% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Fiorillo:456598,
author = {Fiorillo and Vliet, Arjen René van and Morisi, Stefano and
Winter, Walter},
title = {{U}nified thermal model for photohadronic neutrino
production in astrophysical sources},
journal = {Journal of cosmology and astroparticle physics},
volume = {2021},
number = {07},
issn = {1475-7508},
address = {London},
publisher = {IOP},
reportid = {PUBDB-2021-01548, DESY-21-045. arXiv:2103.16577},
pages = {028 (1-38)},
year = {2021},
note = {JCAP 07 (2021) 028. 38 pages, 13 figures; data available at
https://github.com/damianofiorillo/Unified-thermal-model},
abstract = {High-energy astrophysical neutrino fluxes are, for many
applications, modeled as simple power laws as a function of
energy. While this is reasonable in the case of neutrino
production in hadronuclear $pp$ sources, it typically does
not capture the behavior in photohadronic $p\gamma$ sources:
in that case, the neutrino spectrum depends on the
properties of the target photons the cosmic rays collide
with and on possible magnetic-field effects on the secondary
pions and muons. We show that the neutrino production from
known photohadronic sources can be reproduced by a thermal
(black-body) target-photon spectrum if one suitably adjusts
the temperature, thanks to multi-pion production processes.
This allows discussing neutrino production from most known
$p\gamma$ sources, such as gamma-ray bursts, active galactic
nuclei and tidal disruption events, in terms of a few
parameters. We apply this thermal model to study the
sensitivity of different classes of neutrino telescopes to
photohadronic sources: we classify the model parameter space
according to which experiment is most suitable for detection
of a specific source class and demonstrate that different
experiment classes, such as dense arrays, conventional
neutrino telescopes, or radio-detection experiments, cover
different parts of the parameter space. Since the model can
also reproduce the flavor and neutrino-antineutrino
composition, we study the impact on the track-to-shower
ratio and the Glashow resonance.},
keywords = {neutrino: production (INSPIRE) / neutrino: detector
(INSPIRE) / model: thermal (INSPIRE) / neutrino: spectrum
(INSPIRE) / neutrino: flux (INSPIRE) / photon: cosmic
radiation (INSPIRE) / photon hadron (INSPIRE) / magnetic
field: effect (INSPIRE) / gamma ray: burst (INSPIRE) /
neutrino antineutrino (INSPIRE) / temperature (INSPIRE) /
sensitivity (INSPIRE) / black body (INSPIRE) / capture
(INSPIRE) / flavor (INSPIRE) / muon (INSPIRE) / AGN
(INSPIRE)},
cin = {$Z_THAT$},
ddc = {530},
cid = {$I:(DE-H253)Z_THAT-20210408$},
pnm = {613 - Matter and Radiation from the Universe (POF4-613) /
NEUCOS - Neutrinos and the origin of the cosmic rays
(646623)},
pid = {G:(DE-HGF)POF4-613 / G:(EU-Grant)646623},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2103.16577},
howpublished = {arXiv:2103.16577},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2103.16577;\%\%$},
UT = {WOS:000683046300029},
doi = {10.1088/1475-7516/2021/07/028},
url = {https://bib-pubdb1.desy.de/record/456598},
}