2023A&A...679A..46K


Query : 2023A&A...679A..46K

2023A&A...679A..46K - Astronomy and Astrophysics, volume 679A46 (2023/11-1)

Searching for temporary gamma-ray dark blazars associated with IceCube neutrinos.

KUN E., BARTOS I., BECKER TJUS J., BIERMANN P.L., FRANCKOWIAK A., HALZEN F. and MEZO G.

Abstract (from CDS):

Context. Tensions between the diffuse gamma-ray sky observed by the Fermi Large Area Telescope (Fermi-LAT) and the diffuse, high-energy neutrino sky detected by the IceCube South Pole Neutrino Observatory raise questions about our knowledge of high-energy neutrino sources in the gamma-ray regime. While blazars are among the most energetic persistent particle accelerators in the Universe, studies suggest that they could account for up to 10-30% of the neutrino flux measured by IceCube.
Aims. Our recent results highlight that the associated IceCube neutrinos arrived in a local gamma-ray minimum (dip) of three strong neutrino point-source candidates. Here, we increase the sample of neutrino-source candidates in order to study their gamma-ray light curves.
Methods. We generated the one-year Fermi-LAT light curve for eight neutrino-source candidate blazars (RBS 0958, GB6 J1040+0617, PKS 1313-333, TXS 0506+056, PKS 1454-354, NVSS J042025-374443, PKS 0426-380, and PKS 1502+106), centered on the detection time of the associated IceCube neutrinos. We applied the Bayesian block algorithm to the light curves to characterize their variability.
Results. Our results indicate that GB6 J1040+0617 was in a phase of high gamma-ray activity, while none of the other seven neutrino-source candidates were statistically bright during the detection of the corresponding neutrinos; indeed, most of the time neutrinos arrived in a faint gamma-ray phase of the light curves. This suggests either that the eight source candidate blazars (associated with seven neutrino events) in our reduced sample are not the sources of the corresponding IceCube neutrinos, or that an in-source effect (e.g., the suppression of gamma rays due to high gamma-gamma opacity) complicates the multimessenger scenario of neutrino emission for these blazars.

Abstract Copyright: © The Authors 2023

Journal keyword(s): galaxies: active - gamma rays: galaxies - neutrinos - radio continuum: galaxies

Simbad objects: 37

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Number of rows : 37
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 3HSP J010326.0+152624 BLL 01 03 26.0003786544 +15 26 24.650787336   19.75 18.55 16.4   ~ 46 1
2 QSO J0225+1846 Bla 02 25 04.66884683 +18 46 48.7668666   20.0 20.0 19.09   ~ 122 1
3 4FGL J0230.3+1713 gam 02 30 23.4 +17 13 21           ~ 7 0
4 ICRF J024445.6+132007 Bla 02 44 45.69332807 +13 20 07.2213396           ~ 41 1
5 9Y-MST J0420-3744 BLL 04 20 25.07 -37 44 46.8           ~ 39 1
6 WISEA J042840.41-375619.3 BLL 04 28 40.4241894720 -37 56 19.580735832   18.96 19.0 17.21   ~ 343 1
7 PMN J0509+0541 BLL 05 09 25.9644373872 +05 41 35.333820420 15.32 14.95 14.78 15.12   ~ 589 2
8 SDSS J085410.16+275421.7 BLL 08 54 10.1652947088 +27 54 21.774976884   20.92 20.04 19.7   ~ 33 0
9 RX J0946.3+0104 BLL 09 46 20.2166039496 +01 04 52.099953780   20.92 20.17 19.6   ~ 67 1
10 QSO J0948+0022 Bla 09 48 57.32005819 +00 22 25.5596984   18.85 18.61 18.17   ~ 350 2
11 IceCube-141209A ev 10 40.2 +06 34           ~ 12 0
12 87GB 103758.5+063247 BLL 10 40 31.6262333280 +06 17 21.764932476   20.02 16.8 19.73   ~ 81 1
13 RX J1117.1+2014 BLL 11 17 06.2512673640 +20 14 07.380923028           ~ 159 1
14 3FGL J1232.8+1332 Bla 12 33 02.4 +13 33 22           ~ 12 0
15 2MASS J12584805-0447450 BLL 12 58 48.0460059168 -04 47 45.263736096     20.40 18.9   ~ 38 0
16 NVSS J131143+205209 Rad 13 11 43.68 +20 52 08.5           ~ 5 1
17 4FGL J1311.8+2057 Bz? 13 11 52.0 +20 57 31           ~ 14 0
18 QSO B1313-333 Bla 13 16 07.98594757 -33 38 59.1726741   18.04 20.0 17.23   ~ 267 1
19 QSO B1424-41 Bla 14 27 56.29756617 -42 06 19.4376238   18.48 17.7 16.30   ~ 547 1
20 4FGL J1439.5-2525 Bz? 14 39 31.6 -25 25 12           ~ 20 0
21 NVSS J143934-252458 Rad 14 39 34.77 -25 24 58.0           ~ 3 1
22 4FGL J1447.0-2657 Bz? 14 46 56.8503565804 -26 56 58.313021856           ~ 26 1
23 NVSS J144657-265713 Rad 14 46 57.08 -26 57 13.4           ~ 1 0
24 QSO J1457-3539 BLL 14 57 26.71171449 -35 39 09.9716148   17.95 19.50 18.93   ~ 167 1
25 QSO B1502+1041 Bla 15 04 24.97978391 +10 29 39.1985309   18.97 18.56 18.94   ~ 634 1
26 ICRF J150502.3-343256 BLL 15 05 02.37035128 -34 32 56.8199693       18.8   ~ 63 1
27 QSO B1555+001 Bla 15 57 51.43397121 -00 01 50.4137827   20.10 19.72 18.75   ~ 188 1
28 4FGL J1557.9-0001 AG? 15 57 56.4 -00 01 28           ~ 19 0
29 QSO B1741-038 Bla 17 43 58.85613537 -03 50 04.6167326     20.40 17.98   ~ 583 1
30 ATO J272.0480+35.0218 BLL 18 08 11.5301050080 +35 01 18.674593032           ~ 28 1
31 GB6 B1807+3520 BLL 18 08 49.6978870632 +35 20 42.667697076           ~ 13 1
32 3FGL J1809.0+3517 Bz? 18 09 14.8 +35 09 03           ~ 25 0
33 NVSS J203031+223439 BL? 20 30 31.3616464766 +22 34 38.692931262           ~ 18 0
34 RX J2030.8+1935 BLL 20 30 57.1340134032 +19 36 12.930528420           ~ 59 2
35 NVSS J222752+004446 rG 22 27 43.65 +00 57 30.0           ~ 39 0
36 2MASS J22275812+0037055 BLL 22 27 58.1313623424 +00 37 05.426018868   18.00 17.46 18.5   ~ 35 2
37 4FGL J2351.4-2818 gam 23 51 28.5 -28 18 42           ~ 16 0

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