Abstract

Cosmic rays are remarkable tracers of solar events when they are associated with solar flares, but also galactic events such as supernova remnants when they come from outside our solar system. Solar Energetic Particles (SEPs) are correlated with the 11-year solar cycle while Galactic Cosmic Rays (GCRs) are anti-correlated due to their interaction with the heliospheric magnetic field and the solar wind. Our aim is to quantify separately the impact of the amplitude and the geometry of the magnetic field, both evolving during the solar cycle, on the propagation of cosmic rays of various energies in the inner heliosphere (within Earth orbit). We focus especially on the diffusion caused by the magnetic field along and across the field lines. To do so, we use the results of 3D magnetohydrodynamics (MHD) wind simulations running from the lower corona up to 1 AU. This gives us the structure of the wind and the corresponding magnetic field. The wind is modeled using a polytropic approximation, and fits and power laws are used to account for the turbulence. Using these results, we compute the parallel and perpendicular diffusion coefficients of the Parker cosmic ray transport equation, yielding 3D maps of the diffusion of cosmic rays in the inner heliosphere. By varying the amplitude of the magnetic field, we change the amplitude of the diffusion by the same factor, and the radial gradients by changing the spread of the current sheet. By varying the geometry of the magnetic field, we change the latitudinal gradients of diffusion by changing the position of the current sheets. By varying the energy, we show that the distribution of values for SEPs is more peaked than GCRs. For realistic solar configurations, we show that diffusion is highly non-axisymmetric due to the configuration of the current sheets, and that the distribution varies a lot with the distance to the Sun with a drift of the peak value. This study shows that numerical simulations, combined with theory, can help quantify better the influence of the various magnetic field parameters on the propagation of cosmic rays. This study is a first step towards the resolution of the complete Parker transport equation to generate synthetic cosmic rays rates from numerical simulations.

Highlights

  • The Sun possesses a magnetic field that shows a cyclic evolution in time: it has a cycle of 11 years in amplitude and 22 years in polarity on average, the shortest cycle observed being of 9 years and the longest one of 14 years (Hathaway, 2015; Brun & Browning, 2017)

  • During a minimum of activity, the solar magnetic field has the lowest amplitude of the cycle and its geometry is mostly dipolar; during a maximum of activity, its amplitude is at its peak and its geometry is mostly quadrupolar (DeRosa et al, 2012)

  • We consider once again particles with rigidities between 1 and 105 MV, which corresponds to energies between 1 keV and 100 GeV. On these histograms, Solar Energetic Particles (SEPs) are located on the left on Galactic Cosmic Rays (GCRs) on the right, separated by a vertical black line at P = 1.69 Â 103 MV

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Summary

Introduction

The Sun possesses a magnetic field that shows a cyclic evolution in time: it has a cycle of 11 years in amplitude and 22 years in polarity on average, the shortest cycle observed being of 9 years and the longest one of 14 years (Hathaway, 2015; Brun & Browning, 2017). Cosmic rays (CRs) are highly energetic extra-terrestrial particles with energies between 102 MeV and 1011 GeV; they follow a power-law distribution, except for the low-energy part of the distribution (Reames, 1999; Heber & Potgieter, 2006) They can be emitted by the Sun during sudden events such as solar flares or coronal mass ejections; in that case they are called Solar Energetic Particles (SEPs) and correspond to the lowenergy part of the distribution (up to 1 GeV).

Model and equations
Wind model
F 2ðvÞksa2
Parametric study
Influence of amplitude
Influence of geometry
Influence of energy
Application to real configurations
Findings
Conclusions
Full Text
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