Evaporated lithium surface coatings in NSTX
Evaporated lithium surface coatings in NSTX
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DOI:
10.1016/j.jnucmat.2009.01.262
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发表时间:
2009-06
影响因子:
3.1
通讯作者:
H. Kugel;D. Mansfield;R. Maingi;M. Bell;R. Bell;J. Allain;D. Gates;S. Gerhardt;R. Kaita;J. Kallman;S. Kaye;B. LeBlanc;R. Majeski;J. Menard;D. Mueller;M. Ono;S. Paul;R. Raman;A. Roquemore;P. Ross;S. Sabbagh;H. Schneider;C. Skinner;V. Soukhanovskii;T. Stevenson;J. Timberlake;W. Wampler;J. Wilgren;L. Zakharov
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文献类型:
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作者:
H. Kugel;D. Mansfield;R. Maingi;M. Bell;R. Bell;J. Allain;D. Gates;S. Gerhardt;R. Kaita;J. Kallman;S. Kaye;B. LeBlanc;R. Majeski;J. Menard;D. Mueller;M. Ono;S. Paul;R. Raman;A. Roquemore;P. Ross;S. Sabbagh;H. Schneider;C. Skinner;V. Soukhanovskii;T. Stevenson;J. Timberlake;W. Wampler;J. Wilgren;L. Zakharov
Two lithium evaporators were used to evaporate more than 100g of lithium on to the NSTX lower divertor region. Prior to each discharge, the evaporators were withdrawn behind shutters, where they also remained during the subsequent HeGDC applied for periods up to 9.5min. After the HeGDC, the shutters were opened and the LITERs were reinserted to deposit lithium on the lower divertor target for 10min, at rates of 10–70mg/min, prior to the next discharge. The major improvements in plasma performance from these lithium depositions include: (1) plasma density reduction as a result of lithium deposition; (2) suppression of ELMs; (3) improvement of energy confinement in a low-triangularity shape; (4) improvement in plasma performance for standard, high-triangularity discharges; (5) reduction of the required HeGDC time between discharges; (6) increased pedestal electron and ion temperature; (7) reduced SOL plasma density; and (8) reduced edge neutral density.