2006The Astrophysical JournalOpen access

X‐Ray Emission from the Double Neutron Star Binary B1534+12: Powered by the Pulsar Wind?

Oleg Kargaltsev, George G. Pavlov, G. P. Garmire

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Abstract

We report the detection of the double neutron star binary (DNSB) B1534+12 (=J1537+1155) with the Chandra X-Ray Observatory . This DNSB ( P orb = 10.1 hr) consists of the millisecond (recycled) pulsar J1537+1155A ( P A = 37.9 ms) and a neutron star not detected in the radio. After the remarkable double pulsar binary J0737-3039, it is the only other DNSB detected in X-rays. We measured the flux of (2.2 ± 0.6) × 10 -15 ergs s -1 cm -2 in the 0.3-6 keV band. The small number of collected counts allows only crude estimates of spectral parameters. The power-law fit yields the photon index Γ = 3.2 ± 0.5 and the unabsorbed 0.2-10 keV luminosity L X ≈ 6 × 10 29 ergs s -1 ≈ 3 × 10 -4 Ė A , where Ė A is the spin-down power of J1537+1155A. Alternatively, the spectrum can be fitted by a blackbody model with T ≈ 2.2 MK and the projected emitting area of ~5 × 10 3 m 2 . The distribution of photon arrival times over binary orbital phase shows a deficit of X-ray emission around apastron, which suggests that the emission is caused by interaction of the relativistic wind from J1537+1155A with its neutron star companion. We also reanalyzed the Chandra and XMM-Newton observations of J0737-3039 and found that its X-ray spectrum is similar to the spectrum of B1534+12, and its X-ray luminosity is about the same fraction of Ė A , which suggests similar X-ray emission mechanisms. However, the X-ray emission from J0737-3039 does not show orbital phase dependence. This difference can be explained by the smaller eccentricity of J0737-3039 or a smaller misalignment between the equatorial plane of the millisecond pulsar and the orbital plane of the binary.

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We report the detection of the double neutron star binary (DNSB) B1534+12 (=J1537+1155) with the Chandra X-Ray Observatory . This DNSB ( P orb = 10.1 hr) consists of the millisecond (recycled) pulsar J1537+1155A ( P A = 37.9 ms) and a neutron star not detected in the radio. After the remarkable double pulsar binary J0737-3039, it is the only other DNSB detected in X-rays. We measured the flux of (2.2 ± 0.6) × 10 -15 ergs s -1 cm -2 in the 0.3-6 keV band. The small number of collected counts allows only crude estimates of spectral parameters. The power-law fit yields the photon index Γ = 3.2 ± 0.5 and the unabsorbed 0.2-10 keV luminosity L X ≈ 6 × 10 29 ergs s -1 ≈ 3 × 10 -4 Ė A , where Ė A is the spin-down power of J1537+1155A. Alternatively, the spectrum can be fitted by a blackbody model with T ≈ 2.2 MK and the projected emitting area of ~5 × 10 3 m 2 . The distribution of photon arrival times over binary orbital phase shows a deficit of X-ray emission around apastron, which suggests that the emission is caused by interaction of the relativistic wind from J1537+1155A with its neutron star companion. We also reanalyzed the Chandra and XMM-Newton observations of J0737-3039 and found that its X-ray spectrum is similar to the spectrum of B1534+12, and its X-ray luminosity is about the same fraction of Ė A , which suggests similar X-ray emission mechanisms. However, the X-ray emission from J0737-3039 does not show orbital phase dependence. This difference can be explained by the smaller eccentricity of J0737-3039 or a smaller misalignment between the equatorial plane of the millisecond pulsar and the orbital plane of the binary.

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Available abstract

We report the detection of the double neutron star binary (DNSB) B1534+12 (=J1537+1155) with the Chandra X-Ray Observatory . This DNSB ( P orb = 10.1 hr) consists of the millisecond (recycled) pulsar J1537+1155A ( P A = 37.9 ms) and a neutron star not detected in the radio. After the remarkable double pulsar binary J0737-3039, it is the only other DNSB detected in X-rays. We measured the flux of (2.2 ± 0.6) × 10 -15 ergs s -1 cm -2 in the 0.3-6 keV band. The small number of collected counts allows only crude estimates of spectral parameters. The power-law fit yields the photon index Γ = 3.2 ± 0.5 and the unabsorbed 0.2-10 keV luminosity L X ≈ 6 × 10 29 ergs s -1 ≈ 3 × 10 -4 Ė A , where Ė A is the spin-down power of J1537+1155A. Alternatively, the spectrum can be fitted by a blackbody model with T ≈ 2.2 MK and the projected emitting area of ~5 × 10 3 m 2 . The distribution of photon arrival times over binary orbital phase shows a deficit of X-ray emission around apastron, which suggests that the emission is caused by interaction of the relativistic wind from J1537+1155A with its neutron star companion. We also reanalyzed the Chandra and XMM-Newton observations of J0737-3039 and found that its X-ray spectrum is similar to the spectrum of B1534+12, and its X-ray luminosity is about the same fraction of Ė A , which suggests similar X-ray emission mechanisms. However, the X-ray emission from J0737-3039 does not show orbital phase dependence. This difference can be explained by the smaller eccentricity of J0737-3039 or a smaller misalignment between the equatorial plane of the millisecond pulsar and the orbital plane of the binary.

Key concepts: Physics, Neutron star, Astrophysics, Pulsar, Luminosity, Black-body radiation, X-ray binary, X-ray burster

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