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No invariant projective-line probability for two unipotents with distinct fixed lines

Statement

Let P1(R) be the real projective line with the natural action of SL2(R) (The real projective line and the action of SL2(R)). Let u1,u2∈SL2(R) be unipotent matrices, meaning ui≠I and (ui−I)2=0, whose fixed lines in R2 are distinct. There is no Borel probability measure on P1(R) (The Borel sigma-algebra of a topological space, Measures on sigma-algebras, Probability measures and probability spaces) invariant under both u1 and u2, where invariance means μ(uiA)=μ(A) for every Borel set A. In particular, no Borel probability measure is invariant under both u+=(1101) and u−=(1011).

Facts & Assumptions

Given: Two nonidentity unipotent matrices u1,u2∈SL2(R) with distinct fixed lines, and a Borel probability measure on P1(R) invariant under their projective actions.

[F1]

The natural action is a group action by homeomorphisms, and in the projective coordinate t=x/y the point [t:1] is finite while [1:0]=∞ (The real projective line and the action of SL2(R), Homeomorphism, open map, closed map, embedding, and what it means for a property to be topological).

[F2]

A Borel probability measure has total mass 1 and is countably additive on pairwise disjoint Borel sets (The Borel sigma-algebra of a topological space, Measures on sigma-algebras, Probability measures and probability spaces).

[F3]

A homeomorphism and its inverse carry Borel sets to Borel sets; hence pushing a Borel probability forward by a projective action gives a Borel probability (The Borel sigma-algebra of a topological space, Homeomorphism, open map, closed map, embedding, and what it means for a property to be topological).

[F4]

The finite chart is an open copy of R in the one-point compactification model of P1(R); its half-open bounded intervals are Borel (The real projective line and the action of SL2(R), The Borel sigma-algebra of a topological space).

Proof

Breuillard's Exercise §2 III.5 asks for a uniform failure of invariance under two specific elementary matrices and notes the projective-line consequence; it supplies no proof of that exercise. Bekka–de la Harpe–Valette prove the related full-SL2(R) assertion using all translations and inversion. The argument here proves the stated two-element result directly, including arbitrary distinct fixed lines.

Proof technique: conjugate the fixed lines to the coordinate axes, then partition the finite chart into translation intervals.

1.1F1algebra

Write Ni=ui−I. Choose wi with vi:=Niwi≠0. Since Ni2=0, Nivi=0; the vectors vi,wi are independent, because applying Ni to a linear relation forces the coefficient of wi to vanish. They form a basis of R2, and Ni(avi+bwi)=bvi, so im⁡Ni=ker⁡Ni=Rvi, the fixed line Li. Distinctness makes D=det⁡[v1 v2]≠0, so S=[v1 D−1v2]∈SL2(R). In this basis S−1N1S kills the first coordinate vector and has image in its span, while S−1N2S kills the second and has image in its span; both are nonzero. Therefore S−1u1S=(1c01) and S−1u2S=(10c′1) for some c,c′≠0.

2.1F1F2F3step 1.1

Let α=(S−1)∗μ, so α(A)=μ(SA) for Borel A. By [F1, F3], this is a Borel probability measure. If vi=S−1uiS, then α(viA)=μ(SviA)=μ(uiSA)=μ(SA)=α(A), so α is invariant under both displayed matrices.

3.1F2F4step 2.1algebra

The first displayed matrix acts on finite t=x/y by t↦t+c and fixes ∞. Put d=∣c∣>0 and σ=c/d∈{−1,1}, and for each integer k set Ak=[kd,(k+1)d). These Borel sets partition R and translation by c sends Ak to Ak+σ, so invariance gives them all a common mass a≥0. For every n≥0, the 2n+1 disjoint sets A−n,…,An have total mass (2n+1)a≤1; hence a=0. Enumerating the integer indices as 0,1,−1,2,−2,… and using [F2] gives α(R)=α(⋃k∈ZAk)=0, so α({∞})=1.

4.1F2F4step 2.1step 3.1

The second displayed matrix sends [1:0]=∞ to [1:c′], a finite point because c′≠0. Invariance would give α({[1:c′]})=α({∞})=1, contradicting α(R)=0 from step 3.1. Thus no invariant probability measure under both u1,u2 exists.

5.1step 1.1step 4.1algebra∎

The matrices u+ and u− are nonidentity unipotents; their fixed lines are respectively R(1,0) and R(0,1), which are distinct. Applying steps 1.1–4.1 proves the particular assertion as well. A single unipotent does preserve the Dirac probability at its fixed line, so requiring two distinct fixed lines is essential.

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