2011
DOI: 10.1088/0004-637x/729/2/131
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CHANDRAANDRXTEOBSERVATIONS OF 1E 1547.0–5408: COMPARING THE 2008 AND 2009 OUTBURSTS

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Cited by 45 publications
(71 citation statements)
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“…Here and thereafter 1σ c.l uncertainty is reported, unless otherwise specified. These values are consistent with those reported by Kaneko et al (2010) and Ng et al (2011) based on Fermi and RXT E data only, respectively. Time residuals with respect to the timing solution are plotted in Fig.…”
Section: Timing Analysissupporting
confidence: 92%
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“…Here and thereafter 1σ c.l uncertainty is reported, unless otherwise specified. These values are consistent with those reported by Kaneko et al (2010) and Ng et al (2011) based on Fermi and RXT E data only, respectively. Time residuals with respect to the timing solution are plotted in Fig.…”
Section: Timing Analysissupporting
confidence: 92%
“…By includingP component in the fit, we derived a 3σ upper limit of 1.8 × 10 −17 s/s 2 (absolute value). This is smaller then theP component detected during the 2008 outburst Ng et al 2011). The timing solution obtained during 2008 outburst consequently resulted to be more complex then the 2009 timing solution.…”
Section: Timing Analysismentioning
confidence: 78%
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“…However, following the first day, the pulsed fraction was still significantly lower than the preburst pulsed fraction. This anti-correlation between pulsed fraction and flux is presented with the addition of Chandra and XMM-Newton data in Ng et al (2011), who suggest it could be due to an increase in the emitting area of a thermal hot spot, which would cause the emission to be observable during a greater portion of the phase of the pulsar. We note that both correlations (Gotthelf et al 2004;Zhu et al 2008) and anti-correlations (Israel et al 2007;Tam et al 2008) between pulsed fraction and flux have been observed in magnetar outbursts.…”
Section: Persistent Fluxmentioning
confidence: 83%
“…Therefore, in the case of AXPs and SGRs, the spectra provide a handle on the magnetic field strength on the neutron star surface. The magnetic field strengths of numerous sources have been measured by modeling their spectra with strongly magnetic neutron star atmosphere models (Güver et al 2007Özel et al 2008;Gögüş et al 2011;Ng et al 2011;Güver et al 2011). The dipole magnetic field strength B d inferred from their measured rate of spindown using Equation 7 is plotted against the spectroscopic magnetic field strengths B s obtained for these sources in Figure 13.…”
Section: Neutron Star Magnetic Field Geometry and Evolutionmentioning
confidence: 99%