TY - JOUR
T1 - Climatology Analysis of the Daytime Topside Ionospheric Diffusive O+ Flux Based on Incoherent Scatter Radar Observations at Millstone Hill
AU - Cai, Yihui
AU - Wang, Wenbin
AU - Zhang, Shun Rong
AU - Yue, Xinan
AU - Ren, Zhipeng
AU - Liu, Huixin
N1 - Funding Information:
The Authors acknowledge the support by the B‐type Strategic Priority Program of the Chinese Academy of Sciences (Grant No. XDB41000000), the Project of Stable Support for Youth Team in Basic Research Field, CAS (YSBR‐018),the Open Research Project of Large Research Infrastructures of CAS—“Study on the interaction between low/mid‐latitude atmosphere and ionosphere based on the Chinese Meridian Project,” and the National Natural Science Foundation of China (41427901). Long‐term ISR observations at Millstone Hill have been supported by the US NSF through cooperative agreements with MIT over decades, and the data are distributed through the Madrigal database ( http://openmadrigal.org ). Work at MIT is funded through NSF grant AGS‐952737, US AFOSR MURI award FA9559‐16‐1‐0364, and US ONR Grant N00014‐17‐1‐2186.The National Center for Atmospheric Research is sponsored by the National Science Foundation.
Publisher Copyright:
© 2021 The Authors.
PY - 2021/10
Y1 - 2021/10
N2 - This paper reports the characteristics of the topside ionospheric O+ diffusive flux ((Formula presented.)) during both geomagnetically quiet (0 ≤ Kp ≤ 2) and moderate (2 < Kp ≤ 4) times using incoherent scatter radar observations at Millstone Hill (42.6°N, 288.5°E) for solar minimum from 1970 to 2018. (Formula presented.) partially characterizes plasma mass exchange between the upper and lower part of the topside ionosphere through diffusion and sometimes serves as upper boundary conditions for ionosphere-thermosphere models. The altitude where the flux sign changes (mainly during daytime) is termed the transition height and the time when the flux sign changes (mainly at dawn and dusk) is termed the transition time. At quiet times, the daytime transition height is ∼100 km above the (Formula presented.) peak height (hmF2) in summer, and it is about 50 km above hmF2 in other seasons; the transition time is before 18 solar local time (SLT) in spring and winter, but after 18 SLT in summer and autumn. The daytime average upward (Formula presented.) above the transition height shows a significant seasonal variation with a minimum of (Formula presented.) in summer and a maximum of (Formula presented.) in autumn. Under geomagnetically moderate conditions, the transition height increases by ∼20 km in spring, winter, and autumn, but moves up by about 20–50 km in summer. The transition time occurs later by ∼1 hr in summer but ∼1 hr earlier in other seasons. The mean upward (Formula presented.) peaks in summer and minimizes in spring.
AB - This paper reports the characteristics of the topside ionospheric O+ diffusive flux ((Formula presented.)) during both geomagnetically quiet (0 ≤ Kp ≤ 2) and moderate (2 < Kp ≤ 4) times using incoherent scatter radar observations at Millstone Hill (42.6°N, 288.5°E) for solar minimum from 1970 to 2018. (Formula presented.) partially characterizes plasma mass exchange between the upper and lower part of the topside ionosphere through diffusion and sometimes serves as upper boundary conditions for ionosphere-thermosphere models. The altitude where the flux sign changes (mainly during daytime) is termed the transition height and the time when the flux sign changes (mainly at dawn and dusk) is termed the transition time. At quiet times, the daytime transition height is ∼100 km above the (Formula presented.) peak height (hmF2) in summer, and it is about 50 km above hmF2 in other seasons; the transition time is before 18 solar local time (SLT) in spring and winter, but after 18 SLT in summer and autumn. The daytime average upward (Formula presented.) above the transition height shows a significant seasonal variation with a minimum of (Formula presented.) in summer and a maximum of (Formula presented.) in autumn. Under geomagnetically moderate conditions, the transition height increases by ∼20 km in spring, winter, and autumn, but moves up by about 20–50 km in summer. The transition time occurs later by ∼1 hr in summer but ∼1 hr earlier in other seasons. The mean upward (Formula presented.) peaks in summer and minimizes in spring.
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U2 - 10.1029/2021JA029222
DO - 10.1029/2021JA029222
M3 - Article
AN - SCOPUS:85118103739
SN - 2169-9380
VL - 126
JO - Journal of Geophysical Research: Space Physics
JF - Journal of Geophysical Research: Space Physics
IS - 10
M1 - e2021JA029222
ER -