2012ApJ...759...58D


Query : 2012ApJ...759...58D

2012ApJ...759...58D - Astrophys. J., 759, 58 (2012/November-1)

Spin evolution of millisecond magnetars with hyperaccreting fallback disks: implications for early afterglows of gamma-ray bursts.

DAI Z.G. and LIU R.-Y.

Abstract (from CDS):

The shallow decay phase or plateau phase of early afterglows of gamma-ray bursts (GRBs), discovered by Swift, is currently understood as being due to energy injection to a relativistic blast wave. One natural scenario for energy injection invokes a millisecond magnetar as the central engine of GRBs because the conventional model of a pulsar predicts a nearly constant magnetic-dipole-radiation luminosity within the spin-down timescale. However, we note that significant brightening occurs in some early afterglows, which apparently conflicts with the above scenario. Here we propose a new model to explain this significant brightening phenomena by considering a hyperaccreting fallback disk around a newborn millisecond magnetar. We show that for typical values of the model parameters, sufficient angular momentum of the accreted matter is transferred to the magnetar and spins it up. It is this spin-up that leads to a dramatic increase of the magnetic-dipole-radiation luminosity with time and thus significant brightening of an early afterglow. Based on this model, we carry out numerical calculations and fit well early afterglows of 12 GRBs assuming sufficiently strong fallback accretion. If the accretion is very weak, our model turns out to be the conventional energy-injection scenario of a pulsar. Therefore, our model can provide a unified explanation for the shallow decay phase, plateaus, and significant brightening of early afterglows.

Abstract Copyright:

Journal keyword(s): accretion, accretion disks - gamma-ray burst: general - magnetic fields - stars: neutron

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 201 0
2 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 151 0
3 GRB 070714B gB 03 51 22.30 +28 17 51.3           ~ 216 1
4 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 147 0
5 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 193 0
6 M 1 SNR 05 34 30.9 +22 00 53           ~ 6193 1
7 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5261 0
8 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 282 0
9 GRB 060510A gB 06 23 27.980 -01 09 46.20 18.19   18.45     ~ 53 0
10 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 74 0
11 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 144 0
12 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 326 0
13 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 258 0
14 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 107 0
15 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 793 0
16 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 156 0
17 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 189 0
18 GRB 080229 gB 15 12 52.31 -14 42 16.2           ~ 64 0
19 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 84 0
20 GRS G000.90 +00.10 Rad 17 47 21.1 -28 08 19           ~ 19 0
21 GRB 060109 gB 18 50 43.650 +31 59 26.40           ~ 50 0
22 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 807 3
23 GRB 070103 gB 23 30 13.750 +26 52 33.70           ~ 66 0

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