2021A&A...647A..68D


Query : 2021A&A...647A..68D

2021A&A...647A..68D - Astronomy and Astrophysics, volume 647A68-68 (2021/3-1)

Multiwavelength constraints on the unidentified Galactic TeV sources HESS J1427-608, HESS J1458-608, and new VHE γ-ray source candidates.

DEVIN J., RENAUD M., LEMOINE-GOUMARD M. and VASILEIADIS G.

Abstract (from CDS):


Aims. Among the γ-ray sources discovered at high and very-high energies, a large fraction still lack a clear identification. In particular, the H.E.S.S. Galactic Plane Survey (HGPS) revealed 78 TeV sources among which 47 are not clearly associated with a known object. Multiwavelength data can help identify the origin of the very-high energy γ-ray emission, although some bright TeV sources have been detected without clear counterparts. We present a multiwavelength approach to constrain the origin of the emission from unidentified HGPS sources.
Methods. We present a generic pipeline that explores a large database of multiwavelength archival data toward any region in the Galactic plane. Along with a visual inspection of the retrieved multiwavelength observations to search for faint and uncataloged counterparts, we derive a radio spectral index that helps disentangle thermal from nonthermal emission and a mean magnetic field through X-ray and TeV data in case of a leptonic scenario. We also search for a spectral connection between the GeV and the TeV regimes with the Fermi-LAT cataloged sources that may be associated with the unidentified HGPS source. We complete the association procedure with catalogs of known objects (supernova remnants, pulsar wind nebulae, HII regions, etc.) and with the source catalogs from instruments whose data are retrieved.
Results. The method is applied on two unidentified sources, namely HESS J1427-608 and HESS J1458-608, for which the multiwavelength constraints favor the pulsar wind nebula (PWN) scenario. We model their broadband nonthermal spectra in a leptonic scenario with a magnetic field B≤10µG, which is consistent with that obtained from ancient PWNe. We place both sources within the context of the TeV PWN population to estimate the spin-down power and the characteristic age of the putative pulsar. We also shed light on two possibly significant γ-ray excesses in the HGPS: the first is located in the south of the unidentified source HESS J1632-478 and the second is spatially coincident with the synchrotron-emitting supernova remnant G28.6-0.1. The multiwavelength counterparts found toward both γ-ray excesses make these promising candidates for being new very-high energy γ-ray sources.

Abstract Copyright: © J. Devin et al. 2021

Journal keyword(s): gamma rays: ISM - ISM: individual objects: HESS J1427-608 - cosmic rays - radio continuum: ISM - ISM: individual objects: HESS J1458-608 - ISM: supernova remnants

Simbad objects: 35

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Number of rows : 35
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 SNR J052559-660453 SNR 05 26 00.4 -66 05 02     12.71     ~ 456 2
2 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
3 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1314 1
4 NAME Vela X Psr 08 33 08.880 -45 11 24.36           ~ 302 1
5 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
6 PSR J1357-6429 Psr 13 57 02.525 -64 29 29.89           ~ 171 1
7 Suzaku J1427-6051 X 14 27.0 -60 51           ~ 5 1
8 2FGL J1427.6-6048c gam 14 27 14.78 -60 47 56.6           ~ 15 0
9 MGPS J142714-604755 Rad 14 27 14.79 -60 47 55.9           ~ 1 0
10 HESS J1427-608 gam 14 27 52.0 -60 51 00           ~ 25 1
11 MGPS J142755-605038 Rad 14 27 55.0 -60 50 38           ~ 3 0
12 4XMM J142756.7-605214 X 14 27 56.7 -60 52 14           ~ 1 0
13 3FGL J1456.7-6046 gam 14 56 45.1 -60 50 19           ~ 12 0
14 PSR J1459-60 Psr 14 59 30.1228633008 -60 53 20.536602864           ~ 60 0
15 SNR G323.7-01.0 SNR 15 34 30.1 -57 12 03           ~ 25 0
16 4FGL J1533.9-5712e SNR 15 34 43.1982422 -57 09 35.999451           ~ 17 0
17 SNR G336.7+00.5 Rad 16 31 42 -47 20.7           ~ 45 1
18 IGR J16320-4751 HXB 16 32 01.76 -47 52 29.0           BN0.5Ia 188 0
19 PSR J1632-4757 Psr 16 32 16.7704844928 -47 57 33.931138860           ~ 29 0
20 FGES J1633.0-4746 gam 16 33.0 -47 46           ~ 2 0
21 PSR J1633-4805 Psr 16 33 05.4 -48 05 36           ~ 4 0
22 4XMM J163350.4-480707 X 16 33 50.4 -48 07 07           ~ 1 0
23 4XMM J163350.8-480601 X 16 33 50.8 -48 06 01           ~ 1 0
24 HD 148937 SB* 16 33 52.3869185520 -48 06 40.476418740 6.49 7.12 6.71 7.61   O6f?p 417 1
25 4XMM J163353.3-480520 X 16 33 53.3 -48 05 20           ~ 1 0
26 4XMM J163354.9-480659 X 16 33 54.9 -48 06 59           ~ 1 0
27 SNR G347.3-00.5 SNR 17 12 27 -39 41.2     12.27     ~ 761 1
28 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 460 1
29 ARGO J1841-0332 gam 18 43.6 -03 36           ~ 40 0
30 SNR G028.6-00.1 SNR 18 43 55 -03 53.0           ~ 64 1
31 PSR J1844-0346 Psr 18 44 32.90 -03 46 26.6           ~ 45 0
32 SNR G028.78-00.44 SR? 18 45 25 -03 53.6           ~ 8 0
33 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 1034 2
34 SNR G049.1-00.1 SNR 19 23 19.300 +14 09 21.00           ~ 309 0
35 1RXS J194356.1+211731 Bla 19 43 56.24400 +21 18 23.3784           ~ 99 1

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