Coarse Kernels of Group Actions
Abstract.
In this paper, we study the coarse kernel of a group action, namely the normal subgroup of elements that translate every point by a uniformly bounded amount. We give a complete algebraic characterization of this object. We specialize to spaces and show that the coarse kernel must be virtually abelian, characterizing when it is finite or cyclic in terms of the curtain model. As an application, we characterize the relation between the coarse kernels of the action on a space and the induced action on its curtain model. Along the way, we study weakly acylindrical actions on quasi-lines.
1. Introduction
The goal of this paper is to study certain stabilizers of group actions. Within the framework of groups acting on metric spaces, one is often interested in the properties that depend solely on the quasi-isometry type of the action. In other words, the object of interest must remain invariant under -equivariant quasi-isometries. Consequently, the kernels of actions are not ideal objects of investigation. Instead, it is more appropriate to consider their coarse versions, which possess this stability feature. In the current work, we study the coarse kernel of a group action, namely the subgroup consisting of elements that translate every point by a uniformly bounded amount.
Definition 1.1.
Let be a group acting on a metric space . Define the coarse kernel of the action to be
This coarse kernel then serves as a suitable analog to the kernel of a group action. We remark that our coarse kernels are different from the ones of [LV23], where the focus is on the analogue of kernels for coarse groups. Our first result is to show that, quite surprisingly, for a geometric action, the coarse kernel can be described in purely algebraic terms. In the theorem below, denotes the center of the group .
Theorem 1.2.
Let be a group acting properly discontinuously and co-boundedly on a metric space . Then, .
In particular, if is abelian, then , which can be shown to hold for all co-bounded isometric actions. Similarly, in the presence of negative curvature, for instance, when a hyperbolic group acts on its Cayley graph, one expects the coarse kernel to be finite. We focus on spaces, which interpolate between the two cases above, and show the following.
Theorem 1.3.
Let be a co-bounded space, and let act on properly discontinuously. Suppose that has an unbounded orbit in the curtain model Then, is virtually cyclic. Moreover, if an orbit of in is not a quasi-line either, then is finite.
The curtain model was introduced by Petyt, Spriano, and Zalloum in [PSZ24], and is a hyperbolic space associated to a space that \sayencodes the hyperbolicity of . This allows us to make precise the intuition that a group acting on a space that is hyperbolic enough needs to have a small coarse kernel. We remark that does not need to act co-compactly on . When we add that assumption, we obtain a significantly stronger characterization of the coarse kernel. Specifically, we are able to identify the algebraic structure of the coarse kernel based on certain geometric constrains on .
Theorem 1.4.
Let be a space, and let act on geometrically. Then,
(i) is virtually for some .
(ii) If moreover is unbounded, then is virtually cyclic.
(iii) If furthermore is not a quasi-line, then is the largest finite normal subgroup of .
After the first draft of this paper was completed, it was pointed out to us that item (iii) also follows from [BJ24, Corollary 1.6]. However, our proof and their proof uses different techniques.
Our second line of investigation is concerned more directly on the curtain model, and follows on the program started in [PSZ24] of better understanding the group via its action on the curtain model. A natural question to ask is how much the action of on might forget information. We show that, from the perspective of coarse kernels, the action of on retains as much information as the action of on .
Theorem 1.5.
Let be a proper space with being unbounded, and let act on co-compactly. Then, .
Further, for a group acting geometrically the result above gives a complete characterization of when and coincide.
Corollary 1.6.
Let be a group acting geometrically on a space . Then, exactly one of the following holds.
-
(1)
is unbounded and hence ;
-
(2)
is bounded, , and ;
-
(3)
is bounded, has infinite index in and .
1.1. Weak acylindricity
In order to prove Theorem 1.4, we will need to study weakly acylindrical actions on a quasi-line which is a topic of independent interest. We recall the definition of weak acylindrical action.
Definition 1.7.
Let be a group acting on a metric space . The action of is said to be weakly acylindrical if for each there exists such that for any with , only finitely many satisfy .
In this setting, we extend a well-known result for acylindrical actions on a quasi-line.
Theorem 1.8.
Let be a roughly geodesic hyperbolic space. Let act on weakly acylindrically with a quasi-line orbit. Then is virtually .
As a corollary, we establish the following result, which can be viewed as a counterpart to the ping-pong lemmas for spaces, thereby helping us better understand the curtain model towards the Tits Alternative.
Theorem 1.9.
Let be a group acting geometrically on a space . Let be any subgroup of . If , then is virtually .
1.2. Coarse stabilizers of sets
We, in fact, develop the proof of Theorem 1.2 in the broader context of coarse stabilizers of subsets , which generalise the coarse kernel .
Definition 1.10.
Let be a group acting on a metric space and let . Define the coarse stabilizer of Y to be .
The coarse stabilizers are a very well-studied object in geometric group theory. Typically, the set is unbounded; otherwise . In this sense, one can see that by varying , one interpolates between and the coarse kernel . We now give a complete algebraic characterization of the coarse stabilizer when coarsely coincides with an orbit of a finitely generated subgroup of . In particular, this shows that when acts geometrically on , we recover Theorem 1.2. In the theorem below, denotes the centralizer of in .
Theorem 1.11.
Let be a metric space, and suppose acts on properly discontinuously and co-boundedly. Let be finitely generated, and let coarsely coincide with an orbit of . Then, .
Acknowledgement
This work was done as part of an undergraduate research project under the supervision of Davide Spriano. Davide suggested the initial problems which evolved into this paper, and his insights helped me resolve many queries. His dedicated time also helped me acquire the necessary background knowledge and assisted in refining several of the proofs. I am extremely grateful to Davide for taking the time to supervise this project and would like to thank him for all his guidance and support. I would also like to thank Harry Petyt for his kind help, which enhanced my understanding of the topic, and for his helpful input on an earlier draft of the paper.
2. Background
In this section, we present definitions and established results necessary to prove our main theorems later. The references for this material are [PSZ24] and [CCMT15].
2.1. Curtain Model
We briefly discuss the curtain model associated with any space , as defined in [PSZ24]. Essentially, the curtain model is the set equipped with a new metric . We aim to choose the metric so that becomes a hyperbolic space.
The main ingredient in defining is the notions of curtains and that of separation.
Definition 2.1 (Definition 2.1 in [PSZ24]).
Let be a space, and let be a geodesic. For a number with in the interior of , the curtain dual to at is
Here denotes the closest-point projection onto .
Definition 2.2 (Definition 2.2 in [PSZ24]).
Let be a space, and let be a curtain. The halfspaces determined by are and . Note that is a partition of . If and are subsets of such that and , then we say that separates from .
Next, we define chains and the chain distance.
Definition 2.3 (Definition 2.9 in [PSZ24]).
A set of curtains is a chain if separates from for all . We say that separates if every does. The chain distance from to is .
This allows us to define the notion of an -chain.
Definition 2.4 (Definition 2.11 in [PSZ24]).
Let . Disjoint curtains and are said to be -separated if every chain meeting both and has cardinality at most . If is a chain of curtains such that each pair is -separated, then we refer to as an -chain.
Now, we use the notion of -chains to define a family of metric spaces corresponding to .
Definition 2.5 (Definition 2.15 in [PSZ24]).
Given distinct points , set and define .
Remark.
One can check that is indeed a metric on and that for all .
Finally, we define the curtain model by combining all the -metrics on .
Definition 2.6.
Fix a sequence such that
Then, where for any .
We record the following basic fact, which tells us how distances in the curtain model are bounded in terms of the distances in .
Lemma 2.7.
for all .
Proof.
. ∎
Now, we state some properties of the curtain model.
Firstly, we note that is -hyperbolic in the sense of Gromov’s four point condition, for some . We also examine how the properness of a group action on a space is revised when we move to the curtain model .
This is summarised in Theorem 2.8 below, which follows directly from Proposition 9.5, Theorem 9.10, and Proposition 9.16 of [PSZ24].
Theorem 2.8.
Let be a space. Then, is a roughly geodesic hyperbolic space. Moreover, if is a group acting properly discontinuously on , then the induced action of on is weakly acylindrical.
Now, we look at how the Gromov boundary of embeds in the visual boundary of . This will be needed in section 5 to prove Theorem 1.5.
Theorem 2.9 (Theorem L in [PSZ24]).
Let be a proper space. Then the space embeds homeomorphically as an -invariant subspace of , and every point in the image of is a visibility point of . The embedding is induced by the change-of-metric map . Moreover, if is nonempty and is cobounded, then is dense in .
2.2. Actions on a Hyperbolic Space
Here, we briefly review Gromov’s classification of group actions on hyperbolic spaces as given in Section 3.A of [CCMT15]. We will use this in Section 5 to prove Theorem 1.3.
Firstly, we recall Gromov’s classification of isometries of hyperbolic spaces in terms of the translation length.
Definition 2.10.
Let be a metric space and be an isometry of . Then, the translation length of is .
Remark.
One can check that is well-defined and is independent of the choice of .
Let be a hyperbolic space. An isometry of is called -
• Elliptic if has bounded orbits.
• Parabolic if has unbounded orbits and .
• Hyperbolic if .
Next, we recall the notion of the Gromov boundary of a hyperbolic space and that of the limit set of a group in .
Fix a base point . Define the Gromov product of points with respect to as . A sequence in is said to be Cauchy-Gromov if as . For convenience, we will write to mean .
Remark.
Note that . So the notion of a Cauchy-Gromov sequence is independent of the base point .
Define an equivalence relation on the Cauchy-Gromov sequences as follows: two sequences and are equivalent, denoted , if as .
Definition 2.11.
Let be a hyperbolic space. The gromov boundary of is .
Definition 2.12.
Let be a group acting on a hyperbolic space via isometries. The limit set of in is .
Now, we state Gromov’s classification of group actions on hyperbolic spaces.
Theorem 2.13 (Gromov’s Classification).
Let be a group acting on a hyperbolic geodesic metric space . Then exactly one of the following holds, and the action of is said to be -
(i) bounded if the orbits of in are bounded.
(ii) horocyclic if the orbits are unbounded and contains no hyperbolic isometry.
(iii) lineal if contains a hyperbolic isometry, and any two hyperbolic elements have the same endpoints.
(iv) focal if it is not lineal, contains a hyperbolic isometry, and all hyperbolic elements have one common endpoint.
(v) general type if contains two hyperbolic isometries which have no common end-point.
In fact, the above classification can be described in terms of the limit set .
Theorem 2.14 (Proposition 3.1 in [CCMT15]).
Let be a group acting on a hyperbolic geodesic metric space . Then, the action of is -
(i) bounded is empty.
(ii) horocyclic ; then is the unique finite orbit of in .
(iii) lineal ; then contains all the finite orbits of in .
(iv) focal is uncountable and has a fixed point in ; then is the unique finite orbit of in .
(v) general type is uncountable and has no finite orbit in .
In proving Theorem 1.3 using this classification, it will be important for us to be able to rule out horocyclic and lineal actions. We record two lemmas regarding this.
Lemma 2.15.
Let be a hyperbolic geodesic metric space and suppose the action of on is lineal. Then has a quasi-line orbit in .
Proof.
This is well-known, but we include a proof for completeness.
Let be the limit set of .
Since the Gromov boundary is a visibility space, there exists a geodesic with endpoints and . Since fixes , it fixes the endpoints of . Thus, is a geodesic with the same endpoints as for every . By hyperbolicity of , the Hausdorff distance between and is uniformly bounded. In particular, there exists such that for all .
Now, fix a basepoint on . We will show that the orbit of is a quasi-line. The previous argument yields that . Moreover, contains a hyperbolic isometry by Theorem 2.13, and hence we get that the orbit coarsely coincides with a neighbourhood of .
∎
Lemma 2.16.
Let be a group acting co-boundedly on a hyperbolic geodesic metric space . Then the action of on is not horocyclic.
Proof.
Since the action of on is co-bounded, the orbit is quasi-dense in . Consequently, the orbit is quasi-convex. By Proposition 3.2 of [CCMT15], it follows that the action of cannot be horocyclic. ∎
Remark.
3. Coarse stabilizer and the coarse fixed set
We work with a general metric space and give an algebraic characterisation of the coarse stabilizer of .
In particular, we show that if acts geometrically on and coarsely coincides with an orbit of a finitely generated subgroup of , then is the union of centralisers where runs over finite index subgroups of .
In Section 5, we use this to show that for a group, is virtually .
The difficult part of the theorem lies in showing that if , then for some finite index subgroup of .
For this, our strategy will be to show that acts geometrically on a subset of containing . Then, it will follow that must contain a finite index subgroup of , giving us the desired result.
To this end, we define the following.
Definition 3.1.
Let be a group acting on a metric space and let . Define the coarse fixed set of H to be . Here is any constant depending on , chosen so that .
(Note that we can always find such a function . Indeed, fix , then defining ensures that .)
A consequence of Theorem 3.2 below is that if is a group acting geometrically on and is a finitely generated subgroup of then, up to quasi-isometries, does not depend on the choice of the function .
Theorem 3.2.
Let be a metric space and suppose acts on properly discontinuously and co-boundedly. Let be finitely generated, and let coarsely coincide with an orbit of . Then,
(i) acts geometrically on
(ii) .
Proof.
(i) This can be proven in a similar way to Theorem 3.2 in [Rua01].
We include the proof for completeness.
Since is finitely generated, so let generate . It is straightforward to see that . Since acts on properly discontinuously, we have that acts on properly discontinuously.
So it remains to prove that acts on co-boundedly. Let and suppose for a contradiction that does not act co-boundedly on . Then there exists with as . And since is quasi-dense in , so there exists and so that for all . Hence, we have
(1) |
Let . So,
Since acts on properly discontinuously, so there are only finitely many with . Thus, is a finite set.
So, we may restrict to a subsequence of to get that the equation holds for all in the subsequence. Doing the same for we get a further subsequence of so that for all .
Thus, for all and a fixed .
So is bounded as tends to infinity, contradicting equation 1.
(ii) If , then .
Note that depends on a function . But we can choose to satisfy where for all . This ensures .
By (i), acts geometrically on . Thus, if , then is quasi-dense in for some neighborhood of . Since coarsely coincides with some (and hence every) orbit of , the orbit is quasi-dense in some neighborhood of . Therefore, there is a constant such that for all , there exists with . In other words, , and thus , a finite set. This is because the action of on is properly discontinuous, meaning that there are only finitely many with .
So, . Thus, and hence . The last equation is using the fact that for two subgroups it holds , where is the set . Thus, is a finite index subgroup of . Also, because and so commutes with all .
Hence, .
Conversely, if for some finite index subgroup of , then we would have for all . Therefore, . Since is quasi-dense in (as acts co-boundedly on , and ), it follows that . Indeed, let be a constant such that for all , there exists so that . Then, for all , we have
∎
Remark.
In particular, for a finitely generated subgroup we can tell that is infinite just by showing is unbounded for some metric space on which acts geometrically.
Remark.
Note that under the assumptions as above, we also have that, up to quasi-isometries, is independent of the choice of the function .
Indeed, suppose and are two such subsets of corresponding to functions . Pick any . Part (i) of Theorem 3.2 tells us that is quasi-dense in for any function . And since , we have that is quasi-dense in . If we denote by the equivalence relation of quasi-isometry, then we have .
Similarly, we get .
Therefore, .
Corollary 3.3.
Let be a group acting properly discontinuously and co-boundedly on a metric space . Then, .
Proof.
Applying Theorem 3.2 with gives us . Now, implies , and hence . Conversely, if , then for some finite index subgroup of . Letting be the subgroup of generated by , we see that . Moreover, since and , is a finite index subgroup of .
Therefore, .
∎
4. Weakly-acylindrical actions
This is an aside on weakly acylindrical actions on a quasi-line. We show that a group acting weakly acylindrically on a roughly geodesic hyperbolic space with a quasi-line orbit has to be virtually . This will be usefull later while proving Theorem 5.3.
Proposition 4.1.
Let be a roughly geodesic hyperbolic space. Let act on weakly acylindrically with a quasi-line orbit. Then is virtually .
Proof.
Without loss of generality, we may assume that is a geodesic metric space. This is because we may replace by , the injective hull of . Then, there exists , an isometric embedding, which is coarsely surjective and -equivariant. It is straightforward to check that acts weakly acylindrically on . Also, if is a quasi-line orbit of in then is a quasi-line orbit of acting on .
So, let be a geodesic hyperbolic space and be a quasi-line orbit of .
Note that the action of on extends to an action of on . Thus, we get a homomorphism with kernel . Since , we have . Thus, has finite index in . So, an orbit of is quasi-dense in , and hence is a quasi-line. Thus, it suffices to prove the proposition for . It will then follow that , and consequently , is virtually . So, we assume, without loss of generality, that the action of on is trivial.
Now, and hence, by Theorem 2.14, it follows that the action of on is lineal. So, contains a hyperbolic element i.e. there exists satisfying . Since is a quasi-line orbit of , we get that for any , the orbit is quasi-dense in . So, given by , is a quasi-isometry for some .
Now, we will show that has finitely many right cosets in . This implies that is virtually isomorphic to which is isomorphic to .
Fix . Let be a right-coset of .
As is a quasi-isometry, so for some . Let . Then,
(2) |
Similarly, is -close to for some . Moreover, as acts trivially on , so . Thus, as . Hence, for all for some .
Fix and let . Now, is a quasi-geodesic with endpoints . Let be a geodesic from to . By the Morse lemma, the hausdorff distance for some which depends just on , . Thus, there exists which satisfy and .

We hence obtain the following inequalities.
(3) |
(4) |
Thus, we have
(5) |
So, .
As acts weakly acylindrically on , so there exists such that for any with there are only finitely many which satisfy . Since, is quasi-dense in a quasi-line, so we can choose large enough so that . Applying the condition that acts weakly acylindrically on with , , and , we see that there are only finitely many possible values for .
So, there are only finitely many right-cosets of . ∎
We record a consequence of the above proposition, which can be seen as part of the Tits Alternative for groups, serving as a counterpart to the ping-pong lemmas.
Corollary 4.2.
Let be a group acting geometrically on a space . Let be any subgroup of . If then is virtually .
Proof.
5. Spaces
In this section, we specialise to the case when is a space.
First, we relate the coarse kernels and corresponding to the action of on and the induced action of on . In particular, we show that if is a proper space with an unbounded curtain model , and acts co-compactly on , then and coincide.
Our strategy will be to look at the action of on the boundaries and of and respectively. In particular, we look at the elements in which fix the boundaries of and . Define, and . We show that and that . These together give us .
Lemma 5.1.
Let be a space and let be a group acting via isometries on . If , , and are as defined above, then .
Proof.
If , then for all , for some fixed constant . Hence, by Lemma 2.7, we have for all . So, .
If , then for all and some fixed constant .
Thus, if is a Cauchy-Gromov sequence, then is a Cauchy-Gromov sequence equivalent to .
This is because,
Hence, fixes , implying that ∎
Theorem 5.2.
Let be a proper space with being unbounded, and let act on co-compactly. Then, .
Proof.
We start with showing that and coincide.
Claim.
.
Proof of Claim.
We first show that . Fix and . As is unbounded, is unbounded as well, and hence non-compact, and since acts on co-compactly, use Corollary 3 in [GO07] to obtain a constant such that for each there is a geodesic ray with and for some . We claim there exists not depending on such that . We have . Moreover, if then by the convexity of distance we have that which contradicts . Thus, and hence . Since is fixed, does not depend on . So, .
Conversely, if then for any , for some constant . Thus, fixes the point . So . ∎
We claim . We note that in the case that the action of is properly discontinuous as well, the equality follows by Corollary 1.6 of [BJ24].
Observe that acts co-compactly on , and hence co-boundedly on . As is unbounded, so an orbit of in is unbounded as well. So, by Theorem 2.14, is nonempty. Thus, by Theorem 2.9, embeds as an Isom -invariant, dense subspace of .
Now, if , then fixes , and hence also fixes . So . Conversely, if , then fixes , which is dense in . Since is hausdorff and acts as a homeomorphism on , must fix as well. Thus, .
Therefore, . Thus, by Lemma 5.1 we have that . ∎
Next, we examine the structure of the coarse kernel of when the action of on is properly discontinuous but not, in general, co-compact. Specifically, we establish mild conditions concerning the orbit of in the curtain model that ensure the coarse kernel is virtually cyclic, and likewise finite.
Our key strategy will be to look at the action of the coarse kernel on the curtain model and apply the classification of actions on hyperbolic spaces, as discussed in Section 2.2. This will allow us to deduce that the subgroup has either a bounded or quasi-line orbit in . We can then exploit the weak acylindricity of the action of on to obtain the desired result.
Notice, firstly, that for any group acting on a metric space by isometries, is a normal subgroup of . Indeed, if , then for all . Therefore, for all , implying that .
Theorem 5.3.
Let be a co-bounded space, and let act on properly discontinuously (but not necessarily co-boundedly). Suppose that has an unbounded orbit in . Then, is virtually cyclic. Moreover, if an orbit of in is not a quasi-line either, then is finite.
Proof.
By assumption, the orbit of in is not bounded. Firstly, we focus on the case it is not a quasi-line either.
Claim.
If an orbit of on is not a quasi-line, then the action of on is bounded.
Proof of Claim.
Since , we have that fixes the boundary of . Thus, by Theorem 2.14, the action of can be either bounded, horocyclic, or lineal. Indeed, if the action of is focal or of general type, then and fixes at most one point in the boundary . A contradiction.
If the action is horocyclic, then . Since each element of is fixed by the action of , it follows from Theorem 2.14 that . But this is impossible since , and hence , is co-bounded. Indeed, let act co-boundedly on . Then, , implying that the action of on is horocyclic. This contradicts Lemma 2.16.
If the action is lineal, then . Since each element of is fixed by the action of , it follows from Theorem 2.14 that . Therefore, we have . So, , implying that the action of on is lineal. Hence, by Lemma 2.15, the orbit of is a quasi-line, contradicting our assumption.
So the action of on is bounded.
∎
Fix . By the claim above, acts boundedly on , so there is a constant so that for all .
Since acts properly discontinuously on , by Theorem 2.8 we get that the induced action of on is weakly acylindrical. So let satisfy that for any with , only finitely many have .
Now, since has unbounded orbits in , we can always find a point in the orbit with . Let be such a point. Then,
The last inequality follows because , and thus .
So, for all , and . Hence, must be finite. So is finite as well.
Finally, using Theorem 5.3 above alongside Theorem 3.2, we obtain the following results regarding the algebraic structure of the coarse kernel for a group that acts geometrically on a space . Consequently, we prove Corollary 1.6 characterizing when the coarse kernels and coincide.
Theorem 5.4.
Let be a space, and let act on geometrically. Then,
(i) is virtually for some .
(ii) If moreover is unbounded, then is virtually cyclic.
(iii) If furthermore is not a quasi-line, then is the largest finite normal subgroup of .
Proof.
(i) Since acts geometrically on , we can apply Theorem 3.2 to , yielding . Assume that this infinite union cannot be realized as the centraliser of a single finite index subgroup.
Then, we may inductively choose finite index subgroups , as follows:-
Pick . Suppose we have chosen finite index subgroups of so that we get proper inclusions , and . Now, there must exist a finite index subgroup of so that .
If not, then we would have , contradicting our assumption.
Let . Since and are finite index subgroups of , so is . Observe also that is a proper subgroup of because and . In particular, we obtain proper chains , and .
Hence, we have an infinite chain of subgroups of . Moreover, all of these are virtually abelian. Indeed, note that the center of is an abelian subgroup of and we have
(6) |
where is finite as is a finite index subgroup of .
(The third equality in equation 6 follows from the second isomorphism theorem applied to the group with subgroups )
However, this contradicts the Ascending Chain Condition [[BH99], Theorem 7.5].
So, for some finite index subgroup of . Now, from equation 6, we know is a finite index subgroup of . Also, is an abelian subgroup of and hence, by Corollary 7.6 of [BH99], must be finitely generated. Thus, , and hence , is virtually for some .
(ii) As acts on geometrically, so is co-bounded. Also, the orbit of is quasi-dense in and hence the corresponding orbit in is quasi-dense as well. As is unbounded, we have that the orbit of in is unbounded. Therefore, by Theorem 5.3, is virtually cyclic.
(iii) Now, if is not a quasi-line then the orbit of in isn’t a quasi-line either. So, by Theorem 5.3, is finite. Also, is a normal subgroup of . Moreover, if is a finite normal subgroup of , then acts uniformly boundedly on an orbit , which is quasi-dense in . So acts uniformly boundedly on , implying that . Thus, finite normal subgroup. Thus, must be the largest finite normal subgroup of . ∎
Corollary 5.5.
Let be a group acting geometrically on a space . Then exactly one of the following holds.
-
(1)
is unbounded and hence ;
-
(2)
is bounded, , and ;
-
(3)
is bounded, has infinite index in , and .
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