Abstract
When the low-confinement mode (L-mode) edge has relatively high electron temperature and weak ion temperature gradient, for example, as observed in the ECH-heated low-density plasmas, the trapped electron mode (TEM) can play an important role in the low to high confinement (L-H) transition as well as the L-mode edge transport, instead of the resistive ballooning or ion temperature gradient mode (RBM or ITG). Motivated by this, a study is first presented about, among several types of the TEM, which one is the most dominant in the above L-mode edge condition, showing that it is dominated by a mixture of the density gradient driven and dissipative TEMs. The parameter dependence of the growth rate of this dominant TEM type is then checked, showing that it has the scaling qualitatively similar to the H-mode threshold power one observed in plasmas where the TEM can be a dominant mode. Closely related to this, a discussion is also given about the L-H transition expected in plasmas where the TEM is assumed to be dominant. Unlike the typical L-H transition that is believed to occur in the RBM-dominant plasmas, it is conjectured to take place in one-step form, with no generation or negligible role of the limit-cycle-oscillation, thus requiring a larger threshold power.
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