Definition

Let XX be a of complex dimension nn. Its canonical bundle is the top exterior power

KX=nT1,0X=ΩXnK_X=\bigwedge\nolimits^n T^{*1,0}X=\Omega_X^n

of the . It is a whose fiber at xx consists of alternating complex nn-linear forms on Tx1,0XT_x^{1,0}X. In holomorphic coordinates z1,,znz^1,\ldots,z^n, the form dz1dzndz^1\wedge\cdots\wedge dz^n is a local holomorphic frame. Thus local sections are holomorphic top-degree forms, and the bundle is determined without choosing a metric or orientation.

Coordinate transformations

Under a holomorphic coordinate change w=w(z)w=w(z), the standard local frames satisfy

dw1dwn=det(wz)dz1dzn.dw^1\wedge\cdots\wedge dw^n =\det\left(\frac{\partial w}{\partial z}\right) dz^1\wedge\cdots\wedge dz^n.

The is nowhere zero on a coordinate overlap, so these factors are precisely the of KXK_X. This also explains why top forms, rather than their coefficient functions alone, are coordinate-independent objects.

Sections and triviality

A of KXK_X is a holomorphic nn-form. A nowhere-vanishing global holomorphic nn-form determines an isomorphism KXX×CK_X\cong X\times\mathbb C; conversely, any holomorphic trivialization supplies such a form. The form is additional data, however: triviality asserts existence and does not choose a preferred trivializing section.

Examples and scope

On Cn\mathbb C^n, the form dz1dzndz^1\wedge\cdots\wedge dz^n trivializes the canonical bundle. For the Riemann sphere, the coordinate change w=1/zw=1/z gives dw=z2dzdw=-z^{-2}dz; its canonical bundle is therefore nontrivial and has degree 2-2.

References
  1. Daniel Huybrechts, Complex Geometry: An Introduction, Springer, 2005. DOI record. Relevant: §2.2, holomorphic cotangent bundles, exterior powers, and the canonical bundle.
  2. Phillip Griffiths and Joseph Harris, Principles of Algebraic Geometry, Wiley, 1978. DOI record. Relevant: Chapter 0, holomorphic vector bundles and differential forms.