Math 697: Introduction to Geometric Group Theory
Notes from course given by Dick Canary, Fall 2014. August 23, 2016
0 Overview 0.1 A Rambling Geometric group theory is really “a collection of things put together by a state of mind.” These things defi- nitely include hyperbolic group theory, but also various other things such as CAT(0) groups, topological group theory, and so on ... A little more concretely, geometric group theory is the study of groups by looking at their actions on spaces. Given a [finitely-presented] group G = hx1, . . . , xn | r1, . . . , rmi, we can define the word metric distance by setting d(g, h) to be the minimal length of word in {x1, . . . , xn} (and their inverses) over all representations −1 of g h. We define the Cayley graph ΓG of G by taking the vertices to be the elements of G and drawing edges labelled xi joining each g to gxi ∼ Example 0.1. • If G = Z = ha |i, then ΓG is a line (= R.) a a a a ··· ··· a−2 a−1 1 a a2
2 • If G = Z = ha, b | [a.b]i, then ΓG is a 2-dimensional lattice (“what is this? It is graph paper.”)
ab = ba b 0 a
1 1 • If G = F2 = ha, b |i, then ΓG is an infinite 4-valent tree (the universal cover of S ∨ S )—see below
If M is a compact manifold, then π1(M) acts properly discontinuously and co-compactly on M˜ .
2 2 Example 0.2. If M = T , then π1(M) = Z , which acts properly discontinuously and cocompactly on M˜ = R2; we note that R2 “looks like” Z2 (coarsely speaking.) ˜ If M is a compact 3-manifold (e.g. a solid genus-2 torus), M is a thickening of ΓF2 , the infinite 4-valent tree.
We make precise the notion of “looks like” by using the notion of quasi-isometry. Note that our spaces X and Y are usually assumed to be proper (i.e. closed balls are compact) and geodesic (i.e. distance between two points is given by the length of a shortest path.)
1 a−1 ba
b a−1 ba−1 a ba b−1 b−1 a−1 ba a−1 ba b b b a−1 ba−1 a−1 a a ba b−1 b−1 b−1 b−1 a−1 ba a−1 a a−1 a a−1 ba b−1 b−1 b b a−1 ba−1 a ba a−1 ba−1 a ba b b−1 b−1 b−1 b−1 a−1 ba a−1 ba b b b b a−1 ba−1 a−1 a−1 a a a ba b−1 b−1 b−1 b−1 a−1 a a−1 a b−1 b−1 b−1 b−1 a−1 ba−1 a ba a−1 ba−1 a ba b−1 b−1 b−1 b−1 b−1 b−1 b−1 a−1 a a−1 ba a−1 ba a−1 a b−1 b−1 b b a−1 ba−1 a−1 a a ba b−1 b−1 b−1 b−1 a−1 a a−1 a b−1 b−1 b−1 a−1 ba−1 a ba b−1 b−1 b−1 a−1 a b−1
Figure 1: Part of a Cayley graph of a nonabelian free group
1 Definition 0.3. h : X → Y is a quasi-isometric embedding if there exist k, c s.t. k d(x, z) − c ≤ d (h(x), h(z)) ≤ kd(x, z) + c for all x, z ∈ X. h is a quasi-isometry if in addition it is “coarsely surjective”, i.e. there exists D ≥ 0 s.t. for all y ∈ Y , there exists x ∈ X s.t. d(h(x), y) ≤ D.1 A key result in geometric group theory is the Milnor-Svarcˇ lemma, which states that if G acts properly discontinuously and co-compactly on a space X, then X is quasi-isometric to G with the word metric. Note that this notion of quasi-isometry, though seemingly loose and geometric, can capture algebraic aspects of structure (or aspects of algebraic structure.) e.g. G quasi-isometric to a free group implies G virtually free.2 There is also Gromov’s theorem, which states that any group with polynomial growth is virtually nilpotent. In fact, we can also use algebra to clarify geometry, as in the following [re-]formulation of hyperbolic
1Think of the plane, and graph paper. 2“Virtually” or “almost” in this context means true up to (true for a) finite-index subgroup. These adjectives will appear a lot, because quasi-isometry fails to distinguish between the whole group and finite-index subgroups.
2 spaces by Gromov: Fact. Suppose X is simply-connected with (sectional) curvature ≤ −k < 0. Then there exists δ = δ(k) such that any geodesic triangle in X is δ-slim, meaning that if T has vertices x, y, z, then [x, z] ⊂ Nδ([x, y]∪[y, z]), i.e. ∀t ∈ [x, z]: ∃s ∈ [x, y] ∪ [y, z] s.t. d(s, t) < δ. Definition 0.4 (Gromov, possibly Alexander). X is δ-hyperbolic if every geodesic triangle in X is δ-slim. e.g. trees are 0-hyperbolic. A space is hyperbolic if it is δ-hyperbolic for some δ ≥ 0. A group is hyperbolic if it acts properly discontinuously and co-compactly on a hyperbolic space. Hyperbolic groups have some very nice properties: • Hyperbolic groups have solvable word problem (which we might formulate as “can I build the Cayley graph [algorithmically]?”) by Dehn’s algorithm. • They also have solvable conjugacy problem and isomorphism problem.3
• The Tits Alternative: if a hyperbolic group G is not virtually cyclic, it contains a F2.
• A hyperbolic group cannot contain a copy of Z2. • A hyperbolic group has only finitely many conjugacy classzes of finite subgroups. • Being a hyperbolic space / group is a condition invariant under quasi-isometry. Hyperbolic spaces are those with constant negative curvature (-1); we can generalize this notion to look at spaces X with constant non-positive curvature, and this brings us to the theory of CAT(0) groups: Definition 0.5. A simply-connected space X is CAT(0) if every geodesic triangle in X is at least as thin as a Euclidean triangle with the same edge lengths. G is CAT(0) if it acts properly and cocompactly on a CAT(0) space. Definition 0.6. CAT(0) cube complexes are formed by gluing Euclidean unit cubes along faces. e.g. R2 is a CAT(0) cube complex
Example 0.7. Right-Angled Artin Groups (RAAGs) are CAT(0) groups AΓ formed as follows: start with a finite graph Γ; define (0) (1) AΓ = hΓ | vw = wv ⇐⇒ (v, w) ⊂ Γ i
i.e. the elements of AΓ are the vertices of Γ, and we add a commutator relation between two elements iff there is an edge between the corresponding vertices. e.g. if Γ is the empty graph on n vertices, then AΓ = Fn. n If Γ = Kn, then AΓ = Z . 2 2 If Γ consists of two disjoint edges on 4 vertices, then AΓ = Z ∗ Z . These groups are “interpolating between the free group and the free abelian group.” Theorem 0.8 (Agol, Wise). If a hyperbolic group G acts properly discontinuously and cocompactly on a CAT(0) cube complex (in this case we say G is a cubulation), then a finite-index subgroup of G embeds in a RAAG. Theorem 0.9 (Haglund-Wise, Kahn-Markovic). If M is a closed hyperbolic 3-manifold, then M is cubulated. Finally, there is topological group theory. The prototypical result here is the proposition that states that every subgroup of a free group is free, proven using covering spaces. There is also the following generalisation of this:
Theorem 0.10 (Kurosh). If G = G1 ∗ G2 and H ⊂ G, then H = F ∗λ∈Λ Hλ, where F is free, and each HΛ is conjugate to a a subgroup of G1 or G2. (See Figure 2.)
3Something involving Tietze transformations was name-dropped here.
3 Figure 2: A free product may be thought of as the fundamental group of a wedge of spaces.
This has the following corollary:
Corollary. If G is finitely-generated, then G has a unique free decomposition G = G1 ∗ · · · ∗ Gn where each Gi is freely indecomposable (i.e. does not split as a free product.) Other topics that might come under this last heading include JSJ decompositions and Bass-Serre theory.
0.2 Definitions and quasi-isometry Definition 0.11. Given X a metric space and α : [0, 1] → X a path,
n−1 X `X (α) := sup d(α(ti), α(ti+1)) 0=t Definition 0.12. α is rectifiable if `X (α) < ∞. Definition 0.13. α is geodesic if `X (α) = d(α(0), α(1)). Exercise. (1) A subpath of a geodesic is a geodesic, (2) If 0 ≤ s ≤ t ≤ u ≤ 1, then d(α(s), α(t)) + d(α(t), α(u)) = d(α(s), α(u)) if α is a geodesic. Definition 0.14. A metric space is geodesic if any two points are joined by a (by some) geodesic. e.g. Cayley graphs, Riemannian manifolds, curve complexes, etc. Definition 0.15. X is proper if all closed metric balls are compact. Our spaces will be proper geodesic metric spaces (mostly.) We always assume that G acts by isometries on X, i.e. d(x, y) = d(s(x), s(y) for all x, y ∈ X and s ∈ G. This is a common (and apparently commonly unstated!) assumption in geometric group theory. Definition 0.16. An action is properly discontinuous (or proper) if whenever K is compact {g ∈ G | g(K) ∩ K 6= ∅} is finite. Definition 0.17. An action of G is co-compact if X/G is compact. Remark. X/G is a metric space, with the metric given by dX/G([x], [y]) := dX (Gx, Gy). Hence X/G compact =⇒ ∃R s.t. G(BR(x0)) = X—we can take e.g. R = diam(X/G). Fact. If G acts properly and co-compactly on a geodesic proper metric space, then G is finitely generated. Proof. Choose D = B2 diam(X/G)(x), U = int(D). Note U ⊃ Bdiam(X/G)(x). Then G(U) = X. Let S = {g ∈ G | g(D) ∩ D 6= ∅}. S is finite. Claim. S is a generating set. Let H = hSi ⊂ G. If H 6= G, then let V = Hu and W = (G \ H)u: V and W are non-empty and open, and X is connected (since path-connected, since geodesic), so V ∩ W 6= ∅. Let x ∈ V ∩ W . x ∈ V =⇒ ∃h ∈ H, p ∈ U s.t. h(p) = x. x ∈ W =⇒ ∃g ∈ G \ H, q ∈ U s.t. g(q) = x. Then hg−1(p) = q and so hg−1 ∈ S, which implies g ∈ H. Contradiction. 4 Recall that h : X → Y is a (k, c)-quasi-isometric embedding if ∀x, z ∈ X a d(x, z) − c ≤ d(h(x), h(z)) ≤ kd(x, z) + c k (k is a bi-Lipschitz constant, disregard scale ≤ c.) Fact. If h : X → Y is a quasi-isometry, then ∃ quasi-isometry j : X → Y s.t. d(j(h(x)), x), d(h(j(y)), y) ≤ R + for all x ∈ X, y ∈ Y , and some R ∈ R0 . j is called a quasi-inverse. Proof. If y ∈ Y , then ∃x ∈ X s.t. d(y, h(x)) ≤ C. Choose j(y) s.t. d(y, h(j(y)) ≤ C. Then d(j(y), j(z)) ≤ k(d(h(j(y)), h(j(z))) + c ≤ k(d(y, z) + 2c) + c ≤ kd(y, z) + (2kc + c) Now repeat in the other direction, and take R = max{2kc + c, −}. Exercise. A composition of quasi-isometries is a quasi-isometry. Corollary. Quasi-isometric equivalence of metric spaces is an equivalence relation. 0.3 The Milnor-Svarcˇ lemma Lemma 0.18 (Milnor-Svarc)ˇ . Suppose G acts properly and co-compactly by isometries on a (proper geodesic metric) space X, and R is a finite generating set for G; then (G, dR) is quasi-isometric to X (here dR is the word metric associated to R.) Corollary. If G acts properly, co-compactly, and by isometries on two proper geodesic metric spaces X and Y , then X is quasi-isometric to Y . Remarks. (1) The assumptions imply that G is finitely-generated, so that we can choose a finite generating set R and put the word metric dR on G. (2) A Riemannian manifold is proper and geodesic iff it is complete. Proof of Lemma. We construct a quasi-isometry τ : G → X. Pick x0 ∈ X and let τ : G → X be the orbit map given by g 7→ g(x0). hx0 gx0 x0 Figure 3: Balls of radius diam(G\X) cover X. Orbit/s is/are coarsely dense, and the coarse transitivity of the action means the Cayley graph supplies the linear upper bound constants. If D = diam(X/G), then if x ∈ X ∃g ∈ G s.t. d(x, g(x)) ≤ D, and so τ is coarsely D-surjective. 5 To obtain the upper bound, let R = {r1, . . . , rg} and Q = maxi∈[g] d(x0, ri(x0)) for some fixed x0 = τ(1) ∈ X. If g = r1 ··· rn and n = dR(1, g) (i.e. we have a minimal word representation), then d(x0, g(x0)) ≤ Qn, i.e. d(τ(1), τ(n)) ≤ QdR(1, g), i.e. we can extend G,→ X into a map CayG,X ,→ X. Since G acts by isometries on both G and on X, if h ∈ G, then d(τ(h), τ(hg)) = d(τ(1), τ(g)) ≤ Qd(1, g) = Qd(h, hg) and so if g1, g2 ∈ G then d(τ(g1), τ(g2)) ≤ QdR(g1, g2). To obtain the lower bound, let S = {g ∈ G | d(x0, g(x0)) ≤ 3D}. S is finite; let p = maxs∈S dR(1, s). xn g4x0 x1 x2 x4 g3x0 g2x0 g1x0 x3 x0 Figure 4: We obtain the lower bound by approximating our geodesic (black) with a broken curve (red) that takes hops of ≤ 3D between orbit points. Hops between black points are ≤ D apart by construction. j d(x0,g(x0) k Choose a geodesic [x0, g(x0)] and divide it into N = D + 1 segments. For each i, choose gi ∈ G s.t. d(xi, gi(x0)) ≤ D. WMA g0 = id and gN = g. −1 −1 Then d(gi(x0), gi+1(x0)) ≤ 3D =⇒ d(x0, gi gi+1(x0)) ≤ 3D =⇒ gi gi+1 ∈ S. −1 −1 −1 −1 Nu g = g0(g0 g1)(g1 g2) ··· (gN−2gN1 )(gN−1gN ) and so d(x , g(x )) d (1, g) ≤ Np ≤ p 0 0 + 1 . R D 1 Then D( p dR(1, g) − 1) ≤ d(x0, g(x0)). D Hence τ is a (max{Q, p },D)-quasi-isometry. The Milnor-Svarcˇ lemma makes it possible to talk about the growth of groups in a meaningful well-defined way. 0.4 Growth functions of groups If G is generated by a finite set S, define βG,S(n) = #{g ∈ G | dS(1, g) ≤ n}, Example 0.19. • βZ,{1} = 2n + 1 (linear) 2 • β 2 = 2n + n + 1 (quadratic) Z ,{e1,e2} Pn i−1 • βF2,{a,b} = 1 + i=1 4(3 ) (exponential) 6 (Note e.g.) if T is a (finite) generating set for Z2, then every element in T can be written as a word of length ≤ Q in S (for some Q ∈ Z+.) n 2 2 2 Then βZ ,S( Q ) ≤ βZ ,T (n) ≤ βZ ,S(Qn); changing the choice of generating set does not change the order of growth of βG,S. 2 ∼ Corollary. Z =6 F2. Theorem 0.20 (Gromov). G is virtually nilpotent (i.e. has a nilpotent4 subgroup of finite index) iff it has polynomial growth. Example 0.21. The Heisenberg group H may be represented as the group of unipotent upper-triangular matrices 1 a b 0 1 c | a, b, c ∈ Z 0 0 1 1 1 or abstractly as hx, y, z | [x, y] = z, [x, z] = [y, z] = 1i (concretely we may take x = 1 , y = 1 1 1 1 1 1 , and z = 1 .) 1 1 4 It is a result of Milnor that βH = O(n ). Given f, g : N → N, we say that f 4 g if f(n) ≤ Cg(Cn + c) for some C. We say f g (f and g are “quasi-equal”) if g 4 f and f 4 g, and f ≺ g (f is “quasi-less-than” g) if f 4 g and g 46 f. Example 0.22. (1) For 1 < a < b, na ≺ nb. (2) For 1 < α < β, αn βn. (3) na ≺ 2n for all a > 0. Observation. If G is quasi-isometric to H, then βG βH . 2 Corollary. Z is not quasi-isometric to Z or to F2. Proof. Let j : G → H be a (k, c)-quasi-isometry. Then j(BG(1, n)) ⊂ BH (j(1), kn + c), which has size βH,kn+c. −1 1 If h ∈ H, j (h) ⊂ ball in G of radius kc + 1 since d(g1, g2) > kc + 1) =⇒ d(j(g1), j(g2)) ≥ k (kc + 1) − c > 0, and hence βG(n) ≤ βH (kn + c)βG(kc + 1), and βG(kc + 1 is constant w.r.t. n. Hence βG 4 βH . Similarly, βH 4 βG. Therefore βG βH . Which maps are quasi-isometrically equivalent? (1) Finite-index inclusions (2) Quotients by finite-index normal subgroups (3) No other criteria! (“Quasi-isometric rigidity”) 1 Hyperbolic groups 1.1 A whirlwind tour of the upper half-plane The upper half-plane model of hyperbolic geometry takes as the hyperbolic plane H2 = {(x, y) | y > 2 dx2+dy2 2 v·w 0} = {z ∈ C | =(z) > 0} with the metric dshyp = y2 ; so given v, w ∈ Tz(H ), hv, wihyp = =(z)2 and kvk 2 kvkhyp = =(z)2 . This is a conformal model for H : ∠hypv, w = hv, w. 4 A group is nilpotent if its lower central series terminates, i.e. ∃R ∈ N s.t. [g1, [g2,..., [gR−1, gR]] ... ] = 1. 7 0 2 R 1 R 1 |γ (t)| Given a path γ : [0, 1] → H , `hyp(γ) := 0 kγ(t)khypdt = 0 =(γ(t)) dt. dhyp(z1, z2) := infγ:z1 z2 `hyp(γ). |z−w|2 There is an explicit formula given by cosh dhyp(z, w) = 1 + 2=(z)=(w) . Now we want to find what the geodesics in H2 are ... “first we find a geodesic”. Fact. The y-axis is a geodesic in H2. 0 0 Proof. Let p : 2 → {x = 0} be the projection, i.e. p(z) = =(z). d = , and kd (v)k ≤ kvk H p 0 1 p hyp hyp with equality iff v is vertical. Thus (equivalently) `(p ◦ γ) ≤ `(γ) with equality iff γ0x) is vertical for all x, which is equivalent to the assertion that shortest paths joining points on the y-axis are vertical. az+b 2 Fact. z 7→ cz+d , where a, b, c, d ∈ R with ad − bc = 1, is an isometry of H . dh 0 Proof. The “efficient way to do this” is to compute it and show this acts as an isometry on the tangent bundle: dz = h (z) = (cz + d)−2, and =(h(z)) = =(z) , so kdh(v)k = kvk . However, this may be considered a “bad proof”, for “being a good |cz+d|2 hyp hyp Thurston student, I5 believe that no one every learned anything from a computation.” An alternative proof idea is to observe that M¨obiustransformations are products of inversions in circles perpendicular to the x-axis, i.e. to ∂H2. Fact. Every circle (or line) perpendicular to ∂H2 is a geodesic. These are the only geodesics. Proof. These are all images of the y-axis under (appropriate) M¨obiustransformations. Corollary. Geodesics are unique Proof. Any 2 points can be moved onto the y-axis, and geodesics on the y-axis are unique. Fact. Isom(H2) = PSL(2, R) consists of the M¨obiustransformations preserving H2. Idea of proof. PSL(2, R) acts transitively on T 1(H2) and an isometry is determined by the image of one vector in T 1(H2. The Poincar´edisk model 2 2 iz+1 Take a M¨obius transformation U : H → D and push forward the geometry. If we take U(z) = z+i , we 2|dz| obtain dsD2 = 1+|z|2 . Since U is a M¨obiustransformation, we have that Fact. Geodesics in D2 are circles or lines perpendicular to ∂D2. Isom(D2, hyp) is the group of M¨obius 2 1 R r 2 1+r transformations preserving D . If ξ ∈ S , d(0, rξ = 0 1−s2 ds = log 1−r . 2 R Fact. A circle of hyperbolic radius R about 0 ∈ D has Euclidean radius tanh 2 . 1+tanh R/2 Proof. R = log 1−tanh R/2 . Corollary. This circle has hyperbolic length Z 2π 2 Z π tanh ds = sinh 2R = 2π sinh R πeR 2 R 0 1 − tanh 2 0 and the disk it bounds has area ZZ 4 R 2 2 2 dx dy = 2π(cosh(R) − 1) πe . D (1 − x − y ) 5i.e. Dick Canary 8 R θ R θ sinh R = 2 e R Figure 5: Hyperbolic circles have exponential circumference and here we see the exponential divergence of geodesics and exponential growth which are two characteristics of negatively-curved spaces. Note also the constant isopermetric inequality obtained from the above: frac2π(cosh(R) − 1)2π sinh(R) → 1 as R → 0 or as R → ∞. Moreover there are unique geodesics (unlike e.g. in spherical geometry) and the sum of the angles in a triangle add up to < π: these are also characteristics of negatively-curved spaces. Ideal triangles Definition 1.1. An ideal triangle in H2 is a triangle spanned by geodesics with endpoints in ∂H2. Figure 6: Two ideal triangles (in the upper half-space model.) Fact. Ideal triangles are all congruent and have area π. Proof. Every ideal triangle is congruent to the one with vertices at ±1 and ∞ since PSL(2, R) acts transitively on triples of points in ∂H2. R 1 R√∞ 1 The area of this particular ideal triangle is given by −1 1−x2 y2 dy dx = π. Fact. All 2/3-ideal triangles (i.e. triangles in H2 with two of their vertices in ∂H2) with internal angle α are congruent and have area π − α. Proof. All such triangles are congruent to the one obtained by truncating the ideal triangle with vertices at ±1 and ∞. α Figure 7: A 2/3-ideal triangle with a nonzero angle α (in the upper half-space model.) R 1 R√∞ 1 The area of this latter 2/3-ideal triangle is given by cos(π−α) 1−x2 y2 dy dx = π − α. We note in passing that this is in fact (may in fact be obtained as) a special case of the Gauss-Bonnet theorem. Fact. A hyperbolic triangle with angles α, β, γ has area π − (α + β + γ). In particular, α + β + γ ≤ π. Proof. See Figure 8 9 a a c c b b Figure 8: Here a, b, c stand for α, β, γ resp.; they represent the angles of the small white triangle, and also the areas of the shaded 2/3-ideal triangles by the previous Fact. −1 Fact. Triangles in H2 are cosh (2)-slim. −1 Proof. If T has sides S1,S2,S3, and z ∈ S1, d(z, S2 ∪ S3) ≤ cosh (2): if R = d(z, S2 ∪ S3), then half of B(z, R) ⊂ T , so Area(B(z, R)) < 2 Area(T ) 2π cosh(R) − 2π < 2π cosh R < 2 Figure 9: That ball is at most half the triangle in area, and our desired inequality follows. Hyperbolic sports! Let’s think about baseball in hyperbolic space. How many outfielders would you need on a hyperbolic baseball diamond? (Suppose the outfield is the area between 100 and 300 feet out from the pitcher.) Well, 2 π 2 2 2 in Euclidean space E , the outfield has area 4 (300 − 100 ) ≈ 62, 832 square feet. In H , the outfield would 2π 100 have area 4 (cosh 300 − cosh 100) 10 square feet. Even assuming each outfielder could cover an area of 104 square feet ... that doesn’t look good (due to exponential growth in this negatively-curved space.) 2 1 2 (You would also never see the ball coming: in E the visual size of a ball of radius R (e.g.) is πR . In H , 1 2 it is π sinh R ∼ πeR .) Due to this exponential growth, real estate is cheap in hyperbolic space: one could imagine “a sketchy real-estate agent in hyperbolic space” hawking spectacular (but relatively—or worse—worthless) timeshares. But back to sports—maybe we should choose another sport. Let’s try golf. Suppose you were taking a shot at 300 feet, and you were 1 degree off. In E2, that would translate into your being ∼ 5.24 feet off at 2 2π sinh(300) 300 feet. In H , you would be 300 feet off. Oh well. You would have the same problem/s with something like soccer: you would never see the ball coming, and the game would mostly involve passes to nowhere. Or, if one imagined a sort of rectangular field with 10 equally long goal lines on both sides, the center line would be extremely narrow, and then the game would mostly involve the goalies kicking the balls out of bounds. Similarly, hyperbolic space would be a terrible place to go for a walk: you would never find your way home unless you were perfectly precise (due to the exponential divergence of geodesics.) Some notes coming out of the tour ... Definition 1.2. A (complete) n-manifold is hyperbolic if it is locally isometric to Hn. π Example 1.3. Σg is made from a regular hyperbolic 4g-gon with internal angles 2g and has area 2π(2g−2) = 2π|χ(Σg)|. Figure 10: (Left) a torus formed by gluing the sides of a square; (right) a genus-2 surface formed by gluing π the sides of a regular hyperbolic octagon with angles 4 . Recall a proper geodesic metric space is hyperbolic if ∃δ > 0 s.t. all triangles are δ-slim (i.e. if T is a geodesic triangle in X with edges S1,S2,S3 and x ∈ S1, then d(x, S1 ∪ S2) ≤ δ. A group is hyperbolic if it acts co-compactly and by isometries on a hyperbolic metric space. Example 1.4. All finite groups are hyperbolic: in particular G finite =⇒ ΓG (a Cayley graph of G) is diam(ΓG)-hyperbolic. Similarly, all compact hyperbolic metric spaces are δ-hyperbolic. Fn is hyperbolic: it acts on a punctured (hyperbolic) surface. π1(Σg) (with g ≥ 2) is hyperbolic: it acts co-compactly and by isometries on Σg. Z2 is not ... why? (We will find out.) 1.2 The Fellow Traveller Property Definition 1.5. If α : J → X is a (k, c)-quasi-isometric embedding, and J is an interval in R, then α is called a (k, c)-quasi-geodesic. Note that geodesics need not be unique in hyperbolic metric spaces. 2 The universal cover of a hyperbolic surface Σg is H . Since Σg is a simply-connected Riemannian manifold 2 2 locally isometric to H , so π1(Σg) acts properly and co-compactly on H if g ≥ 2. If α :[a, b] → X is a (k, c)-quasi-geodesic and X is δ-hyperbolic, then ∃D = D(k, c, δ) s.t. if [α(a), α(b)] is a geodesic (or even quasi-geodesic) going from α(a) to α(b), then α([a, b]) ⊂ ND[α(a), α(b)] ⊂ N2D(α([a, b])). The key fact used in the proof (which will be given below, along with a more precise statement of the Property) is the exponential divergence of geodesics. For now, we pause to state and prove an important corollary of the fellow traveller property: Corollary. If f : X → Y is a quasi-isometric embedding, and Y is hyperbolic, then X is hyperbolic. Proof. Suppose Y is δ-hyperbolic and f is a (k, c)-quasi-isometric embedding. Consider a (geodesic) triangle in X with sides s1, s2, s3. 0 Let si be a geodesic in Y with the same endpoints as f(si). By the fellow traveller property, there exists 0 0 0 0 0 0 0 p ∈ si s.t. d(f(0), p ) ≤ D = D(k, c, δ). Since s1, s2, s3 form a geodesic triangle, ∃q ∈ s2 ∪ s3 (WLOG s3) 0 0 00 0 00 s.t. d(p , q ) < δ and q = f(q) ∈ f(s2) s.t. d(q , q ) < D. 1 1 Then d(f(p), f(q)) < 2D + δ =⇒ d(n, q) < k (2D + δ) + C =⇒ T is k (2D + δ) + C -hyperbolic. 11 Figure 11: A quasi-isometry maps the (thin) black geodesic triangle on the right to the (thinnish) black quasi-geodesic triangle on the right, which can be straightened to (is uniformly close to) the red geodesic triangle on the right. Fact (Exponential divergence of geodesics). Suppose X is δ-hyperbolic, p lies on a geodesic [x, y] ∈ X, and α : [0, 1] → X is a rectifiable path joining x to y. Then d(p, α(I)) ≤ δ log2(`(α)) + 1. Figure 12: Any rectifiable curve (in particular, quasi-geodesic—grey) which is at least D away in Hausdorff distance (red) from a geodesic (black) is exponentially (≥ 2(D−1)/δ) long. Proof. “A picture I’m going to spend all sorts of time making precise.” Parametrize α proportional to arc-length. Choose N ∈ N s.t. 2−(N+1)`(α) < 1 ≤ 2−N `(α), i.e. 2N ≤ `(α) < 2N+1, i.e. (since we have parametrized k k+1 ∝ arc-length) 1 ≤ ` α 2N , 2N < 2. 1 1 Consider the (geodesic) triangle [x, y], [α(0), α( 2 )], [α( 2 ), α(1)]. 1 1 Pick y1 ∈ [α(0), α( 2 )] ∪ [α( 2 ), α(1)] s.t. d(y1, p) < δ 1 1 1 1 1 If y1 ∈ [α(0), α( 2 )] (say), consider the triangle [α(0), α( 2 )], [α(0), α( 4 )], [α( 4 ), α( 2 )]. 1 1 1 k k+1 Choose y2 ∈ [α(0), α( 2 )]∪[α( 4 ), α( 2 )] s.t. d(y1, y2) < δ. Continue on until you find yN ∈ α 2N , α 2N with d(yN , yN−1) < δ. Figure 13: Starting with p on the geodesic (red dots), we find a sequence of points yi (successive red dots), each within δ of the previous, by δ-hyperbolicity. There are logarithmically many such points before we get within distance 1 of our rectifiable curve. 12 k k+1 Then d(yN , p) < Nδ, and d(yN , α([0, 1]) < 1 since ` α 2N , 2N < 2. (Consider the geodesic triangle with endpoints α k , α k+1 , and y .) 2N 2N N Hence we have d (p, α([0, 1])) ≤ Nδ + 1 ≤ δ log2(`(α)) + 1 We can use this to show, among other things, the following Theorem 1.6 (Fellow Traveller Property). If γ :[a, b] → X is a (k, c)-quasigeodesic, X is δ-hyperbolic and [γ(a), γ(b)] is a geodesic, then there exists D = D(k, c, δ) s.t. γ([a, b]) ⊂ ND([α(a), α(b)]) and [γ(a), γ(b)] ⊂ ND(γ([a, b])). z' y' p z y Figure 14: Sketch of argument that quasigeodesics are uniformly close to geodesics: the dotted red circle is distance D from p; we apply exponential divergence of geodesics to compare the blue rectifiable path with the orange geodesic path. Proof. Let D be the Hausdorff distance between γ and [γ(a), γ(b)], and let p ∈ [γ(a), γ(b)] be s.t. d(p, γ) = D. Let BD(p) be a ball of radius D around p (see diagram above.) Pick y 6= z ∈ [γ(a), γ(b)] outside BD(p), at distance D away from the boundary along [γ(a), γ(b)], and let y0, z0 be points on γ before and after (resp.) 0 0 it intersects BD(p). Note d(y, y ) ≤ d(y, γ) ≤ D and d(z, z ) ≤ d(z, γ) ≤ D. Then, by the triangle inequality, d(y0, z0) ≤ 6D; choosing γ to be a nice quasi-geodesic (and possibly changing the quasi-isometry constants to some other k0, c0 which depend only on k and c—see below), we 0 0 0 0 0 0 have `(γ([y , z ])) ≤ 6Dk + c . Then, since γ([y , z ]) avoids the ball BD(p), exponential divergence of geodesics says that we should have 0 d(p, BD(p)) = D ≤ δ log2(6Dk + c + 4D) + 1 For fixed k, c, once we take large enough D, the LHS will be larger than the RHS; hence in particular there is some maximum D = D(k, c, δ) for which the required inequality will hold. Hence the any point on the quasi-geodesic γ lies relatively close to the geodesic between its endpoints, i.e. γ([a, b]) ⊂ ND([γ(a), γ(b)]). Conversely, to show that any point on the geodesic lies relatively close to the quasi-geodesic i.e. [γ(a), γ(b)] ⊂ ND(γ([a, b])) pick q ∈ γ([a, b]) maximising d(q, [γ(a), γ(b)]). Let p be the corresponding point on γ([a, b]). If d(q, p) ≤ D0 where D0 = D(k, c, δ) was the maximum we found above, we are done (choose D = D0.) If not, choose points q1 ∈ [γ(a), q) ⊂ γ and q2 ⊂ (q, γ(b)] ⊂ γ. Let X = {p ∈ [γ(a), γ(b)] | d(p, q1) ≤ D0} Y = {p ∈ [γ(a), γ(b)] | d(p, q2) ≤ D0} 13 and choose p1 ∈ X, p2 ∈ Y s.t. d(pi, qi) ≤ D0. If s and t are s.t. γ(s) = q1 and γ(t) = q2, then 0 0 `(γ([s, t])) ≤ k (2D0) + c and so 1 d(q, p) ≤ `(γ([s, t])) + max{d(p, q ), d(p, q )} 2 1 2 c ≤ k0D + + D 0 2 0 q q2 q1 p p p1 2 Figure 15: Sketch of argument that geodesics are uniformly close to quasigeodesics: each of the blue segments has length ≤ D0. 0 c and if we now choose D = D1 = k D0 + 2 + D0 then we have our desired result. To show that we can take our quasi-geodesics to be nice (in particular, rectifiable), we will need the following slightly technical lemma: Lemma 1.7. Given a (k, c)-quasi-geodesic γ :[a, b] → X in a geodesic metric space X, there exist k0 and c0 (depending on k and c) and a (k0, c0)-quasi-geodesic β :[a.b] → X s.t. (1) β(a) = γ(a) and β(b) = γ(b). (2) The Hausdorff distance between γ([a, b]) and β([a, b]) is ≤ k + c. (3) `(β[a, b]) ≤ k0d(β(a), β(b)) + c0. Proof. Let S = ([a, b] ∩ Z) ∪ {a, b} = {a = t0 ≤ t1 ≤ · · · ≤ tn = b}. Choose β(t1) = γ(ti)∀ti ∈ S. Note that d(γ(ti), γ(ti+1) ≤ k(1)+c = k+c since γ is a (k, c)-quasi-geodesic. Choose β|[ti,ti+1] to have image a geodesic segment [β(ti, β(ti+1)] parametrized proportional to arc-length.