The first observation of 4D tomography measurement of plasma structures and fluctuations

Abstract 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 a...

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Main Authors: Chanho Moon, Kotaro Yamasaki, Yoshihiko Nagashima, Shigeru Inagaki, Takeshi Ido, Takuma Yamada, Naohiro Kasuya, Yusuke Kosuga, Makoto Sasaki, Yuichi Kawachi, Daiki Nishimura, Taiki Kobayashi, Akihide Fujisawa
Format: Article
Language:English
Published: Nature Portfolio 2021-02-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-021-83191-3
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author Chanho Moon
Kotaro Yamasaki
Yoshihiko Nagashima
Shigeru Inagaki
Takeshi Ido
Takuma Yamada
Naohiro Kasuya
Yusuke Kosuga
Makoto Sasaki
Yuichi Kawachi
Daiki Nishimura
Taiki Kobayashi
Akihide Fujisawa
author_facet Chanho Moon
Kotaro Yamasaki
Yoshihiko Nagashima
Shigeru Inagaki
Takeshi Ido
Takuma Yamada
Naohiro Kasuya
Yusuke Kosuga
Makoto Sasaki
Yuichi Kawachi
Daiki Nishimura
Taiki Kobayashi
Akihide Fujisawa
author_sort Chanho Moon
collection DOAJ
description Abstract 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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spelling doaj.art-5f0ced1a7f654bad8548a3327a9e0c002022-12-21T22:59:20ZengNature PortfolioScientific Reports2045-23222021-02-011111910.1038/s41598-021-83191-3The first observation of 4D tomography measurement of plasma structures and fluctuationsChanho Moon0Kotaro Yamasaki1Yoshihiko Nagashima2Shigeru Inagaki3Takeshi Ido4Takuma Yamada5Naohiro Kasuya6Yusuke Kosuga7Makoto Sasaki8Yuichi Kawachi9Daiki Nishimura10Taiki Kobayashi11Akihide Fujisawa12Research Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityFaculty of Arts and Science, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityInterdisciplinary Graduate School of Engineering Sciences, Kyushu UniversityInterdisciplinary Graduate School of Engineering Sciences, Kyushu UniversityInterdisciplinary Graduate School of Engineering Sciences, Kyushu UniversityResearch Institute for Applied Mechanics, Kyushu UniversityAbstract 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.https://doi.org/10.1038/s41598-021-83191-3
spellingShingle Chanho Moon
Kotaro Yamasaki
Yoshihiko Nagashima
Shigeru Inagaki
Takeshi Ido
Takuma Yamada
Naohiro Kasuya
Yusuke Kosuga
Makoto Sasaki
Yuichi Kawachi
Daiki Nishimura
Taiki Kobayashi
Akihide Fujisawa
The first observation of 4D tomography measurement of plasma structures and fluctuations
Scientific Reports
title The first observation of 4D tomography measurement of plasma structures and fluctuations
title_full The first observation of 4D tomography measurement of plasma structures and fluctuations
title_fullStr The first observation of 4D tomography measurement of plasma structures and fluctuations
title_full_unstemmed The first observation of 4D tomography measurement of plasma structures and fluctuations
title_short The first observation of 4D tomography measurement of plasma structures and fluctuations
title_sort first observation of 4d tomography measurement of plasma structures and fluctuations
url https://doi.org/10.1038/s41598-021-83191-3
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