The equation for the dressed test mode for the nonlinear ballooning mode turbulence in the presence of the radial electric field has been derived [ 1] asIn this equation, normalization is: rIa ~r,We employ the notation 'tAp = aJ f.lomini IB P'Other notation is standard. The eigenfunction is written as
6(s-a)The contour lines of XH are illustrated in Fig.1 on the a-roE 1 plane. The correction appears in the numerical coefficient G1. The cross-field momentum flux can be calculated by the relation Normalized momentum flux is given as Pe.r = J.lHC% 1 , and the normalized velocity gradient is expressed by wE 1 . Figure 2 illustrates Pe as a function of wE 1 . Viscosity is calculated ,r and is close to X H. It is shown that the radial momentum flux is a decreasing function of the velocity shear in the high rotation shear limit. This indicates that, for a fixed momentum flux, two solutions of the rotation shear are available. This provides a basis for the bifurcation in the radial electric field structure in the H-mode modelling.