Changeset 6146 for trunk/MagicSoft
- Timestamp:
- 01/31/05 15:45:14 (20 years ago)
- Location:
- trunk/MagicSoft/GRB-Proposal
- Files:
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- 3 edited
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trunk/MagicSoft/GRB-Proposal/Introduction.tex
r6145 r6146 75 75 76 76 77 \subsection{Observation of Soft Gamma Repeaters(SGRs)} 78 A stronge magnetic neutron star, a so-called ``Soft Gamma Repeaters (SGRs)'' p 79 eriodically emit gamma-ray, and are extremely rare stars. Only four identified 80 SGRs are discovered in the last 20 years: SGR0526-66, SGR1806-20, SGR1900+14, SG 81 R1627-41. GRBs and SGRs can be explained with an unique precessing gamma jet mod 82 el observed at different beam-angle and at different ages. -
trunk/MagicSoft/GRB-Proposal/Strategies.tex
r6145 r6146 6 6 from the claimed GRB observation frequency of about 150-200 GRBs/year by the SWIFT 7 7 collaboration~\cite{SWIFT} and the results of the studies on the MAGIC duty-cycle 8 made by Nicola Galante~\cite{NICOLA} and Satoko Mizobuchi~\cite{SATOKO}.8 made by Nicola Galante~\cite{NICOLA}. 9 9 Considering a MAGIC duty-cycle of about 10\% and a tolerance of 5 hours 10 10 to point the GRB, we should be able to point about 1-2 GRB/month. … … 20 20 yet under observational control. 21 21 22 This reduction of the real duty-cycle w.r.t. the studies~\cite{NICOLA ,SATOKO}22 This reduction of the real duty-cycle w.r.t. the studies~\cite{NICOLA} 23 23 gets compensated by the tolerance of 5 hours for considering the alert observable 24 24 (5 hours more before the beginning of the night -
trunk/MagicSoft/GRB-Proposal/Timing.tex
r6120 r6146 1 1 \section{Timing considerations} 2 2 3 {\ldots \it \bf HAS TO BE UPDATED AND COMPLETED!! \ldots \\}4 3 {\it Here, all possible models should go in with reasonning why certain time 5 4 or flux estimates are proposed. We have now only estimates on extrapolations 6 of the \eg power-laws. Maybe we should include: IC (in many possible combinations), 7 hadronic emission models (see~\cite{TASC}), Cannonball model. } 5 of the \eg power-laws. Maybe we should include: IC (in many possible combinations), hadronic emission models (see~\cite{TASC}), Cannonball model.} 8 6 \par 9 7 10 The EGRET~\cite{EGRET} instrument on the CGRO 11 has detected GeV emission of GRB940217 promptly and 90 min. after 12 the burst onset. 13 \\ 8 The EGRET~\cite{EGRET} instrument on the CGRO has detected GeV emission of GRB940217 promptly and 90 min. after the burst onset.\\ 14 9 \par 15 In~\cite{DERMER}, two peaks in the GeV light curve are calculated. An early maximum coincident 16 with the MeV peak is the high-energy extension of the synchrotron component, some seconds 17 after the burst onset. The second maximum peaking at $\approx$ 1.5 hours is due primarily to 18 SSC radiation with significant emission of up to $10^5$ sec. ($\approx 25$ hours) after the burst. 19 \\ 10 11 In~\cite{DERMER}, two peaks in the GeV light curve are calculated. An early maximum coincident with the MeV peak is the high-energy extension of the synchrotron component, some seconds after the burst onset. The second maximum peaking at $\approx$ 1.5 hours is due primarily to SSC radiation with significant emission of up to $10^5$ sec. ($\approx 25$ hours) after the burst.\\ 20 12 \par 21 Li, Dai and Lu~\cite{LI} suggest GeV emission after pion production and some thermalization of the 22 UHE component with radiation maxima of up to one day or even one week (accompanied by long-term 23 neutrino emission). 13 14 Li, Dai and Lu~\cite{LI} suggest GeV emission after pion production and some thermalization of the UHE component with radiation maxima of up to one day or even one week (accompanied by long-term neutrino emission). 24 15 25 16 \par
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