In algebraic geometry, Kleiman's theorem, introduced by, 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
Vi\toX,i=1,2
gV1 x XV2
\dimV1+\dimV2-\dimX
gV1
V1\toX\overset{g}\toX
Vi
gV1 x XV2
Statement 1 establishes a version of Chow's moving lemma: after some perturbation of cycles on X, their intersection has expected dimension.
We write
fi
Vi\toX
h:G x V1\toX
(1G,f1):G x V1\toG x X
\sigma:G x X\toX
Let
\Gamma=(G x V1) x XV2
h
f2:V2\toX
\Gamma=\{(g,v,w)|g\inG,v\inV1,w\inV2,g ⋅ f1(v)=f2(w)\}
\Gamma
p:\Gamma\toV1 x V2
G
\dim\Gamma=\dimV1+\dimV2+\dimG-\dimX
q:\Gamma\toG
gV1 x XV2
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
p0:\Gamma0:=(G x V1,) x XV2,\toV1, x V2,
q0:\Gamma0\toG
\square