Progress of HL-2A experiments and HL-2M program

2021 ◽  
Author(s):  
Xuru Duan ◽  
Min Xu ◽  
Wulyu Zhong ◽  
Yi Liu ◽  
Xianming Song ◽  
...  

Abstract Since the last IAEA Fusion Energy Conference in 2018, significant progress of the experimental program of HL-2A has been achieved on developing advanced plasma physics, edge localized mode (ELM) control physics and technology. Optimization of plasma confinement has been performed. In particular, high-N H-mode plasmas exhibiting an internal transport barrier have been obtained (normalized plasma pressure N reached up to 3). Injection of impurity improved the plasma confinement. ELM control using resonance magnetic perturbation (RMP) or impurity injection has been achieved in a wide parameter regime, including Types I and III. In addition, the impurity seeding with supersonic molecular beam injection (SMBI) or laser blow-off (LBO) techniques has been successfully applied to actively control the plasma confinement and instabilities, as well as the plasma disruption with the aid of disruption prediction. Disruption prediction algorithms based on deep learning are developed. A prediction accuracy of 96.8% can be reached by assembling convolutional neural network (CNN). Furthermore, transport resulted from a wide variety of phenomena such as energetic particles and magnetic islands have been investigated. In parallel with the HL-2A experiments, the HL-2M mega-ampere class tokamak was commissioned in 2020 with its first plasma. Key features and capabilities of HL-2M are briefly presented.

2013 ◽  
Vol 8 (0) ◽  
pp. 2403079-2403079 ◽  
Author(s):  
Tomoyuki YAMAKAMI ◽  
Kozo YAMAZAKI ◽  
Hideki ARIMOTO ◽  
Tatsuo SHOJI

2012 ◽  
Vol 19 (2) ◽  
pp. 022505 ◽  
Author(s):  
T. Rhee ◽  
J. M. Kwon ◽  
P. H. Diamond ◽  
W. W. Xiao

2016 ◽  
Vol 23 (1) ◽  
pp. 012515 ◽  
Author(s):  
Z. C. Yang ◽  
Z. B. Shi ◽  
W. L. Zhong ◽  
B. Y. Zhang ◽  
Q. C. Fan ◽  
...  

2013 ◽  
Vol 8 (0) ◽  
pp. 1402066-1402066 ◽  
Author(s):  
Linge ZANG ◽  
Nobuhiro NISHINO ◽  
Tohru MIZUUCHI ◽  
Shinsuke OHSHIMA ◽  
Masaki TAKEUCHI ◽  
...  

1988 ◽  
Vol 152 (1) ◽  
pp. 87-93 ◽  
Author(s):  
K. McMillan ◽  
D. Bender ◽  
M. Eliades ◽  
D. Danzeiser ◽  
B.A. Wofford ◽  
...  

2021 ◽  
Vol 92 (4) ◽  
pp. 043539
Author(s):  
Guoliang Xiao ◽  
Jiao Yin ◽  
Chengyuan Chen ◽  
Beibin Feng ◽  
Wulyu Zhong ◽  
...  

2001 ◽  
Vol 3 (4) ◽  
pp. 223-227 ◽  
Author(s):  
A. Giardini Guidoni ◽  
S. Piccirillo ◽  
D. Scuderi ◽  
M. Satta ◽  
T. M. Di Palma ◽  
...  

One and two-color, mass selected R2PI spectra of theS1←S0transitions in the bare(+)-(R)- 1-phenyl-1-ethanol(ER) and its complexes with different solvent molecules (solv) (-)-(R)-2-butanol(BR) or(+)-(S)-2-butanol(BS), (—)-(R)-2-pentanol (TR) or(+)-(S)-2-pentanol(TS) and(-)-(R)-2-butylamine(AR) or(+)-(S)-2-butylamine(AS), have been recorded after a supersonic molecular beam expansion. The one-color R2PI excitation spectra of the diastereomeric complexes are characterized by significant shifts of their band origin relative to that of bareER. The extent and the direction of these spectral shifts are found to depend upon the structure and the configuration ofsolvand are attributed to different short-range interactions in the ground and excited states of the complexes. In analogy with other diastereomeric complexes, the phenomenological binding energy of the homochiral cluster is found to be greater than that of the heterochiral one. Preliminary measurements of excitation spectrum of(+)-(R)-1-Indanol(IR) is also reported.


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