TY - JOUR
T1 - The first observation of 4D tomography measurement of plasma structures and fluctuations
AU - Moon, Chanho
AU - Yamasaki, Kotaro
AU - Nagashima, Yoshihiko
AU - Shigeru, Inagaki
AU - Ido, Takeshi
AU - Yamada, Takuma
AU - Kasuya, Naohiro
AU - Kosuga, Yusuke
AU - Sasaki, Makoto
AU - Kawachi, Yuichi
AU - Nishimura, Daiki
AU - Kobayashi, Taiki
AU - Fujisawa, Akihide
N1 - Funding Information:
This work was partly supported by JSPS KAKENHI Grant numbers JP17H06089, 15H02335, and JP19K23426, and also by NIFS Collaboration Research program NIFS17KOCH002.
Publisher Copyright:
© 2021, The Author(s).
PY - 2021/12
Y1 - 2021/12
N2 - A tomography system is installed as one of the diagnostics of new age to examine the three-dimensional characteristics of structure and dynamics including fluctuations of a linear magnetized helicon plasma. The system is composed of three sets of tomography components located at different axial positions. Each tomography component can measure the two-dimensional emission profile over the entire cross-section of plasma at different axial positions in a sufficient temporal scale to detect the fluctuations. The four-dimensional measurement including time and space successfully obtains the following three results that have never been found without three-dimensional measurement: (1) in the production phase, the plasma front propagates from the antenna toward the end plate with an ion acoustic velocity. (2) In the steady state, the plasma emission profile is inhomogeneous, and decreases along the axial direction in the presence of the azimuthal asymmetry. Furthermore, (3) in the steady state, the fluctuations should originate from a particular axial position located downward from the helicon antenna.
AB - A tomography system is installed as one of the diagnostics of new age to examine the three-dimensional characteristics of structure and dynamics including fluctuations of a linear magnetized helicon plasma. The system is composed of three sets of tomography components located at different axial positions. Each tomography component can measure the two-dimensional emission profile over the entire cross-section of plasma at different axial positions in a sufficient temporal scale to detect the fluctuations. The four-dimensional measurement including time and space successfully obtains the following three results that have never been found without three-dimensional measurement: (1) in the production phase, the plasma front propagates from the antenna toward the end plate with an ion acoustic velocity. (2) In the steady state, the plasma emission profile is inhomogeneous, and decreases along the axial direction in the presence of the azimuthal asymmetry. Furthermore, (3) in the steady state, the fluctuations should originate from a particular axial position located downward from the helicon antenna.
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U2 - 10.1038/s41598-021-83191-3
DO - 10.1038/s41598-021-83191-3
M3 - Article
C2 - 33608562
AN - SCOPUS:85101116079
SN - 2045-2322
VL - 11
JO - Scientific Reports
JF - Scientific Reports
IS - 1
M1 - 3720
ER -