940217 promptly and 90 min. after
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| 12 | the burst onset.
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| 13 | \\
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| 14 | \par
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| 15 | In~\cite{DERMER}, two peaks in the GeV light curve are calculated. An early maximum coincident
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| 16 | with the MeV eak is the high-eneryg extension of the synchrotron component, some seconds
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| 17 | after the burst onset. The second maximum peaking at $\approx$ 1.5 hours is due primarily to
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| 18 | SSC radiation with significant emission of up to $10^5$ sec. ($\approx 25$ hours) after the burst.
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| 19 | \\
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| 20 | \par
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| 21 | Li, Dai and Lu~\cite{LI} suggest GeV emission after pion production and some thermalization of the
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| 22 | UHE component with radiation maxima of up to one day or even one week (accompanied by long-term
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| 23 | neutrino emission).
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| 24 |
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| 25 | \par
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| 26 | \ldots \textit{\bf UNTIL WHEN WILL WE OBSERVE THE BURST AFTER OCCURRANCE} \ldots
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| 27 | \par
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| 28 |
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| 29 | \subsection{Determine reasonable upper limit for observation duration } |
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