First Detection of Plasmoids from Breakout Reconnection on the Sun
Transient collimated plasma ejections (jets) occur frequently throughout the solar corona, in active regions, quiet Sun, and coronal holes. Although magnetic reconnection is generally agreed to be the mechanism of energy release in jets, the factors that dictate the location and rate of reconnection...
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creator | Kumar, Pankaj Karpen, Judith T. Antiochos, Spiro K. Wyper, Peter F. DeVore, C. Richard |
description | Transient collimated plasma ejections (jets) occur frequently throughout the solar corona, in active regions, quiet Sun, and coronal holes. Although magnetic reconnection is generally agreed to be the mechanism of energy release in jets, the factors that dictate the location and rate of reconnection remain unclear. Our previous studies demonstrated that the magnetic breakout model explains the triggering and evolution of most jets over a wide range of scales, through detailed comparisons between our numerical simulations and high-resolution observations. An alternative explanation, the resistive-kink model, invokes breakout reconnection without forming and explosively expelling a flux rope. Here we report direct observations of breakout reconnection and plasmoid formation during two jets in the fan-spine topology of an embedded bipole. For the first time, we observed the formation and evolution of multiple small plasmoids with bidirectional flows associated with fast reconnection in 3D breakout current sheets (BCSs) in the solar corona. The first narrow jet was launched by reconnection at the BCS originating at the deformed 3D null, without significant flare reconnection or a filament eruption. In contrast, the second jet and release of cool filament plasma were triggered by explosive breakout reconnection when the leading edge of the rising flux rope formed by flare reconnection beneath the filament encountered the preexisting BCS. These observations solidly support both reconnection-driven jet models: the resistive kink for the first jet, and the breakout model for the second explosive jet with a filament eruption. |
doi_str_mv | 10.3847/2041-8213/ab45f9 |
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Richard</creator><creatorcontrib>Kumar, Pankaj ; Karpen, Judith T. ; Antiochos, Spiro K. ; Wyper, Peter F. ; DeVore, C. Richard</creatorcontrib><description>Transient collimated plasma ejections (jets) occur frequently throughout the solar corona, in active regions, quiet Sun, and coronal holes. Although magnetic reconnection is generally agreed to be the mechanism of energy release in jets, the factors that dictate the location and rate of reconnection remain unclear. Our previous studies demonstrated that the magnetic breakout model explains the triggering and evolution of most jets over a wide range of scales, through detailed comparisons between our numerical simulations and high-resolution observations. An alternative explanation, the resistive-kink model, invokes breakout reconnection without forming and explosively expelling a flux rope. Here we report direct observations of breakout reconnection and plasmoid formation during two jets in the fan-spine topology of an embedded bipole. For the first time, we observed the formation and evolution of multiple small plasmoids with bidirectional flows associated with fast reconnection in 3D breakout current sheets (BCSs) in the solar corona. The first narrow jet was launched by reconnection at the BCS originating at the deformed 3D null, without significant flare reconnection or a filament eruption. In contrast, the second jet and release of cool filament plasma were triggered by explosive breakout reconnection when the leading edge of the rising flux rope formed by flare reconnection beneath the filament encountered the preexisting BCS. These observations solidly support both reconnection-driven jet models: the resistive kink for the first jet, and the breakout model for the second explosive jet with a filament eruption.</description><identifier>ISSN: 2041-8205</identifier><identifier>ISSN: 2041-8213</identifier><identifier>EISSN: 2041-8213</identifier><identifier>DOI: 10.3847/2041-8213/ab45f9</identifier><language>eng</language><publisher>Austin: The American Astronomical Society</publisher><subject>Collimation ; Computer simulation ; Corona ; Coronal holes ; Current sheets ; Eruptions ; Evolution ; Jets ; Magnetic reconnection ; Mathematical models ; Numerical simulations ; Plasmas (physics) ; Quiet Sun ; Solar corona ; Solar coronal transients ; Solar magnetic bright points ; Solar magnetic fields ; Solar magnetic reconnection ; Spine ; Topology</subject><ispartof>Astrophysical journal. Letters, 2019-11, Vol.885 (1), p.L15</ispartof><rights>2019. The American Astronomical Society. 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Richard</creatorcontrib><title>First Detection of Plasmoids from Breakout Reconnection on the Sun</title><title>Astrophysical journal. Letters</title><addtitle>APJL</addtitle><addtitle>Astrophys. J. Lett</addtitle><description>Transient collimated plasma ejections (jets) occur frequently throughout the solar corona, in active regions, quiet Sun, and coronal holes. Although magnetic reconnection is generally agreed to be the mechanism of energy release in jets, the factors that dictate the location and rate of reconnection remain unclear. Our previous studies demonstrated that the magnetic breakout model explains the triggering and evolution of most jets over a wide range of scales, through detailed comparisons between our numerical simulations and high-resolution observations. An alternative explanation, the resistive-kink model, invokes breakout reconnection without forming and explosively expelling a flux rope. Here we report direct observations of breakout reconnection and plasmoid formation during two jets in the fan-spine topology of an embedded bipole. For the first time, we observed the formation and evolution of multiple small plasmoids with bidirectional flows associated with fast reconnection in 3D breakout current sheets (BCSs) in the solar corona. The first narrow jet was launched by reconnection at the BCS originating at the deformed 3D null, without significant flare reconnection or a filament eruption. In contrast, the second jet and release of cool filament plasma were triggered by explosive breakout reconnection when the leading edge of the rising flux rope formed by flare reconnection beneath the filament encountered the preexisting BCS. These observations solidly support both reconnection-driven jet models: the resistive kink for the first jet, and the breakout model for the second explosive jet with a filament eruption.</description><subject>Collimation</subject><subject>Computer simulation</subject><subject>Corona</subject><subject>Coronal holes</subject><subject>Current sheets</subject><subject>Eruptions</subject><subject>Evolution</subject><subject>Jets</subject><subject>Magnetic reconnection</subject><subject>Mathematical models</subject><subject>Numerical simulations</subject><subject>Plasmas (physics)</subject><subject>Quiet Sun</subject><subject>Solar corona</subject><subject>Solar coronal transients</subject><subject>Solar magnetic bright points</subject><subject>Solar magnetic fields</subject><subject>Solar magnetic reconnection</subject><subject>Spine</subject><subject>Topology</subject><issn>2041-8205</issn><issn>2041-8213</issn><issn>2041-8213</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LxDAQhoMouK7ePQYET9adNEmbHN3VVWFB8eMc0jTFrrtNTdKD_96W6noRTzMMz_sOPAidErikguWzFBhJREroTBeMV3IPTXan_d0O_BAdhbAGSCEjYoLmy9qHiK9ttCbWrsGuwo8bHbauLgOuvNviubf63XURP1njmuaHa3B8s_i5a47RQaU3wZ58zyl6Xd68LO6S1cPt_eJqlRjG8pjkGjJOU1NQwktRWCkK0ETmBoQAlluqtSUlNYUoqBEyp1YLqW1PS2BSA52is7G39e6jsyGqtet8079UKc14JrjIZE_BSBnvQvC2Uq2vt9p_KgJqMKUGFWrQokZTfeRijNSu_e38Bz__A9fteqOE4IqoFeGqLSv6BTFndeQ</recordid><startdate>20191101</startdate><enddate>20191101</enddate><creator>Kumar, Pankaj</creator><creator>Karpen, Judith T.</creator><creator>Antiochos, Spiro K.</creator><creator>Wyper, Peter F.</creator><creator>DeVore, C. Richard</creator><general>The American Astronomical Society</general><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-6289-7341</orcidid><orcidid>https://orcid.org/0000-0002-6442-7818</orcidid><orcidid>https://orcid.org/0000-0002-6975-5642</orcidid><orcidid>https://orcid.org/0000-0003-0176-4312</orcidid><orcidid>https://orcid.org/0000-0002-4668-591X</orcidid></search><sort><creationdate>20191101</creationdate><title>First Detection of Plasmoids from Breakout Reconnection on the Sun</title><author>Kumar, Pankaj ; Karpen, Judith T. ; Antiochos, Spiro K. ; Wyper, Peter F. ; DeVore, C. 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Lett</addtitle><date>2019-11-01</date><risdate>2019</risdate><volume>885</volume><issue>1</issue><spage>L15</spage><pages>L15-</pages><issn>2041-8205</issn><issn>2041-8213</issn><eissn>2041-8213</eissn><abstract>Transient collimated plasma ejections (jets) occur frequently throughout the solar corona, in active regions, quiet Sun, and coronal holes. Although magnetic reconnection is generally agreed to be the mechanism of energy release in jets, the factors that dictate the location and rate of reconnection remain unclear. Our previous studies demonstrated that the magnetic breakout model explains the triggering and evolution of most jets over a wide range of scales, through detailed comparisons between our numerical simulations and high-resolution observations. An alternative explanation, the resistive-kink model, invokes breakout reconnection without forming and explosively expelling a flux rope. Here we report direct observations of breakout reconnection and plasmoid formation during two jets in the fan-spine topology of an embedded bipole. For the first time, we observed the formation and evolution of multiple small plasmoids with bidirectional flows associated with fast reconnection in 3D breakout current sheets (BCSs) in the solar corona. The first narrow jet was launched by reconnection at the BCS originating at the deformed 3D null, without significant flare reconnection or a filament eruption. In contrast, the second jet and release of cool filament plasma were triggered by explosive breakout reconnection when the leading edge of the rising flux rope formed by flare reconnection beneath the filament encountered the preexisting BCS. 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subjects | Collimation Computer simulation Corona Coronal holes Current sheets Eruptions Evolution Jets Magnetic reconnection Mathematical models Numerical simulations Plasmas (physics) Quiet Sun Solar corona Solar coronal transients Solar magnetic bright points Solar magnetic fields Solar magnetic reconnection Spine Topology |
title | First Detection of Plasmoids from Breakout Reconnection on the Sun |
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