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Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales
To improve our understanding of the role of electromagnetic ion cyclotron (EMIC) waves in radiation belt electron dynamics, we perform a comprehensive analysis of EMIC wave‐induced resonant scattering of outer zone relativistic (>0.5 MeV) electrons and resultant electron loss time scales with res...
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Published in: | Journal of geophysical research. Space physics 2015-09, Vol.120 (9), p.7357-7373 |
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description | To improve our understanding of the role of electromagnetic ion cyclotron (EMIC) waves in radiation belt electron dynamics, we perform a comprehensive analysis of EMIC wave‐induced resonant scattering of outer zone relativistic (>0.5 MeV) electrons and resultant electron loss time scales with respect to EMIC wave band, L shell, and wave normal angle model. The results demonstrate that while H+‐band EMIC waves dominate the scattering losses of ~1–4 MeV outer zone relativistic electrons, it is He+‐band and O+‐band waves that prevail over the pitch angle diffusion of ultrarelativistic electrons at higher energies. Given the wave amplitude, EMIC waves at higher L shells tend to resonantly interact with a larger population of outer zone relativistic electrons and drive their pitch angle scattering more efficiently. Obliquity of EMIC waves can reduce the efficiency of wave‐induced relativistic electron pitch angle scattering. Compared to the frequently adopted parallel or quasi‐parallel model, use of the latitudinally varying wave normal angle model produces the largest decrease in H+‐band EMIC wave scattering rates at pitch angles ~5 MeV. At a representative nominal amplitude of 1 nT, EMIC wave scattering produces the equilibrium state (i.e., the lowest normal mode under which electrons at the same energy but different pitch angles decay exponentially on the same time scale) of outer belt relativistic electrons within several to tens of minutes and the following exponential decay extending to higher pitch angles on time scales from |
doi_str_mv | 10.1002/2015JA021466 |
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Key Points
Obliquity of EMIC waves can reduce the scattering efficiency
EMIC wave scattering can cause the top‐hot electron distribution
Different EMIC bands are important for RB electrons at different energies</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1002/2015JA021466</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Amplitudes ; Decay ; Diffusion ; Dynamics ; electron loss time scales ; Electrons ; EMIC waves ; Geophysics ; outer radiation belt ; Pitch angle ; relativistic electrons ; resonant wave-particle interactions ; Resultants ; Scattering ; Time ; Wave scattering ; Waves</subject><ispartof>Journal of geophysical research. Space physics, 2015-09, Vol.120 (9), p.7357-7373</ispartof><rights>2015. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c5587-1ce4958510214624d125927e3a45accef2f86f5689a5c5e841bb33ba727655e43</citedby><cites>FETCH-LOGICAL-c5587-1ce4958510214624d125927e3a45accef2f86f5689a5c5e841bb33ba727655e43</cites><orcidid>0000-0003-1273-4573</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Ni, Binbin</creatorcontrib><creatorcontrib>Cao, Xing</creatorcontrib><creatorcontrib>Zou, Zhengyang</creatorcontrib><creatorcontrib>Zhou, Chen</creatorcontrib><creatorcontrib>Gu, Xudong</creatorcontrib><creatorcontrib>Bortnik, Jacob</creatorcontrib><creatorcontrib>Zhang, Jichun</creatorcontrib><creatorcontrib>Fu, Song</creatorcontrib><creatorcontrib>Zhao, Zhengyu</creatorcontrib><creatorcontrib>Shi, Run</creatorcontrib><creatorcontrib>Xie, Lun</creatorcontrib><title>Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales</title><title>Journal of geophysical research. Space physics</title><addtitle>J. Geophys. Res. Space Physics</addtitle><description>To improve our understanding of the role of electromagnetic ion cyclotron (EMIC) waves in radiation belt electron dynamics, we perform a comprehensive analysis of EMIC wave‐induced resonant scattering of outer zone relativistic (>0.5 MeV) electrons and resultant electron loss time scales with respect to EMIC wave band, L shell, and wave normal angle model. The results demonstrate that while H+‐band EMIC waves dominate the scattering losses of ~1–4 MeV outer zone relativistic electrons, it is He+‐band and O+‐band waves that prevail over the pitch angle diffusion of ultrarelativistic electrons at higher energies. Given the wave amplitude, EMIC waves at higher L shells tend to resonantly interact with a larger population of outer zone relativistic electrons and drive their pitch angle scattering more efficiently. Obliquity of EMIC waves can reduce the efficiency of wave‐induced relativistic electron pitch angle scattering. Compared to the frequently adopted parallel or quasi‐parallel model, use of the latitudinally varying wave normal angle model produces the largest decrease in H+‐band EMIC wave scattering rates at pitch angles < ~40° for electrons > ~5 MeV. At a representative nominal amplitude of 1 nT, EMIC wave scattering produces the equilibrium state (i.e., the lowest normal mode under which electrons at the same energy but different pitch angles decay exponentially on the same time scale) of outer belt relativistic electrons within several to tens of minutes and the following exponential decay extending to higher pitch angles on time scales from <1 min to ~1 h. The electron loss cone can be either empty as a result of the weak diffusion or heavily/fully filled due to approaching the strong diffusion limit, while the trapped electron population at high pitch angles close to 90° remains intact because of no resonant scattering. In this manner, EMIC wave scattering has the potential to deepen the anisotropic distribution of outer zone relativistic electrons by reshaping their pitch angle profiles to “top‐hat.” Overall, H+‐band and He+‐band EMIC waves are most efficient in producing the pitch angle scattering loss of relativistic electrons at ~1–2 MeV. In contrast, the presence of O+‐band EMIC waves, while at a smaller occurrence rate, can dominate the scattering loss of 5–10 MeV electrons in the entire region of the outer zone, which should be considered in future modeling of the outer zone relativistic electron dynamics.
Key Points
Obliquity of EMIC waves can reduce the scattering efficiency
EMIC wave scattering can cause the top‐hot electron distribution
Different EMIC bands are important for RB electrons at different energies</description><subject>Amplitudes</subject><subject>Decay</subject><subject>Diffusion</subject><subject>Dynamics</subject><subject>electron loss time scales</subject><subject>Electrons</subject><subject>EMIC waves</subject><subject>Geophysics</subject><subject>outer radiation belt</subject><subject>Pitch angle</subject><subject>relativistic electrons</subject><subject>resonant wave-particle interactions</subject><subject>Resultants</subject><subject>Scattering</subject><subject>Time</subject><subject>Wave scattering</subject><subject>Waves</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNkctuFDEQRVsIJKIkOz7AEhsWdOK33cvRKExegDQKYmm5nWrk4GkH251k-HrcGYIQCxRvqlw-t6yr2zRvCD4iGNNjiok4X2BKuJQvmj1KZNd2HNOXTz3T-HVzmPMNrkfXERF7zcMachztWFB2thRIfvyG4oDiVHv0M46AEgRb_J3PxTsEAVxJccyo36LNFIrv7XiNTj6eLdG9vYOM5muCXJ_mrU88CjFnVPwG5o8C5IPm1WBDhsPfdb_58uHkannaXn5enS0Xl60TQquWOOCd0II8GqP8mlDRUQXMcmGdg4EOWg5C6s4KJ0Bz0veM9VZRJYUAzvabd7u9tyn-mCAXs_HZQQh2hDhlQ5TCtNNa0GegjGoilJ7Rt_-gN3FKYzVSKSoZ4VzN1Psd5VJ1n2Awt8lvbNoags0cmvk7tIqzHX7vA2z_y5rz1XohKGaqqtqdqgYED39UNn03UjElzNdPK9ORi1Mt1tJ07BffPKZB</recordid><startdate>201509</startdate><enddate>201509</enddate><creator>Ni, Binbin</creator><creator>Cao, Xing</creator><creator>Zou, Zhengyang</creator><creator>Zhou, Chen</creator><creator>Gu, Xudong</creator><creator>Bortnik, Jacob</creator><creator>Zhang, Jichun</creator><creator>Fu, Song</creator><creator>Zhao, Zhengyu</creator><creator>Shi, Run</creator><creator>Xie, Lun</creator><general>Blackwell Publishing Ltd</general><scope>BSCLL</scope><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/0000-0003-1273-4573</orcidid></search><sort><creationdate>201509</creationdate><title>Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales</title><author>Ni, Binbin ; Cao, Xing ; Zou, Zhengyang ; Zhou, Chen ; Gu, Xudong ; Bortnik, Jacob ; Zhang, Jichun ; Fu, Song ; Zhao, Zhengyu ; Shi, Run ; Xie, Lun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c5587-1ce4958510214624d125927e3a45accef2f86f5689a5c5e841bb33ba727655e43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Amplitudes</topic><topic>Decay</topic><topic>Diffusion</topic><topic>Dynamics</topic><topic>electron loss time scales</topic><topic>Electrons</topic><topic>EMIC waves</topic><topic>Geophysics</topic><topic>outer radiation belt</topic><topic>Pitch angle</topic><topic>relativistic electrons</topic><topic>resonant wave-particle interactions</topic><topic>Resultants</topic><topic>Scattering</topic><topic>Time</topic><topic>Wave scattering</topic><topic>Waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ni, Binbin</creatorcontrib><creatorcontrib>Cao, Xing</creatorcontrib><creatorcontrib>Zou, Zhengyang</creatorcontrib><creatorcontrib>Zhou, Chen</creatorcontrib><creatorcontrib>Gu, Xudong</creatorcontrib><creatorcontrib>Bortnik, Jacob</creatorcontrib><creatorcontrib>Zhang, Jichun</creatorcontrib><creatorcontrib>Fu, Song</creatorcontrib><creatorcontrib>Zhao, Zhengyu</creatorcontrib><creatorcontrib>Shi, Run</creatorcontrib><creatorcontrib>Xie, Lun</creatorcontrib><collection>Istex</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><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ni, Binbin</au><au>Cao, Xing</au><au>Zou, Zhengyang</au><au>Zhou, Chen</au><au>Gu, Xudong</au><au>Bortnik, Jacob</au><au>Zhang, Jichun</au><au>Fu, Song</au><au>Zhao, Zhengyu</au><au>Shi, Run</au><au>Xie, Lun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><addtitle>J. Geophys. Res. Space Physics</addtitle><date>2015-09</date><risdate>2015</risdate><volume>120</volume><issue>9</issue><spage>7357</spage><epage>7373</epage><pages>7357-7373</pages><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>To improve our understanding of the role of electromagnetic ion cyclotron (EMIC) waves in radiation belt electron dynamics, we perform a comprehensive analysis of EMIC wave‐induced resonant scattering of outer zone relativistic (>0.5 MeV) electrons and resultant electron loss time scales with respect to EMIC wave band, L shell, and wave normal angle model. The results demonstrate that while H+‐band EMIC waves dominate the scattering losses of ~1–4 MeV outer zone relativistic electrons, it is He+‐band and O+‐band waves that prevail over the pitch angle diffusion of ultrarelativistic electrons at higher energies. Given the wave amplitude, EMIC waves at higher L shells tend to resonantly interact with a larger population of outer zone relativistic electrons and drive their pitch angle scattering more efficiently. Obliquity of EMIC waves can reduce the efficiency of wave‐induced relativistic electron pitch angle scattering. Compared to the frequently adopted parallel or quasi‐parallel model, use of the latitudinally varying wave normal angle model produces the largest decrease in H+‐band EMIC wave scattering rates at pitch angles < ~40° for electrons > ~5 MeV. At a representative nominal amplitude of 1 nT, EMIC wave scattering produces the equilibrium state (i.e., the lowest normal mode under which electrons at the same energy but different pitch angles decay exponentially on the same time scale) of outer belt relativistic electrons within several to tens of minutes and the following exponential decay extending to higher pitch angles on time scales from <1 min to ~1 h. The electron loss cone can be either empty as a result of the weak diffusion or heavily/fully filled due to approaching the strong diffusion limit, while the trapped electron population at high pitch angles close to 90° remains intact because of no resonant scattering. In this manner, EMIC wave scattering has the potential to deepen the anisotropic distribution of outer zone relativistic electrons by reshaping their pitch angle profiles to “top‐hat.” Overall, H+‐band and He+‐band EMIC waves are most efficient in producing the pitch angle scattering loss of relativistic electrons at ~1–2 MeV. In contrast, the presence of O+‐band EMIC waves, while at a smaller occurrence rate, can dominate the scattering loss of 5–10 MeV electrons in the entire region of the outer zone, which should be considered in future modeling of the outer zone relativistic electron dynamics.
Key Points
Obliquity of EMIC waves can reduce the scattering efficiency
EMIC wave scattering can cause the top‐hot electron distribution
Different EMIC bands are important for RB electrons at different energies</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2015JA021466</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0003-1273-4573</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Amplitudes Decay Diffusion Dynamics electron loss time scales Electrons EMIC waves Geophysics outer radiation belt Pitch angle relativistic electrons resonant wave-particle interactions Resultants Scattering Time Wave scattering Waves |
title | Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales |
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