The Radial Distribution of Ion-scale Waves in the Inner Heliosphere
Determining the mechanism responsible for plasma heating and particle acceleration is a fundamental problem in the study of the heliosphere. Due to efficient wave–particle interactions of ion-scale waves with charged particles, these waves are widely believed to be a major contributor to ion energiz...
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description | Determining the mechanism responsible for plasma heating and particle acceleration is a fundamental problem in the study of the heliosphere. Due to efficient wave–particle interactions of ion-scale waves with charged particles, these waves are widely believed to be a major contributor to ion energization, and their contribution considerably depends on the wave occurrence rate. By analyzing the radial distribution of quasi-monochromatic ion-scale waves observed by the Parker Solar Probe, this work shows that the wave occurrence rate is significantly enhanced in the near-Sun solar wind, specifically 21%–29% below 0.3 au, in comparison to 6%–14% beyond 0.3 au. The radial decrease of the wave occurrence rate is not only induced by the sampling effect of a single spacecraft detection, but also by the physics relating to the wave excitation, such as the enhanced ion beam instability in the near-Sun solar wind. This work also shows that the wave normal angle
θ
, the absolute value of ellipticity
ϵ
, the wave frequency
f
normalized by the proton cyclotron frequency
f
cp
, and the wave amplitude
δ
B
normalized by the local background magnetic field
B
0
slightly vary with the radial distance. The median values of
θ
, ∣
ϵ
∣,
f
, and
δ
B
are about 9°, 0.73, 3
f
cp
, and 0.01
B
0
, respectively. Furthermore, this study proposes that the wave mode natures of the observed left-handed and right-handed polarized waves correspond to the Alfvén ion cyclotron mode wave and the fast magnetosonic whistler mode wave, respectively. |
doi_str_mv | 10.3847/1538-4357/acd53b |
format | Article |
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θ
, the absolute value of ellipticity
ϵ
, the wave frequency
f
normalized by the proton cyclotron frequency
f
cp
, and the wave amplitude
δ
B
normalized by the local background magnetic field
B
0
slightly vary with the radial distance. The median values of
θ
, ∣
ϵ
∣,
f
, and
δ
B
are about 9°, 0.73, 3
f
cp
, and 0.01
B
0
, respectively. Furthermore, this study proposes that the wave mode natures of the observed left-handed and right-handed polarized waves correspond to the Alfvén ion cyclotron mode wave and the fast magnetosonic whistler mode wave, respectively.</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.3847/1538-4357/acd53b</identifier><language>eng</language><publisher>Philadelphia: The American Astronomical Society</publisher><subject>Astrophysics ; Charged particles ; Cyclotron frequency ; Cyclotrons ; Ellipticity ; Heliosphere ; Ion beams ; Ions ; Magnetic fields ; Particle acceleration ; Particle interactions ; Plasma heating ; Plasma physics ; Radial distribution ; Solar probes ; Solar wind ; Space plasmas ; Spacecraft ; Wave excitation ; Waves</subject><ispartof>The Astrophysical journal, 2023-07, Vol.951 (1), p.69</ispartof><rights>2023. The Author(s). Published by the American Astronomical Society.</rights><rights>2023. The Author(s). Published by the American Astronomical Society. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c416t-54b3ce5593e7506f263144fa37378ed71b2148b21e0152b0bd2efb26c2b7fc9b3</citedby><cites>FETCH-LOGICAL-c416t-54b3ce5593e7506f263144fa37378ed71b2148b21e0152b0bd2efb26c2b7fc9b3</cites><orcidid>0000-0001-6519-8706 ; 0000-0003-2418-5508 ; 0000-0002-9166-1036 ; 0000-0002-1989-3596 ; 0000-0002-7077-930X ; 0000-0002-3859-6394 ; 0000-0003-3072-6139 ; 0000-0002-8376-7842</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.3847/1538-4357/acd53b/pdf$$EPDF$$P50$$Giop$$Hfree_for_read</linktopdf><link.rule.ids>314,776,780,860,2096,27901,27902,38867,53842</link.rule.ids></links><search><creatorcontrib>Liu, Wen</creatorcontrib><creatorcontrib>Zhao, Jinsong</creatorcontrib><creatorcontrib>Wang, Tieyan</creatorcontrib><creatorcontrib>Dong, Xiangcheng</creatorcontrib><creatorcontrib>Kasper, Justin C.</creatorcontrib><creatorcontrib>Bale, Stuart D.</creatorcontrib><creatorcontrib>Shi, Chen</creatorcontrib><creatorcontrib>Wu, Dejin</creatorcontrib><title>The Radial Distribution of Ion-scale Waves in the Inner Heliosphere</title><title>The Astrophysical journal</title><addtitle>APJ</addtitle><addtitle>Astrophys. J</addtitle><description>Determining the mechanism responsible for plasma heating and particle acceleration is a fundamental problem in the study of the heliosphere. Due to efficient wave–particle interactions of ion-scale waves with charged particles, these waves are widely believed to be a major contributor to ion energization, and their contribution considerably depends on the wave occurrence rate. By analyzing the radial distribution of quasi-monochromatic ion-scale waves observed by the Parker Solar Probe, this work shows that the wave occurrence rate is significantly enhanced in the near-Sun solar wind, specifically 21%–29% below 0.3 au, in comparison to 6%–14% beyond 0.3 au. The radial decrease of the wave occurrence rate is not only induced by the sampling effect of a single spacecraft detection, but also by the physics relating to the wave excitation, such as the enhanced ion beam instability in the near-Sun solar wind. This work also shows that the wave normal angle
θ
, the absolute value of ellipticity
ϵ
, the wave frequency
f
normalized by the proton cyclotron frequency
f
cp
, and the wave amplitude
δ
B
normalized by the local background magnetic field
B
0
slightly vary with the radial distance. The median values of
θ
, ∣
ϵ
∣,
f
, and
δ
B
are about 9°, 0.73, 3
f
cp
, and 0.01
B
0
, respectively. Furthermore, this study proposes that the wave mode natures of the observed left-handed and right-handed polarized waves correspond to the Alfvén ion cyclotron mode wave and the fast magnetosonic whistler mode wave, respectively.</description><subject>Astrophysics</subject><subject>Charged particles</subject><subject>Cyclotron frequency</subject><subject>Cyclotrons</subject><subject>Ellipticity</subject><subject>Heliosphere</subject><subject>Ion beams</subject><subject>Ions</subject><subject>Magnetic fields</subject><subject>Particle acceleration</subject><subject>Particle interactions</subject><subject>Plasma heating</subject><subject>Plasma physics</subject><subject>Radial distribution</subject><subject>Solar probes</subject><subject>Solar wind</subject><subject>Space plasmas</subject><subject>Spacecraft</subject><subject>Wave excitation</subject><subject>Waves</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><sourceid>DOA</sourceid><recordid>eNp1kElLBDEQhYMoOC53jw1ebU1nz1HGbUAQRNFbyFKtGdrOmPQI_nt7bNGTlyrq8epV8SF01OBTqpg8azhVNaNcnlkfOHVbaPYrbaMZxpjVgsrnXbRXynIzEq1naP7wCtW9DdF21UUsQ45uPcTUV6mtFqmvi7cdVE_2A0oV-2oY3Yu-h1zdQBdTWb1ChgO009quwOFP30ePV5cP85v69u56MT-_rT1rxFBz5qgHzjUFybFoiaANY62lkkoFQTaONEyNBXDDicMuEGgdEZ442Xrt6D5aTLkh2aVZ5fhm86dJNppvIeUXY_MQfQdGBcs9YUppFRgToGkbgsUahHbCCTpmHU9Zq5ze11AGs0zr3I_vG6IoJVRzqUcXnlw-p1IytL9XG2w22M2GsdkwNhP2ceVkWolp9Zf5r_0L-SCCEA</recordid><startdate>20230701</startdate><enddate>20230701</enddate><creator>Liu, Wen</creator><creator>Zhao, Jinsong</creator><creator>Wang, Tieyan</creator><creator>Dong, Xiangcheng</creator><creator>Kasper, Justin C.</creator><creator>Bale, Stuart D.</creator><creator>Shi, Chen</creator><creator>Wu, Dejin</creator><general>The American Astronomical Society</general><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0001-6519-8706</orcidid><orcidid>https://orcid.org/0000-0003-2418-5508</orcidid><orcidid>https://orcid.org/0000-0002-9166-1036</orcidid><orcidid>https://orcid.org/0000-0002-1989-3596</orcidid><orcidid>https://orcid.org/0000-0002-7077-930X</orcidid><orcidid>https://orcid.org/0000-0002-3859-6394</orcidid><orcidid>https://orcid.org/0000-0003-3072-6139</orcidid><orcidid>https://orcid.org/0000-0002-8376-7842</orcidid></search><sort><creationdate>20230701</creationdate><title>The Radial Distribution of Ion-scale Waves in the Inner Heliosphere</title><author>Liu, Wen ; Zhao, Jinsong ; Wang, Tieyan ; Dong, Xiangcheng ; Kasper, Justin C. ; Bale, Stuart D. ; Shi, Chen ; Wu, Dejin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c416t-54b3ce5593e7506f263144fa37378ed71b2148b21e0152b0bd2efb26c2b7fc9b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Astrophysics</topic><topic>Charged particles</topic><topic>Cyclotron frequency</topic><topic>Cyclotrons</topic><topic>Ellipticity</topic><topic>Heliosphere</topic><topic>Ion beams</topic><topic>Ions</topic><topic>Magnetic fields</topic><topic>Particle acceleration</topic><topic>Particle interactions</topic><topic>Plasma heating</topic><topic>Plasma physics</topic><topic>Radial distribution</topic><topic>Solar probes</topic><topic>Solar wind</topic><topic>Space plasmas</topic><topic>Spacecraft</topic><topic>Wave excitation</topic><topic>Waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Liu, Wen</creatorcontrib><creatorcontrib>Zhao, Jinsong</creatorcontrib><creatorcontrib>Wang, Tieyan</creatorcontrib><creatorcontrib>Dong, Xiangcheng</creatorcontrib><creatorcontrib>Kasper, Justin C.</creatorcontrib><creatorcontrib>Bale, Stuart D.</creatorcontrib><creatorcontrib>Shi, Chen</creatorcontrib><creatorcontrib>Wu, Dejin</creatorcontrib><collection>IOP Publishing Free Content</collection><collection>IOPscience (Open Access)</collection><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Liu, Wen</au><au>Zhao, Jinsong</au><au>Wang, Tieyan</au><au>Dong, Xiangcheng</au><au>Kasper, Justin C.</au><au>Bale, Stuart D.</au><au>Shi, Chen</au><au>Wu, Dejin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Radial Distribution of Ion-scale Waves in the Inner Heliosphere</atitle><jtitle>The Astrophysical journal</jtitle><stitle>APJ</stitle><addtitle>Astrophys. J</addtitle><date>2023-07-01</date><risdate>2023</risdate><volume>951</volume><issue>1</issue><spage>69</spage><pages>69-</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>Determining the mechanism responsible for plasma heating and particle acceleration is a fundamental problem in the study of the heliosphere. Due to efficient wave–particle interactions of ion-scale waves with charged particles, these waves are widely believed to be a major contributor to ion energization, and their contribution considerably depends on the wave occurrence rate. By analyzing the radial distribution of quasi-monochromatic ion-scale waves observed by the Parker Solar Probe, this work shows that the wave occurrence rate is significantly enhanced in the near-Sun solar wind, specifically 21%–29% below 0.3 au, in comparison to 6%–14% beyond 0.3 au. The radial decrease of the wave occurrence rate is not only induced by the sampling effect of a single spacecraft detection, but also by the physics relating to the wave excitation, such as the enhanced ion beam instability in the near-Sun solar wind. This work also shows that the wave normal angle
θ
, the absolute value of ellipticity
ϵ
, the wave frequency
f
normalized by the proton cyclotron frequency
f
cp
, and the wave amplitude
δ
B
normalized by the local background magnetic field
B
0
slightly vary with the radial distance. The median values of
θ
, ∣
ϵ
∣,
f
, and
δ
B
are about 9°, 0.73, 3
f
cp
, and 0.01
B
0
, respectively. Furthermore, this study proposes that the wave mode natures of the observed left-handed and right-handed polarized waves correspond to the Alfvén ion cyclotron mode wave and the fast magnetosonic whistler mode wave, respectively.</abstract><cop>Philadelphia</cop><pub>The American Astronomical Society</pub><doi>10.3847/1538-4357/acd53b</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0001-6519-8706</orcidid><orcidid>https://orcid.org/0000-0003-2418-5508</orcidid><orcidid>https://orcid.org/0000-0002-9166-1036</orcidid><orcidid>https://orcid.org/0000-0002-1989-3596</orcidid><orcidid>https://orcid.org/0000-0002-7077-930X</orcidid><orcidid>https://orcid.org/0000-0002-3859-6394</orcidid><orcidid>https://orcid.org/0000-0003-3072-6139</orcidid><orcidid>https://orcid.org/0000-0002-8376-7842</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Astrophysics Charged particles Cyclotron frequency Cyclotrons Ellipticity Heliosphere Ion beams Ions Magnetic fields Particle acceleration Particle interactions Plasma heating Plasma physics Radial distribution Solar probes Solar wind Space plasmas Spacecraft Wave excitation Waves |
title | The Radial Distribution of Ion-scale Waves in the Inner Heliosphere |
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