Transition from Diffusion to Drift-Dominated Cosmic Ray Transport and the Origin of the Knee
Abstract
In a magnetic field with a complex topology, as can be the Galactic magnetic field, cosmic ray transport cannot simply be described by diffusion parallel and perpendicular to magnetic field lines, because the gradients and curvature of the large-scale magnetic field induce drift motions. These effects become especially important at high energies. Here we revisit the possibility that the competition between diffusion and drifts may lead to a knee in the cosmic ray spectrum. We carry out test-particle simulations of cosmic ray transport in a mock Galactic magnetic field made of a regular large scale component, with a non-trivial topology and a homogeneous and isotropic turbulent magnetic field, with a spectrum that is assumed to be Kolmogorov-like in the basic setup. These simulations are used to infer the escape time and the grammage accumulated by cosmic rays with energy in the TeV--10 PeV energy range. In the case of a large scale magnetic field with a purely azimuthal structure, the drift due to the curvature of magnetic field lines produces a knee in the PeV range, but the model fails to reproduce the grammage, due to the exceedingly low value of the perpendicular diffusion coefficient. If the large scale magnetic field acquires a component perpendicular to the Galactic disc, the parallel diffusion coefficient becomes quickly dominant in terms of particle escape, and drifts are unable to compete. A knee structure does not appear in such a scenario. However, if the parallel diffusion coefficient becomes energy independent at E≳ 1 TeV, a knee may arise around PeV energies due to drift dominance. We discuss two cases in which this situation may occur.
Versions
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BibTeX
@misc{castro2026transition,
title = {{Transition from Diffusion to Drift-Dominated Cosmic Ray Transport and the Origin of the Knee}},
author = {Luis Enrique Espinosa Castro and Carmelo Evoli and Pasquale Blasi},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2606.28141},
eprint = {2606.28141},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2606.28141},
}
RIS
TY - UNPB
TI - Transition from Diffusion to Drift-Dominated Cosmic Ray Transport and the Origin of the Knee
AU - Luis Enrique Espinosa Castro
AU - Carmelo Evoli
AU - Pasquale Blasi
PY - 2026
DA - 2026/10/16
PB - arXiv
DO - 10.48550/arxiv.2606.28141
UR - https://arxiv.org/abs/2606.28141
AB - In a magnetic field with a complex topology, as can be the Galactic magnetic field, cosmic ray transport cannot simply be described by diffusion parallel and perpendicular to magnetic field lines, because the gradients and curvature of the large-scale magnetic field induce drift motions. These effects become especially important at high energies. Here we revisit the possibility that the competition between diffusion and drifts may lead to a knee in the cosmic ray spectrum. We carry out test-particle simulations of cosmic ray transport in a mock Galactic magnetic field made of a regular large scale component, with a non-trivial topology and a homogeneous and isotropic turbulent magnetic field, with a spectrum that is assumed to be Kolmogorov-like in the basic setup. These simulations are used to infer the escape time and the grammage accumulated by cosmic rays with energy in the TeV--10 PeV energy range. In the case of a large scale magnetic field with a purely azimuthal structure, the drift due to the curvature of magnetic field lines produces a knee in the PeV range, but the model fails to reproduce the grammage, due to the exceedingly low value of the perpendicular diffusion coefficient. If the large scale magnetic field acquires a component perpendicular to the Galactic disc, the parallel diffusion coefficient becomes quickly dominant in terms of particle escape, and drifts are unable to compete. A knee structure does not appear in such a scenario. However, if the parallel diffusion coefficient becomes energy independent at E≳ 1 TeV, a knee may arise around PeV energies due to drift dominance. We discuss two cases in which this situation may occur.
ER -