Definition

Let (M,J)(M,J) be a . A Kähler form is a real differential 22-form ω\omega such that

dω=0,ω(JX,JY)=ω(X,Y),ω(X,JX)>0d\omega=0,\qquad \omega(JX,JY)=\omega(X,Y),\qquad \omega(X,JX)>0

for every nonzero real tangent vector XX. The second condition says that ω\omega has complex type (1,1)(1,1), and the third is positivity. These conditions make ω\omega nondegenerate, so it is also a . The formula

g(X,Y)=ω(X,JY)g(X,Y)=\omega(X,JY)

defines a JJ-invariant Riemannian metric, called the associated Kähler metric.

Equivalent metric formulation

Conversely, the ω(X,Y)=g(JX,Y)\omega(X,Y)=g(JX,Y) of a is a Kähler form exactly when it is closed. Thus specifying a Kähler form on (M,J)(M,J) is equivalent to specifying a , and it makes (M,J,g)(M,J,g) a Voisin, §3.1.

Local potentials

Every Kähler form is locally expressible as

ω=iˉφ\omega=i\,\partial\bar\partial\varphi

for a real strictly plurisubharmonic function φ\varphi, with a constant factor changed under other dcd^c conventions. Adding the real part of a holomorphic function to φ\varphi does not change ω\omega. This potential description is local; a global potential need not exist.

Examples and conventions

The standard form i2jdzjdzˉj\frac{i}{2}\sum_j dz^j\wedge d\bar z^j on Cn\mathbb C^n is Kähler, as is the Fubini–Study form on . Some authors use ω(X,Y)=g(X,JY)\omega(X,Y)=g(X,JY), which reverses the sign relative to the convention here and therefore changes the corresponding positivity inequality.

References
  1. Claire Voisin, Hodge Theory and Complex Algebraic Geometry I, Cambridge University Press, 2002. DOI record. Relevant: §3.1, Kähler metrics and forms.
  2. Daniel Huybrechts, Complex Geometry: An Introduction, Springer, 2005. DOI record. Relevant: Chapter 3, Kähler forms and local potentials.