Transition of Magnetic Reconnection Regimes in Partially Ionized Plasmas

Fuente: arXiv
Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Wang, Liang, Dong, Chuanfei, Huang, Yi-Min, Yuan, Yue, Li, Xinmin, Zhang, Yang
Format: Preprint
Veröffentlicht: 2026
Schlagworte:
Online-Zugang:
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
_version_ 1866915821663551488
author Wang, Liang
Dong, Chuanfei
Huang, Yi-Min
Yuan, Yue
Li, Xinmin
Zhang, Yang
author_facet Wang, Liang
Dong, Chuanfei
Huang, Yi-Min
Yuan, Yue
Li, Xinmin
Zhang, Yang
contents Magnetic reconnection in partially ionized plasmas plays a crucial role in a wide range of solar, astrophysical, and laboratory environments. While reconnection in such plasmas is commonly characterized by the ion-neutral coupling strength and the ionization fraction $χ=n_{i}/(n_{i}+n_{n})$, most previous studies have focused primarily on the former. A systematic exploration of the ionization fraction, particularly in combination with ion-neutral coupling, is still lacking. This study presents the first systematic scan of the two-dimensional parameter space defined by ion-neutral collisionality and ionization fraction, enabling investigation of the transition from strongly coupled reconnection to faster, decoupled reconnection. To achieve this, we employ a new three-fluid, five-moment numerical model that treats electrons, ions, and neutrals as separate species on an equal footing. We find that in the strongly coupled regime, the reconnection rate is consistent with a $χ^{1/4}$ scaling. As collisionality decreases, the system transitions to a fast, ionization-independent regime. On the other hand, in all simulations, the current sheet thins down to the ion inertial length di, rather than the expanded hybrid scale $d_{i}χ^{-1/2}$ predicted by analytic fluid theories. The identified critical thickness and the resulting onset of fast reconnection agree reasonably well with recent fully kinetic simulations and laboratory experiments. In addition, we show that, over a wide range of coupling strengths, the ion outflow velocities remain Alfvénic, scaling with the appropriate ion or hybrid Alfvén speed, while the hybrid outflow velocity scales as $χ^{1/2}$ when normalized by ion Alfvén speed.
format Preprint
id arxiv_https___arxiv_org_abs_2602_23683
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Transition of Magnetic Reconnection Regimes in Partially Ionized Plasmas
Wang, Liang
Dong, Chuanfei
Huang, Yi-Min
Yuan, Yue
Li, Xinmin
Zhang, Yang
Plasma Physics
Solar and Stellar Astrophysics
Space Physics
Magnetic reconnection in partially ionized plasmas plays a crucial role in a wide range of solar, astrophysical, and laboratory environments. While reconnection in such plasmas is commonly characterized by the ion-neutral coupling strength and the ionization fraction $χ=n_{i}/(n_{i}+n_{n})$, most previous studies have focused primarily on the former. A systematic exploration of the ionization fraction, particularly in combination with ion-neutral coupling, is still lacking. This study presents the first systematic scan of the two-dimensional parameter space defined by ion-neutral collisionality and ionization fraction, enabling investigation of the transition from strongly coupled reconnection to faster, decoupled reconnection. To achieve this, we employ a new three-fluid, five-moment numerical model that treats electrons, ions, and neutrals as separate species on an equal footing. We find that in the strongly coupled regime, the reconnection rate is consistent with a $χ^{1/4}$ scaling. As collisionality decreases, the system transitions to a fast, ionization-independent regime. On the other hand, in all simulations, the current sheet thins down to the ion inertial length di, rather than the expanded hybrid scale $d_{i}χ^{-1/2}$ predicted by analytic fluid theories. The identified critical thickness and the resulting onset of fast reconnection agree reasonably well with recent fully kinetic simulations and laboratory experiments. In addition, we show that, over a wide range of coupling strengths, the ion outflow velocities remain Alfvénic, scaling with the appropriate ion or hybrid Alfvén speed, while the hybrid outflow velocity scales as $χ^{1/2}$ when normalized by ion Alfvén speed.
title Transition of Magnetic Reconnection Regimes in Partially Ionized Plasmas
topic Plasma Physics
Solar and Stellar Astrophysics
Space Physics
url https://arxiv.org/abs/2602.23683