2024A&A...689A.147R


Query : 2024A&A...689A.147R

2024A&A...689A.147R - Astronomy and Astrophysics, volume 689A147 (2024/9-1)

The Spectra of IceCube Neutrino (SIN) candidate sources V. Modeling and interpretation of multiwavelength and neutrino data.

RODRIGUES X., KARL M., PADOVANI P., GIOMMI P., PAIANO S., FALOMO R., PETROPOULOU M. and OIKONOMOU F.

Abstract (from CDS):

Context. A correlation has been reported between the arrival directions of high-energy IceCube events and γ-ray blazars classified as intermediate- and high-synchrotron-peaked BL Lacs. Subsequent studies have investigated the optical properties of these sources, compiled and analyzed public multiwavelength data, and constrained their individual neutrino emission based on public IceCube point-source data.
Aims. We provide a theoretical interpretation of public multiwavelength and neutrino point source data for the 32 BL Lac objects in the sample previously associated with an IceCube alert event. We combined the individual source results to draw conclusions regarding the multimesssenger properties of the sample and the required power in relativistic protons.
Methods. We performed particle interaction modeling using open-source numerical simulation software. We constrained the model parameters using a novel and unique approach that simultaneously describes the host galaxy contribution, the observed synchrotron peak properties, the average multiwavelength fluxes, and, where possible, the IceCube point source constraints.
Results. We show that a single-zone leptohadronic model can describe the multiwavelength broadband fluxes from all 32 IceCube candidates. In some cases, the model suggests that hadronic emission may contribute a considerable fraction of the γ-ray flux. The required power in relativistic protons ranges from a few percent to a factor of ten of the Eddington luminosity, which is energetically less demanding compared to other leptohadronic blazar models in recent literature. The model can describe the 68% confidence level IceCube flux for a large fraction of the masquerading BL Lacs in the sample, including TXS 0506+056; whereas, for true BL Lacs, the model predicts a low neutrino flux in the IceCube sensitivity range. Physically, this distinction is due to the presence of photons from broad line emission in masquerading BL Lacs, which increase the efficiency of hadronic interactions. The predicted neutrino flux peaks between a few petaelectronvolt and 100 PeV and scales positively with the flux in the gigaelectronvolt, megaelectronvolt, X-ray, and optical bands. Based on these results, we provide a list of the brightest neutrino emitters, which can be used for future searches targeting the 10-100 PeV regime.

Abstract Copyright: © The Authors 2024

Journal keyword(s): astroparticle physics - neutrinos - radiation mechanisms: non-thermal - galaxies: active - BL Lacertae objects: general - galaxies: jets

Simbad objects: 54

goto Full paper

goto View the references in ADS

Number of rows : 54
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 PMN J0158+0101 BLL 01 58 52.7700514128 +01 01 32.909527020           ~ 44 1
2 9Y-MST J0224+1615 Bla 02 24 16.3 +16 16 00           ~ 24 0
3 ICE2016 16 ev 02 26 +19.1           ~ 10 0
4 RX J0232.8+2017 BLL 02 32 48.6148874688 +20 17 17.486717388     18.00 13.96   ~ 387 1
5 NVSS J023927+132738 BLL 02 39 27.2338101624 +13 27 38.504055421           ~ 33 1
6 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
7 IceCube-161103A ev 02 43.3 +12 34           ~ 12 0
8 ICRF J024445.6+132007 Bla 02 44 45.69332807 +13 20 07.2213396           ~ 41 1
9 IceCube-150831A ev 03 39.4 +33 58           ~ 10 0
10 1RXS J034424.5+343016 BL? 03 44 24.9562591815 +34 30 18.017699047           ~ 19 0
11 PMN J0509+0541 BLL 05 09 25.9644373872 +05 41 35.333820420 15.32 14.95 14.78 15.12   ~ 589 2
12 1RXS J062753.2-152011 Bla 06 27 53.3767394644 -15 19 57.183152008           ~ 20 1
13 IceCube-170321A ev 06 33.3 -14 29           ~ 15 0
14 ICE2013 58 ev 06 48 -32.4           ~ 7 0
15 1RXS J064933.8-313914 BLL 06 49 33.5989252036 -31 39 20.286354937           ~ 45 0
16 SDSS J085410.16+275421.7 BLL 08 54 10.1652947088 +27 54 21.774976884   20.92 20.04 19.7   ~ 33 0
17 ICE2016 32 ev 08 56 +28.0           ~ 11 0
18 RX J0946.3+0104 BLL 09 46 20.2166039496 +01 04 52.099953780   20.92 20.17 19.6   ~ 67 1
19 RX J0955.1+3550 BLL 09 55 07.8818398488 +35 51 00.885435048   21.04 20.36 19.1   ~ 68 0
20 IceCube-200107A ev 09 55 07.90 +35 51 00.9           ~ 30 0
21 IceCube-190819A ev 09 55.2 +01 23           ~ 18 0
22 4FGL J1003.4+0205 BLL 10 03 26.6372116104 +02 04 55.633275840   19.0 19.58 18.9   ~ 28 0
23 IceCube-171015A ev 10 51.4 -15 26           ~ 11 0
24 4FGL J1055.7-1807 gam 10 55 47.7 -18 07 15           ~ 9 0
25 IceCube-130408A ev 11 08.7 +20 40           ~ 10 0
26 RX J1117.1+2014 BLL 11 17 06.2512673640 +20 14 07.380923028           ~ 159 1
27 4FGL J1124.0+2045 BLL 11 24 05.3522345064 +20 45 53.777018484       19.6   ~ 23 0
28 4FGL J1124.9+2143 BLL 11 25 03.6435263400 +21 43 00.120275328       18.1   ~ 22 0
29 SDSS J125821.45+212351.3 BLL 12 58 21.4555723595 +21 23 51.346858831           ~ 24 1
30 2MASS J12584805-0447450 BLL 12 58 48.0460059168 -04 47 45.263736096     20.40 18.9   ~ 38 0
31 4FGL J1300.0+1753 BLL 13 00 08.5217830272 +17 55 38.004634308       19.2   ~ 19 0
32 ICE2016 33 ev 13 10 +19.9           ~ 9 0
33 7C 1312+2404 BLL 13 14 43.8062104200 +23 48 26.782554060 17.15 16.83 16.57 15.4   ~ 99 2
34 ICE2016 17 ev 13 15 +32.0           ~ 14 0
35 4FGL J1321.9+3219 Bz? 13 21 55.2 +32 19 53           ~ 20 0
36 IceCube-181014A ev 15 00.6 -34 48           ~ 11 0
37 3FGL J1507.6-3710 BLL 15 07 20.8116025251 -37 09 03.020415990           ~ 29 1
38 1RXS J152836.5+200423 Bla 15 28 35.7704227448 +20 04 20.131877748           ~ 21 0
39 RX J1533.1+1854 BLL 15 33 11.2518579384 +18 54 29.054401704           ~ 64 0
40 RX J1554.4+2011 BLL 15 54 24.1304763192 +20 11 25.399984632     17.70     ~ 112 1
41 ATO J272.0480+35.0218 BLL 18 08 11.5301050080 +35 01 18.674593032           ~ 28 1
42 ICE2016 13 ev 18 09 +35.5           ~ 11 0
43 GB6 B1807+3520 BLL 18 08 49.6978870632 +35 20 42.667697076           ~ 13 1
44 3FGL J1809.0+3517 Bz? 18 09 14.8 +35 09 03           ~ 25 0
45 NVSS J203031+223439 BL? 20 30 31.3616464766 +22 34 38.692931262           ~ 18 0
46 RX J2030.8+1935 BLL 20 30 57.1340134032 +19 36 12.930528420           ~ 59 2
47 NVSS J213314+252858 BLL 21 33 14.3614671839 +25 28 59.125195032           ~ 37 0
48 ICE2016 30 ev 21 42 +26.1           ~ 9 0
49 SDSS J222329.57+010226.6 BLL 22 23 29.5712726232 +01 02 26.654394588           ~ 46 0
50 IceCube-140114A ev 22 26.8 -45 55           ~ 9 0
51 NVSS J222752+004446 rG 22 27 43.65 +00 57 30.0           ~ 39 0
52 SDSS J232625.63+011208.6 Bz? 23 26 18.0 +01 13 18           ~ 21 0
53 ICRF J232625.6+011208 QSO 23 26 25.64373844 +01 12 08.6936906           ~ 26 1
54 IceCube-160510A ev 23 29.4 +02 05           ~ 11 0

To bookmark this query, right click on this link: simbad:objects in 2024A&A...689A.147R and select 'bookmark this link' or equivalent in the popup menu