2016A&A...591A..71M


Query : 2016A&A...591A..71M

2016A&A...591A..71M - Astronomy and Astrophysics, volume 591A71-71 (2016/7-1)

Embedded star clusters as sources of high-energy cosmic rays Modelling and constraints.

MAURIN G., MARCOWITH A., KOMIN N., KRAYZEL F. and LAMANNA G.

Abstract (from CDS):

Context. Massive stars are mainly found in stellar associations. These massive star clusters occur in the heart of giant molecular clouds. The strong stellar wind activity in these objects generates large bubbles and induces collective effects that could accelerate particles up to high energy and produce γ-rays. The best way to input an acceleration origin to the stellar wind interaction in massive stellar cluster is to observe young massive star clusters in which no supernova explosion has occurred yet.
Aims. This work aims to constrain the part of stellar wind mechanical energy that is converted into energetic particles using the sensitivity of the ongoing Fermi-LAT instrument. This work further provides detailed predictions of expected γ-ray fluxes in the view of the on-set of the next generation of imaging atmospheric Cherenkov telescopes.
Methods. A one-zone model where energetic particles are accelerated by repeated interactions with strong supersonic shocks occurring in massive star clusters was developed. The particle escape from the star cluster and subsequent interaction with the surrounding dense material and magnetic fields of the HII region was computed. We applied this model to a selection of eight embedded star clusters constricted by existing observations. We evaluated the γ-ray signal from each object, combining both leptonic and hadronic contributions. We searched for these emissions in the Fermi-LAT observations in the energy range from 3 to 300GeV and compared them to the sensitivity of the Cherenkov Telescope Array (CTA).
Results. No significant γ-ray emission from these star clusters has been found. Less than 10% of stellar wind luminosities are supplied to the relativistic particles. Some clusters even show acceleration efficiency of less than 1%. The CTA would be able to detect γ-ray emission from several clusters in the case of an acceleration efficiency of close to one percent.

Abstract Copyright: © ESO, 2016

Journal keyword(s): acceleration of particles - astroparticle physics - radiation mechanisms: non-thermal - stars: massive - gamma rays: general - HII regions

Simbad objects: 43

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Number of rows : 43
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 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
2 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1708 1
3 M 42 HII 05 35 16.8 -05 23 15           ~ 4411 0
4 NAME 30 Dor C Rad 05 36 07.70 -69 11 52.6           ~ 87 1
5 3FGL J0538.8-0341 gam 05 38 50 -03 41.8           ~ 4 0
6 3FGL J0539.2-0536 Bz? 05 39 45.8 -05 21 20           ~ 14 0
7 3FGL J0605.9+2039c gam 06 05 54 +20 39.2           ~ 4 0
8 3FGL J0609.3+2131 gam 06 09 00.0 +21 36 32           ~ 9 0
9 3FGL J0609.2+2051c gam 06 09 17 +20 51.8           ~ 4 0
10 NGC 2175 OpC 06 09 39 +20 29.2   7.0 6.8     ~ 270 3
11 3FGL J0611.5+1957 gam 06 11 36 +19 57.6           ~ 4 0
12 2FGL J0631.6+0640 Psr 06 31 38 +06 44.5           ~ 12 0
13 NAME Rosette OB Association As* 06 31.7 +04 58           ~ 148 0
14 NGC 2244 OpC 06 32 06.9 +04 54 19           ~ 673 1
15 NAME Rosette Nebula HII 06 32 26.76 +04 47 37.1           ~ 522 1
16 PSR J0633+0632 Psr 06 33 44.136 +06 32 29.48           ~ 93 1
17 3FGL J0634.1+0424 gam 06 34 07 +04 24.4           ~ 10 0
18 NAME MONOCEROS NEB SNR 06 38 43 +06 30.2           ~ 264 0
19 SH 2-305 HII 07 30 04.1 -18 32 13           ~ 55 0
20 1FGL J0731.2-1910c gam 07 31 16 -19 10.1           ~ 14 0
21 NGC 2467 OpC 07 52 18 -26 25.7           ~ 190 1
22 3FGL J0755.2-2633 Bz? 07 55 12 -26 33.7           ~ 6 0
23 PSR J1028-5819 Psr 10 28 27.888 -58 19 06.14           ~ 122 1
24 3FGL J1030.0-5809 Bz? 10 30 02 -58 09.2           ~ 5 0
25 3FGL J1031.4-5855 gam 10 31 27 -58 55.2           ~ 4 0
26 1RXS J103332.0-503539 BLL 10 33 32.1477198726 -50 35 28.942977592           ~ 35 0
27 3FGL J1034.0-5731c gam 10 34 04 -57 31.0           ~ 4 0
28 2FGL J1036.4-5828c gam 10 36 22.6 -58 33 47           ~ 17 0
29 NGC 3324 OpC 10 37 20.8 -58 37 26           ~ 145 1
30 3FGL J1039.1-5809 gam 10 37 50.4 -58 10 58           ~ 12 0
31 3FGL J1040.5-5926c gam 10 40 33 -59 26.0           ~ 4 0
32 3FGL J1043.6-5930 gam 10 43 37 -59 30.3           ~ 6 0
33 3FGL J1043.8-5851 Bz? 10 43 54 -58 51.5           ~ 5 0
34 PSR J1044-5737 Psr 10 44 32.791 -57 37 19.39           ~ 44 0
35 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
36 1FGL J1127.7-6244c gam 11 30 31.7 -62 36 35           ~ 13 0
37 IC 2944 OpC 11 38 20.00 -63 22 22.0           ~ 191 0
38 PSR J1139-6247 Psr 11 39 17.0837402 -62 47 24.566345           ~ 20 0
39 Cl Westerlund 1 OpC 16 47 02.4 -45 51 07           ~ 655 1
40 3FGL J1820.3-1529c gam 18 19 57.6 -15 30 10           ~ 11 0
41 NGC 6618 341 ** 18 20 29.86200 -16 10 44.9328 17.04 16.566 13.922 13.026   O4+O4 63 0
42 NGC 6618 OpC 18 20 47 -16 10.3           ~ 1700 0
43 Ass Cyg OB 2 As* 20 33.2 +41 19           ~ 1023 0

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