2018MNRAS.475.4011B


Query : 2018MNRAS.475.4011B

2018MNRAS.475.4011B - Mon. Not. R. Astron. Soc., 475, 4011-4019 (2018/April-2)

Long-term radio and X-ray evolution of the tidal disruption event ASASSN-14li.

BRIGHT J.S., FENDER R.P., MOTTA S.E., MOOLEY K., PERROTT Y.C., VAN VELZEN S., CAREY S., HICKISH J., RAZAVI-GHODS N., TITTERINGTON D., SCOTT P., GRAINGE K., SCAIFE A., CANTWELL T. and RUMSEY C.

Abstract (from CDS):

We report on late time radio and X-ray observations of the tidal disruption event candidate ASASSN-14li, covering the first 1000 d of the decay phase. For the first ∼200 d the radio and X-ray emission fade in concert. This phase is better fitted by an exponential decay at X-ray wavelengths, while the radio emission is well described by either an exponential or the canonical t–5/3 decay assumed for tidal disruption events. The correlation between radio and X-ray emission during this period can be fitted as L_ R_∝L_ X_^1.9±0.2^. After 400 d the radio emission at 15.5 GHz has reached a plateau level of 244 ± 8 µJy which it maintains for at least the next 600 d, while the X-ray emission continues to fade exponentially. This steady level of radio emission is likely due to relic radio lobes from the weak AGN-like activity implied by historical radio observations. We note that while most existing models are based upon the evolution of ejecta which are decoupled from the central black hole, the radio-X-ray correlation during the declining phase is also consistent with core-jet emission coupled to a radiatively efficient accretion flow.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - black hole physics - galaxies: jets - X-rays: individual: ASASSN-14li

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 - 2026
#notes
1 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
2 XMMSL1 J074008.2-853927 X 07 40 08.2 -85 39 27           ~ 52 0
3 SWIFT J1112.2-8238 X 11 11 47.797 -82 38 44.71           ~ 81 0
4 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
5 ICRF J125531.7+181750 Bla 12 55 31.75992592 +18 17 50.9103856   20.57 19.78 18.85   ~ 46 1
6 IGR J12580+0134 gam 12 58 05.1 +01 34 26           ~ 50 0
7 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
8 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
9 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
10 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
11 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0

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