2016ApJ...826...63L


Query : 2016ApJ...826...63L

2016ApJ...826...63L - Astrophys. J., 826, 63-63 (2016/July-3)

Expectation on observation of supernova remnants with the LHAASO project.

LIU Y., CAO Z., CHEN S., CHEN Y., CUI S., HE H., HUANG X., MA X., YUAN Q. and ZHANG X.

Abstract (from CDS):

Supernova remnants (SNRs) are believed to be the most important acceleration sites for cosmic rays (CRs) below ∼1015 eV in the Galaxy. High-energy photons, either directly from the shocks of the SNRs or indirectly from the interaction between SNRs and the nearby clouds, are crucial probes for the CR acceleration. Big progresses on observations of SNRs have been achieved by space- and ground-based γ-ray facilities. However, whether γ-rays come from accelerated hadrons or not, as well as their connection with the CRs observed at Earth, remains in debate. Large High Altitude Air Shower Observatory (LHAASO), a next-generation experiment, is designed to survey the northern part of the very high energy γ-ray sky from ∼0.3 TeV to PeV with the sensitivity of <=1% of the Crab Nebula flux. In this paper, we indicate that LHAASO will be dedicated to enlarging the γ-ray SNR samples and improving the spectral and morphological measurements. These measurements, especially at energies above 30 TeV, will be important for us to finally understand the CR acceleration in SNRs.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): acceleration of particles - cosmic rays - gamma rays: general

Simbad objects: 33

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Number of rows : 33
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 SN 1572A SN* 00 25 21.5 +64 08 27           B8 1188 1
2 3C 66A BLL 02 22 39.6114771888 +43 02 07.799534304   15.71 15.21 14.5   ~ 887 1
3 IC 443 SNR 06 17 00.0000000 +22 34 11.998901           ~ 1235 1
4 NAME Vela Jr SN BL? 08 52.0 -46 20           ~ 474 2
5 ESO 134-11 HII 14 40 29 -62 38.7           ~ 565 1
6 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1329 1
7 1FGL J1711.7-3944c BL? 17 12 27 -39 41.2     12.27     ~ 723 1
8 SNR G353.6-00.7 SNR 17 31 55.0 -34 42 36           ~ 143 0
9 2MASS J18324516-0921545 XB* 18 32 45.162 -09 21 54.55           ~ 27 0
10 SNR G023.3-00.3 SNR 18 34 51.80 -08 44 38.2           ~ 218 0
11 ARGO J1839-0627 Psr 18 40 55.0 -05 33 00           ~ 59 1
12 SNR G034.6-00.5 SNR 18 56 10.650 +01 13 21.30           ~ 964 2
13 4FGL J1857.7+0246e Psr 18 57 11.0 +02 40 00           ~ 51 0
14 HESS J1858+020 gam 18 58 20.0 +02 05 24           ~ 41 0
15 ARGO J1907+0627 gam 19 08 12.24 +06 23 30.8           ~ 80 0
16 W 49b SNR 19 11 09.000 +09 06 24.00           ~ 463 1
17 ARGO J1912+1026 gam 19 12 14.9 +10 21 06           ~ 45 0
18 PSR J1913+1011 Psr 19 13 20.341 +10 11 22.97           ~ 75 0
19 SNR G049.1-00.1 SNR 19 23 19.300 +14 09 21.00           ~ 283 0
20 W 51a HII 19 23 29.3 +14 31 38           ~ 173 0
21 W 51b SFR 19 23 32.8 +14 29 56           ~ 84 0
22 W 51 SNR 19 23 50 +14 06.0           ~ 1278 1
23 SNR G074.9+01.2 SNR 20 16 02.4 +37 12 48           ~ 182 2
24 ARGO J2021+4038 gam 20 19 00.0 +40 42 00           ~ 32 1
25 2HWC J2019+367 gam 20 19.8 +36 48           ~ 21 0
26 MGRO J2019+37 gam 20 20.1 +36 43           ~ 63 0
27 NAME Cyg X BL? 20 30 04.7973633 +40 51 36.002197           ~ 845 1
28 TeV J2032+4130 gam 20 31.7 +41 31           ~ 136 0
29 NAME Cyg Complex reg 20 32 +45.0           ~ 601 0
30 NAME Cyg Superbubble PoC 20 47 +41.2           ~ 83 1
31 SNR G106.3+02.7 SNR 22 27.5 +60 50           ~ 76 1
32 PSR J2229+6114 Psr 22 29 05.262 +61 14 08.48           ~ 221 2
33 3C 461 BL? 23 23 24.000 +58 48 54.00     14.30     ~ 2792 1

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