TY - JOUR
T1 - XMM-Newton and SUZAKU detection of an X-ray emitting shell around the pulsar wind nebula G54.1+0.3
AU - Bocchino, F.
AU - Bandiera, R.
AU - Gelfand, J.
PY - 2010
Y1 - 2010
N2 - Context. X-ray observations have proven to be very effective in detecting previously unknown supernova remnant shells around pulsar wind nebulae (PWNe), and in these cases the characteristics of the shell provide information about the evolutionary stage of the embedded PWN. However, it is not clear why some PWNe are "naked". Aims. We perform an X-ray observational campaign targeting the PWN G54.1+0.3, the "close cousin" of the Crab Nebula, to try to detect the associated SNR shell. Methods. We analyze XMM-Newton and Suzaku observations of G54.1+0.3 to model the contribution of a dust scattering halo. Results. We detecte an intrinsic faint diffuse X-ray emission surrounding the PWN out to ∼ 6' (∼10 pc) from the pulsar, characterized by a hard spectrum, which can be modeled with either a power law (γ = 2.9) or a thermal plasma model (kT = 2.0 keV.) Conclusions. Assuming the shell to be thermal, we derive an explosion energy E = 0.5-1.6×1051 erg, a pre-shock ISM density of 0.2 cm-3, and an age of ∼2000 yr. Using these results in the MHD model of PWN-SNR evolution, we obtain excellent agreement between the predicted and observed location of the shell and PWN shock.
AB - Context. X-ray observations have proven to be very effective in detecting previously unknown supernova remnant shells around pulsar wind nebulae (PWNe), and in these cases the characteristics of the shell provide information about the evolutionary stage of the embedded PWN. However, it is not clear why some PWNe are "naked". Aims. We perform an X-ray observational campaign targeting the PWN G54.1+0.3, the "close cousin" of the Crab Nebula, to try to detect the associated SNR shell. Methods. We analyze XMM-Newton and Suzaku observations of G54.1+0.3 to model the contribution of a dust scattering halo. Results. We detecte an intrinsic faint diffuse X-ray emission surrounding the PWN out to ∼ 6' (∼10 pc) from the pulsar, characterized by a hard spectrum, which can be modeled with either a power law (γ = 2.9) or a thermal plasma model (kT = 2.0 keV.) Conclusions. Assuming the shell to be thermal, we derive an explosion energy E = 0.5-1.6×1051 erg, a pre-shock ISM density of 0.2 cm-3, and an age of ∼2000 yr. Using these results in the MHD model of PWN-SNR evolution, we obtain excellent agreement between the predicted and observed location of the shell and PWN shock.
KW - ISM: supernova remnants
KW - dust, extinction
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U2 - 10.1051/0004-6361/201014298
DO - 10.1051/0004-6361/201014298
M3 - Article
AN - SCOPUS:77957721008
SN - 0004-6361
VL - 520
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
IS - 10
M1 - A71
ER -