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Miscellaneous :
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Tuerler et al. 2012 ATel 3947:
- Discovery and detection both by JEM-X and ISGRI onboard INTEGRAL
- Combined JEM-X and IBIS/ISGRI spectrum => cut-off power-law (Γ~-0.5, Ecut~4.9 keV)
+ broad Gaussian absorption line at ~20.8 keV
- If absorption line = cyclotron scattering => source is a high mass X-ray binary pulsar
with B~1.7e12 G
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Halpern 2012: ATel 3949
- Swift XRT observation=>strong signal in the periodogram at 11.82s
- Pulse fraction of 27%.
- Interpreted as the signature of a HMXB with pulsar
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Li et al. 2012: ATel 3950
- Swift XRT observation=>refined X-ray position (after correction for pile up)
- Spectra (2 Swift observations) => absorbed power law with NH,1=11.0 x 1022 cm-2 and NH,2=15.1 x 1022cm-2
Γ1=0.4 and Γ2=0.7
- 3-10 keV fluxes compatible with JEMX detection
- 2MASS J18175218-1621316 (RA =274.467438 dec=-16.358791) is a Ks=11.4 IR counterpart
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Finger et al. 2012: ATel 3961
- Detection of 11.82s pulsations with Fermi/GBM
- Pulsations detected at 84.5896 mHz (84.5908 mHz) with rms amplitude 5.9 mCrab (8.5 mCrab) in data of Feb. 20-23 (Feb. 24-27)
2012.
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Paizis et al. 2012: ATel 3988
- Chandra refined position
- 2MASS has Ks=13.136 and is confirmed as the IR counterpart
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Li et al. 2012 (MNRAS) and Bozzo et al.2012 (A&A):
- Swift and INTEGRAL observations
- Confirm the detection of a 11.82s pulsation, with a pulse fraction of 22%
- Presence of an absorption feature at 21.5 keV in addition
to an absorbed (NH=12.3 x1022 cm-2) cutoff power law (Γ=0.59, Ecut =9.97 keV)
- Absorption line, ifattributed to a cyclotron resonant scattering feature, => B~2.4e12 G
- Source is an accreting pulsar.
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Nowak et al. 2012 (ApJ):
- Chandra and NIR observations
- NIR observations => source compatible with 2MASS source, with Ks=13.14, Hn=16.0 and Jn> 18
- No variability in NIR source when comparing to previous (eg UKIDSS) measurements at time of no
X-ray emission
- Strong periodic signal at 11.82s confirming pulsating nature of the source
- Quasi simultaneous Chandra+Swift spectra => absorbed power law (NH2.2 x
1023 cm-2, Γ=0.4)
- LMXB nature unlikely, and an HMXB is preferred although the source is unusual in many ways
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