General relativity is derived from an action which is quadratic in the
covariant derivative of certain spinor 1-form gravitational potential
s. Either a pair of two-component spinor 1-forms or a single Dirac spi
nor 1-form can be employed. The metric is a quadratic function of thes
e spinor 1-forms. In the two-component spinor formulation the action d
iffers from the usual chiral action for general relativity by a total
differential. In the Dirac spinor formulation the action is the real p
art of the former one. The Hamiltonian is related to the ones in posit
ive energy proofs and spinorial quasilocal mass constructions.