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Hyperbolic Spaces and Hyperbolic Groups
1 · Prerequisites
- Absolute and Conditional Convergence; Rearrangement; Products
- Asymptotic Cones and the Sublinear Triangle Criterion
- Binary Operations, Monoids, Groups and Subgroups
- Cayley Graphs, Word Metrics and Quasi-Isometry
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Connectedness
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Covering Spaces and Lifting
- Decision Problems for Finitely Presented Groups
- Filters and Ultrafilters
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Free Groups and Presentations
- Graphs, Walks and Connectivity
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Homotopy and Homotopy Equivalence
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Metric Spaces
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Power Series and Real-Analytic Functions
- Properties of the Integral and the Working FTC
- Quantitative Hyperbolic Geometry Toolkit
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Small Cancellation and Dehn Algorithms
- Small-Cancellation Disc Diagrams and the Torsion Toolkit
- Subspaces, Products, and Quotients
- Suprema and Infima
- Sylow's Theorems, p-Groups and Nilpotent Groups
- The Derivative and the Mean Value Theorems
- The Exponential Function
- The Fundamental Group
- The Fundamental Group of the Circle
- The Logarithm and General Powers
- The Riemann Integral: Definition and Integrability
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Vector Spaces, Linear Subspaces, Span and Direct Sums
2 · Summary
This page develops the standard first pass through Gromov hyperbolicity: slim triangles, equivalent formulations, quasi-geodesic stability, quasi-isometry invariance, hyperbolic groups, algorithmic consequences, elementary subgroup structure, and the boundary of a proper geodesic hyperbolic space. The small-cancellation bridge uses the proved linear-isoperimetric criterion and its explicit Axiom of Choice hypothesis.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Geodesic segments, geodesic triangles, and geodesic metric spaces
Definition
Let be a metric space.
A geodesic segment from to is an isometric map
with and .
A geodesic triangle in is the union of three chosen geodesic segments joining three points pairwise.
The metric space is a geodesic metric space if every pair of points is joined by at least one geodesic segment.
Delta-slim triangles and hyperbolic spaces
Definition
Let be a geodesic metric space and let .
A geodesic triangle in is -slim if each side lies in the closed -neighborhood of the union of the other two sides.
The space is Gromov hyperbolic if there exists such that every geodesic triangle in is -slim.
Cayley trees are 0-hyperbolic
Statement
Every tree is -hyperbolic. In particular, the Cayley graph of a free group with respect to a free basis is -hyperbolic.
Facts & Assumptions
Given: A tree with its path metric.
The Cayley graph of a free group with respect to a free basis is a tree (The Cayley graph of a free group with respect to a free basis is a tree).
In a tree, any two vertices are joined by a unique geodesic segment.
Proof
Let be a geodesic triangle in . By [A1], the three geodesic segments , , and are unique, so their union is a tripod with a single branch point.
In a tripod, each side is contained in the union of the other two sides. Thus every geodesic triangle in is -slim, so is -hyperbolic. The final sentence follows from [L1].
The Gromov product based at a point
Definition
Let be a metric space, let , and let . The Gromov product of and with respect to is
Slim triangles, the Gromov product, and the four-point condition are equivalent up to constants
Statement
Let be a nonempty geodesic metric space. The following are equivalent up to changing the constant:
- is hyperbolic, that is, all geodesic triangles are -slim for some .
- For every basepoint there exists such that one has
for all . 3. For some , one has
for all .
Facts & Assumptions
Given: A nonempty geodesic metric space .
-slim triangles give the product inequality with constant at every basepoint (Slim triangles imply the gromov product inequality).
A geodesic space satisfying the four-point condition with constant has -slim triangles (The four point condition implies slim triangles).
Proof
If triangles are -slim, [F1] proves condition (2) with the same constant at every basepoint.
Now assume (2) and fix just one point . Let . For any four points , write and . On these four points define to be the maximum, over all simple edge paths from to in the complete graph, of the least -value of an edge on the path; put . There are finitely many paths. The one-edge path gives . Along a two-edge path the assumed product inequality gives , and along a three-edge path it gives . Hence . Also , since the first and last edges of every path satisfy these respective bounds.
Concatenate paths attaining and and erase any loops. Erasing loops cannot lower the minimum edge value. Thus : is an exact ultrametric similarity on these four labels. For completeness, its positive threshold relations are nested equivalence relations (on labels with ). Make a finite rooted tree from these nested clusters, with each leaf at height and each common ancestor of at height . Nonnegative edge lengths follow from the bound in step 1.2. The tree distance between leaves is . Removing the finite subtree spanned by four leaves at its central edge or central vertex shows that the largest two of its three opposite-pair distance sums are equal: each uses the central edge twice, while the third uses it zero times; zero-length edges and repeated leaves follow by the same calculation.
The original metric satisfies , so . Each opposite-pair sum therefore differs from its tree counterpart by a number in . Since the two largest tree sums are equal, the largest and second-largest original sums differ by at most : the two original sums corresponding to those equal tree sums both lie in one interval of length , while the remaining original sum can only increase the second-largest if it becomes larger. This is the four-point condition with constant (additive error ). The bound uses the one fixed basepoint , so condition (2)'s per-basepoint quantifier causes no uniformity gap.
Finally (3) is the four-point condition with constant . By [F2] every triangle is -slim. This proves (1) and closes the cycle.
Hyperbolic spaces have thin geodesic quadrilaterals
Statement
Let be a geodesic -hyperbolic space. Then every geodesic quadrilateral in is -thin: each side lies in the closed -neighborhood of the union of the other three sides.
Facts & Assumptions
Given: A geodesic -hyperbolic space and a geodesic quadrilateral with vertices .
Every geodesic triangle in is -slim (Delta-slim triangles and hyperbolic spaces).
The diagonal cuts the quadrilateral into the geodesic triangles and .
Proof
By [A1], each point of the side lies either within distance of or within distance of by applying [L1] to triangle .
If such a point lies near , then applying [L1] to triangle shows that the nearby point on lies within distance of . Hence every point of lies within distance of . Cyclic symmetry gives the same bound for each side, so the quadrilateral is -thin.
Morse stability of quasi-geodesics
Statement
Assume the Axiom of Choice. For every and every quasi-geodesic constants , , there exists with the following property: if is a geodesic -hyperbolic space and are -quasi-geodesics in with the same endpoints, then the Hausdorff distance between the images of and is at most . No properness or continuity of the quasi-geodesics is required.
Facts & Assumptions
Given: AC, a geodesic -hyperbolic space and two -quasi-geodesics with the same endpoints.
Under AC, every such quasi-geodesic has Hausdorff distance at most from every specified endpoint geodesic, including both Hausdorff inclusions (Morse stability with explicit parameter dependence).
AC is used through [F1] to choose its projection family (The Axiom of Choice).
Proof
Choose one geodesic joining the common endpoints. By [F1], each image has Hausdorff distance at most from . This means both that every point of is within distance of and that every point of is within distance of , with infimum distances understood as in [F1].
Fix and . Choose with , then with . Thus ; letting decrease to zero gives . Reverse the roles of for the other inclusion. Therefore their Hausdorff distance is at most , as claimed.
Hyperbolicity is a quasi-isometry invariant of geodesic spaces
Statement
Assume the Axiom of Choice. If two geodesic metric spaces are quasi-isometric and one of them is hyperbolic, then so is the other.
Facts & Assumptions
Given: AC and a quasi-isometry between geodesic metric spaces and .
Under AC, a quasi-isometric embedding of geodesic spaces transports slimness from its target to its source, with an explicit bound. A quasi-isometry also has a controlled coarse inverse, so the implication works in both directions (Hyperbolicity is transported by a quasi isometry).
AC is used by [F1] for the Morse bound and construction of the controlled inverse (The Axiom of Choice).
Proof
Let be the given quasi-isometry. If is -slim, [F1] first extracts uniform quasi-isometric embedding constants for and then gives an explicit slimness constant for . The extraction uses the supplied coarse inverse and both bounded composite errors; the transport uses the two Hausdorff inclusions of Morse stability.
If instead is hyperbolic, [F1] gives a controlled quasi-isometric inverse . Applying the same transport assertion to makes hyperbolic. In the empty-space case the quasi-isometry convention forces both spaces empty and the claim is vacuous. Thus hyperbolicity is invariant in both directions.
Hyperbolic groups
Definition
A finitely generated group is a hyperbolic group if there exists a finite generating set such that the geometric realization of the Cayley graph , with every edge realized as a unit interval and equipped with the induced path metric, is a hyperbolic geodesic metric space. On the vertex set , this path metric restricts to the word metric associated with .
Hyperbolicity of a finitely generated group is independent of the finite generating set
Statement
Assume the Axiom of Choice. Let be a finitely generated group. If the Cayley graph of is hyperbolic for one finite generating set, then it is hyperbolic for every finite generating set.
Facts & Assumptions
Given: AC, a finitely generated group and two finite generating sets .
Two finite generating sets of a group give bilipschitz equivalent word metrics (The identity map between the word metrics of two finite generating sets is a bilipschitz equivalence).
Hyperbolicity is a quasi-isometry invariant of geodesic spaces (Hyperbolicity is a quasi-isometry invariant of geodesic spaces).
AC is used in [L2] through its Morse and controlled-inverse suppliers (The Axiom of Choice).
Proof
By [L1], the identity map on the vertex sets is bilipschitz for the two word metrics. Extend it over each edge of by a chosen shortest -path for that edge label, and conversely for -edges. Because the generating sets are finite, these paths can be fixed by finitely many choices. The resulting maps are quasi-isometries of the geometric Cayley graphs: every point is within of a vertex, and the vertex metrics have the bilipschitz bounds from [L1].
By [L2], under [A1] hyperbolicity transfers from one geometric Cayley graph to the other. Since were arbitrary finite generating sets, the definition does not depend on the set.
Finite groups and free groups are hyperbolic
Statement
Every finite group and every finitely generated free group is hyperbolic.
Facts & Assumptions
Given: Either a finite group with a finite generating set , or a finitely generated free group with free basis .
Cayley trees are -hyperbolic (Cayley trees are 0-hyperbolic).
The Cayley graph of a free group with respect to a free basis is a tree (The Cayley graph of a free group with respect to a free basis is a tree).
Proof
If is finite, then its Cayley graph has finite diameter. Every geodesic triangle in a finite-diameter space is -slim, so is hyperbolic.
If is free, then [L2] says that its Cayley graph is a tree, and [L1] therefore makes it -hyperbolic. Hence is hyperbolic.
Free abelian groups of rank at least two are not hyperbolic
Statement
If is a free abelian group of rank at least , then is not hyperbolic.
Facts & Assumptions
Given: A free abelian group with a basis of cardinality at least two, possibly infinite (Free abelian group on a set).
A hyperbolic group is finitely generated and has a hyperbolic unit-edge Cayley graph for some finite generating set (Hyperbolic groups).
Cayley edges correspond to the nonzero elements of the symmetric generating set (The Cayley graph of a group with respect to a subset).
In a geodesic -hyperbolic space every geodesic quadrilateral is -thin (Hyperbolic spaces have thin geodesic quadrilaterals).
Proof
If the basis is infinite, every finite set of group elements uses only finitely many basis coordinates and cannot generate . Thus [L0] excludes hyperbolicity. Otherwise identify with , , and fix any finite generating set. Replace it by its nonzero symmetric closure , which leaves the geometric Cayley graph unchanged by [L1]. It spans .
Choose of maximal Euclidean norm. The linear functional satisfies and for every , by Cauchy–Schwarz and maximality. Since spans a space of dimension at least two, choose independent of and put . Then , and . Choose maximizing . Symmetry gives a positive maximum and on . Hence has , and on . In particular are independent.
Extend these linear functions from graph vertices affinely over each edge. Their slopes have absolute value at most one, so they are 1-Lipschitz for the graph path metric. Thus a path of successive -edges, or successive -edges, has endpoints at distance exactly : the path supplies the upper bound and , respectively , supplies the lower bound. Translates and reversals are likewise geodesics. Therefore the four such paths through form a geodesic quadrilateral.
Choose linear functionals on with , , and ; solving the nonsingular two-vector Gram system constructs them. Let . Their affine extensions to graph edges are -Lipschitz. At the midpoint of the side to , their values are . On each of the other three sides, either , , or . Consequently every point on those sides is at distance at least from that midpoint. Taking arbitrarily large contradicts [L2] for every proposed hyperbolicity constant. Since the finite generating set was arbitrary, [L0] excludes hyperbolicity of .
Hyperbolic groups admit finite Dehn presentations
Statement
Let be a hyperbolic group. Then admits a finite presentation with the following Dehn property: every nonempty freely reduced word over representing the identity in contains a subword such that is longer than half of some cyclic conjugate of a relator in .
Facts & Assumptions
Given: A hyperbolic group .
For , every -local arc-length geodesic in a geodesic -slim space is a -quasi-geodesic; for , every positive-radius local geodesic is globally geodesic (Local geodesics in a hyperbolic space are uniform quasi geodesics).
For a fixed finite generating set, there are only finitely many words of length at most .
Proof
Choose a finite generating set for and a positive slimness constant for its Cayley graph. Choose an integer . By [F1], any -local geodesic arc is a -quasi-geodesic. If such an arc has the same initial and terminal vertex and positive length , the quasi-geodesic inequality gives , hence ; then the whole arc lies within the local-geodesic radius and would have to be geodesic, impossible between equal endpoints. Let be the finite set of nonempty freely reduced words over of length at most that represent the identity. Finiteness follows from [A2], and presents once the Dehn property below is proved.
Suppose a nonempty freely reduced trivial word contains no subword longer than half of a cyclic conjugate of a member of . If an ordinary subword of of length at most were nongeodesic, choose one of minimal length and call it , and choose a shorter geodesic word with the same endpoints. Minimality of implies that and share neither an initial nor a terminal edge: deleting such a common edge would give a shorter nongeodesic subword. Hence the loop word is freely and cyclically reduced. It belongs to , has length , and contains as more than half of a cyclic conjugate, a contradiction. Thus every ordinary length-at-most- subword of is geodesic. Read as the parameterized open path from the identity vertex back to itself; all its short consecutive segments are geodesic, so this open path is -local geodesic. No condition is imposed across a cyclic junction of .
Step 1.1 forbids a nonempty -local geodesic arc with equal endpoints, contradicting step 2.1. Hence every nonempty freely reduced trivial word has the required long relator subword. Replacing that subword by the shorter complementary piece of its relator, then freely reducing, strictly decreases word length while preserving its value in . Finite induction reduces every trivial word to the empty word using relations from , so presents and has the Dehn property.
Hyperbolic groups have solvable word problem
Statement
Every hyperbolic group has solvable word problem.
Facts & Assumptions
Given: A hyperbolic group with a finite Dehn presentation .
In a Dehn presentation, every nonempty freely reduced trivial word contains a subword longer than half of a relator (Hyperbolic groups admit finite Dehn presentations).
Replacing such a long subword by the complementary shorter subword strictly decreases word length and preserves the represented group element.
Proof
Fix the finite alphabet and finite relator list supplied by [L1]. Freely reduce the input word. At each stage enumerate its finitely many subwords and the finitely many cyclic conjugates of relators in ; if a subword is longer than half of one of those relators, replace it by the inverse of the complementary piece and freely reduce again. Choose the first match in a fixed finite ordering. Each replacement preserves the group element and strictly decreases length, so this effective procedure terminates.
If the algorithm stops at the empty word, then in . Conversely, if in and the current freely reduced word is nonempty, [L1] supplies another enumerated shortening move, so the procedure cannot stop there. Thus it decides whether represents the identity.
Linear isoperimetric characterisation of hyperbolic groups
Statement
Assume the Axiom of Choice. A finitely generated group is hyperbolic if and only if it admits a finite presentation satisfying a linear isoperimetric inequality for van Kampen area: there is a constant such that every null-homotopic word has a van Kampen diagram with at most -cells.
Facts & Assumptions
Given: AC and a finitely generated group .
Hyperbolic groups admit finite Dehn presentations (Hyperbolic groups admit finite Dehn presentations).
Under AC, a finite presentation with algebraic relator area at most and bounded relator lengths has uniformly slim triangles in its labelled geometric Cayley graph (Linear isoperimetry implies uniformly thin geodesic bigons).
An expression with relator factors produces a singular planar van Kampen diagram with no more than faces (Relator expressions admit singular planar diagrams with controlled incidence). The least number of such factors is algebraic relator area (Algebraic relator area and the Dehn function of a finite presentation).
AC is used in [F2] for its cone and uniformity arguments (The Axiom of Choice).
Proof
If is hyperbolic, [F1] gives a finite presentation with the Dehn reduction property. For every nonempty null word, one reduction replaces a subword longer than half a defining relator by the complementary shorter subword, using one conjugate of that relator; the resulting freely reduced word is strictly shorter. Iterate. There are at most reductions before the empty word, so reversing them gives an expression of as at most conjugated relators. By [F3] it has a van Kampen diagram with at most cells. The empty word has an empty diagram. Thus the displayed linear inequality holds, with (or any larger positive constant).
Conversely suppose a finite presentation has diagrams with at most cells for every null word. The boundary word of any finite disc diagram is a product of conjugates of its face relators: choose a spanning tree of its edges, cut along that tree, and peel cells from the exterior; each peel contributes one conjugated relator and the cut-tree traversals cancel freely. Repeated vertices and edges are treated by their separate directed occurrences. Thus the algebraic relator area of is at most . If the given bound is real, take ; the area is integral, so the same inequality holds. Since the relator set is finite, its lengths have a finite bound .
By [F2] and [A1], the bound in step 1.2 makes the labelled geometric Cayley graph uniformly slim. Hence is hyperbolic. Together with step 1.1 this proves the equivalence.
Finite C'(1/6) presentations define hyperbolic groups
Statement
Assume the Axiom of Choice. Let be a finite presentation satisfying the metric small-cancellation condition . Then is hyperbolic.
Facts & Assumptions
Given: AC and a finite presentation satisfying .
Finite presentations satisfy a linear isoperimetric inequality for van Kampen area (Finite C prime(1/6) presentations satisfy a linear isoperimetric inequality).
A finite presentation with linear isoperimetric inequality defines a hyperbolic group (Linear isoperimetric characterisation of hyperbolic groups).
AC is used through [L1]'s linear-area-to-slimness supplier (The Axiom of Choice).
Proof
By [L0], the given presentation satisfies a linear isoperimetric inequality.
Therefore [L1] applies under [A1], and the presented group is hyperbolic.
Infinite-order elements of hyperbolic groups are undistorted
Statement
Let be a hyperbolic group and let have infinite order. Then the cyclic subgroup is undistorted in : for some constants ,
for all , where is word length with respect to a finite generating set of .
Facts & Assumptions
Given: A hyperbolic group , a finite generating set , and an infinite-order element .
For an infinite-order element of a finitely generated hyperbolic group, there is a positive integer such that for all integers (Infinite order elements have positive stable translation length).
Word metrics from two finite generating sets are bilipschitz equivalent (The identity map between the word metrics of two finite generating sets is a bilipschitz equivalence).
Proof
By the definition of a hyperbolic group, some finite generating set has a hyperbolic geometric Cayley graph. Apply [L1] with : for some , for every integer . The proof of [L1] is choice-free.
By [L2] there is a finite with for all . Thus . Take and any . This proves undistortion for the stated arbitrary finite without importing a choice-dependent hyperbolicity transfer theorem.
The centralizer of an infinite-order element in a hyperbolic group is virtually cyclic
Statement
Let be a hyperbolic group and let have infinite order. Then its centralizer
contains a cyclic subgroup of finite index.
Facts & Assumptions
Given: A hyperbolic group and an infinite-order element .
Infinite-order elements are undistorted (Infinite-order elements of hyperbolic groups are undistorted).
In a finitely generated -slim hyperbolic group, if an infinite-order element has a power orbit with quasi-isometry constants , then its centralizer contains its cyclic subgroup with finite index; each coset has a representative in a ball whose radius depends only on (Axis fellow travelling controls the centralizer).
Proof
The standing hyperbolic-group convention supplies a finite generating set whose geodesic Cayley realization is -slim. By [L1], the power orbit of is quasi-isometrically embedded; fix its constants . The hypotheses of [L2] are therefore met.
Apply [L2]. It gives finitely many cosets of in , with a representative of each in one finite word ball. Thus is a cyclic subgroup of finite index in the centralizer, as claimed.
Abelian subgroups of hyperbolic groups are virtually cyclic
Statement
Every abelian subgroup of a hyperbolic group contains a cyclic subgroup of finite index.
Facts & Assumptions
Given: An abelian subgroup of a hyperbolic group .
The orders of finite subgroups of have a common finite bound (Finite subgroups of a hyperbolic group have uniformly bounded order).
Centralizers of infinite-order elements are virtually cyclic (The centralizer of an infinite-order element in a hyperbolic group is virtually cyclic).
Proof
If contains an element of infinite order, then . By [L1], the cyclic subgroup has finite index in . Thus has finite index in and is cyclic as a subgroup of . Hence is virtually cyclic.
If every element of has finite order, each finitely generated subgroup of is finite: for generators of orders , commutativity makes it a quotient of the finite group . By [L2] it has at most elements. Were to contain distinct elements, their finitely generated subgroup would contradict this bound. So is finite, hence virtually cyclic. The two cases prove the claim.
Finite subgroups of a hyperbolic group have uniformly bounded order
Statement
Let be a hyperbolic group and fix a finite generating set . Then there exists a constant such that every finite subgroup satisfies .
Facts & Assumptions
Given: A hyperbolic group with finite generating set . Choose a finite generating set witnessing hyperbolicity and a slim-triangle constant for its Cayley graph ; the bound obtained from also supplies the asserted .
The geometric Cayley graph is a geodesic metric space in which every geodesic triangle is -slim (Hyperbolic groups, Delta-slim triangles and hyperbolic spaces).
The vertex ball of any fixed integer radius in is finite because is finite. Left translation by is free and transitive on Cayley vertices: for a vertex implies .
Proof
Let be finite and put , a finite set of vertices of . For a vertex define . The nonempty set of integer values has a least value , attained at some vertex . Left translation by each preserves and distances, so . Thus the center set is -invariant and contains the orbit .
Let , write , and let be the midpoint of a geodesic . For any , slimness of the triangle with vertices gives a point on or with . In the first case, and , so ; the second case is symmetric. Choose a vertex of the edge containing , with . Then . Minimality of forces . Hence every two vertices of , and in particular of , are at distance at most .
The map is injective by [L2]. The orbit lies in the vertex ball about of radius , whose cardinality is the fixed finite number by Cayley vertex transitivity. Thus for every finite . Taking proves the assertion for the given .
Elementary and non-elementary hyperbolic groups
Definition
A hyperbolic group is elementary if it is finite or contains a cyclic subgroup of finite index. A hyperbolic group that is not elementary is non-elementary.
Non-elementary hyperbolic groups contain a rank-two free subgroup
Statement
Every non-elementary hyperbolic group contains a free subgroup of rank .
Facts & Assumptions
Given: A non-elementary hyperbolic group .
Every non-elementary hyperbolic group contains independent infinite-order elements with pairwise disjoint attracting and repelling neighborhoods . Their boundary actions have north--south dynamics: for all sufficiently large , (Kapovich--Benakli, Theorem 2.28, Proposition 4.2, and Theorem 4.3.)
Proof
By [A1], choose independent infinite-order elements with disjoint attracting and repelling neighborhoods on the boundary.
Choose large enough for all four north--south inclusions in [A1]. Write , , , and . If is a nonempty reduced word in , choose a letter distinct from both and and a point . Acting from right to left, [A1] gives successively. [A1, step 1.1, choose] because reducedness says . Thus , while , and these domains are disjoint. Hence , so is not trivial. Therefore and freely generate a free subgroup of rank .
The Gromov boundary via asymptotic sequences
Definition
Let be a proper geodesic hyperbolic space and fix a basepoint .
A sequence in is a Gromov sequence if
Two Gromov sequences and are asymptotic if
After Asymptoticity of Gromov sequences is an equivalence relation ↗ shows that this is an equivalence relation, the Gromov boundary is defined to be the set of asymptoticity classes of Gromov sequences.
Asymptoticity of Gromov sequences is an equivalence relation
Statement
In a proper geodesic hyperbolic space, asymptoticity of Gromov sequences is an equivalence relation.
Facts & Assumptions
Given: A proper geodesic hyperbolic space with basepoint .
The slim-triangle definition of hyperbolicity gives a Gromov-product inequality for a fixed (Slim triangles imply the gromov product inequality).
Reflexivity and symmetry are immediate from the definition of asymptoticity.
Proof
By [A1], every Gromov sequence is asymptotic to itself, and if is asymptotic to then is asymptotic to .
Suppose is asymptotic to and is asymptotic to . By [L1], there is with for all . Given , choose so both mixed products exceed whenever both of their indices are at least . For every , taking in the inequality gives . Hence , so is asymptotic to .
The boundary topology defined by Gromov products
Definition
Let be a proper geodesic hyperbolic space, let , and let be the boundary defined by Gromov sequences.
For boundary classes and , define
where the supremum runs over all representatives of the two classes.
For and , let
The boundary topology consists of the sets such that, for every , some satisfies . Each is a neighbourhood of ; it need not itself be open. The next theorem proves that this criterion defines a topology and is independent of the chosen basepoint.
The boundary topology is well defined and quasi-isometry invariant
Statement
Assume the Axiom of Choice. For a proper geodesic hyperbolic space, the topology defined on the Gromov boundary by Gromov products is well defined. Moreover, a quasi-isometry between proper geodesic hyperbolic spaces induces a homeomorphism of their boundaries.
Facts & Assumptions
Given: AC and proper geodesic hyperbolic spaces and .
The supremal boundary product and any supplied representative product differ by at most , changing basepoints shifts products by at most their distance, and the threshold-neighbourhood criterion gives a Hausdorff topology (Boundary products have controlled representative and basepoint dependence).
Under AC a quasi-isometry of geodesic hyperbolic spaces induces a continuous boundary map, bounded-distance maps induce the same map, and a controlled quasi-inverse supplies a continuous inverse (Quasi isometries extend to boundary homeomorphisms).
AC is used in [F2] for the Morse projection families and coarse-inverse selection (The Axiom of Choice).
Proof
The boundary product in The boundary topology defined by Gromov products is the supremal product of [F1]. Its comparison with every representative product proves independence of representatives; the basepoint inequality gives cofinal threshold neighbourhoods at any two basepoints.
The definition's open-set criterion is exactly the one proved in [F1], including its treatment of threshold sets as neighbourhoods that need not be open. Hence it is a topology and is Hausdorff.
By [F2] under [A1], the quasi-isometry induces a continuous map of these boundary topologies. Its controlled quasi-inverse induces a continuous inverse because the bounded-distance composites induce identity maps. This proves the claimed homeomorphism; properness is included in the statement but not required by [F1] or [F2].
5 · Examples, counterexamples and false statements
FALSE: a hyperbolic group is just a group with a hyperbolic-plane subgroup
Statement
False claim: every hyperbolic group contains a subgroup isometric to the hyperbolic plane.
This is the load-bearing direction behind the misleading slogan that hyperbolicity "means" containing a hyperbolic-plane subgroup.
Facts & Assumptions
Given: A nonabelian finitely generated free group .
Free groups are hyperbolic (Finite groups and free groups are hyperbolic).
Every finitely generated group is countable, whereas the hyperbolic plane is uncountable.
Refutation
By [L1], the free group is hyperbolic.
The group is countable, but [A1] says that is uncountable. So cannot contain the hyperbolic plane as a subgroup or even as an underlying set, yet it is hyperbolic by step 1.1. Therefore the claim is false.
FALSE: the same delta works after every finite change of generating set
Statement
False claim: once a finitely generated group is hyperbolic, one numerical slimness constant works for the Cayley graph of every finite generating set.
Facts & Assumptions
Given: The free group and, for each integer , the generating set .
Write . A word over with signed total exponent of and length has abelianization only if Indeed, its remaining - and -letters must supply the respective coordinate differences.
Refutation
The generating set gives a tree Cayley graph, so is -hyperbolic for that choice.
Let , and choose an even with . The paths labelled from to and from to have length . They are geodesic: for every integer , [A1] gives respective lower bounds and . The edge labelled joins to , so these paths form a geodesic triangle.
Its midpoint vertex is distance from . For any word from to , [A1] gives for every integer : the first term is at least , and either or the second term is positive. Thus is at distance at least from the one-edge side , including its interior. Every vertex on the other long side, , is also at distance at least from , since the first term of the lower bound is at least for every integer . The same bound holds for points inside its edges. Therefore this geodesic triangle is not -slim.
Since was arbitrary, no single constant works for all finite generating sets of . Therefore the claim is false.
FALSE: every abelian group is hyperbolic
Statement
False claim: every abelian group is hyperbolic.
Facts & Assumptions
Given: The abelian group .
Free abelian groups of rank at least two are not hyperbolic (Free abelian groups of rank at least two are not hyperbolic).
Refutation
The group is abelian.
The group has rank , so [L1] shows that it is not hyperbolic. Therefore the claim is false.
FALSE: all quasi-geodesics in all metric spaces stay uniformly close to geodesics
Statement
False claim: in every metric space, quasi-geodesics stay within a uniform distance of geodesics with the same endpoints.
Facts & Assumptions
Given: In the Euclidean plane, for each , the broken path from to to to .
The straight geodesic between the path endpoints is the horizontal segment from to .
Refutation
Parametrize each broken path by arclength. For two points on the same side of the path, the subpath length equals their Euclidean distance. For points on adjacent sides, the subpath has two perpendicular legs, so its length is at most times their distance. For points on the two vertical sides, their distance is at least while their subpath length is at most . Thus every path is a -quasi-geodesic under the definition, with constants independent of . The midpoint of the top side is distance from the straight segment between the endpoints.
Their distance from the corresponding geodesic segments is unbounded as , so no uniform fellow-traveling constant exists. Hence the global claim is false.
FALSE: a proposed Gromov boundary quotient needs no equivalence check
Statement
False claim: once a class of boundary sequences and a proposed "asymptotic" relation have been written down, one may form the Gromov boundary as their quotient without proving that asymptoticity is an equivalence relation.
Facts & Assumptions
Given: The boundary construction on this page.
The quotient by asymptoticity is justified only after proving that asymptoticity is an equivalence relation (Asymptoticity of Gromov sequences is an equivalence relation).
Refutation
A quotient set consists of equivalence classes, so it is defined only when the proposed relation is an equivalence relation. The sequence model on this page therefore depends essentially on [L1].
Consequently the proposed quotient cannot be licensed merely by writing down the relation: reflexivity, symmetry, and transitivity must be checked. The properness hypothesis used elsewhere on this page is a scope choice for this construction, not a claim that every possible boundary model requires properness.
The hyperbolic plane is hyperbolic
Example
The hyperbolic plane is a hyperbolic geodesic metric space.
Facts & Assumptions
Given: The standard geodesic metric on .
Löh's cited lecture notes state in Example 4.3.2 that is geodesic and state on p. 153 that all geodesic triangles in are uniformly slim, citing Theorem A.3.27 of Löh's Geometric Group Theory: An Introduction. Thus some single works for every geodesic triangle in .
A geodesic metric space is hyperbolic exactly when all geodesic triangles are -slim for some (Delta-slim triangles and hyperbolic spaces).
Verification
By the external geometric result [F1], is geodesic and all its geodesic triangles are -slim for a single .
Therefore [L1] shows that is hyperbolic.
Sources
- Clara Löh, Geometric Group Theory, Section 6.2.1
- Clara Löh, Geometric Group Theory, Section 6.2.4
- Clara Löh, Geometric Group Theory, Sections 6.1.2-6.2.1
- Brian H. Bowditch, A course on geometric group theory, Sections 1.2-2.1
- Clara Löh, Geometric Group Theory, Section 6.2.3
- Brian H. Bowditch, A course on geometric group theory, Section 2.1
- Brian H. Bowditch, A course on geometric group theory, Section 2.2
- Clara Löh, Geometric Group Theory, Section 6.3
- Clara Löh, Geometric Group Theory, Sections 6.2.4 and 6.3
- Clara Löh, Geometric Group Theory, Section 6.5.4
- Clara Löh, Geometric Group Theory, Section 6.4
- Brian H. Bowditch, A course on geometric group theory, Section 2.3
- Clara Löh, Geometric Group Theory, Section 6.4.1
- Nicholas Touikan, An introduction to combinatorial and geometric group theory, Section 3.5
- Clara Löh, Geometric Group Theory, Section 6.5.1
- Clara Löh, Geometric Group Theory, Section 6.5.2
- Clara Löh, Geometric Group Theory, Section 6.2.1 (slim-triangle background; the finite-orbit argument is proved below)
- Clara Löh, Geometric Group Theory, Section 6.5
- Brian H. Bowditch, A course on geometric group theory, Section 6.11.1 (S4)
- Ilya Kapovich and Nadia Benakli, Boundaries of hyperbolic groups, Theorem 2.28, Proposition 4.2, and Theorem 4.3
- Brian H. Bowditch, A course on geometric group theory, Section 5.3
- Clara Löh, Geometric Group Theory lecture notes (2022), Example 4.3.2, Section 6.1 p. 153, and Example 6.2.3 (citing Löh, Geometric Group Theory: An Introduction, Theorem A.3.27)