Global Distribution of EMIC Waves and Its Association to Subauroral Proton Precipitation During the 27 May 2017 Storm: Modeling and Multipoint Observations

Recent simulation studies using the RAM‐SCB model showed that proton precipitation contributes significantly to the total energy flux deposited into the subauroral ionosphere thereby affecting the magnetosphere‐ionosphere coupling. In this study, we use the BATS‐R‐US + RAM‐SCB model to understand th...

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Veröffentlicht in:Journal of geophysical research. Space physics 2024-06, Vol.129 (6), p.n/a
Hauptverfasser: Shreedevi, P. R., Yu, Yiqun, Miyoshi, Yoshizumi, Tian, Xingbin, Zhu, Minghui, Jordanova, Vania K., Nakamura, Satoko, Jun, Chae‐Woo, Kumar, Sandeep, Shiokawa, Kazuo, Connors, Martin, Hori, T., Shoji, Masafumi, Shinohara, I., Yokota, S., Kasahara, S., Keika, K., Matsuoka, A., Kadokura, Akira, Tsuchiya, Fuminori, Kumamoto, Atsushi, Kasahara, Yoshiya
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container_issue 6
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container_title Journal of geophysical research. Space physics
container_volume 129
creator Shreedevi, P. R.
Yu, Yiqun
Miyoshi, Yoshizumi
Tian, Xingbin
Zhu, Minghui
Jordanova, Vania K.
Nakamura, Satoko
Jun, Chae‐Woo
Kumar, Sandeep
Shiokawa, Kazuo
Connors, Martin
Hori, T.
Shoji, Masafumi
Shinohara, I.
Yokota, S.
Kasahara, S.
Keika, K.
Matsuoka, A.
Kadokura, Akira
Tsuchiya, Fuminori
Kumamoto, Atsushi
Kasahara, Yoshiya
description Recent simulation studies using the RAM‐SCB model showed that proton precipitation contributes significantly to the total energy flux deposited into the subauroral ionosphere thereby affecting the magnetosphere‐ionosphere coupling. In this study, we use the BATS‐R‐US + RAM‐SCB model to understand the evolution of ElectroMagnetic Ion Cyclotron (EMIC) waves in the inner magnetosphere, their correspondence to the proton precipitation into the subauroral ionosphere, and to assess the performance of the model in reproducing the EMIC wave‐particle interactions. During the 27 May 2017 storm, Arase and RBSP‐A satellites observed typical signatures of EMIC waves in the inner magnetosphere. Within this interval, Defense Meteorological Satellite Program (DMSP) and National Oceanic and Atmospheric Administration (NOAA)/MetOp satellites observed significant proton precipitation in the dusk‐midnight sector. Simulation results show that H‐ and He‐band EMIC waves are excited within regions of strong temperature anisotropy near the plasmapause. The simulated growth rates of EMIC waves show a similar trend to that of the EMIC wave power observed by the Arase and RBSP‐A satellites, suggesting that the model can reproduce the EMIC wave activity qualitatively. The simulated H‐band waves in the dusk sector are stronger than He‐band waves possibly due to the presence of excess protons in the boundary conditions obtained from the BATS‐R‐US code. The precipitating proton fluxes reproduced by the simulation with EMIC waves are found to agree reasonably well with the DMSP and NOAA/MetOp satellite observations. It is suggested that EMIC wave scattering of ring current ions can account for proton precipitation observed by the DMSP and MetOp satellites during the 27 May 2017 storm. Plain Language Summary During geomagnetic storms, plasma waves are generated in the Earth's magnetosphere. Among these waves, ElectroMagnetic Ion Cyclotron (EMIC) waves can scatter protons from the ring current, causing them to precipitate into the subauroral ionosphere. Such precipitation not only affects the midlatitude ionosphere but also impacts the dynamics of the magnetosphere. Understanding the origin of magnetospheric plasma waves and how they interact with the magnetospheric populations, along with their subsequent impact on the ionosphere, is crucial for predicting space weather accurately. In our study, we combined ground and satellite observations with simulations using the BATS‐R‐US + RAM‐SCB to
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R. ; Yu, Yiqun ; Miyoshi, Yoshizumi ; Tian, Xingbin ; Zhu, Minghui ; Jordanova, Vania K. ; Nakamura, Satoko ; Jun, Chae‐Woo ; Kumar, Sandeep ; Shiokawa, Kazuo ; Connors, Martin ; Hori, T. ; Shoji, Masafumi ; Shinohara, I. ; Yokota, S. ; Kasahara, S. ; Keika, K. ; Matsuoka, A. ; Kadokura, Akira ; Tsuchiya, Fuminori ; Kumamoto, Atsushi ; Kasahara, Yoshiya</creator><creatorcontrib>Shreedevi, P. R. ; Yu, Yiqun ; Miyoshi, Yoshizumi ; Tian, Xingbin ; Zhu, Minghui ; Jordanova, Vania K. ; Nakamura, Satoko ; Jun, Chae‐Woo ; Kumar, Sandeep ; Shiokawa, Kazuo ; Connors, Martin ; Hori, T. ; Shoji, Masafumi ; Shinohara, I. ; Yokota, S. ; Kasahara, S. ; Keika, K. ; Matsuoka, A. ; Kadokura, Akira ; Tsuchiya, Fuminori ; Kumamoto, Atsushi ; Kasahara, Yoshiya ; Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)</creatorcontrib><description>Recent simulation studies using the RAM‐SCB model showed that proton precipitation contributes significantly to the total energy flux deposited into the subauroral ionosphere thereby affecting the magnetosphere‐ionosphere coupling. In this study, we use the BATS‐R‐US + RAM‐SCB model to understand the evolution of ElectroMagnetic Ion Cyclotron (EMIC) waves in the inner magnetosphere, their correspondence to the proton precipitation into the subauroral ionosphere, and to assess the performance of the model in reproducing the EMIC wave‐particle interactions. During the 27 May 2017 storm, Arase and RBSP‐A satellites observed typical signatures of EMIC waves in the inner magnetosphere. Within this interval, Defense Meteorological Satellite Program (DMSP) and National Oceanic and Atmospheric Administration (NOAA)/MetOp satellites observed significant proton precipitation in the dusk‐midnight sector. Simulation results show that H‐ and He‐band EMIC waves are excited within regions of strong temperature anisotropy near the plasmapause. The simulated growth rates of EMIC waves show a similar trend to that of the EMIC wave power observed by the Arase and RBSP‐A satellites, suggesting that the model can reproduce the EMIC wave activity qualitatively. The simulated H‐band waves in the dusk sector are stronger than He‐band waves possibly due to the presence of excess protons in the boundary conditions obtained from the BATS‐R‐US code. The precipitating proton fluxes reproduced by the simulation with EMIC waves are found to agree reasonably well with the DMSP and NOAA/MetOp satellite observations. It is suggested that EMIC wave scattering of ring current ions can account for proton precipitation observed by the DMSP and MetOp satellites during the 27 May 2017 storm. Plain Language Summary During geomagnetic storms, plasma waves are generated in the Earth's magnetosphere. Among these waves, ElectroMagnetic Ion Cyclotron (EMIC) waves can scatter protons from the ring current, causing them to precipitate into the subauroral ionosphere. Such precipitation not only affects the midlatitude ionosphere but also impacts the dynamics of the magnetosphere. Understanding the origin of magnetospheric plasma waves and how they interact with the magnetospheric populations, along with their subsequent impact on the ionosphere, is crucial for predicting space weather accurately. In our study, we combined ground and satellite observations with simulations using the BATS‐R‐US + RAM‐SCB to investigate EMIC wave‐particle interactions in the inner magnetosphere and the resulting proton precipitation during the 27 May 2017 storm. We found that EMIC waves were excited in the dusk‐midnight sector during the storm's main phase, within the regions of strong temperature anisotropy. The simulations reproduced the proton precipitation observed in the dusk‐midnight sector by the Defense Meteorological Satellite Program /National Oceanic and Atmospheric Administration MetOP satellites fairly well. The model qualitatively captured the growth of the EMIC waves during the storm and showed that the EMIC waves, by scattering the ring current, were responsible for the proton precipitation into the dusk‐midnight sector during the storm. Key Points ElectroMagnetic Ion Cyclotron (EMIC) wave activity and proton precipitation were observed simultaneously in the dusk‐midnight sector during the 27 May 2017 storm The BATS‐R‐US + RAM‐SCB model can capture the EMIC wave growth during the storm qualitatively The EMIC wave scattering of ring current ions can account for the proton precipitation in the dusk‐midnight sector during the storm</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1029/2023JA032337</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Anisotropy ; ASTRONOMY AND ASTROPHYSICS ; Boundary conditions ; Cyclotrons ; DMSP satellites ; Earth magnetosphere ; EMIC waves ; Energy flux ; geomagnetic storm ; Geomagnetic storms ; global modeling ; Heliospheric and Magnetospheric Physics ; Ionosphere ; Magnetic storms ; Magnetospheric plasma ; Magnetospheric plasma waves ; Meteorological satellite program ; Meteorological satellites ; Particle interactions ; Performance assessment ; Plasma waves ; Plasmapause ; Precipitation ; Proton precipitation ; Protons ; Ring current ions ; Ring currents ; Satellite observation ; Satellites ; Simulation ; Space weather ; Storms ; Wave power ; Wave scattering ; wave‐particle interaction</subject><ispartof>Journal of geophysical research. Space physics, 2024-06, Vol.129 (6), p.n/a</ispartof><rights>2024. American Geophysical Union. 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R.</creatorcontrib><creatorcontrib>Yu, Yiqun</creatorcontrib><creatorcontrib>Miyoshi, Yoshizumi</creatorcontrib><creatorcontrib>Tian, Xingbin</creatorcontrib><creatorcontrib>Zhu, Minghui</creatorcontrib><creatorcontrib>Jordanova, Vania K.</creatorcontrib><creatorcontrib>Nakamura, Satoko</creatorcontrib><creatorcontrib>Jun, Chae‐Woo</creatorcontrib><creatorcontrib>Kumar, Sandeep</creatorcontrib><creatorcontrib>Shiokawa, Kazuo</creatorcontrib><creatorcontrib>Connors, Martin</creatorcontrib><creatorcontrib>Hori, T.</creatorcontrib><creatorcontrib>Shoji, Masafumi</creatorcontrib><creatorcontrib>Shinohara, I.</creatorcontrib><creatorcontrib>Yokota, S.</creatorcontrib><creatorcontrib>Kasahara, S.</creatorcontrib><creatorcontrib>Keika, K.</creatorcontrib><creatorcontrib>Matsuoka, A.</creatorcontrib><creatorcontrib>Kadokura, Akira</creatorcontrib><creatorcontrib>Tsuchiya, Fuminori</creatorcontrib><creatorcontrib>Kumamoto, Atsushi</creatorcontrib><creatorcontrib>Kasahara, Yoshiya</creatorcontrib><creatorcontrib>Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)</creatorcontrib><title>Global Distribution of EMIC Waves and Its Association to Subauroral Proton Precipitation During the 27 May 2017 Storm: Modeling and Multipoint Observations</title><title>Journal of geophysical research. Space physics</title><description>Recent simulation studies using the RAM‐SCB model showed that proton precipitation contributes significantly to the total energy flux deposited into the subauroral ionosphere thereby affecting the magnetosphere‐ionosphere coupling. In this study, we use the BATS‐R‐US + RAM‐SCB model to understand the evolution of ElectroMagnetic Ion Cyclotron (EMIC) waves in the inner magnetosphere, their correspondence to the proton precipitation into the subauroral ionosphere, and to assess the performance of the model in reproducing the EMIC wave‐particle interactions. During the 27 May 2017 storm, Arase and RBSP‐A satellites observed typical signatures of EMIC waves in the inner magnetosphere. Within this interval, Defense Meteorological Satellite Program (DMSP) and National Oceanic and Atmospheric Administration (NOAA)/MetOp satellites observed significant proton precipitation in the dusk‐midnight sector. Simulation results show that H‐ and He‐band EMIC waves are excited within regions of strong temperature anisotropy near the plasmapause. The simulated growth rates of EMIC waves show a similar trend to that of the EMIC wave power observed by the Arase and RBSP‐A satellites, suggesting that the model can reproduce the EMIC wave activity qualitatively. The simulated H‐band waves in the dusk sector are stronger than He‐band waves possibly due to the presence of excess protons in the boundary conditions obtained from the BATS‐R‐US code. The precipitating proton fluxes reproduced by the simulation with EMIC waves are found to agree reasonably well with the DMSP and NOAA/MetOp satellite observations. It is suggested that EMIC wave scattering of ring current ions can account for proton precipitation observed by the DMSP and MetOp satellites during the 27 May 2017 storm. Plain Language Summary During geomagnetic storms, plasma waves are generated in the Earth's magnetosphere. Among these waves, ElectroMagnetic Ion Cyclotron (EMIC) waves can scatter protons from the ring current, causing them to precipitate into the subauroral ionosphere. Such precipitation not only affects the midlatitude ionosphere but also impacts the dynamics of the magnetosphere. Understanding the origin of magnetospheric plasma waves and how they interact with the magnetospheric populations, along with their subsequent impact on the ionosphere, is crucial for predicting space weather accurately. In our study, we combined ground and satellite observations with simulations using the BATS‐R‐US + RAM‐SCB to investigate EMIC wave‐particle interactions in the inner magnetosphere and the resulting proton precipitation during the 27 May 2017 storm. We found that EMIC waves were excited in the dusk‐midnight sector during the storm's main phase, within the regions of strong temperature anisotropy. The simulations reproduced the proton precipitation observed in the dusk‐midnight sector by the Defense Meteorological Satellite Program /National Oceanic and Atmospheric Administration MetOP satellites fairly well. The model qualitatively captured the growth of the EMIC waves during the storm and showed that the EMIC waves, by scattering the ring current, were responsible for the proton precipitation into the dusk‐midnight sector during the storm. Key Points ElectroMagnetic Ion Cyclotron (EMIC) wave activity and proton precipitation were observed simultaneously in the dusk‐midnight sector during the 27 May 2017 storm The BATS‐R‐US + RAM‐SCB model can capture the EMIC wave growth during the storm qualitatively The EMIC wave scattering of ring current ions can account for the proton precipitation in the dusk‐midnight sector during the storm</description><subject>Anisotropy</subject><subject>ASTRONOMY AND ASTROPHYSICS</subject><subject>Boundary conditions</subject><subject>Cyclotrons</subject><subject>DMSP satellites</subject><subject>Earth magnetosphere</subject><subject>EMIC waves</subject><subject>Energy flux</subject><subject>geomagnetic storm</subject><subject>Geomagnetic storms</subject><subject>global modeling</subject><subject>Heliospheric and Magnetospheric Physics</subject><subject>Ionosphere</subject><subject>Magnetic storms</subject><subject>Magnetospheric plasma</subject><subject>Magnetospheric plasma waves</subject><subject>Meteorological satellite program</subject><subject>Meteorological satellites</subject><subject>Particle interactions</subject><subject>Performance assessment</subject><subject>Plasma waves</subject><subject>Plasmapause</subject><subject>Precipitation</subject><subject>Proton precipitation</subject><subject>Protons</subject><subject>Ring current ions</subject><subject>Ring currents</subject><subject>Satellite observation</subject><subject>Satellites</subject><subject>Simulation</subject><subject>Space weather</subject><subject>Storms</subject><subject>Wave power</subject><subject>Wave scattering</subject><subject>wave‐particle interaction</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp9kc9KAzEQxoMoWKo3HyDo1Woy2X_xVmqtlRbFKh5DkmZtZN3UJKv0WXxZt66CJ-cywze_-fhgEDqi5IwS4OdAgN0MCQPG8h3UA5rxAU8I7P7OrCD76DCEF9JW0Uo07aHPSeWUrPClDdFb1UTrauxKPJ5PR_hJvpuAZb3E0xjwMASnrfwmosOLRsnGO98e33kXW_HOG23XNnbIZeNt_YzjymDI8VxuMBCa40V0_vUCz93SVNv91n3eVNGuna0jvlXB-Pdvh3CA9kpZBXP40_vo8Wr8MLoezG4n09FwNtAAFAZZWjC2zEGXJUgoSsIKUCwpTcmVNlSmqVQ04YRIo2mR5UrzjHBNpVJSgWasj447XxeiFUHbaPRKu7o2OgpISJYltIVOOmjt3VtjQhQvrvF1m0swklMOOWtz9NFpR2nvQvCmFGtvX6XfCErE9k3i75tanHX4h63M5l9W3Ezuh2mRcGBfwESTbg</recordid><startdate>202406</startdate><enddate>202406</enddate><creator>Shreedevi, P. 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R. ; Yu, Yiqun ; Miyoshi, Yoshizumi ; Tian, Xingbin ; Zhu, Minghui ; Jordanova, Vania K. ; Nakamura, Satoko ; Jun, Chae‐Woo ; Kumar, Sandeep ; Shiokawa, Kazuo ; Connors, Martin ; Hori, T. ; Shoji, Masafumi ; Shinohara, I. ; Yokota, S. ; Kasahara, S. ; Keika, K. ; Matsuoka, A. ; Kadokura, Akira ; Tsuchiya, Fuminori ; Kumamoto, Atsushi ; Kasahara, Yoshiya</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2212-65833d72cff2a28f0382b34fef9bce1a55ab14900aec1867bc9609c1abbab2c33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Anisotropy</topic><topic>ASTRONOMY AND ASTROPHYSICS</topic><topic>Boundary conditions</topic><topic>Cyclotrons</topic><topic>DMSP satellites</topic><topic>Earth magnetosphere</topic><topic>EMIC waves</topic><topic>Energy flux</topic><topic>geomagnetic storm</topic><topic>Geomagnetic storms</topic><topic>global modeling</topic><topic>Heliospheric and Magnetospheric Physics</topic><topic>Ionosphere</topic><topic>Magnetic storms</topic><topic>Magnetospheric plasma</topic><topic>Magnetospheric plasma waves</topic><topic>Meteorological satellite program</topic><topic>Meteorological satellites</topic><topic>Particle interactions</topic><topic>Performance assessment</topic><topic>Plasma waves</topic><topic>Plasmapause</topic><topic>Precipitation</topic><topic>Proton precipitation</topic><topic>Protons</topic><topic>Ring current ions</topic><topic>Ring currents</topic><topic>Satellite observation</topic><topic>Satellites</topic><topic>Simulation</topic><topic>Space weather</topic><topic>Storms</topic><topic>Wave power</topic><topic>Wave scattering</topic><topic>wave‐particle interaction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shreedevi, P. R.</creatorcontrib><creatorcontrib>Yu, Yiqun</creatorcontrib><creatorcontrib>Miyoshi, Yoshizumi</creatorcontrib><creatorcontrib>Tian, Xingbin</creatorcontrib><creatorcontrib>Zhu, Minghui</creatorcontrib><creatorcontrib>Jordanova, Vania K.</creatorcontrib><creatorcontrib>Nakamura, Satoko</creatorcontrib><creatorcontrib>Jun, Chae‐Woo</creatorcontrib><creatorcontrib>Kumar, Sandeep</creatorcontrib><creatorcontrib>Shiokawa, Kazuo</creatorcontrib><creatorcontrib>Connors, Martin</creatorcontrib><creatorcontrib>Hori, T.</creatorcontrib><creatorcontrib>Shoji, Masafumi</creatorcontrib><creatorcontrib>Shinohara, I.</creatorcontrib><creatorcontrib>Yokota, S.</creatorcontrib><creatorcontrib>Kasahara, S.</creatorcontrib><creatorcontrib>Keika, K.</creatorcontrib><creatorcontrib>Matsuoka, A.</creatorcontrib><creatorcontrib>Kadokura, Akira</creatorcontrib><creatorcontrib>Tsuchiya, Fuminori</creatorcontrib><creatorcontrib>Kumamoto, Atsushi</creatorcontrib><creatorcontrib>Kasahara, Yoshiya</creatorcontrib><creatorcontrib>Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)</creatorcontrib><collection>CrossRef</collection><collection>Meteorological &amp; Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological &amp; Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shreedevi, P. R.</au><au>Yu, Yiqun</au><au>Miyoshi, Yoshizumi</au><au>Tian, Xingbin</au><au>Zhu, Minghui</au><au>Jordanova, Vania K.</au><au>Nakamura, Satoko</au><au>Jun, Chae‐Woo</au><au>Kumar, Sandeep</au><au>Shiokawa, Kazuo</au><au>Connors, Martin</au><au>Hori, T.</au><au>Shoji, Masafumi</au><au>Shinohara, I.</au><au>Yokota, S.</au><au>Kasahara, S.</au><au>Keika, K.</au><au>Matsuoka, A.</au><au>Kadokura, Akira</au><au>Tsuchiya, Fuminori</au><au>Kumamoto, Atsushi</au><au>Kasahara, Yoshiya</au><aucorp>Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Global Distribution of EMIC Waves and Its Association to Subauroral Proton Precipitation During the 27 May 2017 Storm: Modeling and Multipoint Observations</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2024-06</date><risdate>2024</risdate><volume>129</volume><issue>6</issue><epage>n/a</epage><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>Recent simulation studies using the RAM‐SCB model showed that proton precipitation contributes significantly to the total energy flux deposited into the subauroral ionosphere thereby affecting the magnetosphere‐ionosphere coupling. In this study, we use the BATS‐R‐US + RAM‐SCB model to understand the evolution of ElectroMagnetic Ion Cyclotron (EMIC) waves in the inner magnetosphere, their correspondence to the proton precipitation into the subauroral ionosphere, and to assess the performance of the model in reproducing the EMIC wave‐particle interactions. During the 27 May 2017 storm, Arase and RBSP‐A satellites observed typical signatures of EMIC waves in the inner magnetosphere. Within this interval, Defense Meteorological Satellite Program (DMSP) and National Oceanic and Atmospheric Administration (NOAA)/MetOp satellites observed significant proton precipitation in the dusk‐midnight sector. Simulation results show that H‐ and He‐band EMIC waves are excited within regions of strong temperature anisotropy near the plasmapause. The simulated growth rates of EMIC waves show a similar trend to that of the EMIC wave power observed by the Arase and RBSP‐A satellites, suggesting that the model can reproduce the EMIC wave activity qualitatively. The simulated H‐band waves in the dusk sector are stronger than He‐band waves possibly due to the presence of excess protons in the boundary conditions obtained from the BATS‐R‐US code. The precipitating proton fluxes reproduced by the simulation with EMIC waves are found to agree reasonably well with the DMSP and NOAA/MetOp satellite observations. It is suggested that EMIC wave scattering of ring current ions can account for proton precipitation observed by the DMSP and MetOp satellites during the 27 May 2017 storm. Plain Language Summary During geomagnetic storms, plasma waves are generated in the Earth's magnetosphere. Among these waves, ElectroMagnetic Ion Cyclotron (EMIC) waves can scatter protons from the ring current, causing them to precipitate into the subauroral ionosphere. Such precipitation not only affects the midlatitude ionosphere but also impacts the dynamics of the magnetosphere. Understanding the origin of magnetospheric plasma waves and how they interact with the magnetospheric populations, along with their subsequent impact on the ionosphere, is crucial for predicting space weather accurately. In our study, we combined ground and satellite observations with simulations using the BATS‐R‐US + RAM‐SCB to investigate EMIC wave‐particle interactions in the inner magnetosphere and the resulting proton precipitation during the 27 May 2017 storm. We found that EMIC waves were excited in the dusk‐midnight sector during the storm's main phase, within the regions of strong temperature anisotropy. The simulations reproduced the proton precipitation observed in the dusk‐midnight sector by the Defense Meteorological Satellite Program /National Oceanic and Atmospheric Administration MetOP satellites fairly well. The model qualitatively captured the growth of the EMIC waves during the storm and showed that the EMIC waves, by scattering the ring current, were responsible for the proton precipitation into the dusk‐midnight sector during the storm. Key Points ElectroMagnetic Ion Cyclotron (EMIC) wave activity and proton precipitation were observed simultaneously in the dusk‐midnight sector during the 27 May 2017 storm The BATS‐R‐US + RAM‐SCB model can capture the EMIC wave growth during the storm qualitatively The EMIC wave scattering of ring current ions can account for the proton precipitation in the dusk‐midnight sector during the storm</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2023JA032337</doi><tpages>24</tpages><orcidid>https://orcid.org/0000-0003-0475-8743</orcidid><orcidid>https://orcid.org/0000-0001-8451-6941</orcidid><orcidid>https://orcid.org/0000-0002-4529-3383</orcidid><orcidid>https://orcid.org/0000-0002-9304-8235</orcidid><orcidid>https://orcid.org/0000-0002-3479-772X</orcidid><orcidid>https://orcid.org/0000-0003-0265-4318</orcidid><orcidid>https://orcid.org/0000-0002-0979-0833</orcidid><orcidid>https://orcid.org/0000-0001-9606-9253</orcidid><orcidid>https://orcid.org/0000-0002-6105-9562</orcidid><orcidid>https://orcid.org/0000-0003-0634-9599</orcidid><orcidid>https://orcid.org/0000-0001-6573-525X</orcidid><orcidid>https://orcid.org/0000-0002-6842-1552</orcidid><orcidid>https://orcid.org/0000-0003-2700-0353</orcidid><orcidid>https://orcid.org/0000-0001-8851-9146</orcidid><orcidid>https://orcid.org/0000-0002-1013-6505</orcidid><orcidid>https://orcid.org/0000-0001-7998-1240</orcidid><orcidid>https://orcid.org/0000-0002-3107-7364</orcidid><orcidid>https://orcid.org/0000-0003-2914-2910</orcidid><orcidid>https://orcid.org/0000000245293383</orcidid><orcidid>https://orcid.org/0000000261059562</orcidid><orcidid>https://orcid.org/0000000209790833</orcidid><orcidid>https://orcid.org/0000000306349599</orcidid><orcidid>https://orcid.org/0000000293048235</orcidid><orcidid>https://orcid.org/0000000196069253</orcidid><orcidid>https://orcid.org/0000000179981240</orcidid><orcidid>https://orcid.org/0000000302654318</orcidid><orcidid>https://orcid.org/000000016573525X</orcidid><orcidid>https://orcid.org/0000000210136505</orcidid><orcidid>https://orcid.org/000000023479772X</orcidid><orcidid>https://orcid.org/0000000329142910</orcidid><orcidid>https://orcid.org/0000000184516941</orcidid><orcidid>https://orcid.org/0000000327000353</orcidid><orcidid>https://orcid.org/0000000188519146</orcidid><orcidid>https://orcid.org/0000000268421552</orcidid><orcidid>https://orcid.org/0000000231077364</orcidid><orcidid>https://orcid.org/0000000304758743</orcidid></addata></record>
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identifier ISSN: 2169-9380
ispartof Journal of geophysical research. Space physics, 2024-06, Vol.129 (6), p.n/a
issn 2169-9380
2169-9402
language eng
recordid cdi_osti_scitechconnect_2406641
source Wiley Online Library Journals Frontfile Complete
subjects Anisotropy
ASTRONOMY AND ASTROPHYSICS
Boundary conditions
Cyclotrons
DMSP satellites
Earth magnetosphere
EMIC waves
Energy flux
geomagnetic storm
Geomagnetic storms
global modeling
Heliospheric and Magnetospheric Physics
Ionosphere
Magnetic storms
Magnetospheric plasma
Magnetospheric plasma waves
Meteorological satellite program
Meteorological satellites
Particle interactions
Performance assessment
Plasma waves
Plasmapause
Precipitation
Proton precipitation
Protons
Ring current ions
Ring currents
Satellite observation
Satellites
Simulation
Space weather
Storms
Wave power
Wave scattering
wave‐particle interaction
title Global Distribution of EMIC Waves and Its Association to Subauroral Proton Precipitation During the 27 May 2017 Storm: Modeling and Multipoint Observations
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