2013
DOI: 10.1007/s13538-013-0137-y
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Pulsars and Magnetars

Abstract: The high-energy sources known as anomalous X-ray pulsars (AXPs) and soft γ-ray repeaters (SGRs) are well explained as magnetars: isolated neutron stars powered by their own magnetic energy. After explaining why it is generally believed that the traditional energy sources at work in other neutron stars (accretion, rotation, residual heat) cannot power the emission of AXPs/SGRs, I review the observational properties of the twenty AXPs/SGRs currently known and describe the main features of the magnetar model. In … Show more

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Cited by 36 publications
(42 citation statements)
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References 194 publications
(161 reference statements)
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“…They are commonly called magnetars, because they are thought to have super-strong magnetic fields (10 14 −10 15 G). For recent reviews see Woods & Thompson (2006) and Mereghetti (2008Mereghetti ( , 2013. Two main models have been proposed to explain the observational data; the classical magnetar model (e.g., Thompson & Duncan 1993 and the fallback disk one (Chatterjee et al 2000;Alpar 2001).…”
Section: Introductionmentioning
confidence: 99%
“…They are commonly called magnetars, because they are thought to have super-strong magnetic fields (10 14 −10 15 G). For recent reviews see Woods & Thompson (2006) and Mereghetti (2008Mereghetti ( , 2013. Two main models have been proposed to explain the observational data; the classical magnetar model (e.g., Thompson & Duncan 1993 and the fallback disk one (Chatterjee et al 2000;Alpar 2001).…”
Section: Introductionmentioning
confidence: 99%
“…The NPB can also be important in X-ray superbursts in accreting NSs (e.g. [16]), and in thermal evolution of magnetars [17], as well as in massive cooling white dwarfs.…”
Section: Discussionmentioning
confidence: 99%
“…According to the most popular point of view, anomalous X-ray pulsars (AXPs) and soft gamma repeaters (SGRs) [38][39][40][41][42] are magnetars. For these objects, the estimate (1) most often (although not always) gives B ∼ 10 14 G, but in order to explain their energy balance, magnetic fields reaching up to B ∼ 10 16 -10 17 G in the core at the birth of the star are considered (see [43] and references therein).…”
Section: Magnetic Fieldsmentioning
confidence: 99%
“…Indeed, for a characteristic poloidal component B pol of a neutronstar magnetic field to be stable, a toroidal component B tor must be present, such that, by order of magnitude, B pol B tor 10 16 G B pol /(10 13 G) [47]. Meanwhile, there is increasing evidence for the absence of a clear distinction between AXPs and SGRs [48], as well as between these objects and other neutron stars [41,42,49]. There has even appeared the paradoxical name "a lowfield magnetar," applied to those AXPs and SGRs that have B ≪ 10 14 G (e.g., [50,51], and references therein).…”
Section: Magnetic Fieldsmentioning
confidence: 99%
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