2008
DOI: 10.1086/589145
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X‐Ray Observations of Parsec‐scale Tails behind Two Middle‐Aged Pulsars

Abstract: Chandra and XMM-Newton resolved extremely long tails behind two middle-aged pulsars, J1509-5850 and J1740+1000. The tail of PSR J1509-5850 is discernible up to 5.6 from the pulsar, which corresponds to the projected length l ⊥ = 6.5d 4 pc, where d = 4d 4 kpc is the distance to the pulsar. The observed tail flux is 2 × 10 −13 erg s −1 cm −2 in the 0.5-8 keV band. The tail spectrum fits an absorbed power-law (PL) model with the photon index Γ = 2.3 ± 0.2, corresponding to the 0.5-8 keV luminosity of 1 × 10 33 d … Show more

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Cited by 64 publications
(56 citation statements)
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“…The model of Gaensler & Slane (2006) predicts a low-scale termination shock of ∼0 6 fo J2055 (at 600 pc), thus not resolved by XMM-Newton, even in the case of typical ambient densities (0.01 atoms cm −3 ) and pulsar velocities (some hundreds ofkilometers per second). In that case, part of the flux we assign to the pulsar comes instead from the termination shock (Kargaltsev & Pavlov 2008a). Along their main axis, the brightness profiles of both nebulae are consistent with an almost flat behavior, with a sudden decrease at the end.…”
Section: The Nebulaementioning
confidence: 57%
See 1 more Smart Citation
“…The model of Gaensler & Slane (2006) predicts a low-scale termination shock of ∼0 6 fo J2055 (at 600 pc), thus not resolved by XMM-Newton, even in the case of typical ambient densities (0.01 atoms cm −3 ) and pulsar velocities (some hundreds ofkilometers per second). In that case, part of the flux we assign to the pulsar comes instead from the termination shock (Kargaltsev & Pavlov 2008a). Along their main axis, the brightness profiles of both nebulae are consistent with an almost flat behavior, with a sudden decrease at the end.…”
Section: The Nebulaementioning
confidence: 57%
“…If the pulsar moves supersonically, shocked pulsar wind is expected to flow in an elongated region downstream of the termination shock (basically, the cavity in the interstellar medium (ISM)created by the moving neutron star and its wind), confined by ram pressure. X-ray emission is due to synchrotron emission from the wind particles accelerated at the termination shock, which is typically seen (if angular resolution permits) as the brightest portion of the extended structure (see, e.g., Kargaltsev & Pavlov 2008a), as predicted by MHD simulations (Bucciantini 2002; Van der Swaluw 2003;Bucciantini et al 2005). In order to produce a population of high-energy particles, a highly energetic pulsar is required (Ė greater than ∼10 34 ; see, e.g., Kargaltsev & Pavlov 2008b).…”
Section: Introductionmentioning
confidence: 99%
“…Note that this argument is independent of the possible X-ray "tail" of PSR J1740+1000 (Kargaltsev et al 2008), whose orientation could be interpreted as indicating motion parallel to the Galactic plane. In any case, the tail may not be real, because the 64 ks Chandra image of PSR J1740+1000 from 2010 does not clearly show it.…”
Section: Comparison With Psr J1740+1000mentioning
confidence: 82%
“…The pulsar's position is from D' Amico et al (2001). PSR J1509−5850 (see Figure 2): The pulsar is located inside an X-ray (Kargaltsev et al 2008) and radio (Hui & Becker 2007) wind nebula. Weltevrede et al (2009) report the gamma-ray detection of the pulsar.…”
Section: Results: Fermi Pulsarsmentioning
confidence: 99%