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Projective bundle

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In mathematics, a projective bundle is a fiber bundle whose fibers are projective spaces.

By definition, a scheme X over a Noetherian scheme S is a Pn-bundle if it is locally a projective n-space; i.e., {\displaystyle X\times _{S}U\simeq \mathbb {P} _{U}^{n and transition automorphisms are linear. Over a regular scheme S such as a smooth variety, every projective bundle is of the form {\displaystyle \mathbb {P} (E)} for some vector bundle (locally free sheaf) E.[1]

The projective bundle of a vector bundle#edit

Every vector bundle over a variety X gives a projective bundle by taking the projective spaces of the fibers, but not all projective bundles arise in this way: there is an obstruction in the cohomology group H2(X,O*). To see why, recall that a projective bundle comes equipped with transition functions on double intersections of a suitable open cover. On triple overlaps, any lift of these transition functions satisfies the cocycle condition up to an invertible function. The collection of these functions forms a 2-cocycle which vanishes in H2(X,O*) only if the projective bundle is the projectivization of a vector bundle. In particular, if X is a compact Riemann surface then H2(X,O*)=0, and so this obstruction vanishes.

The projective bundle of a vector bundle E is the same thing as the Grassmann bundle {\displaystyle G_{1}(E)} of 1-planes in E.

The projective bundle P(E) of a vector bundle E is characterized by the universal property that says:[2]

Given a morphism f: T → X, to factorize f through the projection map p: P(E) → X is to specify a line subbundle of f*E.

For example, taking f to be p, one gets the line subbundle O(-1) of p*E, called the tautological line bundle on P(E). Moreover, this O(-1) is a universal bundle in the sense that when a line bundle L gives a factorization f = p ∘ g, L is the pullback of O(-1) along g. See also Cone#O(1) for a more explicit construction of O(-1).

On P(E), there is a natural exact sequence (called the tautological exact sequence):

{\displaystyle 0\to {\mathcal {O_{\mathbf {P} (E)}(-1)\to p^{*}E\to Q\to 0}

where Q is called the tautological quotient-bundle.

Let E ⊂ F be vector bundles (locally free sheaves of finite rank) on X and G = F/E. Let q: P(F) → X be the projection. Then the natural map O(-1) → q*F → q*G is a global section of the sheaf hom Hom(O(-1), q*G) = q* G ⊗ O(1). Moreover, this natural map vanishes at a point exactly when the point is a line in E; in other words, the zero-locus of this section is P(E).

A particularly useful instance of this construction is when F is the direct sum E ⊕ 1 of E and the trivial line bundle (i.e., the structure sheaf). Then P(E) is a hyperplane in P(E ⊕ 1), called the hyperplane at infinity, and the complement of P(E) can be identified with E. In this way, P(E ⊕ 1) is referred to as the projective completion (or "compactification") of E.

The projective bundle P(E) is stable under twisting E by a line bundle; precisely, given a line bundle L, there is the natural isomorphism:

{\displaystyle g:\mathbf {P} (E){\overset {\sim }{\to \mathbf {P} (E\otimes L)}

such that {\displaystyle g^{*}({\mathcal {O(-1))\simeq {\mathcal {O(-1)\otimes p^{*}L.}[3] (In fact, one gets g by the universal property applied to the line bundle on the right.)

Examples#edit

Many non-trivial examples of projective bundles can be found using fibrations over {\displaystyle \mathbb {P} ^{1 such as Lefschetz fibrations. For example, an elliptic K3 surface {\displaystyle X} is a K3 surface with a fibration

{\displaystyle \pi :X\to \mathbb {P} ^{1

such that the fibers {\displaystyle E_{p for {\displaystyle p\in \mathbb {P} ^{1 are generically elliptic curves. Because every elliptic curve is a genus 1 curve with a distinguished point, there exists a global section of the fibration. Because of this global section, there exists a model of {\displaystyle X} giving a morphism to the projective bundle[4]

{\displaystyle X\to \mathbb {P} ({\mathcal {O_{\mathbb {P} ^{1(4)\oplus {\mathcal {O_{\mathbb {P} ^{1(6)\oplus {\mathcal {O_{\mathbb {P} ^{1)}

defined by the Weierstrass equation

{\displaystyle y^{2}z+a_{1}xyz+a_{3}yz^{2}=x^{3}+a_{2}x^{2}z+a_{4}xz^{2}+a_{6}z^{3

where {\displaystyle x,y,z} represent the local coordinates of {\displaystyle {\mathcal {O_{\mathbb {P} ^{1(4),{\mathcal {O_{\mathbb {P} ^{1(6),{\mathcal {O_{\mathbb {P} ^{1, respectively, and the coefficients

{\displaystyle a_{i}\in H^{0}(\mathbb {P} ^{1},{\mathcal {O_{\mathbb {P} ^{1(2i))}

are sections of sheaves on {\displaystyle \mathbb {P} ^{1. Note this equation is well-defined because each term in the Weierstrass equation has total degree {\displaystyle 12} (meaning the degree of the coefficient plus the degree of the monomial. For example, {\displaystyle {\text{deg(a_{1}xyz)=2+(4+6+0)=12}).

The contact bundles, and more generally Grassmann bundles, are projective bundles. The unit tangent bundle of a Riemannian manifold is a double cover of its projectivized tangent bundle.

Cohomology ring and Chow group#edit

Let X be a complex smooth projective variety and E a complex vector bundle of rank r on it. Let p: P(E) → X be the projective bundle of E. Then the cohomology ring H*(P(E)) is an algebra over H*(X) through the pullback p*. Then the first Chern class ζ = c1(O(1)) generates H*(P(E)) with the relation

{\displaystyle \zeta ^{r}+c_{1}(E)\zeta ^{r-1}+\cdots +c_{r}(E)=0}

where ci(E) is the i-th Chern class of E. One interesting feature of this description is that one can define Chern classes as the coefficients in the relation; this is the approach taken by Grothendieck.

Over fields other than the complex field, the same description remains true with Chow ring in place of cohomology ring (still assuming X is smooth). In particular, for Chow groups, there is the direct sum decomposition

{\displaystyle A_{k}(\mathbf {P} (E))=\bigoplus _{i=0}^{r-1}\zeta ^{i}A_{k-r+1+i}(X).}

As it turned out, this decomposition remains valid even if X is not smooth nor projective.[5] In contrast, Ak(E) = Ak-r(X), via the Gysin homomorphism, morally because that the fibers of E, the vector spaces, are contractible.

See also#edit

References#edit

  1. ^ Hartshorne 1977, Ch. II, Exercise 7.10. (c).
  2. ^ Hartshorne 1977, Ch. II, Proposition 7.12.
  3. ^ Hartshorne 1977, Ch. II, Lemma 7.9.
  4. ^ Propp, Oron Y. (2019-05-22). "Constructing explicit K3 spectra". arXiv:1810.08953 [math.AT].
  5. ^ Fulton 1998, Theorem 3.3.

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