TY - JOUR
T1 - The X-Ray spectrum of the Vela pulsar resolved with the Chandra X-Ray Observatory
AU - Pavlov, G. G.
AU - Zavlin, V. E.
AU - Sanwal, D.
AU - Burwitz, V.
AU - Garmire, G. P.
N1 - Funding Information:
We are grateful to Leisa Townsley, George Chartas, and Glenn Allen for the useful advice on the analysis of ACIS data. We thank Gottfried Kanbach and Volker Schönfelder for providing the EGRET and COMPTEL fluxes in a digital form. G. G. P., V. E. Z., and D. S. are thankful to the Institute for Theoretical Physics (UCSB), where a part of this work was done. This research was supported by NASA grants NAG5-7017 and NAS8-38252, SAO grant GO1-2071X, NSF grant PHY 99-07949, and DLR grant 50.OO.9501.9.
PY - 2001/5/10
Y1 - 2001/5/10
N2 - We report the results of the spectral analysis of two observations of the Vela pulsar with the Chandra X-Ray Observatory. The spectrum of the pulsar does not show statistically significant spectral lines in the observed 0.25-8.0 keV band. Similar to middle-aged pulsars with detected thermal emission, the spectrum consists of two distinct components. The softer component can be modeled as a magnetic hydrogen atmosphere spectrum - for the pulsar magnetic field B = 3 × 1012 G and neutron star mass M = 1.4 M⊙ and radius R∞ = 13 km, we obtain T∞eff = 0.68 ± 0.03 MK, L∞bol = (2.6 ± 0.2) × 1032 ergs s-1, and d = 210 ± 20 pc (the effective temperature, bolometric luminosity, and radius are as measured by a distant observer). The effective temperature is lower than that predicted by standard neutron star cooling models. A standard blackbody fit gives T∞ = 1.49 ± 0.04 MK, L∞bol = (1.5 ± 0.4) × 1032d2250 ergs s-1 (d250 is the distance in units of 250 pc); the blackbody temperature corresponds to a radius R∞ = (2.1 ± 0.2)d250 km, much smaller than realistic neutron star radii. The harder component can be modeled as a power-law spectrum, with parameters depending on the model adopted for the soft component: γ = 1.5 ± 0.3, Lx = (1.5 ± 0.4) × 1031d2250 ergs s-1 and γ = 2.7 ± 0.4, Lx = (4.2 ± 0.6) × 1031d2250 ergs s-1 for the hydrogen atmosphere and blackbody soft component, respectively (γ is the photon index; Lx is the luminosity in the 0.2-8 keV band). The extrapolation of the power-law component of the former fit toward lower energies matches the optical flux at γ ≃ 1.35-1.45.
AB - We report the results of the spectral analysis of two observations of the Vela pulsar with the Chandra X-Ray Observatory. The spectrum of the pulsar does not show statistically significant spectral lines in the observed 0.25-8.0 keV band. Similar to middle-aged pulsars with detected thermal emission, the spectrum consists of two distinct components. The softer component can be modeled as a magnetic hydrogen atmosphere spectrum - for the pulsar magnetic field B = 3 × 1012 G and neutron star mass M = 1.4 M⊙ and radius R∞ = 13 km, we obtain T∞eff = 0.68 ± 0.03 MK, L∞bol = (2.6 ± 0.2) × 1032 ergs s-1, and d = 210 ± 20 pc (the effective temperature, bolometric luminosity, and radius are as measured by a distant observer). The effective temperature is lower than that predicted by standard neutron star cooling models. A standard blackbody fit gives T∞ = 1.49 ± 0.04 MK, L∞bol = (1.5 ± 0.4) × 1032d2250 ergs s-1 (d250 is the distance in units of 250 pc); the blackbody temperature corresponds to a radius R∞ = (2.1 ± 0.2)d250 km, much smaller than realistic neutron star radii. The harder component can be modeled as a power-law spectrum, with parameters depending on the model adopted for the soft component: γ = 1.5 ± 0.3, Lx = (1.5 ± 0.4) × 1031d2250 ergs s-1 and γ = 2.7 ± 0.4, Lx = (4.2 ± 0.6) × 1031d2250 ergs s-1 for the hydrogen atmosphere and blackbody soft component, respectively (γ is the photon index; Lx is the luminosity in the 0.2-8 keV band). The extrapolation of the power-law component of the former fit toward lower energies matches the optical flux at γ ≃ 1.35-1.45.
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U2 - 10.1086/320342
DO - 10.1086/320342
M3 - Article
AN - SCOPUS:0035592066
SN - 0004-637X
VL - 552
SP - L129-L133
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2 PART 2
ER -