Restrict an isometric action of $G$ on $X$ to an action of a subgroup $K \leq G$.
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The orbit $E \cdot x = \{g \cdot x \mid g \in E\}$ of a point $x$ under a subset $E$ of the group.
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The image $E \cdot Y = \{g \cdot y \mid g \in E,\, y \in Y\}$ of a subset $Y \subseteq X$ under a subset $E$ of the group.
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The stabilizer subgroup $\mathrm{Stab}(x) = \{g \in G \mid g \cdot x = x\}$ of a point $x \in X$.
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A package of data and axioms needed to relate bounded subgroups of a group $G^t$ acting on a $\mathrm{CAT}(0)$ space $X$ to point stabilizers: an isometric action satisfying the negative-curvature inequality, a generalised BN-pair, a group bornology, a base chamber point, and compatibility axioms ensuring boundedness is equivalent to having a bounded orbit.
- X : Type u_5
- metricSpace : MetricSpace self.X
- completeSpace : CompleteSpace self.X
- nci : NegativeCurvatureInequality self.X
- action : IsometricAction Gt self.X
- gbnpair : GeneralizedBNPair Gt M
- bruhatProps : self.gbnpair.strictBNPair.BruhatProperties
- born : CompactSubgroups.GroupBornology Gt
- chamber_point : self.X
- borel_fixes_chamber_point (b : Gt) : b ∈ Subgroup.map self.gbnpair.G.subtype self.gbnpair.strictBNPair.B → self.action.smul b self.chamber_point = self.chamber_point
- Tt_fixes_chamber_point (t : Gt) : t ∈ self.gbnpair.Tt → self.action.smul t self.chamber_point = self.chamber_point
- born_bounded_orbit_at_chamber_point (E : Set Gt) : self.born.isBounded E → Bornology.IsBounded (orbitSet self.action E self.chamber_point)
- orbit_bounded_at_chamber_point_born_bounded (E : Set Gt) : Bornology.IsBounded (orbitSet self.action E self.chamber_point) → self.born.isBounded E
- stabilizer_of_bounded_orbit (x : self.X) (H : Subgroup Gt) : pointStabilizer self.action x ≤ H → Bornology.IsBounded (orbitSet self.action (↑H) x) → H ≤ pointStabilizer self.action x
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The orbit of $x$ under a subgroup $K$ is non-empty (it contains $x$ itself).
The orbit $K \cdot x$ is stable under the restricted action of $K$ on $X$.
If $x_0$ is a fixed point of the restricted action of $K$, then $K$ is contained in the stabilizer of $x_0$.
The orbit of $x$ under its stabilizer is exactly $\{x\}$.
If a subset $E \subseteq G^t$ is bounded with respect to the group bornology, then its orbit $E \cdot x$ is bounded in $X$ for every point $x$.
Converse: if some orbit $E \cdot x$ is bounded in $X$, then $E$ itself is bounded in the group bornology.
Maximality of stabilizers: any strictly larger subgroup $H$ than $\mathrm{Stab}(x)$ fails to be bounded.
If $K$ is a maximal bounded subgroup and $k = \sigma g$ with $\sigma$ in the small torus $T^t$, then $g \in K$ — left factors from $T^t$ can be absorbed into $K$.
Every point stabilizer is bounded in the group bornology.
If both $E \cdot x_0$ and a set $Y$ are bounded, then the action set $E \cdot Y$ is bounded as well.
Acting on the singleton $\{x\}$ recovers the orbit $E \cdot x$.
A cyclic equivalence of three notions of boundedness for a subset $E \subseteq G^t$: boundedness in the group bornology, having a bounded orbit, and producing only bounded images of bounded subsets of $X$.
Every point stabilizer $\mathrm{Stab}(x_0)$ is a maximal bounded subgroup in the group bornology.
Restatement of decomp_stable_in_stabilizer in the finite-type
$B_{\mathrm{idx}}$ setting: $T^t$-factors can be absorbed into a maximal
bounded subgroup.