A hyper-Hermitian manifold is a (M,I,J,K)(M,I,J,K) together with a gg that is Hermitian for each member of the hypercomplex triple:

g(IX,IY)=g(JX,JY)=g(KX,KY)=g(X,Y)g(IX,IY)=g(JX,JY)=g(KX,KY)=g(X,Y)

for all tangent vectors X,YX,Y at the same point. Equivalently, every complex structure aI+bJ+cKaI+bJ+cK with a2+b2+c2=1a^2+b^2+c^2=1 is orthogonal for gg. The triple (I,J,K)(I,J,K) and metric gg are chosen data. No closedness or parallelism condition is imposed on the associated fundamental two-forms, so hyper-Hermitian is strictly weaker than hyperkähler.

Associated two-forms

The metric determines three real two-forms

ωI(X,Y)=g(IX,Y),ωJ(X,Y)=g(JX,Y),ωK(X,Y)=g(KX,Y).\omega_I(X,Y)=g(IX,Y),\qquad \omega_J(X,Y)=g(JX,Y),\qquad \omega_K(X,Y)=g(KX,Y).

They encode the same pointwise compatibility as the metric, but they need not be closed. The structure is hyperkähler precisely when all three forms are closed; equivalently, the preserves I,J,KI,J,K.

HKT condition

An is a hyper-Hermitian metric whose three Hermitian Bismut connections coincide. Equivalently, after fixing one complex structure, the corresponding complex two-form satisfies a \partial-closedness condition. Thus HKT adds a differential condition to the pointwise hyper-Hermitian data but is weaker than the hyperkähler condition.

Examples and scope

Quaternionic Hn\mathbb H^n, with its flat metric and complex structures given by multiplication by i,j,ki,j,k, is hyper-Hermitian and in fact hyperkähler. More generally, every is hyper-Hermitian after forgetting the closedness of its three .

A hypercomplex manifold equipped with a Riemannian metric that is Hermitian only for II is a near miss: invariance under JJ and KK is part of the definition and does not follow from invariance under one complex structure.

References
  1. Dominic D. Joyce, Compact Manifolds with Special Holonomy, Oxford University Press, 2000. Oxford DOI record. Relevant: Chapter 7, hyperkähler structures and their underlying hyper-Hermitian data.