Definition

Let XX be a with complex structure JJ. A Kähler metric is a Riemannian metric gg whose associated real fundamental 22-form

ω(X,Y)=g(JX,Y)\omega(X,Y)=g(JX,Y)

is closed:

dω=0.d\omega=0.

Equivalently, ω\omega is a , and (X,J,g)(X,J,g) is a with specified metric data. The positivity and JJ-invariance belong to the Hermitian hypothesis, while closedness is the additional Kähler condition. The metric gg is real bilinear; the corresponding Hermitian form on the is sesquilinear.

Equivalent characterizations

For a , the Kähler condition is equivalent to J=0\nabla J=0 for the Levi–Civita connection. It is also equivalent to the Levi–Civita and on the holomorphic tangent bundle agreeing. In holomorphic coordinates, the Hermitian coefficient matrix (gjkˉ)(g_{j\bar k}) satisfies

gjkˉz=gkˉzj.\frac{\partial g_{j\bar k}}{\partial z^\ell} = \frac{\partial g_{\ell\bar k}}{\partial z^j}.

The closed-form and local-coordinate conditions are given in Demailly, Chapter VI, §4, Definition 4.1.

Structure and consequences

The fundamental form of a Kähler metric is nondegenerate, so it also makes XX a . The Levi–Civita connection preserves gg, JJ, and ω\omega, and its holonomy is contained in U(n)U(n). Locally, the metric coefficients are complex Hessians of real . These compatibilities are special: an arbitrary Hermitian metric need not have closed .

Examples and non-examples

The Euclidean metric on Cn\mathbb C^n, flat Hermitian metrics on complex tori, and the on are Kähler. If n>1n>1, multiplying a Kähler metric by efe^f for a nonconstant real function ff usually gives only a Hermitian metric, because its fundamental form is efωe^f\omega and

d(efω)=efdfωd(e^f\omega)=e^f\,df\wedge\omega

need not vanish.

References
  1. Daniel Huybrechts, Complex Geometry: An Introduction, Springer, 2005. Publisher record. Relevant: §3.1, Kähler metrics and their fundamental forms.
  2. Jean-Pierre Demailly, Complex Analytic and Differential Geometry, 2012. Author-hosted text. Relevant: Chapter VI, §4, especially Definition 4.1 and Theorem 4.8.