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Kleiman's theorem

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In algebraic geometry, Kleiman's theorem, introduced by Kleiman (1974), concerns dimension and smoothness of scheme-theoretic intersection after some perturbation of factors in the intersection.

Precisely, it states: given a connected algebraic group G acting transitively on an algebraic variety X over an algebraically closed field k and V i X , i = 1 , 2 {\displaystyle V_{i}\to X,i=1,2} morphisms of varieties, G contains a nonempty open subset such that for each g in the set,

  1. either g V 1 × X V 2 {\displaystyle gV_{1}\times _{X}V_{2}} is empty or has pure dimension dim V 1 + dim V 2 dim X {\displaystyle \dim V_{1}+\dim V_{2}-\dim X} , where g V 1 {\displaystyle gV_{1}} is V 1 X g X {\displaystyle V_{1}\to X{\overset {g}{\to }}X} ,
  2. (Kleiman–Bertini theorem) If V i {\displaystyle V_{i}} are smooth varieties and if the characteristic of the base field k is zero, then g V 1 × X V 2 {\displaystyle gV_{1}\times _{X}V_{2}} is smooth.

Statement 1 establishes a version of Chow's moving lemma: after some perturbation of cycles on X, their intersection has expected dimension.

Sketch of proof

We write f i {\displaystyle f_{i}} for V i X {\displaystyle V_{i}\to X} . Let h : G × V 1 X {\displaystyle h:G\times V_{1}\to X} be the composition that is ( 1 G , f 1 ) : G × V 1 G × X {\displaystyle (1_{G},f_{1}):G\times V_{1}\to G\times X} followed by the group action σ : G × X X {\displaystyle \sigma :G\times X\to X} .

Let Γ = ( G × V 1 ) × X V 2 {\displaystyle \Gamma =(G\times V_{1})\times _{X}V_{2}} be the fiber product of h {\displaystyle h} and f 2 : V 2 X {\displaystyle f_{2}:V_{2}\to X} ; its set of closed points is

Γ = { ( g , v , w ) | g G , v V 1 , w V 2 , g f 1 ( v ) = f 2 ( w ) } {\displaystyle \Gamma =\{(g,v,w)|g\in G,v\in V_{1},w\in V_{2},g\cdot f_{1}(v)=f_{2}(w)\}} .

We want to compute the dimension of Γ {\displaystyle \Gamma } . Let p : Γ V 1 × V 2 {\displaystyle p:\Gamma \to V_{1}\times V_{2}} be the projection. It is surjective since G {\displaystyle G} acts transitively on X. Each fiber of p is a coset of stabilizers on X and so

dim Γ = dim V 1 + dim V 2 + dim G dim X {\displaystyle \dim \Gamma =\dim V_{1}+\dim V_{2}+\dim G-\dim X} .

Consider the projection q : Γ G {\displaystyle q:\Gamma \to G} ; the fiber of q over g is g V 1 × X V 2 {\displaystyle gV_{1}\times _{X}V_{2}} and has the expected dimension unless empty. This completes the proof of Statement 1.

For Statement 2, since G acts transitively on X and the smooth locus of X is nonempty (by characteristic zero), X itself is smooth. Since G is smooth, each geometric fiber of p is smooth and thus p 0 : Γ 0 := ( G × V 1 , sm ) × X V 2 , sm V 1 , sm × V 2 , sm {\displaystyle p_{0}:\Gamma _{0}:=(G\times V_{1,{\text{sm}}})\times _{X}V_{2,{\text{sm}}}\to V_{1,{\text{sm}}}\times V_{2,{\text{sm}}}} is a smooth morphism. It follows that a general fiber of q 0 : Γ 0 G {\displaystyle q_{0}:\Gamma _{0}\to G} is smooth by generic smoothness. {\displaystyle \square }

Notes

  1. Fulton (1998, Appendix B. 9.2.)
  2. Fulton (1998, Example 11.4.5.)

References


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