Strong shaping, favourable for stability and improved energy confineme
nt, together with a significant expansion of the central region of imp
roved confinement in negative central magnetic shear target plasmas, i
ncreased the maximum fusion power produced in DIII-D by a factor of 3.
Using deuterium plasmas, the highest fusion power gain, the ratio of
fusion power to input power, Q, was 0.0015, corresponding to an equiva
lent Q of 0.32 in a deuterium-tritium plasma, which is similar to valu
es achieved in tokamaks of larger size and magnetic field. A simple tr
ansformation relating Q to the stability parameters is presented.