The ion thermal diffusivities (chi (i)) in DIII-D [J. L. Luxon and L. G. Da
vis, Fusion Technol. 8, 441 (1985)] discharges exhibit a strong nonlinear d
ependence on the measured temperature gradients. In low confinement mode (L
-mode) discharges with low toroidal rotation, the ion thermal diffusivity,
chi (i), has an approximately Heaviside function dependence on the major ra
dius divided by the radial scale length of the ion temperature, R/L-Ti. Whe
n R/L-Ti is less than a critical value, the chi (i)'s are very small. When
R/L-Ti is about equal to the critical value, chi (i) increases rapidly. Alt
hough the gradient profiles for high confinement (H-mode) have a different
shape, they still show a critical gradient type of behavior. This type of d
ependence is consistent with the predictions for transport, which is domina
ted by ion temperature gradient modes and is a strong indicator that these
modes are the main contributors toward L-mode transport in DIII-D and a maj
or contributor to transport in a certain region of DIII-D H-mode discharges
. When strong rotational shear is present, the thermal confinement is impro
ved in regions of the plasma. In these regions, the dependence of the diffu
sivities on the gradients is changed. The type of change is consistent with
the physical picture that when the ExB shearing frequency is greater than
the maximum linear growth rate of the modes as calculated without shear, th
en the modes are stabilized and the transport is reduced. (C) 2001 American
Institute of Physics.