% 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{Karavola:618942,
author = {Karavola, Despina and Petropoulou, M. and Fiorillo, Damiano
Francesco Giuseppe and Comisso, L. and Sironi, L.},
title = {{N}eutrino and pair creation in reconnection-powered
coronae of accreting black holes},
reportid = {PUBDB-2024-07253, arXiv:2410.12638},
year = {2024},
note = {DFGF is supported by the Alexander vonHumboldt Foundation
(Germany)},
abstract = {A ubiquitous feature of accreting black hole systems is
their hard X-ray emission which is thought to be produced
through Comptonization of soft photons by electrons and
positrons in the vicinity of the black hole, in a region
with optical depth of order unity. The origin and
composition of this Comptonizing region, known as the
corona, is a matter open for debate. In this paper we
investigate the role of relativistic protons accelerated in
black-hole magnetospheric current sheets for the pair
enrichment and neutrino emission of AGN coronae. Our model
has two free parameters, namely the proton plasma
magnetization $\sigma_{\rm p}$, which controls the peak
energy of the neutrino spectrum, and the Eddington ratio
$\lambda_{\rm Edd}$ (defined as the ratio between X-ray
luminosity $L_{\rm X}$ and Eddington luminosity $L_{\rm
Edd}$), which controls the amount of energy transferred to
secondary particles. For sources with $\lambda_{\rm Edd}
\gtrsim \lambda_{\rm Edd, crit}$ (where $\lambda_{\rm Edd,
crit} \sim 10^{-1}$ for $\sigma_{\rm p}=10^5$ or $\sim
10^{-2}$ for $\sigma_{\rm p}=10^7$), proton-photon
interactions and $ \gamma \gamma$ annihilation produce
enough secondary pairs to achieve Thomson optical depths
$\tau_{\rm T} \sim 0.1-10$. Additionally, we find that the
neutrino luminosity scales as $L^2_{\rm X}/L_{\rm Edd}$ for
$\lambda_{\rm Edd} \lesssim \lambda_{\rm Edd, crit}$, while
it is proportional to $L_{\rm X}$ for higher $\lambda_{\rm
Edd}$ values. We apply our model to four Seyfert galaxies,
including NGC 1068, and discuss our results in light of
recent IceCube observations.},
cin = {$Z_THAT$},
cid = {$I:(DE-H253)Z_THAT-20210408$},
pnm = {613 - Matter and Radiation from the Universe (POF4-613) /
INTERACTIONS - NBIA INTERACTIONS POSTDOCTORAL PROGRAMME
(847523)},
pid = {G:(DE-HGF)POF4-613 / G:(EU-Grant)847523},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)25},
eprint = {2410.12638},
howpublished = {arXiv:2410.12638},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2410.12638;\%\%$},
url = {https://bib-pubdb1.desy.de/record/618942},
}