“…The structures obtained in this way define a holonomy reduction to the group SU (1, 1) ∼ = SL(2, R) and are an indefinite analog of hyperkähler structures which have holonomy SU (2) ∼ = Sp (1). Mathematically, these structures are described by quadruples (g, I, S, T ) where g is a signature (2, 2) metric and I, S, T are parallel endomorphisms of the tangent bundle such that: I 2 = −S 2 = −1, T = IS = −SI, g(IX, IY ) = −g(SX, SY ) = g(X, Y ) (1) In the literature such structures are called hypersymplectic [18], neutral hyperkähler [22], para-hyperkähler [8,12], pseudo-hyperkähler [13], etc. They are not preserved by a conformal change of the metric and a natural conformally invariant generalization is to relax the condition for covariant constancy of I, S, T to their integrability (see Section 2).…”