📝 Original Info
- Title: SWIFT-BAT observations of the recently discovered magnetar SGR 0501+4516
- ArXiv ID: 1004.4036
- Date: 2015-05-18
- Authors: Researchers from original ArXiv paper
📝 Abstract
We present results on the Soft Gamma Repeater (SGR) 0501+4516, discovered by the SWIFT Burst Alert Telescope (BAT) on 2008 August 22. More than 50 bursts were identified from this source, out of which 18 bursts had enough counts to carry out spectral analysis. We performed time-averaged spectral analysis on these 18 bursts using 8 models, among which the cut-off powerlaw and the two-blackbody models provided the best fit in the 15-150 keV energy range. The cut-off powerlaw model fit yields a mean photon index Gamma_{CPL} = 0.54+/-0.11 and a cut-off energy E_C = 19.1+/-1.8 keV for the bursts. The mean hard and soft blackbody temperatures are found to be kT_{BB_h} = 12.8+/-0.7 keV and kT_{BB_s} = 4.6+/-0.5 keV, respectively, and are anti-correlated with the square of the radii of the hard and soft emitting regions (R_{BB_h} and R_{BB_s}) as R_{BB_h}^2 $\propto$ kT^{-5.8} and R_{BB_s}^2 $\propto$ kT^{-2.7}, respectively. The soft and hard component temperatures with different indices support the idea of two distinct emitting regions with the hard component corresponding to a smaller radius and the soft component corresponding to a larger radius, which further corroborate the idea of the propagation of extraordinary (E) and ordinary (O) mode photons across the photosphere, as predicted in the magnetar model. We notice strong burst fluence-duration correlation as well as hardness ratio-duration and hardness ratio-fluence anti-correlations for the SGR 0501+4516 bursts. The burst fluences range from ~ 4.4\times10^{-9} ergs/cm^-2 to ~ 2.7\times10^{-6} ergs/cm^{-2}, consistent with those observed for typical short SGR bursts.
💡 Deep Analysis
Deep Dive into SWIFT-BAT observations of the recently discovered magnetar SGR 0501+4516.
We present results on the Soft Gamma Repeater (SGR) 0501+4516, discovered by the SWIFT Burst Alert Telescope (BAT) on 2008 August 22. More than 50 bursts were identified from this source, out of which 18 bursts had enough counts to carry out spectral analysis. We performed time-averaged spectral analysis on these 18 bursts using 8 models, among which the cut-off powerlaw and the two-blackbody models provided the best fit in the 15-150 keV energy range. The cut-off powerlaw model fit yields a mean photon index Gamma_{CPL} = 0.54+/-0.11 and a cut-off energy E_C = 19.1+/-1.8 keV for the bursts. The mean hard and soft blackbody temperatures are found to be kT_{BB_h} = 12.8+/-0.7 keV and kT_{BB_s} = 4.6+/-0.5 keV, respectively, and are anti-correlated with the square of the radii of the hard and soft emitting regions (R_{BB_h} and R_{BB_s}) as R_{BB_h}^2 $\propto$ kT^{-5.8} and R_{BB_s}^2 $\propto$ kT^{-2.7}, respectively. The soft and hard component temperatures with different indices supp
📄 Full Content
arXiv:1004.4036v1 [astro-ph.HE] 23 Apr 2010
Accepted for publication in the Astrophysical Journal: April 20, 2010
Preprint typeset using LATEX style emulateapj v. 11/10/09
SWIFT-BAT OBSERVATIONS OF THE RECENTLY DISCOVERED MAGNETAR SGR 0501+4516
Harsha S. Kumar1, Alaa. I. Ibrahim2,3 & Samar Safi-Harb1,4
Accepted for publication in the Astrophysical Journal: April 20, 2010
ABSTRACT
We present results on the Soft Gamma Repeater (SGR) 0501+4516, discovered by the Swift Burst
Alert Telescope (BAT) on 2008 August 22. More than 50 bursts were identified from this source, out
of which 18 bursts had enough counts to carry out spectral analysis. We performed time-averaged
spectral analysis on these 18 bursts using 8 models, among which the cut-offpowerlaw and the two-
blackbody models provided the best fit in the 15–150 keV energy range. The cut-offpowerlaw model fit
yields a mean photon index ΓCP L = 0.54±0.11 and a cut-offenergy EC = 19.1±1.8 keV for the bursts.
The mean hard and soft blackbody temperatures are found to be kTBBh = 12.8±0.7 keV and kTBBs
= 4.6±0.5 keV, respectively, and are anti-correlated with the square of the radii of the hard and soft
emitting regions (RBBh and RBBs) as R2
BBh ∝kT −5.8 and R2
BBs ∝kT −2.7, respectively. The soft and
hard component temperatures with different indices support the idea of two distinct emitting regions
with the hard component corresponding to a smaller radius and the soft component corresponding to a
larger radius, which further corroborate the idea of the propagation of extraordinary (E) and ordinary
(O) mode photons across the photosphere, as predicted in the magnetar model. We notice strong
burst fluence–duration correlation as well as hardness ratio–duration and hardness ratio–fluence anti-
correlations for the SGR 0501+4516 bursts. The burst fluences range from ∼4.4×10−9 ergs cm−2 to
∼2.7×10−6 ergs cm−2, consistent with those observed for typical short SGR bursts.
Subject headings: gamma rays: bursts — stars: individual (SGR 0501+4516) — stars: neutron —
X-rays: bursts
1. INTRODUCTION
The Swift mission (Gehrels et al.
2004), launched
in November 2004 to explore the gamma-ray bursts
(GRBs), has provided an excellent opportunity to de-
tect and study the γ-ray activities from known Soft
Gamma Repeaters (SGRs) as well as to discover new
SGRs. SGRs, belonging to the class of ‘magnetars’ (Dun-
can & Thompson 1992), are highly magnetized (B ∼
1014−15 G) and slowly rotating (P ∼2−12 s) neutron
stars characterized by short, bright bursts of hard X-
rays and soft γ-rays (see Mereghetti 2008 for a recent
review). During its active state, an SGR can go through
periods of intense bursting activity lasting from a few
days to months, however, it can also remain dormant for
many years. The bursts, often varying in duration, are
classified into three main categories: short, intermediate
and giant flares. The short bursts are the typical kind
observed during an outburst, marked by timescales ∼
0.1–0.5 s and luminosities ∼1038–1041 ergs s−1, whereas
the intermediate bursts have timescales ∼1–60 s and lu-
minosities ∼1041–1043 ergs s−1 (Mereghetti 2008). Gi-
ant flares, the rare and unique events, are distinguished
by their extreme energies (1044–1047 ergs s−1), long du-
rations (∼hundreds of seconds), and the presence of a
coherent pulsating decaying tail, consistent with the spin
period of the neutron star. Persistent X-ray emission, in-
1 Department
of
Physics
&
Astronomy,
University
of
Manitoba,
Winnipeg,
MB
R3T
2N2,
Canada;
har-
sha@physics.umanitoba.ca
2 Department of Physics,
American University in Cairo;
Faculty of Science, Cairo University, Cairo, Egypt
3 Kavli
Institute
for
Astrophysics
and
Space
Research,
Massachusetts Institute of Technology, Cambridge, MA 02139,
USA; ai@space.mit.edu
4 Canada Research Chair; samar@physics.umanitoba.ca
terpreted as originating due to the magnetospheric cur-
rents driven by twists in the evolving ultra-high magnetic
field (Thompson & Duncan 1995), has also been observed
from SGRs in the 0.1–10 keV band with a typical X-ray
luminosity of ∼1035 ergs s−1, and the spectrum is gen-
erally described by an absorbed powerlaw (PL) plus a
blackbody component (Mereghetti 2008).
According to the magnetar model (Thompson & Dun-
can 1995), the dominant form of energy powering an SGR
is its decaying ultra-strong magnetic field. The surface
of the neutron star is heated and fractured by instabil-
ities generating Alfv´en waves that accelerate electrons,
and in turn give away their energy in short bursts. The
model also suggests that the high-energy dissipated re-
mains trapped in the magnetosphere as the ‘trapped fire-
ball’, and it shrinks in size with time. Alternatively, the
bursts can arise from heating of the corona by magnetic
reconnection in the stellar magnetosphere resulting in
intermediate-type flares (Lyubarsky 2002).
The giant
flares are caused by the sudden rearrangement of the
star’s magnetic field producing global crustal fractures
(Thompson & Duncan 19
…(Full text truncated)…
Reference
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