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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Dotani, Tadayasu
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Publications (5/5 displayed)
- 2008In-Orbit Timing Calibration of the Hard X-Ray Detector on Board Suzakucitations
- 2008Low/Hard State Spectra of GRO J1655-40 Observed with Suzaku
- 2008Low/Hard State Spectra of GRO J1655-40 Observed with Suzakucitations
- 2007Suzaku observation of the black hole transient 4U1630-472: discovery of absorption linescitations
- 2006Soft x-ray imager (SXI) onboard the NeXT satellitecitations
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article
Low/Hard State Spectra of GRO J1655-40 Observed with Suzaku
Abstract
The Galactic black-hole binary GROJ1655-40,a source harboring superluminal jets,was observed with Suzaku on 2005 September 22-23. The source was detected over a broad and continuous energy range of 0.7-300keV, with an intensity of ̃50mCrab at 20keV. At a distance of 3.2kpc, the0.7-300keV luminosity was ̃5.2 × 10<SUP>36</SUP> ergs<SUP>-1</SUP> (̃0.7% of the Eddington luminosity for a 6M<SUB>odot</SUB> black hole). The source was in a typical low/hard state, exhibiting a power-lawshaped continuumwith a photon index of ̃1.6. During the observation, the source intensity gradually decreased by 25%at energies above ̃3keV, and by 35% below 2keV.This, together with the soft X-ray spectra taken with the X-ray Imaging Spectrometer (XIS), suggests the presence of an independent soft component that can be represented by emission from a cool (̃0.2keV) disk. The hard X-ray spectra obtained with the Hard X-ray Detector reveal a high-energy spectral cutoff,with an e-folding energy of ̃200keV. The entire 0.7-300keV spectrum cannot be reproduced by a single thermal Comptonization model, even when considering reflection effects. Instead, the spectrum (except the soft excess) can be successfully explained by invoking two thermal-Comptonization components with different y-parameters. In contrast tothe high/soft state spectra of this object, in which narrow iron absorption lines are detectedwithequivalent widths of 60-100eV, the present XIS spectra bear no such features beyond an upper-limit equivalent width of 23eV.