日本地球惑星科学連合2022年大会

講演情報

[E] ポスター発表

セッション記号 P (宇宙惑星科学) » P-EM 太陽地球系科学・宇宙電磁気学・宇宙環境

[P-EM12] 太陽地球系結合過程の研究基盤形成

2022年6月3日(金) 11:00 〜 13:00 オンラインポスターZoom会場 (5) (Ch.05)

コンビーナ:山本 衛(京都大学生存圏研究所)、コンビーナ:小川 泰信(国立極地研究所)、野澤 悟徳(名古屋大学宇宙地球環境研究所)、コンビーナ:吉川 顕正(九州大学大学院理学研究院地球惑星科学部門)、座長:山本 衛(京都大学生存圏研究所)、小川 泰信(国立極地研究所)、野澤 悟徳(名古屋大学宇宙地球環境研究所)、吉川 顕正(九州大学大学院理学研究院地球惑星科学部門)

11:00 〜 13:00

[PEM12-P10] Recent results from aurora and airglow observations by an optical spectrograph at Tromsø, Norway

*津田 卓雄1、前田 哲郎1西山 尚典2細川 敬祐1野澤 悟徳3、川端 哲也3水野 亮3大山 伸一郎3栗原 純一4、Nielsen Kim5 (1.電気通信大学、2.国立極地研究所、3.名古屋大学、4.北海道大学、5.Utah Valley University)

キーワード:Optical spectrograph、Aurora、Airglow、Tromsø

We have been operating an optical spectrograph for aurora and airglow observations at Tromsø, Norway (69.6ºN, 19.2ºE) since October 2016. The aperture of the spectrograph, i.e. F-number, is 4. The field-of-view (FOV) is 0.03ºx2º, which is pointed at the local magnetic field-aligned direction. As an advantage, this spectrograph is capable to change its resolution and range in the observation wavelength by switching between multiple diffraction gratings.

One of research targets is the pulsating aurora (PsA). The PsA is a diffuse-type aurora, which is characterized by a repetition of brighter (ON) and darker (OFF) auroral emissions with periods of a few to a few tens of seconds. For PsA observation, the spectrograph is mainly tuned for visible range from 480 to 880 nm with a resolution of 1.6 nm and an interval of 0.4 nm. The time resolution is 1 second, and thus it can observe PsAs, which have periods of a few seconds or longer. We performed the data analysis of multiple PsA events, and revealed the PsA spectra for the first time. As the results, the OI 630.0-nm emissions and the N2 1PG emissions were found in the both spectra during ON and OFF in the PsA events. The spectra of pulsations were derived as difference spectra between the ON and OFF spectra. From the obtained spectra of pulsations, it is found that dominant pulsations at 630.0 nm were coming from the N2 1PG (10,7) band, and there were less or minor contributions of the OI 630.0 nm to pulsations at 630.0 nm.

Another target is the sodium (Na) nightglow from Na D1 (589.756 nm) and D2 (589.158 nm) transitions, which are chemically produced emissions in the sodium layer in the mesosphere and lower thermosphere (MLT). The chemical process in the Na D1 and D2 emissions have been explaned by the Chapman mechanism for many years. The Chapman mechanism expects that the ratio between Na D1 and D2 emissions should be constant. On the other hand, some recent observations indicate the D2/D1 ratio can be variable, and propose a modification to the Chapman mechanism. To contribute this issue, we have been making spectral observations in the Na D1 and D2 lines. By switching to the 4x higher resolution diffraction grating in the spectrograph, the observation wavelength can be tuned for 540-640 nm with 0.4-nm resolution and 0.1-nm interval. Such high wavelength resolution enables that the Na D1 and D2 lines can be measured seperately.

In the presentation, we will introduce some recent results obtained from such spectral observations in aurora and airglow above Tromsø.