2012ApJ...753..177P


Query : 2012ApJ...753..177P

2012ApJ...753..177P - Astrophys. J., 753, 177 (2012/July-2)

X-ray emission from transient jet model in black hole binaries.

PE'ER A. and MARKOFF S.

Abstract (from CDS):

While the non-thermal radio through at least near-infrared emission in the hard state in X-ray binaries (XRBs) is known to originate in jets, the source of the non-thermal X-ray component is still uncertain. We introduce a new model for this emission, which takes into account the transient nature of outflows, and show that it can explain the observed properties of the X-ray spectrum. Rapid radiative cooling of the electrons naturally accounts for the break often seen below around 10 keV, and for the canonical spectral slope Fν∝ν–1/2 observed below the break. We derive the constraints set by the data for both synchrotron- and Compton-dominated models. We show that for the synchrotron-dominated case, the jet should be launched at radii comparable to the inner radius of the disk (∼few 100 rs for the 2000 outburst of XTE J1118+480), with typical magnetic field B ≳ 106 G. We discuss the consequences of our results for the possible connection between the inflow and outflow in the hard state of XRBs.

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Journal keyword(s): radiation mechanisms: non-thermal - stars: winds, outflows - X-rays: binaries - X-rays: bursts - X-rays: individual: XTE J1118+480

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
2 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
3 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
4 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
5 2CXO J180112.3-254436 HXB 18 01 12.4783119670 -25 44 35.694663099           AV 417 1
6 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0

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