2013ApJ...768L..35R


Query : 2013ApJ...768L..35R

2013ApJ...768L..35R - Astrophys. J., 768, L35 (2013/May-2)

An evolving compact jet in the black hole X-ray binary MAXI J1836-194.

RUSSELL D.M., RUSSELL T.D., MILLER-JONES J.C.A., O'BRIEN K., SORIA R., SIVAKOFF G.R., SLAVEN-BLAIR T., LEWIS F., MARKOFF S., HOMAN J., ALTAMIRANO D., CURRAN P.A., RUPEN M.P., BELLONI T.M., CADOLLE BEL M., CASELLA P., CORBEL S., DHAWAN V., FENDER R.P., GALLO E., GANDHI P., HEINZ S., KORDING E.G., KRIMM H.A., MAITRA D., MIGLIARI S., REMILLARD R.A., SARAZIN C.L., SHAHBAZ T. and TUDOSE V.

Abstract (from CDS):

We report striking changes in the broadband spectrum of the compact jet of the black hole transient MAXI J1836-194 over state transitions during its discovery outburst in 2011. A fading of the optical-infrared (IR) flux occurred as the source entered the hard-intermediate state, followed by a brightening as it returned to the hard state. The optical-IR spectrum was consistent with a power law from optically thin synchrotron emission, except when the X-ray spectrum was softest. By fitting the radio to optical spectra with a broken power law, we constrain the frequency and flux of the optically thick/thin break in the jet synchrotron spectrum. The break gradually shifted to higher frequencies as the source hardened at X-ray energies, from ∼1011 to ∼4x1013 Hz. The radiative jet luminosity integrated over the spectrum appeared to be greatest when the source entered the hard state during the outburst decay (although this is dependent on the high-energy cooling break, which is not seen directly), even though the radio flux was fading at the time. The physical process responsible for suppressing and reactivating the jet (neither of which are instantaneous but occur on timescales of weeks) is uncertain, but could arise from the varying inner accretion disk radius regulating the fraction of accreting matter that is channeled into the jet. This provides an unprecedented insight into the connection between inflow and outflow, and has implications for the conditions required for jets to be produced, and hence their launching process.

Abstract Copyright:

Journal keyword(s): accretion, accretion disks - black hole physics - ISM: jets and outflows - X-rays: binaries

Simbad objects: 11

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Number of rows : 11
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184 13.00 13.50 13.2     M4.5V 651 1
2 M 1 SNR 05 34 30.9 +22 00 53           ~ 6193 1
3 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 822 0
4 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
5 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2079 0
6 QSO J1820-2528 QSO 18 20 57.84869964 -25 28 12.5840414   18.56       ~ 105 0
7 MAXI J1836-194 XB* 18 35 43.440 -19 19 10.48           ~ 143 0
8 QSO B1908-202 QSO 19 11 09.65289294 -20 06 55.1090664   18.21   18.14   ~ 282 0
9 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 868 0
10 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4337 0
11 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 2848 2

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