2022ApJ...927L..35D


Query : 2022ApJ...927L..35D

2022ApJ...927L..35D - Astrophys. J., 927, L35-L35 (2022/March-2)

Possible TeV Gamma-Ray Binary Origin of HESS J1828-099.

DE SARKAR A., ROY N., MAJUMDAR P., GUPTA N., BRUNTHALER A., MENTEN K.M., DZIB S.A., MEDINA S.N.X. and WYROWSKI F.

Abstract (from CDS):

The High Energy Stereoscopic System (H.E.S.S.) observatory has carried out a deep survey of the Galactic plane, in the course of which the existence of a significant number of (∼78) TeV γ-ray sources was confirmed, many of which remain unidentified. HESS J1828-099 is a point-like (Gaussian standard deviation < 0.°07) unidentified source among the 17 confirmed point-like sources in the H.E.S.S. Galactic Plane Survey (HGPS) catalog. This source is also unique because it does not seem to have any apparent association with any object detected at other wavelengths. We investigate the nature and association of HESS J1828-099 with multiwavelength observational data. A high-mass X-ray binary (HMXB)-composed of the pulsar XTE J1829-098 and a companion Be star-has been observed earlier in the X-ray and infrared bands, 14' away from HESS J1828-099. With 12 yr of Fermi-LAT γ-ray data, we explore the possibility of 4FGL J1830.2-1005 being the GeV counterpart of HESS J1828-099. Within the RXTE confidence region, a steep-spectrum (αradio = -0.746 ± 0.284) plausible counterpart is detected in data from existing radio frequency surveys. In this Letter, we probe for the first time, using multiwavelength data, whether HESS J1828-099, 4FGL J1830.2-1005, and the HMXB system have a common origin. Our study indicates that HESS J1828-099 might be a TeV high-mass γ-ray binary source.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Galactic radio sources - Massive stars - High mass x-ray binary stars - Gamma-ray sources - High energy astrophysics

Simbad objects: 20

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Number of rows : 20
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 LS I +61 303 HXB 02 40 31.6644419688 +61 13 45.593918580 11.27 11.61 10.75 10.19 9.55 B0Ve 903 2
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
4 HD 259440 HXB 06 32 59.2566076656 +05 48 01.160755848 9.17 9.63 9.15     B0pe 256 0
5 1FGL J1018.6-5856 HXB 10 18 55.5875706288 -58 56 45.975246900   13.638 12.683     O6V((f)) 156 0
6 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
7 2MASS J14051441-6118282 HXB 14 05 14.41560 -61 18 28.2168           O6.5III 53 0
8 V* V479 Sct HXB 18 26 15.0561548880 -14 50 54.247274304 12.02 12.23 11.27 11.04   ON6V((f))z 613 2
9 SNR G020.4+00.1 SNR 18 27.8 -11 00           ~ 25 0
10 HESS J1828-099 gam 18 28 -09.9           ~ 9 0
11 PSR J1828-1007 Psr 18 28 30.36 -10 07 10.1           ~ 6 0
12 2CXO J182943.9-095123 HXB 18 29 44.01 -09 51 23.0           ~ 44 1
13 GLOSTAR G021.684+00.129 SR? 18 30 14.8 -09 56 14           ~ 3 0
14 GLOSTAR G021.492-00.010 SR? 18 30 23.2 -10 10 18           ~ 3 0
15 GLOSTAR G021.861+00.169 SR? 18 30 26.2 -09 45 42           ~ 2 0
16 SNR G021.5-00.1 SNR 18 30.8 -10 09           ~ 20 0
17 GLOSTAR G021.596-00.179 SR? 18 31 11.4 -10 09 28           ~ 2 0
18 2MASS J18324516-0921545 XB* 18 32 45.162 -09 21 54.55           ~ 37 0
19 SNR G022.7-00.2 SNR 18 33 15 -09 13.0           ~ 87 1
20 [MT91] 213 Psr 20 32 13.1247390384 +41 27 24.346666440 13.12 13.08 11.266     B0Vp 334 0

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