Algebraic representations of ergodic actions
Based on joint work with Alex Furman, and earlier litterature.
Thanks to Sami Douba for his help with notetaking.
Today, we start with basics on measure spaces and algebraic varieties. Later on, we shall merge both subjects together.
1. Ergodic theory of algebraic varieties
1.1. Algebraic actions
is a local field. For simplicity, characteristic is but most of what I will say extends to positive characteristic. Also to nonlocal complete normed fields. is an algebraic group acting algebraically on an algebraic variety . Then acts on . We equip with the -topology, it is second countable and locally compact.
Questions. What can one say of the structure of orbits?
Examples. acting on has orbits, one open and one closed. Let , triangular matrices, diagonal matrices, unipotent matrices. Then -orbits are concentric circles, -orbits are the origin, two halflines and two halfplanes. -orbits are the origin, four halflines and branches of hyperbolas. -orbits are points of the -axis and two halplanes.
We observe that orbits are open or closed, except for halflines which are nearly closed: intersections of an open and a closed set. We call such sets locally closed
Fact: Orbits of algebraic actions are locally closed.
Consequences.
-invariant open sets separate points in distinct orbit in . It follows that the quotient topology on is second countable and (topology separates points). This is known as Chevalley Theorem (combined with a result of Borel-Serre).
The Borel structure on is countably separated. It follows that there exists a Borel embedding of to .
A fundamental theorem of Descriptive Set Theory states that all uncountable Polish topological spaces (completely metrizable, admitting a countable dense subset) are isomorphic as Borel spaces. See Kechris’ book. Such Borel spaces are called standard Borel spaces.
Examples. Finite sets, countable sets, a separable Hilbert space.
A Borel space is said to be countably separated if there exists a countable collection of Borel sets that separates points (equivalently, space has a Borel embedding into ). Standard Borel sets have this property.
We take this encouraging fact as an invitation to do ergodic theory.
1.2. measures and measure classes
Say two measures on a Borel space are equivalent if they have the same sigma-ideal of null sets. A measure class could be understood as the choice of a sigma-ideal.
Warning. Not every sigma-ideal comes from a measure. For instance, the sigma-ideal of meager sets does not arise from a measure.
Examples.
has a natural volume measure class.
has the Haar measure class.
For every closed subgroup , has a unique -invariant measure class, called the Haar class. Warning: very rarely does admit a -invariant measure. For instance, acting on projective space has no invariant measure in the Haar class. More generally, when is simple and is parabolic, has no invariant measure in the Haar class.
If is a locally compact group, Haar measure is finite iff is compact. If is a closed normal subgroup, then has a finite invariant measure iff is cocompact in .
Definition 1 Say that a -invariant measure class on is ergodic if every -invariant Borel set is either null or full (complement is null).
Equivalently, every a.e. defined Borel -invariant map is a.e. constant. Here, can be replaced with any countably separated space.
Corollary 2 Every -ergodic measure class on is supported on a single orbit. Moreover, it coincides with the Haar class on this orbit.
Indeed, think of the action as a -map where is a -ergodic space. Since is countably separated, this map must be a.e. constant. This leads to a map to an orbit. This must be a Borel and measure class isomorphism, thanks to the uniqueness of the Haar class.
In the nonergodic case, one can use ergodic decompositions.
Definition 3 Given a -measure class on , since is countably separated, for every measure in the class, there exists a family of -invariant measures on , , such that is a Haar measure on the orbit denoted by , and
This is the ergodic decomposition of .
In particular, the measure class is fully determined by the class of the pushed-forward measure .
1.3. Classification of -invariant probability measures
If is a normal -algebraic subgroup, which is cocompact, then has a finite Haar measure. By Noetherianity, there exists a minimal element among such cocompact normal -algebraic subgroups. In fact, is a least element. Indeed, given and , maps to a closed subset of hence is compact.
Theorem 4 If has no compact factors (i.e. ), then every -invariant probability measure on is supported on fixed points.
In general, every -invariant probability measure on is supported on the -fixed points.
Example. For acting on , the only -invariant probability measure is the Dirac mass at the origin. Same picture for , and (with as many invariant measures as there are measure on the -axis). However, has a lot of invariant measures.
This implies Borel’s density theorem.
Theorem 5 (Borel) If has no compact factor, and is a lattice, then is Zariski-dense in .
Indeed, let be the Zariski closure of , then push the -invariant probability measure from to . It must be supported on a fixed point, i.e. is a point.
1.4. Generalization
Fix a locally compact sigma-compact group and a representation . Then acts on . The orbit space is complicated, but still is a -map. Same reasoning yields: every -invariant ergodic measure is supported on a unique -orbit.
Theorem 6 There exists a minimal normal -subgroup such that
has precompact image.
Every -invariant measure on a -algebraic variety is supported on the -fixed points.
Consider , for .
Corollary 7 The stabilizer of a measure is compact modulo the fixator of the Zariski-support of .
Fact (Zimmer). The action of on has locally closed leaves.
1.5. Some more ergodic theory
A Lebesgue space is a standard Borel space equipped with a measure class.
By a map from a Lebesgue space to a Borel space , we mean an equivalence class of Borel maps : defined almost everywhere, up to almost everywhere equality. The space of such maps is denoted by .
A morphism of Lebesgue spaces is a map which sends null sets to null sets.
Let be a locally compact second countable group. Then has a standard Borel space structure and a Lebesgue space structure. An -Lebesgue space is a Lebesgue space with a homomorphism such that is a morphism.
An action of on is ergodic if every -invariant map is essentially constant, for every standard Borel space .
Definition 8 Fix an action of on . Say it is
- Doubly ergodic if the diagonal action on is ergodic.
- metrically ergodic if for every isometric action of on a separable metric space , every -equivariant map is (essentially) constant.
- Weakly mixing if for every ergodic probability measure preserving action of on , the diagonal action on is ergodic.
- Has no compact factors if for every continuous homomorphism to a compact group and any compact subgroup , for every map (equipped with Haar measure), .
Easy fact. .
Indeed, if is doubly ergodic and acts isometrically on , the distance defines an invariant function on , hence constant. If the constant is not zero, the ilage of is discrete in , hence countable (since is separable), contradiction.
If is metrically ergodic and has a pmp action on , an invariant function on gives rise to an equivariant map . Since probability measure is invariant, is equivariant and the action on is isometric. Now is separable, so is constant.
If is weakly mixing and is a compact factor, one can assume . Take . The map is -equivariant , hence constant, so is a single point.
Easy fact. If the action of on is probability measure preserving, then .
Indeed, it suffices to prove that . One can assume that metric space has an invariant probability measure , fully supported, and that is complete. One easily shows that is compact. Then is compact. It must act transitively on , . Under assumption 4, is a point, this is .
1.6. metric ergodicity
Nonexample. Let be a compact subgroup. Let be a homomorphism. Then the action of on is not metrically ergodic.
Example. Let be a countable group. Let be a probability space. Then the shift action of on is metrically ergodic.
Indeed, , and the shift action on is ergodic.
Claim. Let be a noncompact -simple algebraic group. Let be a lattice, a noncompact closed subgroup. Then the action of on and the action of on is metrically ergodic.
Indeed, metric ergodicity passes to lattices (pass from to ). For the action, this follows from Howe-Moore. Indeed, the action of on the pmp space is mixing. This implies decay of coefficients. Their restrictions to any closed noncompact subgroup decay, hence the mixing action of .
1.7. Amenability
Definition 9 (Zimmer) The action of on is amenable if there exists an -equivariant conditional expectation
Note that amenability implies the following weaker “baby amenability”, which is often used: for every compact convex -space , there exists an -map .
Example. If is an amenable subgroup, the action of on is amenable.
Fact. For every locally compact second countable group , there exists an action of on some Lebesgue space which is both amenable and metrically ergodic (the Furstenberg boundary).
Example. Let be a noncompact -simple algebraic group. Let be a lattice, let be a noncompact amenable subgroup. Then the action of on is both amenable and metrically ergodic.
2. Algebraic representations of ergodic actions
Now we merge algebraic groups and ergodic actions. Fix a locally compact second countable group , an action of on a Lebesgue space , a local field and an algebraic -group , . Fix a continuous homomorphism .
Definition 10 An algebraic representation of the action of on with respect to is a –-variety and an -equivariant map .
A morphism between to such AREAs and is a –-morphism such that .
Example. Let be a closed subgroup. Consider the action of on . Every algebraic representation of this action is given by a pair and a point in which is fixed by the Zariski closure of in .
If is Zariski dense, we get a map from to , where
We get an AREA , and for every AREA , we have a unique morphism such that .
In other words, is an initial object in the category of AREAs of . This holds in general.
Theorem 11 Let act ergodically on . Then there exists an initial object in the category of AREAs associated with , of the form
We think of an ergodic action of as a generalization of a closed subgroup, up to conjugacy. The theorem states that the initial object is indeed a Zariski-closed subgroup.
Proof of Theorem 11. Consider the set of -algebraic subgroups of such that there exists a, AREA . This is nonempty. By Noetherianity, one can pick a minimal element (it will turn out to be a minimum, up to conjugacy, but it is harder). We show that the map is an initial object.
Consider an other AREA . Consider the diagonal representation
By ergodicity, the image of lies in one single -orbit . Composing with projection, we get a -map , hence an embedding up to conjugacy. By minimality, . The other projection provides us with a -map , which is unique.
Theorem 12 Assume the action of on is pmp, is -simple and is unbounded (i.e. not contained in a compact subgroup). Then the initial object is trivial: any representation of is constant. Indeed, an -invariant probability measure on exists only if is precompact.
2.1. Consequences
Theorem 13 (Bader-Furman-Gorodnik-Weiss) Let be a noncompact -simple algebraic group. Let be a lattice, let be a noncompact -algebraic subgroup. Consider the -action on . For the inclusion of into , the initial object is the identity .
Application. Every Borel map which commutes with is a homothety.
Indeed, let be a -map. Let be the composition of with . Set
Then is right--invariant and left--invariant. Since the action of on is pmp and weakly mixing, is constant. Thus there exists such that , , i.e. is a -map.
Theorem 14 Let be an amenable and metrically ergodic -space. Let be a -simple algebraic group. Let be an unbounded homomorphism. Then there exists an initial object where is a proper subgroup.
Indeed, let be a parabolic subgroup of . Since acts on the convex space , by amenability, there exists an -map . Since -orbits in are locally closed, the image of the -map is contained in a single orbit , where is the stabilizer of a measure . By the structure theorem on measure stabilizers, the fixator of the Zariski hull of the support of is cocompact in . Up to conjugacy, it is contained in .
Assume that is trivial. Then is compact, acts by isometries on the separable space . By metric ergodicity, the -map is constant, which contradicts the assumption that is unbounded in .
Therefore, is not normal. is contained in the normalizer of in , which is a proper -algebraic subgroup of . The composition is a nontrivial AREA for with respect to .
3. Lattices in products
Today, we are aiming at rigidity results for lattices. Before entering the subject, let me sum up where we had reached last time.
3.1. AREAs continued
The tension between ergodicity and the very simple structure of algebraic actions creates an initial object in the category of AREAs. We call gate the initial object, because it is our entrance gate into the algebraic world.
Two theorems:
- Theorem 12. For a pmp and metrically ergodic action, the gate is trivial.
- Theorem 14. For amenable and metrically ergodic actions, the gate is nontrivial.
Remark: unbounded amenable subgroups of are not Zariski-dense.
3.2. Leftover from last time : functoriality
Proposition 15 Fix . The gate defines a functor from the category of -ergodic actions and the category of -algebraic -(coset)-varieties.
3.3. Introduction to lattices in products
Examples.
is a lattice in .
is a lattice in .
is a lattice in .
Definition 16 A lattice in a product is irreducible if its projections to both factors are dense subgroups.
Equivalently, the action of on each factor is ergodic.Equivalently, the actions of and of on are ergodic.
Equivalently, the action of each on is ergodic.
Indeed, the action of on equipped with the weak topology is continuous.
3.4. Commensurability
Assume that is totally disconnected locally compact. Then there exists a compact open subgroup . Any two are commensurable. Say a subgroup is commensurated if for all , and are commen surable.
Let be an irreducible lattice. Let be a compact open subgroup. Then
is commensurated in , it is a lattice in . Hence is a lattice which is commensurated by the dense subgroup .
Conversely, assume that where is a lattice, is commensurated and is dense. Then one can reconstruct from these data. There exists a totally disconnected group , a dense embedding , and a precompact embedding such that is an irreducible lattice. It is called the Schlichting completion of .
This indicates that lattices in products Lietdlc are simpler that lattices in Lie groups, in the sens that we have a dual way of looking at them.
3.5. Superrigidity
Theorem 17 Let be an irreducible lattice. Let be a -simple group, let is Zariski dense and unbounded. Then superrigidity holds: extends uniquely to a continuous homomorphism and factors through one of the factors.
Corollary 18 If are as above (i.e. is commensurated and is dense), is -simple and is Zariski dense and unbounded on , then extends uniquely to a continuous homomorphism .
Indeed, the case where extends to is excluded.
3.6. Application to arithmeticity
Apply previous theorem to a lattice in and conclude that a lattice is arithmetic iff it has a dense commensurator.
3.7. Preparation for the proof
Fix an action of on a Lebesgue space which is amenable and metrically ergodic.
Claim. The diagonal action of on is amenable and metrically ergodic.
Indeed, assume is a nonempty -compact convex space. Then is nonempty, it is an -compact convex space (viewed as a subset of ). Therefore, there exists an -map . I.e., there exists an -map . This proves amenability.
Let be an -isometric metric space. Any -map is a.e. independant on the variable, and on the variable, therefore a.e. constant.
Corollary 19 For every irreducible lattice in , the action of on is amenable and metrically ergodic.
Of course, the action of on is not ergodic, it is proper, but
Claim. The action of on is ergodic.
Before proving the claim, let us start with a general fact.
Given an action of on , when is the restriction to ergodic? Answer is : iff the action of on is ergodic. Indeed, one can mod out by a proper action: the space of -orbits in , denoted by , is well defined, since the diagonal -action on is conjugated to the action on the -factor only, trivial on the factor. In fact, .
Applying this to the claim, ergodic on ergodic on ergodic on is implies by metric ergodicity of on .
This proves the claim.
3.8. Proof of superrigidity theorem
Again, fix an action of on a Lebesgue space which is amenable and metrically ergodic. The action of on is amenable and metrically ergodic. According to Theorem 14, the gate is nontrivial, i.e. .
Pick a generic -orbit in , identify it with . Get a map . The ergodic action of on yields a gate , the normalizer of in . Mod out by , get a -map . By ergodicity, we get a map .
3.9. Assume that
By simplicity of , . So the -action on has a nontrivial representation , whence a -representation . There exists a gate where . By ergodicity of the -action on , we get a -equivariant map (where , where is the normalizer of ) from to . Again by ergodicity, there is a -invariant point in . It also fixed by the Zariski-closure of , which is . Hence , is normal in . By simplicity, . So the above morphism to was to . The formula
defines an -invariant (hence constant) map . In other words, . This implies that . Composing with the projection , we get whose restriction to equals . So we are done under the assumption that . This was the easiest case.
3.10. From no on, assume that
Then , so . We have an -equivariant map (equivariant w.r.t. ).
Compose this map with , the diagonal. This is an AREA of to . By ergodicity of on , there is a gate where . Let us show that we are done if .
Assume that . Let us mod out the left -action. This mods out the -action in the gate, thus I get an -map from to a nontrivial quotient of . As before, we get an extension of to .
From now on, assume that . acts on . Since is equal ti its own normalizer in , the gate factors via a map , so extends as before.
4. Margulis superrigidity
Let be a real semisimple group of higher rank, let be an irreducible lattice. Margulis superrigidity states that every Zariski-dense unbounded homomorphism uniquely extends to .
The case when is a product has been treated. Next time, I will prove the case when is simple. I explain now that we are not too far from it.
Consider , . It is amenable, noncompact, and its centralizer is the upper diagonal . The -action on is amenable and metrically ergodic. acts on and we get a gate .
I would like to indicate a related geometric context without groups acting, that of -buildings, covered by Caprace-Lecureux. At infinity, such buildings have an exotic projective plane. It has a large group of projectivities (in fact a pseudogroup of maps from lines to lines). This yields a large group acting on the boundary of a tree. It plays the role of . It is not too hard to show that this group is linear iff the building is classical. It follows that is linear iff the building is classical.
4.1. Remarks on lattices in products
- The superrigidity theorem holds for lattices in products of factors for any .
- Nonarithmetic examples are known only for yet.
- The examples are Kac-Moody groups acting on twin buildings and Burger-Mozes and Wise examples acting on products of trees.
4.2. A new category of representations
For the proof of Margulis superrigidity, we need to modify the concept of AREA. Up to now, we represented an action on Lebesgue space . Now we need to represent pairs of closed subgroups of a locally compact second countable group .
The objects in our category are now the following data:
- two closed subgroups and of ,
- an algebraic -group ,
- a -algebraic subgroup that commutes with ,
- a homomorphism and a continuous and Zariski-dense homomorphism ,
- a representation, i.e. a measurable map which is -equivariant.
Theorem 20 Let be a lattice. Assume that the action of on is ME. Then there exists an initial object (a gate), i.e. a -equivariant map
where and .
The proof follows similar lines as Theorem 11. Pick a minimal .
4.3. The nontriviality theorem
Theorem 21 Let be a lattice. Assume that the action of on is ME. Assume further that is amenable, is -simple and is unbounded, then the gate is not trivial.
Indeed, consider the action on . By amenability and ME, there exists a proper subgroup and a representation , under homomorphism . The gate will be a deeper object, but this suffices to prove that the gate is nontrivial.
4.4. Functoriality
Assume that is a noncompact simple -algebraic group. Let be a lattice. Recall that for every closed noncompact , the actions of on and of on are ME (this is Howe-Moore’s theorem). We now show that this gives right to extra invariants.
Fix , . Consider the category of -actions, i.e.
- the objects are closed, noncompact subgroups ,
- the morphisms are elements of acting on the right and conjugating the right action of into the right action of on .
Consider next the category of -spaces:
- the objects are ‘s acting on -space , commuting with ,
- the morphisms are –-morphisms of varieties .
The gate functor assigns to a -action of on an orbit with action of . To a morphism given by element , the gate associates a unique morphism of algebraic varieties .
In particular, we get a map . The group . On the other hand, . This homomorphism is a nontrivial datum: it gives extra invariance to the representation .
Corollary 22 If normalize each other. Then they have the same gate .
I really mean, the same map serves as a gate for both.
4.5. Proof of Margulis superrigidity
Recall our goal. Let be a real semisimple group of higher rank, let be an irreducible lattice. Margulis superrigidity states that every Zariski-dense unbounded homomorphism uniquely extends to .
Fact. There exist closed noncompact abelian subgroups generating such that each commutes with .
In fact, this is equivalent to higher rank.
Example. . The first three ‘s are -parameter subgroups of the Heisenberg group of upper unipotent matrices, the three next are -parameter subgroups of the opposite Heisenberg group of lower unipotent matrices.
Geometrically speaking, it means that one can move from any geodesic to any other by travelling within finitely many maximal flats.
Now we embark in the proof. By Corollary 22, all the ‘s have the same gate , equivariant with respect to . By ergodicity, the -invariant point is invariant under the Zariski closure of , i.e; b y , so , is normal in . Since is amenable, so .
So the gate is , equivariant with respect to .
defines a pull-back map from the algebra of polynomial functions on , , to -valued functions on , . It is injective, since its Zariski support is . This embeds as a -invariant subalgebra of for all , hence an -invariant subalgebra. This gives an -action of on extending the actions of the . Thus acts on on the right, when a homomorphism . The gate is -equivariant, this implies that extends to . End of proof.
4.6. Rank one
Let be a real semisimple group of rank one, let be an irreducible lattice. Let be a Zariski-dense unbounded homomorphism. What extra assumptions should we make to show that extends?
For , let , , , ,… denote the -gate.
Lemma 23 Let be a parabolic. If , then extends.
Indeed, consider , hence , .
Since and generate , extends as before.
Lemma 24 Assume that there exists a simple, noncompact subgroup and a -representation , equivariant with respect to , with . Then is not in the kernel of .
Indeed, is noncompact. By a finite number of up and down steps of taking normalizers we reach (two steps should be sufficient). All these intermediate normalizers have the same gate. Assume by contradiction that . Then the -gate equals the -gate, which thus factors by . This map is both and -invariant, but and generate . Thus , contradiction.
Note that the assumption of Lemma 24 never holds if and is nonarchimedean.
4.7. Relation to arithmeticity
Definition 25 Say that is compatible (with ) if for all proposer subgroups of , , where .
Let where . Le ne an orreducible lattice.
Fact. There exists a unique minimal number field such that is defined over and up to conjugation and finite index.
Theorem 26 (Margulis arthmeticity criterion) is arithmetic if and only iff its image is precompact in any place other than . I.e. for every embedding to a local field, either is precompact or and .
Supperrigidity implies arithmeticity. Indeed, take . Can assume that it is adjoint. For every embedding , the image of the composition is precompact unless . By an argument of Borel-Tits, one gets .
Observe that one need only a few targets to get arithmeticity.
Theorem 27 (Bader-Fisher-Miller-Stover) If there exists in infinitely many immersed maximal totally geodesic subspaces of dimension , then the assumption of Lemma 24 holds for all ‘s relevant to arithmeticity.
Corollary 28 is defined over the ring of integers of a number field.
Exercise. For , , the group is compatible. In particular, if there exist infinitely many immersed maximal totally geodesic subspaces of dimension , then is arithmetic. (Special care is needed for ).
5. Apafic Gregs
Talk given in Fanny Kassel’s seminar, on Oct. 11th, 2021, dedicated to Margulis, Perlman and Baldi.
Joint work with Alex Furman.
How to produce a random element of a group? In fact, a sequence. We will study linear representations of such random elements.
5.1. GREGs
Definition 29 Let be a probability space. Let be an ergodic invertible pmp transformation of . Let be a locally compact second countable group. Let be a map. The Greg is the data .
Examples.
Compact. Let , , an irrational rotation.
Random walk. Fix and a probability measure on . Let , shift, projection to the -th coordinate. The resulting Greg is a random walk.
Markov chain. Fix a graph with probability transitions (i.e. for each vertex , a probability measure on the set of edges emanating from ), set of paths in the graph, some Gibbs measure associate. Decorate edges with elements of . This defines a map .
Geodesic flow. Let be a compact negatively curved Riemannian manifold. Let denote the unit tangent bundle of . geodesic flow. Let . Fix a fundamental domain. For each time , there is a map which tells which group element drags back to the fundamental domain. One can decorate the picture with a flat bundle.
5.2. Associated constructions
Let be the minimal -algebra such that is measurable. Given , let . Assume that .
Let equipped with the future -algebra . Let equipped with the past -algebra (I view these as factors of ). Then maps , . It turns out that can be reconstructed from the pair , using the natural extension construction.
Definition 30 Let be a pmp map which is not invertible. One constructs another system, with an invertible transformation, by taking the inverse limit of
Example. , shift, then the natural extension is .
Theorem 31 If is ergodic on , then its natural extension on is metrically ergodic.
Here, metrically ergodic means that for every metric extension (i.e. a family of complete separable metric spaces on which a lift of acts isometrically, there exists an equivariant section.
Fact. The map defines a cocycle as follows. For , , and for ,
The cocycle identity
holds. Then a map is defined by
Whence an action of on .
The projections and , when modded out by , yield the factors and . If instead one mods out by , one gets the space of -ergodic components of , and factors and . I think of these as ideal futures and pasts.
Theorem 32 , and are amenable -spaces, the maps and are -metrically ergodic.
5.3. Asymptotic past and future independence condition
Definition 33 Say that the asymptotic past and future independence condition (apafic) is satisfied if the map is measure class preserving.
In other words, if you were born poor, you still may become rich. It holds for all examples above but the compact example.
If the Greg is Apafic, then the pair is called a Boundary pair. The spaces are amenable and the maps and are metrically ergodic.
Theorem 34 Let be a simple -algebraic group. Let be Zariski-dense. Then there exist opposite parabolic subgroups and measurable equivariant maps , and .
Moreover, if , is the minimal parabolic.
View the Cartan projection as a leftinvariant -valued metric on . Let be the composition of with and Cartan projection,
Subadditivity shows that converges to an interior point of the Weyl chamber . This is called “simplicity of the spectrum”.
I view apafic gregs as a useful generalization of random walks, and we see that the simplicity of the spectrum theorem holds for them.
Tholozan, Ledrappier: See Avila-Viana for the Markov chain version.
> Let be a simple -algebraic group. Let be Zariski-dense. Then there exist opposite parabolic subgroups and measurable equivariant maps , and .
Moreover, if , is the minimal parabolic.
View the Cartan projection as a leftinvariant -valued metric on . Let be the composition of with and Cartan projection,
Subadditivity shows that converges to an interior point of the Weyl chamber . This is called “simplicity of the spectrum”.
I view apafic gregs as a useful generalization of random walks, and we see that the simplicity of the spectrum theorem holds for them.
Tholozan, Ledrappier: See Avila-Viana for the Markov chain version.