Solution

ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2013/iii/paper-17/1/solution

The divisor determines the bundle through its local equations. Choose an open cover on which has a reduced holomorphic defining equation , using on sets disjoint from . Because is a complex submanifold of codimension of a submanifold one, its ideal is locally generated by a coordinate; consequently is a nowhere-zero holomorphic function on each overlap. Inside the sheaf of meromorphic functions on a complex manifold, consider the locally free sheaf of rank one
These local descriptions agree on overlaps. With , its transition functions of a vector bundle are specified by
The ratios satisfy the Čech cocycle condition, and the associated holomorphic line bundle associated to a divisor is . The section is holomorphic and vanishes to order one along . Replacing by , with a holomorphic unit, replaces the frame by without changing the subsheaf of meromorphic functions. Refining the cover changes no local sections either. This proves choice independence up to isomorphism rather than merely producing a bundle for one cover.
For a complex manifold of dimension , the canonical bundle is
It is the holomorphic line bundle of holomorphic top-degree differential forms. To compute it on Complex projective space, let be the complex tautological line bundle, so that is the hyperplane line bundle. At a line , the tangent space is . Tensoring the tautological quotient sequence by gives the Euler sequence on complex projective space
Taking the top exterior power gives ; taking its dual bundle yields
Here a negative tensor power means the corresponding positive tensor power of the dual bundle.
The proposed sections over form a sheaf: compatible maps into glue uniquely, and their projections remain . Addition and multiplication by holomorphic functions are defined in the fibres of , making this a sheaf of -modules. If is a holomorphic local frame of on , every section over has the unique expression
Thus the sheaf is a locally free sheaf of rank one. Its transition functions of a vector bundle are those of composed with , so the corresponding pullback vector bundle is precisely . This proves invertibility locally and compatibility globally.
For the local blowup of a complex manifold at a point, work on the projective chart and write
All the incidence equations reduce to . Therefore gives a holomorphic coordinate chart isomorphic to . On an overlap with ,
which is a biholomorphism where . The incidence subset is closed in the product of two Hausdorff spaces and is covered by these charts; hence it is a complex manifold of dimension . In each chart the exceptional fibre is , so it is a smooth complex submanifold, with its induced projective coordinates giving
Away from the origin the inverse of the projection is , which is holomorphic; the projection is therefore a biholomorphism outside .
To find the canonical bundle, pull back the nowhere-zero top form on . In the chart above, its Jacobian determinant gives
The sign depends only on the ordering of the coordinates. This is a section of with divisor on a complex manifold exactly : it has that vanishing order in every exceptional chart and no zeros elsewhere. A nonzero meromorphic section of a holomorphic line bundle with divisor identifies its holomorphic line bundle with , by sending the local generator of to the nowhere-zero frame obtained by dividing the section by . Consequently
This also includes , when the local map is an isomorphism and the exponent is zero.
For a general complex manifold, choose a coordinate neighbourhood of , with sent to , and replace by the inverse image of this coordinate neighbourhood in the local blowup of a complex manifold at a point. Glue this space to along using the preceding biholomorphism. The resulting charts give a complex manifold and a holomorphic map ; the exceptional fibre is and the map is a biholomorphism off that fibre. For completeness, the local projection is proper because its inverse image over a compact subset is closed in that subset times compact Complex projective space. This ensures the gluing is Hausdorff: separate points with distinct images downstairs, and points over inside the local blowup. The atlas is second countable as well.
The top exterior power of the differential defines a global holomorphic bundle map . Equivalently, it is a section of . The same local Jacobian determinant has vanishing order on , and the differential is invertible elsewhere. Applying the holomorphic line bundle associated to a divisor construction gives the canonical bundle formula for a point blowup

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