Bourbaki

Lemma 4

Tag 09ME, permanent. Cite it as [Bourbaki, Tag 09ME].

Integration, chapter VIII, § 5. The space of closed subgroups

If the group G satisfies the condition (L), the mapping α↦α({e})\alpha \mapsto \alpha(\{e\}) of Γd\Gamma_d into R+∗\mathbf{R}_+^* is vaguely continuous.

Let us consider a measure α∈Γd\alpha \in \Gamma_d; let V0V_0 be a relatively compact open neighborhood of ee in GG such that Hα∩V0={e}H_\alpha \cap V_0 = \{e\} and such that there exists no finite subgroup of GG contained in V0V_0 and not reduced to ee. Let VV be a symmetric compact neighborhood of ee such that V3⊂V0V^3 \subset V_0, and let UU be a symmetric neighborhood of ee such that U2⊂VU^2 \subset V. Let φ\varphi (resp. ψ\psi) be a function in H+(G)\mathscr{H}_+(G), with values in [0,1][0, 1], equal to 1 on V3V^3 (resp. at the point ee) and with support contained in V0V_0 (resp. in UU). The set of measures β∈Γd\beta \in \Gamma_d such that ∣β(φ)−α(φ)∣≤ε|\beta(\varphi) - \alpha(\varphi)| \leq \varepsilon and ∣β(ψ)−α(ψ)∣≤ε|\beta(\psi) - \alpha(\psi)| \leq \varepsilon is a neighborhood WW of α\alpha. We propose to show that, provided ε\varepsilon is taken to be sufficiently small, Hβ∩V={e}H_\beta \cap V = \{e\} for every β∈W\beta \in W; it will then follow that β(ψ)=β({e})\beta(\psi) = \beta(\{e\}), hence that ∣β({e})−α({e})∣≤ε|\beta(\{e\}) - \alpha(\{e\})| \leq \varepsilon, which will prove the lemma.

It will suffice to show that, for β∈W\beta \in W,

(V2−V)∩Hβ=∅. (V^2 - V) \cap H_\beta = \varnothing.

For, suppose that this point is established: then, for xx and yy in V∩HβV \cap H_\beta, one has xy−1∈V2∩Hβxy^{-1} \in V^2 \cap H_\beta; but, by virtue of (8), this implies xy−1∈V∩Hβxy^{-1} \in V \cap H_\beta; in other words, V∩HβV \cap H_\beta is a subgroup of GG, which is obviously discrete and compact, hence finite; but then, by the choice of V0V_0, this implies that indeed V∩Hβ={e}V \cap H_\beta = \{e\}.

Let us argue by contradiction and so assume that there exists a point zz of V2−VV^2 - V that belongs to HβH_\beta; by the choice of UU and VV, we have ψ(sz−1)+ψ(s)≤φ(s)\psi(sz^{-1}) + \psi(s) \leq \varphi(s) in GG, the relation z∉U2z \notin U^2 implying Uz∩U=∅Uz \cap U = \varnothing. Since

∫ψ(sz−1) dβ(s)=∫ψ(s) dβ(s), \int \psi(sz^{-1})\, d\beta(s) = \int \psi(s)\, d\beta(s),

it follows that 2β(ψ)≤β(φ)≤α(φ)+ε2\beta(\psi) \leq \beta(\varphi) \leq \alpha(\varphi) + \varepsilon; but we also have

β(ψ)≥α(ψ)−ε, \beta(\psi) \geq \alpha(\psi) - \varepsilon,
and by construction α(φ)=α(ψ)=α({e})\alpha(\varphi) = \alpha(\psi) = \alpha(\{e\}). We thus arrive at a contradiction by taking ε<α({e})/3\varepsilon < \alpha(\{e\})/3. Q.E.D.

In graphic terms, a group GG satisfying the condition (L) is said to not have arbitrarily small finite subgroups. It can be shown that every Lie group satisfies the condition (L); but this condition is not characteristic of Lie groups; for example, the multiplicative group of pp-adic integers congruent to 1 mod pp satisfies (L).*

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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Cites

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Transcribed from the printed volume. Not translated.