TY - JOUR
T1 - Development of the heating scenarios to achieve high-ion temperature plasma in the large helical device
AU - LHD Experiment Group
AU - Takeiri, Yasuhiko
AU - Kaneko, Osamu
AU - Osakabe, Masaki
AU - Nagaoka, Kenichi
AU - Murakami, Sadayoshi
AU - Takahashi, Hiromi
AU - Nakano, Haruhisa
AU - Ida, Katsumi
AU - Morita, Shigeru
AU - Yokoyama, Masayuki
AU - Yoshinuma, Mikiro
AU - Fujii, Keisuke
AU - Goto, Motoshi
AU - Suzuki, Chihiro
AU - Seki, Ryosuke
AU - Tsumori, Katsuyoshi
AU - Ikeda, Katsunori
AU - Kisaki, Masashi
AU - Mutoh, Takashi
AU - Yamada, Hiroshi
AU - Komori, Akio
N1 - Publisher Copyright:
© 2015 The Japan Society of Plasma Science and Nuclear Fusion Research.
PY - 2015
Y1 - 2015
N2 - High-ion temperature experiments in the Large Helical Device (LHD) are categorized in terms of the heating scenarios that are closely related to the development of neutral beam injection (NBI) systems. Although highenergy tangential negative-NBI heating has greatly contributed to extending the plasma parameter regime in LHD, the ion temperature does not increase because the electron heating is dominant with negative-NBIs. In the high-Z discharges, it was demonstrated that the ion temperature increased with an increasing ion heating power and achieved 13.5 keV with the negative-NBIs. Low-energy perpendicular positive-NBIs were installed for the ion heating, and the ion temperature was increased to more than 7 keV in hydrogen discharges. In the high-ion temperature plasmas, an ion internal transport barrier (ion ITB) was formed, and the impurity hole was observed in the core. Long-pulse ion cyclotron range of frequency heating (ICH)/electron cyclotron resonance heating (ECRH) helium discharges are effective for wall conditioning, leading to a decrease in the neutral density and a peaked density profile. Consequently, the ion heating efficiency increases in the core, and the central Ti is raised up to 7.5 keV. With the superposition of high-power ECRH, high-performance plasmas of Ti ~ Te ~ 6 keV were obtained. In the planned deuterium experiment, the ion heating power will be increased with the deuterium beam injection, and Ti = 10 keV is expected.
AB - High-ion temperature experiments in the Large Helical Device (LHD) are categorized in terms of the heating scenarios that are closely related to the development of neutral beam injection (NBI) systems. Although highenergy tangential negative-NBI heating has greatly contributed to extending the plasma parameter regime in LHD, the ion temperature does not increase because the electron heating is dominant with negative-NBIs. In the high-Z discharges, it was demonstrated that the ion temperature increased with an increasing ion heating power and achieved 13.5 keV with the negative-NBIs. Low-energy perpendicular positive-NBIs were installed for the ion heating, and the ion temperature was increased to more than 7 keV in hydrogen discharges. In the high-ion temperature plasmas, an ion internal transport barrier (ion ITB) was formed, and the impurity hole was observed in the core. Long-pulse ion cyclotron range of frequency heating (ICH)/electron cyclotron resonance heating (ECRH) helium discharges are effective for wall conditioning, leading to a decrease in the neutral density and a peaked density profile. Consequently, the ion heating efficiency increases in the core, and the central Ti is raised up to 7.5 keV. With the superposition of high-power ECRH, high-performance plasmas of Ti ~ Te ~ 6 keV were obtained. In the planned deuterium experiment, the ion heating power will be increased with the deuterium beam injection, and Ti = 10 keV is expected.
KW - Deuterium experiment
KW - High-Z discharge
KW - High-ion temperature plasma
KW - Ion ITB
KW - Ion and electron root
KW - Large helical device
KW - Long-pulse discharge cleaning
KW - NBI heating
KW - impurity hole
UR - http://www.scopus.com/inward/record.url?scp=84924764866&partnerID=8YFLogxK
U2 - 10.1585/pfr.10.1402001
DO - 10.1585/pfr.10.1402001
M3 - Article
AN - SCOPUS:84924764866
SN - 1880-6821
VL - 10
SP - 1
EP - 9
JO - Plasma and Fusion Research
JF - Plasma and Fusion Research
IS - 2015
M1 - 1402001
ER -