Simulations of the L–H transition dynamics with different heat and particle sources<xref ref-type="fn" rid="cpb150792fn1">*</xref>

Simulations of the L–H transition dynamics with different heat and particle sources*

Li Hui-Dong^a), Wang Zhan-Hui^b), Weiland Jan^c), Feng Hao^a), Sun Wei-Guo^a),^d)

Profiles of (a) electron density n _e, (b) electron temperature T _e, (c) ion temperature T _i, (d) poloidal velocity V _p, (e) toroidal velocity V _t (for velocity V , positive refers to the clockwise direction and negative the anticlockwise direction), and (f) the E × B flow shear rate ω _{E × B} profiles (lines with circles) at t = 140 ms and the initial profiles at t = 0 ms (lines with squares). Transport barriers of the electron density, electron temperature, and the ion temperature produced. The flow shear near the boundary is observed.