Answer: There is none.
The issue at hand is that the Kaehler invariance is just that - an invariance, not a continuous symmetry of the fields. Most prominently the superpotential must transform as
W→We−h
A general superpotential that leads to consistent theories is
W=12mabϕaϕb+13Yabcϕaϕbϕc
with at least one of the
mab and Yabc non-zero. From this is is obvious, that no transformation of the
fields ϕa exists, such that
W→We−h without redefining the couplings.
Thus, there is a Kaehler invariance, which involves a redefinition of the couplings and has its value on its own (e.g. on non-simply connected internal spaces, the Kaehler potential might only be defined locally, with definitions on different charts being equal up to Kaehler transformations K′=K+f(ϕ)+ˉf(ˉϕ)), but this is not a symmetry in the sense of Noether's theorem.
This post imported from StackExchange Physics at 2014-03-07 13:18 (UCT), posted by SE-user Neuneck