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Long Duration High Energy Transients. S. R. Kulkarni. An interlude – compactness problem. From sari’s talk (circa 2000). Energy. We measure F~10 -6 erg/cm 2 Cosmological: D ~ 10 28 cm E = 4 D 2 F ~ 10 51 erg. Temporal Variability. dT<1s, T~100 N=T/dT>100.
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Long Duration High Energy Transients S. R. Kulkarni
Energy • We measure F~10-6 erg/cm2 • Cosmological: D ~ 1028cm • E = 4D2F ~ 1051erg
Temporal Variability • dT<1s, T~100 N=T/dT>100
Implications of short timescale dt=R/c R/c
COMPACTNESS PROBLEM g + g e+ + e- • dT ~ 1ms R < 3•107 cm • E ~ 1051ergs 1057 photonshigh photon density(many above 500 keV). • Optical depth T n R~1015>>1 • Inconsistent with the non thermal spectrum! Spectrum: Optically thin Size & Energy: Optically thick ? Paradox ?
C R A ~1/ D B R R Relativistic Time-Scales • tB-tA~ R (1-) / c ~ R/22c • tC-tA~ R(1-cos )/c ~ R/22c • tD-tA~ /c
The Solution:Relativistic Motion • Due to Relativistic Motion • R = g2 c dT • Eph (emitted) = Eph (obs) / g • tgg = g-(4+2a) nsTR ~ 1015/g4+2a (Goodman; Paczynski; Krolik & Pier; Fenimore; Woods & Loeb; Piran & Shemi; Lithwick & RS 01) g > 100
Relativistic Motion (Lithwick & RS 2001)
References • F. J. Virigili et al. 2013 (ApJ 778) • A. J. Levan et al. 2013 (astroph)
GRB091024A z=1.09
Need a long lived engine • Collapsar model: What determines the duration of the engine? • Tidal Disruption Event • Long duration nicely explained • Magnetar powered?
Observational difficulties • Most GRB missions work on “triggers” – spikes of emission • Such events are best seen in “imaging triggers” • But satellite must be pointed to the same piece of sky for 1000 s (not the case with Swift) • I wonder how well has the BAT data been analyzed for such objects (or for that matter WFC data)
Tests • Does the object coincide with the nucleus? • Is there a 1998bw-like supernova associated with the object? • What is the total energy loss? (relative to say 1052 erg)