2021MNRAS.503.3522M


Query : 2021MNRAS.503.3522M

2021MNRAS.503.3522M - Mon. Not. R. Astron. Soc., 503, 3522-3539 (2021/May-3)

Using interstellar clouds to search for Galactic PeVatrons: gamma-ray signatures from supernova remnants.

MITCHELL A.M.W., ROWELL G.P., CELLI S. and EINECKE S.

Abstract (from CDS):

Interstellar clouds can act as target material for hadronic cosmic rays; gamma rays subsequently produced through inelastic proton-proton collisions and spatially associated with such clouds can provide a key indicator of efficient particle acceleration. However, even in the case that particle acceleration proceeds up to PeV energies, the system of accelerator and nearby target material must fulfil a specific set of conditions in order to produce a detectable gamma-ray flux. In this study, we rigorously characterize the necessary properties of both cloud and accelerator. By using available supernova remnant (SNR) and interstellar cloud catalogues, we produce a ranked shortlist of the most promising target systems, those for which a detectable gamma-ray flux is predicted, in the case that particles are accelerated to PeV energies in a nearby SNR. We discuss detection prospects for future facilities including CTA, LHAASO and SWGO; and compare our predictions with known gamma-ray sources. The four interstellar clouds with the brightest predicted fluxes >100 TeV identified by this model are located at (l,b) = (330.05, 0.13), (15.82, -0.46), (271.09, -1.26), and (21.97, -0.29). These clouds are consistently bright under a range of model scenarios, including variation in the diffusion coefficient and particle spectrum. On average, a detectable gamma-ray flux is more likely for more massive clouds; systems with lower separation distance between the SNR and cloud; and for slightly older SNRs.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): ISM: clouds - cosmic rays - ISM: supernova remnants

Errata: erratum vol. 520, p. 300 (2023)

Status at CDS : Examining the need for a new acronym.

Simbad objects: 71

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Number of rows : 71
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 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1235 1
2 FGES J1023.3-5747 gam 10 23 15.18313 -57 46 34.7840           ~ 57 0
3 Cl Westerlund 2 OpC 10 23 58.1 -57 45 49           ~ 356 0
4 V* V906 Car No* 10 36 15.4286177568 -59 35 53.696262804           ~ 89 1
5 SNR G293.8+00.6 SNR 11 35 00 -60 54.0           ~ 35 0
6 SNR G294.1-00.0 SNR 11 36.2 -61 38           ~ 14 0
7 SNR G308.1-00.7 SNR 13 37.6 -63 04           ~ 16 0
8 PSR J1418-6058 Psr 14 18 42.725 -60 58 01.89           ~ 120 0
9 PSR J1420-6048 Psr 14 20 08.190 -60 48 14.85           ~ 196 0
10 NAME Frying Pan SNR 14 38.4 -60 11           ~ 32 0
11 SNR G318.2+00.1 SNR 14 54.8 -59 04           ~ 31 0
12 SNR G320.6-01.6 SNR 15 17.8 -59 16           ~ 15 0
13 SNR G321.9-00.3 SNR 15 20 39.000 -57 33 42.00           ~ 84 0
14 SNR G321.9-01.1 SNR 15 23.7 -58 13           ~ 17 0
15 SNR G327.4+01.0 SNR 15 46.8 -53 20           ~ 22 0
16 SNR G330.2+01.0 SNR 16 01.1 -51 34           ~ 85 1
17 SNR G329.7+00.4 SNR 16 01.3 -52 18           ~ 19 0
18 SNR G332.0+00.2 SNR 16 13.3 -50 53           ~ 47 0
19 PSR J1615-5137 Psr 16 15 12.62 -51 34 53.3           ~ 60 0
20 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 512 3
21 HESS J1634-472 gam 16 34 51.11927 -47 14 01.9360           ~ 28 0
22 SNR G337.8-00.1 SNR 16 39.0 -46 59           ~ 76 0
23 SNR G337.2-00.7 Rad 16 39 15.0 -47 48 27           ~ 62 1
24 AX J1640.7-4632 BL? 16 40 43.2 -46 31 48           ~ 158 2
25 HESS J1641-463 gam 16 41 01.7 -46 18 11           ~ 24 0
26 SNR G338.5+00.1 SNR 16 41 09 -46 19.0           ~ 44 0
27 HESS J1646-458 gam 16 46 00.0 -45 48 00           ~ 12 0
28 SNR G340.4+00.4 SNR 16 46.5 -44 39           ~ 37 0
29 Cl Westerlund 1 Cl* 16 47 02.4 -45 51 07           ~ 566 0
30 SNR G344.7-00.1 SNR 17 03 49 -41 42.5           ~ 87 0
31 SNR G006.4-00.1 SNR 18 00 31.2011719 -23 25 48.001099           ~ 737 1
32 SNR G016.0-00.5 SNR 18 21.9 -15 14           ~ 21 0
33 SNR G016.4-00.5 Rad 18 22.6 -14 55           ~ 18 1
34 eHWC J1825-134 gam 18 25.0 -13 26           ~ 17 0
35 PSR J1826-1256 Psr 18 26 08.570 -12 56 33.53           ~ 131 1
36 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 420 1
37 V* V479 Sct HXB 18 26 15.0561548880 -14 50 54.247274304 12.02 12.23 11.27 11.04   ON6V((f))z 572 2
38 HESS J1828-099 gam 18 28 -09.9           ~ 6 0
39 SNR G018.9-01.1 SNR 18 29.8 -12 58           ~ 62 0
40 SNR G021.0-00.4 SNR 18 31.2 -10 47           ~ 19 0
41 2MASS J18324516-0921545 XB* 18 32 45.162 -09 21 54.55           ~ 27 0
42 SNR G021.5-00.9 SNR 18 33 33.612 -10 34 07.69           ~ 461 1
43 SNR G021.6-00.8 SNR 18 33 36 -10 25.4           ~ 17 0
44 SNR G024.7+00.6 SNR 18 34 46 -07 05.8           ~ 89 0
45 MAGIC J1835-069 ? 18 35.4 -06 56           ~ 3 0
46 PSR J1838-0655 Psr 18 38 03.13 -06 55 33.4           ~ 99 1
47 ARGO J1839-0627 Psr 18 40 55.0 -05 33 00           ~ 59 1
48 ARGO J1841-0332 gam 18 43 56.6 -03 28 16           ~ 30 0
49 SNR G029.6+00.1 Rad 18 44 52 -02 56.5           ~ 56 1
50 4C -00.73 Rad 18 51 46.9 -00 03 19           ~ 100 1
51 HESS J1852-000 gam 18 52 +00.0           ~ 10 0
52 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 964 2
53 PSR J1856+0245 Psr 18 56 50.80 +02 45 50.2           ~ 41 0
54 4FGL J1857.7+0246e Psr 18 57 11.0 +02 40 00           ~ 51 0
55 MAGIC J1857+029 gam 18 57.6 +02 58           ~ 8 0
56 SNR G035.6-00.4 Rad 18 57 55 +02 13.0           ~ 47 1
57 HESS J1858+020 gam 18 58 20.0 +02 05 24           ~ 41 0
58 SNR G036.6-00.7 Rad 19 00.6 +02 56           ~ 44 1
59 eHWC J1907+063 gam 19 07 +06.3           ~ 9 0
60 ARGO J1907+0627 gam 19 08 12.24 +06 23 30.8           ~ 80 0
61 2HWC J1914+117 gam 19 14 42.5 +11 52 20           ~ 6 0
62 PSR J1915+1144 Psr 19 15.0 +11 44           ~ 5 0
63 PSR J1915+1149 Psr 19 15.0 +11 49           ~ 5 0
64 1FGL J1916.0+1110c Q? 19 16 24.000 +11 09 00.00           ~ 54 0
65 HESS J1923+141 gam 19 23.0 +14 06           ~ 13 0
66 SNR G049.1-00.1 SNR 19 23 19.300 +14 09 21.00           ~ 283 0
67 PSR J1928+1746 Psr 19 28 42.8 +17 46 27           ~ 55 0
68 SNR G054.1+00.3 SNR 19 30 10.6 +18 50 22           ~ 238 1
69 SNR G084.2-00.8 SNR 20 53.3 +43 27           ~ 78 0
70 SNR G113.0+00.2 SNR 23 36 35 +61 22.0           ~ 18 0
71 SNR G114.3+00.3 SNR 23 37 05.780 +61 51 01.69           ~ 120 1

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