2025A&A...695A..11M


Query : 2025A&A...695A..11M

2025A&A...695A..11M - Astronomy and Astrophysics, volume 695A11 (2025/3-1)

Exploring the capability of the HH 80-81 protostellar jet to accelerate relativistic particles.

MENDEZ-GALLEGO J., LOPEZ-COTO R., DE ONA WILHELMI E., FEDRIANI R., OTERO-SANTOS J. and CANTURK Y.

Abstract (from CDS):

Context. Protostellar jets driven by massive protostars are collimated outflows producing high-speed shocks through dense interstellar medium. Fast shocks can accelerate particles up to relativistic energies via diffusive shock acceleration, producing non-thermal emission that can generate γ-ray photons. HH 80-81 is one of the most powerful collimated protostellar jets in our Galaxy, with non-thermal emission detected in radio, X-ray, and γ-ray bands. Characterizing the γ-ray emission that originates in the accelerated particles of the region is crucial for demonstrating the capability of protostars to accelerate cosmic rays.
Aims. Our goal is to determine the particle distribution that is producing the γ-ray spectrum of HH 80-81 in order to ascertain the leptonic or hadronic origin of the γ-ray emission. We aim to associate the high-energy emission in the region with the HH 80-81 system, characterize its spectrum, and elaborate emission models based on what we expect from the diffusive shock acceleration.
Methods. We use the 15 yr database provided by the Fermi-LAT satellite to study the high-energy emission of the jet, spanning from 300 MeV to 100 GeV. In addition, we perform a source association based on positional arguments. Then, we employ the naima and Gamera softwares to analyze the possible mechanisms that are producing γ-rays, considering the ambient conditions. We perform a radiative fitting and study the nature of the particles behind the γ-ray emission.
Results. By analyzing all the candidates to produce the γ-ray emission that we detect, we conclude that HH 80-81 is the most probable candidate to explain the γ-ray emission in the region. The detected spectrum can be explained by both hadronic and leptonic particle components.

Abstract Copyright: © The Authors 2025

Journal keyword(s): acceleration of particles - radiation mechanisms: non-thermal - cosmic rays - Herbig-Haro objects - gamma rays: stars - ISM: individual objects: HH 80-81

Simbad objects: 25

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Number of rows : 25
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 MMB G192.600-00.048 Y*O 06 12 54.0100 +17 59 23.200           ~ 430 0
2 3FGL J0823.3-4205c gam 08 22 52.3 -42 07 47           ~ 12 0
3 HH 219 HH 08 22 54.044 -42 08 47.19           ~ 9 1
4 IRAS 15254-5621 Y*? 15 29 19.33 -56 31 22.8           ~ 108 0
5 [BHC2016] MM1 cor 17 20 53.415 -35 46 57.88           ~ 121 0
6 MMB G358.931-00.030 SFR 17 43 10.02 -29 51 45.8           ~ 70 0
7 [HMW2016] G011.497-01.485 Mas 18 16 22.128 -19 41 27.39           ~ 4 0
8 PSR J1817-1938 Psr 18 17 06.82 -19 38 36.0           ~ 5 0
9 4FGL J1817.2-1946c gam 18 17 14.9 -19 46 48           ~ 2 0
10 4FGL J1818.1-2000 gam 18 18 07.9 -20 00 58           ~ 6 0
11 NAME HH 80-81 HH 18 19 06 -20 51.4           ~ 236 0
12 HH 80 HH 18 19 06.1 -20 51 49           ~ 104 0
13 HH 81 HH 18 19 06.7 -20 51 06           ~ 93 0
14 2MASS J18191051-2046578 Y*O 18 19 10.5152674584 -20 46 57.813394620   12.61   11.74 10.54 ~ 14 0
15 NAME HH 80-81 IRS HII 18 19 11.8 -20 47 35           ~ 157 0
16 [FCG2011] MM1 cor 18 19 12.114 -20 47 30.61           ~ 31 0
17 2MASS J18191220-2047297 Y*O 18 19 12.21 -20 47 29.7           B1 137 0
18 [FCG2011] MM2 cor 18 19 12.488 -20 47 27.30           ~ 11 0
19 HH 80N HH 18 19 19.74 -20 41 34.9           ~ 41 0
20 2MASS J18192208-2045368 Y*O 18 19 22.0893639600 -20 45 36.908831664           ~ 8 0
21 3FGL J1819.5-2045c gam 18 19 30 -20 46.0           ~ 10 0
22 PMN J1819-2036 Rad 18 19 36.89548117 -20 36 31.5727797           ~ 14 1
23 LDN 291 DNe 18 20.0 -20 59           ~ 24 0
24 Cl* NGC 6618 GBL 2 Y*O 18 20 23.02 -16 11 47.9           ~ 15 0
25 1FGL J1846.8-0233c gam 18 46 55.2 -02 27 08           ~ 18 1

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