Deligne–Lusztig theory: Difference between revisions

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{{for|the linguistics term |Positive (linguistics)}}
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In [[complex geometry]], the term ''positive form''
refers to several classes of real differential forms
of [[Hodge decomposition#Hodge_decomposition|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
:<math>\Lambda^{p,p}(M)\cap \Lambda^{2p}(M,{\Bbb R}).</math>
A real (1,1)-form <math>\omega</math>
is called '''positive''' if any of the
following equivalent conditions hold
 
#<math>\sqrt{-1}\omega</math> is an imaginary part of a positive (not necessarily positive definite) [[Hermitian form]].
#For some basis <math>dz_1, ... dz_n</math> in the space <math>\Lambda^{1,0}M</math> of (1,0)-forms,<math>\sqrt{-1}\omega</math> can be written diagonally, as <math> \sqrt{-1}\omega = \sum_i \alpha_i dz_i\wedge d\bar z_i,</math> with <math>\alpha_i</math> real and non-negative.
#For any (1,0)-tangent vector <math>v\in T^{1,0}M</math>, <math>-\sqrt{-1}\omega(v, \bar v) \geq 0</math>
#For any real tangent vector <math>v\in TM</math>, <math>\omega(v, I(v)) \geq 0</math>, where <math>I:\; TM\mapsto TM</math> is the [[complex structure]]{{dn|date=September 2012}} operator.
 
== Positive line bundles ==
 
In algebraic geometry, positive (1,1)-forms arise as curvature
forms of [[ample line bundle]]s (also known as
''positive line bundles''). Let ''L'' be a holomorphic Hermitian line
bundle on a complex manifold,
 
:<math> \bar\partial:\; L\mapsto L\otimes \Lambda^{0,1}(M)</math>
 
its complex structure operator. Then ''L'' is equipped with a unique connection preserving the Hermitian structure and satisfying
 
:<math>\nabla^{0,1}=\bar\partial</math>.
 
This connection is called ''the [[Hermitian connection|Chern connection]]''.
 
The curvature <math>\Theta</math>  of a Chern connection is always a
purely imaginary (1,1)-form. A line bundle ''L'' is called ''positive'' if
 
:<math>\sqrt{-1}\Theta</math>  
 
is a positive definite (1,1)-form. The [[Kodaira embedding theorem]] claims that a positive line bundle is ample, and conversely, any [[ample line bundle]] admits a Hermitian metric with <math>\sqrt{-1}\Theta</math> positive.
 
== Positivity for ''(p, p)''-forms ==
 
Positive (1,1)-forms on ''M'' form a [[convex cone]].
When ''M'' is a compact [[complex surface]],
<math>dim_{\Bbb C}M=2</math>, this cone is
[[Convex cone#Dual_cone|self-dual]], with respect
to the Poincaré pairing
:<math> \eta, \zeta \mapsto \int_M \eta\wedge\zeta</math>
 
For ''(p, p)''-forms, where <math>2\leq p \leq dim_{\Bbb C}M-2</math>,
there are two different notions of positivity. A form is called
'''strongly positive''' if it is a linear combination of
products of positive forms, with positive real coefficients.
A real ''(p, p)''-form <math>\eta</math> 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
<math>\int_M \eta\wedge\zeta\geq 0 </math>.
 
Weakly positive and strongly positive forms
form convex cones. On compact manifolds
these cones are [[Convex cone#Dual_cone|dual]]
with respect to the Poincaré pairing.
 
==References==
 
*Phillip Griffiths and Joseph Harris (1978), ''Principles of Algebraic Geometry'', Wiley. ISBN 0-471-32792-1
 
*J.-P. Demailly, ''[http://arxiv.org/abs/alg-geom/9410022 L<sup>2</sup> 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)]''.
 
 
 
[[Category:Complex manifolds]]
[[Category:Algebraic geometry]]
[[Category:Differential forms]]

Latest revision as of 12:55, 30 September 2014

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