On a complex manifold, a divisor on a complex manifold is a locally finite formal sum , where ranges over irreducible complex analytic hypersurfaces and . The local algebra needed here is that the local ring , identified in coordinates with convergent power-series germs, is a regular local ring and a unique factorization domain. In particular, each height-one prime is generated by one irreducible germ, and a nonzero meromorphic germ is a quotient of holomorphic germs. Reduced local equations of the same hypersurface differ by a holomorphic unit. These facts include local branches when a globally irreducible hypersurface has several branches at a singular point.
The order of a meromorphic function along a hypersurface is the exponent of its reduced local equation in the quotient's factorization. Equivalently, at a generic smooth point of , write , with a transverse local equation of and a holomorphic unit; then . Changing a reduced equation multiplies it by a unit and leaves unchanged. These local orders agree on overlaps and are constant along the generic smooth locus of an irreducible hypersurface. A nonzero global meromorphic function therefore defines its principal divisor on a complex manifold
Positive coefficients record zeros and negative coefficients record poles.
A local defining function for on is a nonzero meromorphic function whose orders there equal the coefficients of . It can be constructed as the product of local reduced hypersurface equations to the prescribed integer powers. On an overlap, has no zero or pole along any hypersurface. The unique factorization domain property then makes it a nowhere-zero holomorphic function, after choosing representatives of the germs. The holomorphic line bundle associated to a divisor is obtained by gluing holomorphic frames using
These ratios satisfy the cocycle condition, and the expressions agree on overlaps. They form the canonical meromorphic section of a holomorphic line bundle with divisor .
If globally, is a holomorphic unit on , and is a global nowhere-zero holomorphic section. Hence is holomorphically trivial. Conversely, if has a nowhere-zero global holomorphic frame , write with holomorphic units. The coefficients of the canonical meromorphic section of a holomorphic line bundle agree on overlaps and give a nonzero global meromorphic function . Since multiplication by a unit does not change orders, . Therefore
For a smooth hypersurface , the adjunction formula is
Indeed, the holomorphic conormal sequence has first term ; taking its determinant yields , which gives the formula. Here the canonical bundle is the top exterior power of the holomorphic cotangent bundle.
Apply this first to . Its degree- equation is a section of , so . Since , we obtain . The restricted second equation cuts out in and has associated bundle . A second application of adjunction formula gives the canonical bundle of a regular projective complete intersection
It remains to prove that a nonzero exponent cannot yield a trivial holomorphic line bundle on . Choose a connected component and a hyperplane meeting but not containing it. Such a hyperplane exists: a positive-dimensional compact projective submanifold cannot lie entirely in an affine chart, since all its affine coordinate functions would be global holomorphic functions and hence constant. A hyperplane through one point and not another consequently meets properly. Its equation gives a holomorphic section of that has both a zero and a nonzero value. For , the th power has the same two properties. Were trivial, this section would be represented by a global holomorphic function, contradicting its constancy on compact connected . For , triviality would imply triviality of its positive dual power. This proves nontrivial hyperplane powers on a compact projective submanifold and hence
The degrees are positive because the two equations define a hypersurface and a surface of the specified dimensions.
The calculation uses “non-singular” in the usual smooth complete-intersection sense: the equations define reduced smooth divisors, with independent differentials along . If only their reduced zero sets are required to be smooth, polynomial multiplicities cannot determine the canonical bundle. For example, and have the same smooth quartic surface in the hyperplane for every . That surface has trivial canonical bundle, while the displayed polynomial degree sum is . Thus unreduced equations must not be substituted into the adjunction formula for the reduced surface.