2019
DOI: 10.1093/mnras/stz1406
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Continued cooling of the accretion-heated neutron star crust in the X-ray transient IGR J17480–2446 located in the globular cluster Terzan 5

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Cited by 15 publications
(14 citation statements)
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“…We therefore hypothesise that the presence of pasta (in an NS with either a cold or a hot core) would not explain the decay and subsequent rise in our observed kT ∞ eff evolution because this would only produce a decay in the cooling curve and no subsequent rise. Cooling-curve modelling including a pasta layer has previously been carried out for several crustcooling sources (MXB 1659−29, MAXI J0556−332, and Terzan 5 X-3;Horowitz et al 2015;Parikh et al 2017;Ootes et al 2019) which showed the expected behaviour we hypothesised for XTE J1701−462 and EXO 0748−676 here.…”
Section: Nuclear Pastasupporting
confidence: 71%
“…We therefore hypothesise that the presence of pasta (in an NS with either a cold or a hot core) would not explain the decay and subsequent rise in our observed kT ∞ eff evolution because this would only produce a decay in the cooling curve and no subsequent rise. Cooling-curve modelling including a pasta layer has previously been carried out for several crustcooling sources (MXB 1659−29, MAXI J0556−332, and Terzan 5 X-3;Horowitz et al 2015;Parikh et al 2017;Ootes et al 2019) which showed the expected behaviour we hypothesised for XTE J1701−462 and EXO 0748−676 here.…”
Section: Nuclear Pastasupporting
confidence: 71%
“…IGR J17480-2446 also displayed a clear evidence of a fast-moving disk wind with ejection velocity up to ∼3000 km s −1 , a rare feature in NSs hosted in LMXB and much more common in systems harboring accreting BHs (Miller et al, 2011). In addition, the source endured an extremely high level of crustal heating during the outburst, which did not seem to have cooled completely even 5.5 years since the end of the outburst (Degenaar et al, 2011(Degenaar et al, , 2013Ootes et al, 2019).…”
Section: Thermonuclear Type-i X-ray Burstsmentioning
confidence: 99%
“…The thermal relaxation of the crust is still not fully understood. In particular, the interpretation of the cooling data requires the existence of some unknown heat sources in the shallow layers of the crust [10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27], as summarized in Table I. In most cases, the extra heat, typically released in the outer crust at densities below about 10 10 g cm −3 , amounts to about 1-2 MeV per accreted nucleon with the notable exceptions of MAXI J0556−332 and Aql X-1.…”
Section: Introductionmentioning
confidence: 99%