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Holomorphic line bundles and meromorphic sections on a Riemann surface

Definition

Let X be a Riemann surface with maximal holomorphic atlas A (Riemann surfaces and holomorphic atlases). A smooth complex line bundle π:E→X is a smooth real rank-two vector bundle whose fibres carry complex vector-space structures and which has local trivializations θi:E∣Ui→Ui×C that are complex-linear on each fibre. The transition functions are defined by θi∘θj−1(x,v)=(x,gij(x)v),gij:Ui∩Uj→C×. A holomorphic line bundle is such a bundle with a trivializing cover by domains of holomorphic charts for which every gij is holomorphic. These functions obey gijgjk=gik on triple overlaps. Conversely, a holomorphic C×-valued cocycle on a supplied countable open cover constructs a holomorphic line bundle: regard each scalar as its real 2×2 multiplication matrix, apply the smooth cocycle construction, and note that the resulting transitions commute with multiplication by i and are holomorphic.

Write ei=θi−1(1) for the associated local frame. A smooth section has the form s=fiei locally, with fi∈C∞(Ui;C) and fi=gijfj on overlaps. It is holomorphic when each fi is holomorphic; H0(X,E) denotes the complex vector space of holomorphic sections. A meromorphic section is a family of meromorphic functions fi with the same transition law. For a nonzero meromorphic section, define its order at p by ord⁡p(s):=ord⁡zi(p)(fi) in any holomorphic chart and local frame. Its divisor is (s):=∑p∈Xord⁡p(s) p; this sum is locally finite and is finite when X is compact.

The canonical bundle is K:=Λ1,0T∗X. If zi,zj are holomorphic coordinates on an overlap, then its transition function in the convention above is gij=dzj/dzi: a local differential satisfies fi dzi=fj dzj. Hence holomorphic sections of K are precisely holomorphic differentials, and meromorphic sections of K are meromorphic differentials (Meromorphic differentials, orders and residues). The conjugate cocycle gij‾ defines Λ0,1T∗X=K‾, while Λ0,0T∗X=X×C. Thus the bundles of E-valued (0,0)- and (0,1)-forms are E and Λ0,1T∗X⊗E; locally the latter has the form f(z) dzˉ⊗e (Bigraded complex forms and the Dolbeault operators, The exterior power bundle of the cotangent bundle).

For a holomorphic line bundle E, the Dolbeault operator is ∂ˉE:C∞(X,E)⟶C∞(X,Λ0,1T∗X⊗E),∂ˉE(fei):=(∂zˉf) dzˉ⊗ei in a holomorphic frame ei and coordinate z. It is C-linear, satisfies ∂ˉE(fs)=∂ˉf⊗s+f ∂ˉEs, and ∂ˉEs=0 exactly when s is holomorphic. It extends coefficientwise to E-valued forms: in a holomorphic frame, ∂ˉE(α⊗ei)=(∂ˉα)⊗ei. This extension satisfies ∂ˉE2=0 and ∂ˉE(β∧s)=∂ˉβ∧s+(−1)deg⁡ββ∧∂ˉEs for complex-valued forms β. The complex dual E∗ has inverse holomorphic cocycle gij−1 and its corresponding Dolbeault operator.

Facts & Assumptions

Given: A connected Riemann surface X with its maximal atlas, a smooth complex line bundle E→X, holomorphic trivializations and their transition functions, and a meromorphic section when order or divisor is discussed.

[F1]
[F2]

A smooth vector bundle is locally trivial with linear fibre maps; smooth sections have smooth local components in a frame. A smooth cocycle on a supplied countable cover constructs a smooth real vector bundle (Smooth vector bundles, rank, fibres, and trivial bundles, Vector bundle charts and transition functions, Construction of a vector bundle from a smooth cocycle, Local and global frames of a vector bundle, Smooth sections, local sections, and support, Smoothness of a section is equivalent to smooth local components).

[F3]

Complex forms split by type, d=∂+∂ˉ, and the scalar Dolbeault operator obeys the square-zero and graded Leibniz identities (A smooth differential k-form, The wedge product of differential forms, The exterior power bundle of the cotangent bundle, Bigraded complex forms and the Dolbeault operators, The d, partial and dbar identities).

[F4]

A meromorphic function has isolated zeros and poles unless it is identically zero; a nonzero holomorphic function has a finite zero order and a local factorization by that power. The identity theorem applies on each connected chart. The transition law for a meromorphic differential is hj(w)=hi(z(w))z′(w), equivalently hi dzi=hj dzj (Meromorphic functions on a plane domain, Isolated singularities: removable, poles, and essential singularities, Identity theorem for holomorphic functions, The order of a zero is the exponent in its local holomorphic factorization, Holomorphic maps and meromorphic functions on Riemann surfaces, Meromorphic differentials, orders and residues).

[F6]

The smooth dual of a vector bundle is defined fibrewise; for a complex line the complex-linear dual transition is the inverse scalar (Dual and Hom vector bundles).

Proof

technique · direct local verification
1.1F1F2given

The fibrewise complex-linear trivializations give smooth transitions in C× and composition of the maps θi∘θj−1 gives gijgjk=gik. For a supplied countable holomorphic cocycle, its real multiplication matrices are smooth GL(2,R) transitions, so [F2] constructs the underlying smooth rank-two bundle; these matrices commute with the standard complex structure, and their holomorphicity makes the local total-space charts holomorphic.

1.2F1F3F4givenalgebra

In a local frame ei, the cotangent line K is spanned by dzi. If zj=ϕ(zi), then dzj=ϕ′(zi)dzi and a differential ω=fidzi=fjdzj has fi=(dzj/dzi)fj. Since ϕ′ is holomorphic and nowhere zero, these are holomorphic line-bundle transitions; a local section of K is holomorphic or meromorphic exactly when its coefficient fi is, so these sections are precisely the corresponding differentials. Conjugation gives the stated transitions for K‾, and the type decomposition gives the local formulas for E-valued forms.

1.3F1F4given

Let Z be the set of points having a neighborhood on which the section is zero. It is open. If p is in its closure, choose a connected chart and frame around p; the meromorphic coefficient has zeros accumulating at p. A pole at p is impossible because its finite principal part is nonzero on a punctured neighborhood, and otherwise the holomorphic identity theorem makes the coefficient identically zero near p. Thus Z is closed; since X is connected and the section is nonzero, Z=∅. Each local representative consequently has a finite Laurent order at every point. Under a change of frame it is multiplied by a holomorphic unit, and under a coordinate change its argument is composed with a biholomorphism with nonzero derivative; neither operation changes the zero or pole order. Its zeros and poles are therefore locally isolated, so the divisor is locally finite and has finite support on compact X.

1.4F3F5givenalgebra

On an overlap with zj=ϕ(zi) and ej=gijei, a section has coefficients fi=gijfj. The chain rule and holomorphy of gij give ∂ˉfi=gij∂ˉfj as (0,1)-forms, so the local formula defines a global operator. The same calculation applies to E-valued forms; the scalar graded Leibniz rule gives the displayed rule, and scalar ∂ˉ2=0 gives ∂ˉE2=0. By [F5], its kernel on sections is exactly the holomorphic sections.

2.1F2F6step 1.1step 1.2step 1.3step 1.4∎

In the complex-linear dual frame the transition is gij−1, which is holomorphic and nonvanishing, so the dual is a holomorphic line bundle and the same local construction defines ∂ˉE∗. The preceding coordinate and frame calculations establish all stated definitions and well-definedness claims. No choice principle is used.

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