惑星分光観測衛星プロジェクトチーム

Minami Yoshida

  (吉田 南)

Profile Information

Affiliation
Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency
Degree
Master's degree(Mar, 2023, The University of Tokyo)
Ph.D.(Mar, 2026, The University of Tokyo)

Contact information
yoshida.minamijaxa.jp
J-GLOBAL ID
202501006587054427
researchmap Member ID
R000046724

Research History

 3

Papers

 4
  • Minami Yoshida, Toshifumi Shimizu, Shin Toriumi, Haruhisa Iijima
    The Astrophysical Journal, 1001(1) 23-23, Apr 2, 2026  Peer-reviewedLead author
    Abstract The evolution of the global solar magnetic field directly impacts the interplanetary magnetic field (IMF). During the solar maximum of Cycle 24, the monthly averaged IMF strength doubled over five Carrington rotations (CRs) in late 2014. To understand the physical origin of this increase, we investigate the temporal evolution of open magnetic flux resulting from the emergence and decay of bipolar magnetic regions (BMRs). Using surface flux transport and potential field source surface models, we simulated how BMR characteristics, spatial distributions, and interaction with background magnetic fields affect open flux evolution. Our simulation confirmed that the relative configuration of BMRs can either inhibit open flux expansion via closed loops or promote it through favorable connections. The increase in open flux is primarily driven by the equatorial dipole component, which is enhanced by differential rotation acting on tilted BMRs. These behaviors suggest that large open field structures develop from equatorial dipole components formed by these stretched BMRs. We attribute the rapid IMF increase in 2014 (CRs 2152–2157) to the combination of the following three factors: (1) a specific sunspot configuration that facilitated the expansion of the southern coronal hole, (2) the emergence of a giant sunspot group (active region 12192) with high magnetic intensity, and (3) the diffusion of these regions, which reinforced the global magnetic field. These results imply that rapid open flux variations during solar maximum are governed not only by the characteristics of emerging BMRs but also by their interaction with preexisting large coronal holes.
  • Yuto Kondo, Daiki Yamasaki, Minami Yoshida, Akiko Tei, Mizuho Uchiyama, Toshifumi Shimizu
    Proceedings of the SPIE, 13100, Aug 26, 2024  
  • 鄭, 祥子, 長谷川, 隆祥, 藤島, 早織, 合田, 雄哉, 村尾, 一, 吉田, 南, 清水, 敏文, 久保, 雅仁, 津野, 克彦
    宇宙航空研究開発機構研究開発報告, 巻JAXA-RR-23-002, Feb 13, 2024  
  • Minami Yoshida, Toshifumi Shimizu, Shin Toriumi
    The Astrophysical Journal, 950(2) 156-156, Jun 20, 2023  Peer-reviewedLead author
    Abstract The solar magnetic structure changes over the solar cycle. It has a dipole structure during solar minimum, where the open flux extends mainly from the polar regions into the interplanetary space. During maximum, a complex structure is formed with low-latitude active regions and weakened polar fields, resulting in spread open field regions. However, the components of the solar magnetic field that are responsible for long-term variations in the interplanetary magnetic field (IMF) are not clear, and the IMF strength estimated based on the solar magnetic field is known to be underestimated by a factor of 3–4 against the actual in situ observations (the open flux problem). To this end, we decomposed the coronal magnetic field into the components of the spherical harmonic function of degree and order (ℓ, m) using the potential field source surface model with synoptic maps from SDO/HMI for 2010–2021. As a result, we found that the IMF rapidly increased in 2014 December (7 months after the solar maximum), which coincided with the increase in the equatorial dipole, (ℓ, m) = (1, ±1), corresponding to the diffusion of active regions toward the poles and in the longitudinal direction. The IMF gradually decreased until 2019 December (solar minimum) and its variation corresponded to that of the nondipole component ℓ ≥ 2. Our results suggest that the understanding of the open flux problem may be improved by focusing on the equatorial dipole and the nondipole component and that the influence of the polar magnetic field is less significant.

Presentations

 34

Professional Memberships

 3

Research Projects

 1

Social Activities

 8

Media Coverage

 2