Diffuse neutrino flux from coronal magnetospheric current sheets of accreting black holes
Despina Karavola, Maria Petropoulou, Damiano F. G. Fiorillo, Luca Comisso, Lorenzo Sironi
TL;DR
This study investigates whether protons accelerated in magnetospheric current sheets of accreting black holes can power AGN coronae and contribute to the diffuse high-energy neutrino background. It introduces a photohadronic coronal framework with two key parameters, $σ_p$ and $λ_{X,Edd}$, and derives a population-level neutrino flux by applying spectral templates to a combined AGN catalog. The results show that $σ_p = 10^5$ reproduces the IceCube diffuse neutrino spectrum in both flux and slope, with NGC 1068 as a prominent contributor. This work links coronal magnetization and accretion physics to the high-energy neutrino background and highlights calorimetric effects at high fields as a direction for future work.
Abstract
Non-jetted AGN exhibit hard X-ray emission with a power law spectrum above $\sim$2 keV, which is thought to be produced through Comptonization of soft photons by electrons and positrons (pairs) in the vicinity of the black hole. The origin and composition of this plasma source, known as the corona, is a matter open for debate. Our study focuses on the role of relativistic protons accelerated in black-hole magnetospheric current sheets in the neutrino production of AGN coronae. We present a model that has two free parameters, namely the proton plasma magnetization $σ_{\rm p}$, which controls the peak energy of the neutrino spectrum, and the Eddington ratio $λ_{\rm Edd}$ (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. Furthermore, we combine our coronal model with an AGN population in order to provide a prediction for the diffuse neutrino flux measured on Earth. We compare our results with the observational data by IceCube and we find a satisfactory agreement on both the flux value and the slope of the neutrino distribution when we assume a $σ_{\rm p}$ value of $10^5$ for all the sources in our sample.
