TY - JOUR
T1 - First Simultaneous Observation of a Night Time Medium-Scale Traveling Ionospheric Disturbance From the Ground and a Magnetospheric Satellite
AU - Kawai, K.
AU - Shiokawa, K.
AU - Otsuka, Y.
AU - Oyama, S.
AU - Kasaba, Y.
AU - Kasahara, Y.
AU - Tsuchiya, F.
AU - Kumamoto, A.
AU - Nakamura, S.
AU - Matsuoka, A.
AU - Imajo, S.
AU - Kazama, Y.
AU - Wang, S. Y.
AU - Tam, S. W.Y.
AU - Chang, T. F.
AU - Wang, B. J.
AU - Asamura, K.
AU - Kasahara, S.
AU - Yokota, S.
AU - Keika, K.
AU - Hori, T.
AU - Miyoshi, Y.
AU - Jun, C.
AU - Shoji, M.
AU - Shinohara, I.
N1 - Funding Information:
The authors thank Yasuo Katoh, Yoshiyuki Hamaguchi, Yuka Yamamoto, and Takumi Adachi, technical staff of the ISEE at Nagoya University, for their helpful support when installing the ground‐based instruments at Gakona, Alaska. The airglow camera installed at Gakona are optically calibrated at the National Institute of Polar Research (Ogawa et al., 2020 ). Database construction for the PWING ground‐based instruments were supported by the ERG Science Center ( https://ergsc.isee.nagoya-u.ac.jp/ ) and the Inter‐university Upper atmosphere Global Observation Network (IUGONET) project ( http://www.iugonet.org/ ). The development and operation of LEP‐e was partly funded by Academia Sinica and National Cheng Kung University of Taiwan, and also through the support of the Ministry of Science and Technology of Taiwan under contracts 106‐2111‐M‐001‐011 and 105‐3111‐Y‐001‐042. The ionosonde at Gakona is operated by Air Force Research Laboratory, and provided by Terence W. Bullett through Global Ionosphere Radio Observatory (GIRO). This work was supported by JSPS KAKENHI [15H05815 (Y. Miyoshi), 16H06286 (K. Shiokawa and Y. Miyoshi), 20H01959 (Y. Miyoshi), 15H05747 (S. Oyama and Y. Miyoshi)].
Funding Information:
The authors thank Yasuo Katoh, Yoshiyuki Hamaguchi, Yuka Yamamoto, and Takumi Adachi, technical staff of the ISEE at Nagoya University, for their helpful support when installing the ground-based instruments at Gakona, Alaska. The airglow camera installed at Gakona are optically calibrated at the National Institute of Polar Research (Ogawa et al., 2020). Database construction for the PWING ground-based instruments were supported by the ERG Science Center (https://ergsc.isee.nagoya-u.ac.jp/) and the Inter-university Upper atmosphere Global Observation Network (IUGONET) project (http://www.iugonet.org/). The development and operation of LEP-e was partly funded by Academia Sinica and National Cheng Kung University of Taiwan, and also through the support of the Ministry of Science and Technology of Taiwan under contracts 106-2111-M-001-011 and 105-3111-Y-001-042. The ionosonde at Gakona is operated by Air Force Research Laboratory, and provided by Terence W. Bullett through Global Ionosphere Radio Observatory (GIRO). This work was supported by JSPS KAKENHI [15H05815 (Y. Miyoshi), 16H06286 (K. Shiokawa and Y. Miyoshi), 20H01959 (Y. Miyoshi), 15H05747 (S. Oyama and Y. Miyoshi)].
Publisher Copyright:
© 2021. American Geophysical Union. All Rights Reserved.
PY - 2021/9
Y1 - 2021/9
N2 - Medium-scale traveling ionospheric disturbances (MSTIDs) are a phenomenon widely and frequently observed over the ionosphere from high to low latitudes. Night time MSTIDs are caused generally by the polarization electric field in the ionosphere. However, propagation of this polarization electric field to the magnetosphere has not yet been identified. Here, we report the first observation of the polarization electric field and associated density variations of a night time MSTID in the magnetosphere. The MSTID event was observed by an all-sky airglow imager at Gakona (geographical latitude: 62.39°N, geographical longitude: 214.78°E, magnetic latitude: 63.20°N), Alaska. The Arase satellite passed over the MSTID in the inner magnetosphere at 0530–0800 UT (2030–2300 LT) on November 3, 2018. This MSTID, observed in 630 nm airglow images, was propagating westward with a horizontal wavelength of ∼165 km, a north–south phase front, and a phase velocity of ∼80 m/s. The Arase satellite footprint on the ionosphere crossed the MSTID in the direction nearly perpendicular to the MSTID phase fronts. The electric field and electron density observed by the Arase satellite showed periodic variation associated with the MSTID structure with amplitudes of ∼2 mV/m and ∼150 cm−3, respectively. The electric field variations projected to the ionosphere are mainly in the east-west direction and are consistent with the direction of the polarization electric field expected from MSTID growth by E × B drift. This observation indicates that the polarization electric field associated with the MSTID in the ionosphere is projected onto the magnetosphere, causing plasma density fluctuations in the magnetosphere.
AB - Medium-scale traveling ionospheric disturbances (MSTIDs) are a phenomenon widely and frequently observed over the ionosphere from high to low latitudes. Night time MSTIDs are caused generally by the polarization electric field in the ionosphere. However, propagation of this polarization electric field to the magnetosphere has not yet been identified. Here, we report the first observation of the polarization electric field and associated density variations of a night time MSTID in the magnetosphere. The MSTID event was observed by an all-sky airglow imager at Gakona (geographical latitude: 62.39°N, geographical longitude: 214.78°E, magnetic latitude: 63.20°N), Alaska. The Arase satellite passed over the MSTID in the inner magnetosphere at 0530–0800 UT (2030–2300 LT) on November 3, 2018. This MSTID, observed in 630 nm airglow images, was propagating westward with a horizontal wavelength of ∼165 km, a north–south phase front, and a phase velocity of ∼80 m/s. The Arase satellite footprint on the ionosphere crossed the MSTID in the direction nearly perpendicular to the MSTID phase fronts. The electric field and electron density observed by the Arase satellite showed periodic variation associated with the MSTID structure with amplitudes of ∼2 mV/m and ∼150 cm−3, respectively. The electric field variations projected to the ionosphere are mainly in the east-west direction and are consistent with the direction of the polarization electric field expected from MSTID growth by E × B drift. This observation indicates that the polarization electric field associated with the MSTID in the ionosphere is projected onto the magnetosphere, causing plasma density fluctuations in the magnetosphere.
KW - Arase satellite
KW - MSTID
KW - airglow imager
KW - electric field
KW - electron density
KW - traveling ionospheric disturbance
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U2 - 10.1029/2020JA029086
DO - 10.1029/2020JA029086
M3 - Article
AN - SCOPUS:85115671030
SN - 2169-9380
VL - 126
JO - Journal of Geophysical Research: Space Physics
JF - Journal of Geophysical Research: Space Physics
IS - 9
M1 - e2020JA029086
ER -