P. F. Wyper, B. J. Lynch, C. R. DeVore, P. Kumar, S. K. Antiochos, L. K. S. Daldorff
{"title":"A Model for Flux Rope Formation and Disconnection in Pseudostreamer Coronal Mass Ejections","authors":"P. F. Wyper, B. J. Lynch, C. R. DeVore, P. Kumar, S. K. Antiochos, L. K. S. Daldorff","doi":"arxiv-2409.08126","DOIUrl":null,"url":null,"abstract":"Coronal mass ejections (CMEs) from pseudostreamers represent a significant\nfraction of large-scale eruptions from the Sun. In some cases, these CMEs take\na narrow jet-like form reminiscent of coronal jets; in others, they have a much\nbroader fan-shaped morphology like CMEs from helmet streamers. We present\nresults from a magnetohydrodynamic simulation of a broad pseudostreamer CME.\nThe early evolution of the eruption is initiated through a combination of\nbreakout interchange reconnection at the overlying null point and ideal\ninstability of the flux rope that forms within the pseudostreamer. This stage\nis characterised by a rolling motion and deflection of the flux rope toward the\nbreakout current layer. The stretching out of the strapping field forms a flare\ncurrent sheet below the flux rope; reconnection onset there forms low-lying\nflare arcade loops and the two-ribbon flare footprint. Once the CME flux rope\nbreaches the rising breakout current layer, interchange reconnection with the\nexternal open field disconnects one leg from the Sun. This induces a whip-like\nrotation of the flux rope, generating the unstructured fan shape characteristic\nof pseudostreamer CMEs. Interchange reconnection behind the CME releases\ntorsional Alfv\\'en waves and bursty dense outflows into the solar wind. Our\nresults demonstrate that pseudostreamer CMEs follow the same overall magnetic\nevolution as coronal jets, although they present different morphologies of\ntheir ejecta. We conclude that pseudostreamer CMEs should be considered a class\nof eruptions that are distinct from helmet-streamer CMEs, in agreement with\nprevious observational studies.","PeriodicalId":501068,"journal":{"name":"arXiv - PHYS - Solar and Stellar Astrophysics","volume":"61 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Solar and Stellar Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.08126","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Coronal mass ejections (CMEs) from pseudostreamers represent a significant
fraction of large-scale eruptions from the Sun. In some cases, these CMEs take
a narrow jet-like form reminiscent of coronal jets; in others, they have a much
broader fan-shaped morphology like CMEs from helmet streamers. We present
results from a magnetohydrodynamic simulation of a broad pseudostreamer CME.
The early evolution of the eruption is initiated through a combination of
breakout interchange reconnection at the overlying null point and ideal
instability of the flux rope that forms within the pseudostreamer. This stage
is characterised by a rolling motion and deflection of the flux rope toward the
breakout current layer. The stretching out of the strapping field forms a flare
current sheet below the flux rope; reconnection onset there forms low-lying
flare arcade loops and the two-ribbon flare footprint. Once the CME flux rope
breaches the rising breakout current layer, interchange reconnection with the
external open field disconnects one leg from the Sun. This induces a whip-like
rotation of the flux rope, generating the unstructured fan shape characteristic
of pseudostreamer CMEs. Interchange reconnection behind the CME releases
torsional Alfv\'en waves and bursty dense outflows into the solar wind. Our
results demonstrate that pseudostreamer CMEs follow the same overall magnetic
evolution as coronal jets, although they present different morphologies of
their ejecta. We conclude that pseudostreamer CMEs should be considered a class
of eruptions that are distinct from helmet-streamer CMEs, in agreement with
previous observational studies.