2018ApJ...867..120H


Query : 2018ApJ...867..120H

2018ApJ...867..120H - Astrophys. J., 867, 120-120 (2018/November-2)

High-energy and very high energy emission from stellar-mass black holes moving in gaseous clouds.

HIROTANI K., PU H.-Y., OUTMANI S., HUANG H., KIM D., SONG Y., MATSUSHITA S. and KONG A.K.H.

Abstract (from CDS):

We investigate the electron-positron pair cascade taking place in the magnetosphere of a rapidly rotating black hole. Because of the spacetime frame dragging, the Goldreich-Julian charge density changes sign in the vicinity of the event horizon, which leads to the occurrence of a magnetic-field-aligned electric field, in the same way as the pulsar outer-magnetospheric accelerator. In this lepton accelerator, electrons and positrons are accelerated in the opposite directions, to emit copious gamma rays via the curvature and inverse Compton processes. We examine a stationary pair cascade and show that a stellar-mass black hole moving in a gaseous cloud can emit a detectable very high energy flux, provided that the black hole is extremely rotating and that the distance is less than about 1 kpc. We argue that the gamma-ray image will have a point-like morphology, and we demonstrate that their gamma-ray spectra have a broad peak around 0.01-1 GeV and a sharp peak around 0.1 TeV, that the accelerators become most luminous when the mass accretion rate becomes about 0.01% of the Eddington rate, and that the predicted gamma-ray flux changes little in a wide range of magnetospheric currents. An implication of the stability of such a stationary gap is discussed.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): acceleration of particles - gamma rays: stars - magnetic fields - methods: analytical - methods: numerical - stars: black holes

Simbad objects: 16

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Number of rows : 16
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 HESS J1427-608 gam 14 27 52.0 -60 51 00           ~ 22 1
2 SNR G318.2+00.1 SNR 14 54.8 -59 04           ~ 31 0
3 HESS J1626-490 gam 16 26 04.0 -49 05 13           ~ 15 0
4 HESS J1634-472 gam 16 34 51.11927 -47 14 01.9360           ~ 28 0
5 HESS J1641-463 gam 16 41 01.7 -46 18 11           ~ 24 0
6 HESS J1702-420 gam 17 02 44.0 -42 00 57           ~ 42 0
7 HESS J1708-410 gam 17 08 24.0 -41 05 24           ~ 19 0
8 SNR G348.5+00.1 SNR 17 14 31.780 -38 28 34.50           ~ 220 3
9 2CG 359+00 BL? 17 45 11 -30 11.9           ~ 100 0
10 HESS J1800-240B gam 17 57 11 -24 05.5           ~ 27 0
11 HESS J1800-240C gam 17 58 52 -24 03.1           ~ 21 0
12 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 738 1
13 4FGL J1801.8-2358 BL? 18 01 49.1 -23 58 58           ~ 28 0
14 1AGLR J1807-2103 gam 18 03 52.1 -21 10 54           ~ 73 0
15 SNR G023.3-00.3 SNR 18 34 51.80 -08 44 38.2           ~ 218 0
16 ARGO J1839-0627 Psr 18 40 55.0 -05 33 00           ~ 59 1

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