2009ApJ...706L.221Y


Query : 2009ApJ...706L.221Y

2009ApJ...706L.221Y - Astrophys. J., 706, L221-L225 (2009/December-1)

The newly born magnetars powering gamma-ray burst internal-plateau emission: are there strange stars?

YU Y.-W., CAO X.-F. and ZHENG X.-P.

Abstract (from CDS):

The internal-plateau X-ray emission of gamma-ray bursts (GRBs) indicates that a newly born magnetar could be the central object of some GRBs. The observed luminosity and duration of the plateaus suggest that, for such a magnetar, a rapid spin with a sub- or millisecond period is sometimes able to last thousands of seconds. In this case, the conventional neutron star (NS) model for the magnetar may be challenged, since the rapid spin of nascent NSs would be remarkably decelerated within hundreds of seconds due to r-mode instability. In contrast, the r-modes can be effectively suppressed in nascent strange stars (SSs). In other words, to a certain extent, only SSs can keep nearly constant extremely rapid spin for a long period of time during the early ages of the stars. We thus propose that the sample of the GRB rapidly spinning magnetars can be used to test the SS hypothesis based on the distinct spin limits of NSs and SSs.

Abstract Copyright: ∼

Journal keyword(s): gamma rays: bursts - stars: neutron

Simbad objects: 10

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Number of rows : 10
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
2 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
3 GRB 070616 gB 02 08 36.430 +56 56 44.91           ~ 79 0
4 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
5 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 102 0
6 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
7 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
8 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
9 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
10 GRB 071021 gB 22 42 34.33 +23 43 05.4           ~ 104 0

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