| HETE Burst H2380 |
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Burst H2380 summary
Evaluation
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Y. Shirasaki, C. Graziani, M. Matsuoka, T. Tamagawa, K. Torii, T. Sakamoto, A. Yoshida, E. Fenimore, M. Galassi, T. Tavenner, and T. Donaghy, on behalf of the HETE WXM Team; G. Ricker, J-L Atteia, N. Kawai, D. Lamb, and S. Woosley on behalf of the HETE Science Team; J. Villasenor, R. Vanderspek, J. Doty, G. Crew, G. Monnelly, N. Butler, T. Cline, J.G. Jernigan, A. Levine, F. Martel, E. Morgan, G. Prigozhin, G. Azzibrouck, J. Braga, R. Manchanda, and G. Pizzichini, on behalf of the HETE Operations and HETE Optical-SXC Teams; M. Boer, J-F Olive, J-P Dezalay, and K. Hurley on behalf of the HETE FREGATE Team; write: At 12:06:13.57 UTC (43573.57 s UT) on 4 Oct 2002, the HETE FREGATE, WXM, and SXC instruments detected event H2380, a long GRB. The WXM flight localization was correct and was reported in a GCN Position Notice at 12:07:02 UT, 49 sec after the beginning of the burst. Ground analysis of the WXM data for the burst produced a refined location, which was reported in a GCN Position Notice at 13:19:54 UT, 73 minutes after the burst. The WXM localization SNR was 14. The WXM location can be expressed as a 90% confidence circle that is 10 arcminutes in radius and is centered at RA = 00h 26m 47s, Dec = +18d 59' 13" (J2000). Ground analysis of the SXC data for the burst produced a further refinement in the location, which was reported in a GCN Position Notice at 14:39:51 UT, 154 minutes after the burst. The SXC localization SNR was 9. The SXC location can be expressed as a 90% confidence circle that is 2 arcminutes in radius and is centered at RA = 00h 26m 57s, Dec = +18d 55' 44" (J2000). The SXC localization may be improved. In the FREGATE 8-40 keV band, the burst had a duration of ~100 seconds. In the WXM 2-25 keV band, the burst also had a duration of ~100 seconds. A light curve for GRB021004 is provided at the following URL: http://space.mit.edu/HETE/Bursts/ This message is citable.
J. Doty, G. Crew, J.G. Jernigan, R. Vanderspek, J. Villasenor, G. Monnelly, N. Butler, T. Cline, A. Levine, F. Martel, E. Morgan, G. Prigozhin, G. Azzibrouck, J. Braga, R. Manchanda, and G. Pizzichini, on behalf of the HETE Optical-SXC and HETE Operations Teams; G. Ricker, J-L Atteia, N. Kawai, D. Lamb, and S. Woosley on behalf of the HETE Science Team; C. Graziani, Y. Shirasaki, M. Matsuoka, T. Tamagawa, K. Torii, T. Sakamoto, A. Yoshida, E. Fenimore, M. Galassi, T. Tavenner, and T. Donaghy, on behalf of the HETE WXM Team; M. Boer, J-F Olive, J-P Dezalay, and K. Hurley on behalf of the HETE FREGATE Team; write: Analysis of the full data set derived from the HETE Soft X-ray Camera (SXC) has resulted in a revised location for GRB021004(=H2380; Shirasaki et al, GCN Circular #1565). The revised SXC location can be expressed as a 90% confidence circle that is 62 arcsec in radius and is centered at: RA = 00h 26m 55.7s, Dec = +18d 56' 18.6" (J2000) This revised SXC localization is shifted 38 arcsec with respect to, but lies fully within, the original 120 arcsec radius SXC error circle reported by Shirasaki et al in GCN1565. The fading optical transient reported by Fox in GCN1564 is 40 arcsec from the center of, and is within, this revised SXC error circle. Further information regarding GRB021004 is provided at the following URL: http://space.mit.edu/HETE/Bursts/ This message is citable.
D. Lamb, G. Ricker, J-L Atteia, N. Kawai, and S. Woosley on behalf of
the HETE Science Team;
J-F Olive, M. Boer, J-P Dezalay, and K. Hurley on behalf of the HETE
FREGATE Team;
Y. Shirasaki, M. Matsuoka, T. Tamagawa, K. Torii, T. Sakamoto,
A. Yoshida, E. Fenimore, M. Galassi, T. Tavenner, C. Graziani, and
T. Donaghy, on behalf of the HETE WXM Team;
J. Villasenor, R. Vanderspek, J. Doty, G. Crew, G. Monnelly, N. Butler,
T. Cline, J.G. Jernigan, A. Levine, F. Martel, E. Morgan, G. Prigozhin,
G. Azzibrouck, J. Braga, R. Manchanda, and G. Pizzichini, on behalf of
the HETE Operations and HETE Optical-SXC Teams;
write:
Analysis of the FREGATE data for GRB021004 (=H2380) shows that
the fluence-averaged photon number spectrum of the burst is well-fit
by a single power-law spectrum with slope alpha = 1.64 +/- 0.09, and
gives the following values for the fluences of the burst:
S = 1.8 x 10-6 erg cm-2 (50-300 keV), and
S = 3.2 x 10-6 erg cm-2 (7-400 keV).
Using the latter value and assuming Omega_Lambda = 0.7, Omega_m = 0.3,
and H_0 = 70 km s-1 Mpc-1, the isotropic-equivalent energy of the
burst is
E_iso = 2.06 x 10^(52) ergs.
Using this value of E_iso and equation (1) of Frail et al. (ApJ 562,
L55, 2001) [see also Sari et al. (ApJ 519, L17, 1999)] to estimate the
jet break time, we find
t_j = 1.3 [(1+z)/2.60] (theta_j/0.070)^(8/3) [E_iso/2 x 10^(52) ergs]
x (eta/0.2)^(-1/8) (n/0.1 cm-3)^(-1/8) days.
Analysis of the WXM data for GRB021004 gives the following value for the
fluence of the burst in the WXM energy band:
S = 7.5 x 10-7 erg cm-2 (2-25 keV).
The fluence ratio S(2-25)/S(50-300)= (7.5 x 10-7)/(1.8 x 10-6) = 0.42
implies that GRB021004 is an X-ray rich GRB [log (S_x/S_gamma) > -0.5].
This message is citable.