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Energetic particle acceleration and transport with the novel Icarus plus PARADISE model

Husidic Edin; Wijsen Nicolas; Baratashvili Tinatin; Poedts Stefaan; Vainio Rami

Energetic particle acceleration and transport with the novel Icarus plus PARADISE model

Husidic Edin
Wijsen Nicolas
Baratashvili Tinatin
Poedts Stefaan
Vainio Rami
Katso/Avaa
swsc230063.pdf (2.720Mb)
Lataukset: 

EDP Sciences
doi:10.1051/swsc/2024009
URI
https://www.swsc-journal.org/articles/swsc/full_html/2024/01/swsc230063/swsc230063.html
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Julkaisun pysyvä osoite on:
https://urn.fi/URN:NBN:fi-fe2025082786126
Tiivistelmä

With the rise of satellites and mankind’s growing dependence on technology, there is an increasing awareness of space weather phenomena related to high-energy particles. Shock waves driven by coronal mass ejections (CMEs) and corotating interaction regions (CIRs) occasionally act as potent particle accelerators, generating hazardous solar energetic particles (SEPs) that pose risks to satellite electronics and astronauts. Numerical simulation tools capable of modelling and predicting large SEP events are thus highly demanded. We introduce the new Icarus + PARADISE model as an advancement of the previous EUHFORIA + PARADISE model. Icarus, based on the MPI-AMRVAC framework, is a three-dimensional magnetohydrodynamic code that models solar wind configurations from 0.1 au onwards, encompassing transient structures like CMEs or CIRs. Differing from EUHFORIA’s uniform-only grid, Icarus incorporates solution adaptive mesh refinement (AMR) and grid stretching. The particle transport code PARADISE propagates energetic particles as test particles through these solar wind configurations by solving the focused transport equation in a stochastic manner. We validate our new model by reproducing EUHFORIA + PARADISE results. This is done by modelling the acceleration and transport of energetic particles in a synthetic solar wind configuration containing an embedded CIR. Subsequently, we illustrate how the simulation results vary with grid resolution by employing different levels of AMR. The resulting intensity profiles illustrate increased particle acceleration with higher levels of AMR in the shock region, better capturing the effects of the shock.

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