Properties of Riemannian, Kähler and hyperKähler manifolds could be seen through dimensional reductions of source spaces (domains) of corresponding quantum SUSY non-linear sigma-models, models whose target spaces (codomains) are the above mentioned manifolds, e.g. you get $N=2$ SUSY QM i.e. quantum superparticle moving in a Riemannian manifold as a dimensional reduction of 2d $N=1+1$ quantum non-linear sigma-model over superMinkowski spacetime (1+1)|(1,1), a quantum non-linear sigma-model which is again a dimensional reduction of 3d $N=2$ quantum non-linear sigma model over superMinkowski spacetime (1+2)|2. $\mathbb{Z}$-grading of forms on a Riemannian manifold is the relic of $R$-symmetry i.e $SO(2)$-group of superPoincare group $P^{3|2}$.
Deformations of the above mentioned SUSY non-linear models are done via superpotentials which are expressed by corresponding real or holomorphic Morse functions.
Read Dan Freed's book about the above mentioned.
Regarding your question, see also:
http://arxiv.org/abs/hep-th/0311064
http://arxiv.org/abs/hep-th/0401175
http://arxiv.org/abs/hep-th/0407122
http://arxiv.org/abs/hep-th/0509163
and
http://arxiv.org/abs/hep-th/0702137
http://arxiv.org/abs/hep-th/0610149
http://arxiv.org/abs/0803.3302
http://golem.ph.utexas.edu/~distler/blog/archives/001030.html
http://golem.ph.utexas.edu/category/2012/07/notes_from_stringmath_2012.html