2017
DOI: 10.1093/mnras/stx2241
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Chandra studies of the globular cluster 47 Tucanae: a deeper X-ray source catalogue, five new X-ray counterparts to millisecond radio pulsars and new constraints to r-mode instability window

Abstract: We combined Chandra ACIS observations of the globular cluster 47 Tucanae (hereafter, 47 Tuc) from 2000, 2002, and 2014-15 to create a deeper X-ray source list, and study some of the faint radio millisecond pulsars (MSPs) present in this cluster. We have detected 370 X-ray sources within the half-mass radius (2 .79) of the cluster, 81 of which are newly identified, by including new data and using improved source detection techniques. The majority of the newly identified sources are in the crowded core region, … Show more

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Cited by 53 publications
(70 citation statements)
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References 103 publications
(153 reference statements)
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“…The X-ray spectrum, indeed, could be equally described by a black-body with temperature of 0.8 ± 0.4 keV. It is perfectly consistent with the temperatures of other samples of X-ray pulsars (see, for instance, Bogdanov et al (2006) and Bhattacharya et al (2017) for a spectral analysis of the MSPs of the GC 47 Tucanae).…”
Section: Discussionsupporting
confidence: 83%
See 1 more Smart Citation
“…The X-ray spectrum, indeed, could be equally described by a black-body with temperature of 0.8 ± 0.4 keV. It is perfectly consistent with the temperatures of other samples of X-ray pulsars (see, for instance, Bogdanov et al (2006) and Bhattacharya et al (2017) for a spectral analysis of the MSPs of the GC 47 Tucanae).…”
Section: Discussionsupporting
confidence: 83%
“…Thermal emission is often observed from faint MSPs, where the total power generated is log 10 (L x )=30-32 erg s −1 (Bogdanov et al 2006, Forestell et al 2014, Bhattacharya et al 2017) and the magnetic field is low, typically B 10 9 G (Zavlin et al 1996. The intensity of the magnetic field at the surface of the NS, in the simple case of a magnetic dipole, is given by B surf = 3.2 × 10 19 (P P) 1/2 G (Manchester & Taylor 1977), where P and P are respectively the spin period and the spin-down rate of the NS.…”
Section: Discussionmentioning
confidence: 99%
“…There are two ways to account for the observation of stars within this region: (1) there are additional damping mechanisms that shift the instability curves upwards; (2) although small-amplitude r-modes are unstable inside the Vshaped regions, non-linear mechanisms saturate their amplitude at a low value α sat . Spectral X-ray observations of LMXBs and millisecond pulsars have put a bound on the saturation amplitude α sat 10 −9 − 10 −8 [82,83,84]. This bound is obtained by looking for the heating that would be produced by the dissipation required to saturate the mode.…”
Section: Oscillations and Spin-downmentioning
confidence: 99%
“…This conservative approach allows us to account for all MSPs within 47 Tuc, even those below the detection sensitivity threshold of the Fermi-LAT. In addition, we considered a second scenario where we determined the number of γ-ray bright MSPs by considering Chandra x-ray observations, which have resolved 23 MSPs within 47 Tuc [16,17,19]. The γ-ray flux expected from these 23 x-ray bright MSPs was calculated using the x-ray-to-γ-ray MSP flux ratio of hlogðG 100 =F X Þi ¼ 2.31 derived in the 2PC [3].…”
Section: Interpretation a Millisecond Pulsarsmentioning
confidence: 99%