Positive form#Positive line bundles

{{for|the linguistics term |Positive (linguistics)}}

In complex geometry, the term positive form refers to several classes of real differential forms of Hodge type (p, p).

(1,1)-forms

Real (p,p)-forms on a complex manifold M are forms which are of type (p,p) and real, that is, lie in the intersection \Lambda^{p,p}(M)\cap \Lambda^{2p}(M,{\mathbb R}). A real (1,1)-form \omega is called semi-positiveHuybrechts (2005) (sometimes just positiveDemailly (1994)), respectively, positiveHuybrechts (2005) (or positive definiteDemailly (1994)) if any of the following equivalent conditions holds:

  1. -\omega is the imaginary part of a positive semidefinite (respectively, positive definite) Hermitian form.
  2. For some basis dz_1, ... dz_n in the space \Lambda^{1,0}M of (1,0)-forms, \omega can be written diagonally, as \omega = \sqrt{-1} \sum_i \alpha_i dz_i\wedge d\bar z_i, with \alpha_i real and non-negative (respectively, positive).
  3. For any (1,0)-tangent vector v\in T^{1,0}M, -\sqrt{-1}\omega(v, \bar v) \geq 0 (respectively, >0).
  4. For any real tangent vector v\in TM, \omega(v, I(v)) \geq 0 (respectively, >0), where I:\; TM\mapsto TM is the complex structure operator.

Positive line bundles

In algebraic geometry, positive definite (1,1)-forms arise as curvature forms of ample line bundles (also known as positive line bundles). Let L be a holomorphic Hermitian line bundle on a complex manifold,

: \bar\partial:\; L\mapsto L\otimes \Lambda^{0,1}(M)

its complex structure operator. Then L is equipped with a unique connection preserving the Hermitian structure and satisfying

:\nabla^{0,1}=\bar\partial.

This connection is called the Chern connection.

The curvature \Theta of the Chern connection is always a

purely imaginary (1,1)-form. A line bundle L is called positive if \sqrt{-1}\Theta is a positive (1,1)-form. (Note that the de Rham cohomology class of \sqrt{-1}\Theta is 2\pi times the first Chern class of L.) The Kodaira embedding theorem claims that a positive line bundle is ample, and conversely, any ample line bundle admits a Hermitian metric with \sqrt{-1}\Theta positive.

Positivity for ''(p, p)''-forms

Semi-positive (1,1)-forms on M form a convex cone. When M is a compact complex surface, dim_{\mathbb C}M=2, this cone is self-dual, with respect to the Poincaré pairing : \eta, \zeta \mapsto \int_M \eta\wedge\zeta

For (p, p)-forms, where 2\leq p \leq dim_{\mathbb C}M-2, there are two different notions of positivity.Demailly (1994) A form is called

strongly positive if it is a linear combination of products of semi-positive forms, with positive real coefficients. A real (p, p)-form \eta on an n-dimensional complex manifold M is called weakly positive if for all strongly positive (n-p, n-p)-forms ζ with compact support, we have \int_M \eta\wedge\zeta\geq 0 .

Weakly positive and strongly positive forms form convex cones. On compact manifolds these cones are dual with respect to the Poincaré pairing.

Notes

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References

  • P. Griffiths and J. Harris (1978), Principles of Algebraic Geometry, Wiley. {{isbn|0-471-32792-1}}
  • {{cite web |url=https://hdl.handle.net/20.500.12111/7881 |hdl=20.500.12111/7881 |title=Positivity and Vanishing Theorems |date=3 January 2020 |last1=Griffiths |first1=Phillip }}
  • J.-P. Demailly, [https://arxiv.org/abs/alg-geom/9410022 L2 vanishing theorems for positive line bundles and adjunction theory, Lecture Notes of a CIME course on "Transcendental Methods of Algebraic Geometry" (Cetraro, Italy, July 1994)].
  • {{Citation | author1-last=Huybrechts | author1-first=Daniel | author1-link=Daniel Huybrechts | title=Complex Geometry: An Introduction | publisher=Springer | year=2005 | isbn=3-540-21290-6 | mr=2093043}}
  • {{Citation | author1-last=Voisin | author1-first=Claire | author1-link=Claire Voisin | title=Hodge Theory and Complex Algebraic Geometry (2 vols.) | publisher=Cambridge University Press | year=2007 | orig-year=2002 | isbn=978-0-521-71801-1 | mr=1967689 | doi=10.1017/CBO9780511615344}}

Category:Complex manifolds

Category:Algebraic geometry

Category:Differential forms