LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS

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LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS 1. The Bishop-Gromov Volume Comparison Theorem Recall that the Riemannian volume density is defined, in an open chart, to be dvol = G x 1 dx 1 dx m, where G = det(g ij ) and dx 1 dx m is the Lebesgue measure on R m. Now let (M, g) be a complete Riemannian manifold. We have already known (from PSet 3) that the exponential map exp p is a diffeomorphism onto the dense open set M \ Cut(p). We denote Σ(p) = exp 1 (M \ Cut(p)), then it is an open star-shaped domain in T p M. We can regard the triple {exp 1 p, M\ Cut(p), Σ(p)} as a coordinate chart on M. On Σ(p) (or T p M) we will decompose the Lebesgue measure into via polar coordinates dx 1 dx m = r m 1 drdθ, where dθ is the usual surface measure on S m 1. It follows that there exists a function µ(r, Θ) = G exp p (r, Θ)r m 1 inside Σ(p), so that dvol = µ(r, Θ)drdΘ. For simplicity we will set µ(r, Θ) = 0 outside Σ(p). Note that by definition B r (p) = exp p (B r (0)) = exp p (B r (0) Σ(p) ). Since Cut(p) is of measure zero in M, we get Vol(B r (p)) = µ(r, Θ)drdΘ = B r(0) Σ(p) B r(0) µ(r, Θ)drdΘ. To calculate the function µ(r, Θ), we will fix a direction Θ S p M and consider Jacobi fields along the geodesic γ(t) = exp p (tθ). Proposition 1.1. Let V 2,, V m be normal Jacobi fields along the geodesic γ with V j (0) = 0. Suppose γ(0) V 2,, γ(0) V m are linearly independent. Then for any point (r, Θ) Σ(p), µ(r, Θ) = det(v 2(r),, V m (r)) det( γ(0) V 2,, γ(0) V m ), 1

2LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS where the determinant is taken with respect to an orthonormal basis in ( γ(t)). Proof. Fix any Θ S p M. Let e 1 = Θ, e 2 = γ(0) V 2,, e m = γ(0) V m. Since they are linearly indepedent, using e 1,, e m one can define a set of global linear coordinates u 1,, u m on T p M. Then obviously du 1 du m = According to lecture 13 (see also lecture 20), r m 1 det(e 2,, e m ) drdθ. V j (t) = t(d exp p ) tθ (e j ). Note that under exp p, u 1,, u m also gives a coordinate system near exp p (rθ) if rθ Σ(p). For this coordinate system, we have (at exp p (rθ)) It follows 1 = γ(r), j = 1 r V j(r) (j 2). r 2 g ij (r, Θ) = r 2 i, j = V i (r), V j (r) for i, j 2. Since γ is a normal geodesic, 1, 1 = 1. Also by Gauss lemma, 1, i = 0 for i 2. It follows It follows G = det(g ij ) = r 2m+2 det( V i, V j ) i,j 2 = r 2m+2 det(v 2 (r),, V m (r)) 2. Gdu1 du m = det(v 2(r),, V m (r)) det( γ(0) V 2,, γ(0) V m ) drdθ. Now we compare the volume deisities. In what follows we will denote by µ k (r) the function µ(r, Θ) for the space form Mk m (it is obviously independent of p and independent of Θ). Lemma 1.2. If (M, g) is a complete Riemannian manifold with Ric (m 1)k, then for any fixed Θ S p M and any r with rθ Σ(p), we have µ (r, Θ) µ(r, Θ) µ k (r) µ k (r), where the first derivative is taken with respect to r. Proof. Let γ be the normal geodesic starting at p in the direction Θ. Consider a parallel orthonormal frame {e i (t)} along γ with e 1 (t) = γ(t). Let V j (t) be a Jacobi field along γ such that V j (0) = 0 and V j (r) = e j (r).

LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS3 For simplicity we will denote A(t) = ( V i (t), V j (t) ) i,j 2 and d(t) = det A(t) = (det(v 2 (r),, V m (r))) 2. Then we have A(r) = Id. By matrix algebra (c.f. Lecture 5), So we have d (t) = d(t)tr(a 1 (t)a (t)). µ (r, Θ) µ(r, Θ) = 1 d m (r) 2 d(r) = V j (r), γ(r) V j (r) = Now consider (c.f. lecture 21) H j (t) = sn k(t) sn k (r) e j(t), I(V j, V j ). where sn k (t) = sin( kt) k or t or sinh( kt) k, depending on whether k is positive, zero or negative. Then H j and V j have the same values at end points. So I(V j, V j ) I(H j, H j ). Moreover, a direct computation shows r ( ) 2 snk (t) I(H j, H j ) = [(n 1)k Ric( γ, γ)]dt + sn k (r) 0 H j (r), γ(r) H j. On the other hand, one can repeat the above computation for the space form Mk m, and get µ k (r) m µ k (r) = Hj k (r), γ(r) Hj k = H j (r), γ(r) H j. So we conclude µ (r, Θ) µ(r, Θ) µ k (r) µ k (r). Now we are ready to prove the Bishop-Gromov volume comparison theorem: Theorem 1.3 (Bishop-Gromov). If (M, g) is a complete Riemannian manifold with Ric (m 1)k, and p M is an arbitrary point. Then the function r Vol(B r(p)) Vol(B k r ) is a non-increasing function which tends to 1 as r goes to 0, where B k r is a geodesic ball of radius r in the space form M m k. In particular, Vol(B r(p)) Vol(B k r ).

4LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS Proof. For simplicity we will denote a(r) = µ(r, Θ)dΘ, b(r) = µ k (r)dθ. S m 1 S m 1 Then d dr ( log Vol(B ) r(p)) Vol(Br k ) = a(r) b(r) r r a(t)dt b(t)dt = 0 0 r 0 (a(r)b(t) a(t)b(r))dt ( r a(t)dt) ( r b(t)dt). 0 0 To prove the first part, it suffices to prove a(r)b(t) a(t)b(r) 0 for t r, i.e. a(t) b(t) is non-increasing. But since µ k (r) is independent of Θ, a(t) b(t) = S m 1 µ(t, Θ) µ k (t) dθ. So it suffices to prove that the function µ(t,θ) µ k is non-increasing in t for any fixed Θ. (t) This follows from lemma 1.2 and d dt ( log µ(t, Θ) µ k (t) ) = µ (t, Θ) µ(t, Θ) µ k (t) µ k (t). Note that if tθ Σ(p), then one cannot apply lemma 1.2. However, since µ(t, Θ) = 0 in that case, the function t µ(t,θ) µ k is still non-increasing. (t) The second part follows from theorem 2.5 in lecture 14. Remark. By carefully checking the proof of lemma 2.1, one can see that under the assumption of Bishop-Gromov s theorem, Vol(B r (p)) = Vol(B k r ) or Vol(B r (p)) Vol(B k r ) = Vol(B R(p)) Vol(B k R ) (r < R) if and only if B r (p) (or B R (p) in the second case) is isometric to B k r. [Prove this!] 2. Applications of the volume comparison theorem Let (M, g) be a complete Riemannian manifold with Ric 0. Bishop-Gromov volume comparison theorem, Vol(B r (p)) Vol(B 0 r ) = ω m r m, According to where ω m is the volume of unit ball in R m, with equality holds if and only if (M, g) is isometric with (R m, g 0 ). This gives an upper bound of the volume growth. A natural question is: what is the lower bound of the volume growth? In other words, what is the largest α such that for all r (large enough), Vol(B r (p)) cr α? Of course this question makes sense only for non-compact Riemannian manifolds.

LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS5 Theorem 2.1 (Calabi-Yau). Let (M, g) be a complete non-compact Riemannian manifold with Ric 0. Then there exists a positive constant c depending only on p and m so that Vol(B r (p)) cr for any r > 2. Proof. (Following Gromov.) Since M is complete and non-compact, for any p M there exists a ray, i.e. a geodesic γ : [0, ) M with γ(0) = p such that dist(p, γ(t)) = t for all t > 0. (Exercise: Prove the existence of a ray.) For any t > 3, using the Bishop-Gromov volume comparison theorem, we get 2 Vol(B t+1 (γ(t))) Vol(B t 1 (γ(t))) ω m(t + 1) m (t + 1)m = ω m (t 1) m (t 1). m On the other hand, by triangle inequality, B 1 (p) B t+1 (γ(t))\b t 1 (γ(t)). It follows i.e. Vol(B 1 (p)) Vol(B t 1 (γ(t))) Vol (B t+1(γ(t))\b t 1 (γ(t))) Vol(B t 1 (γ(t))) (t + 1)m (t 1) m (t 1) m, (t 1) m Vol(B t 1 (γ(t))) Vol(B 1 (p)) (t + 1) m (t 1) C(m)Vol(B 1(p))t, m wehre C(m) is the infimum of the function 1 (t 1) m on [ 3, ), which is positive. t (t+1) m (t 1) m 2 Now the theorem follows from the fact B r (p) B r+1 1(γ(r + 1 2 2 )). As a second application of volume comparison theorem, we will prove Theorem 2.2 (S.Y. Cheng). Let (M, g) be a complete Riemanniian manifold with Ric (n 1)k for some k > 0, and diam(m, g) = π k, then M is isometric to the standard sphere of radius 1 k. Proof. (Following Shiohama) For simplicity we may assume k = 1. By Bishop-Gromov volume comparison theorem, for any p M, Vol(B π/2 (p)) Vol(M) = Vol(B π/2(p)) Vol(B π (p)) Vol(B1 π/2 ) Vol(B 1 π) = 1 2. Now let p, q M so that dist(p, q) = π. The the above inequality implies Vol(B π/2 (p)) 1 2 Vol(M), Vol(B π/2(q)) 1 2 Vol(M).

6LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS Since B π/2 (p) B π/2 (q) =, we must have Vol(B π/2 (p)) Vol(B π (p)) = Vol(B1 π/2 ) Vol(B 1 π) = 1 2, Vol(B π/2 (q)) Vol(B π (q)) = Vol(B1 π/2 ) Vol(B 1 π) = 1 2. According to Bishop-Gromov comparison theorem, B π/2 (p) and B π/2 (q) are both isometric to half sphere. It follows that M is isometric to S m. Finally we will describe some applications of the volume comparison theorem to the fundamental group of complete noncompact Riemannian manifolds with nonnegative Ricci curvatures. Let s start with some abstract definitions in algebra. Let G be a group. G is said to be finitely generated if there exists a finite subset Γ = {g 1,, g N } of G so that any element in G can be represented as group multiplications (or inverse) of elements in Γ. Note that if the group identity element e is in Γ, we can always remove it. Now let s fix a set Γ of generators of G. The growth function of G with respect to Γ is defined to be the number of group elements that can be represented as a product of at most k generators, i.e. N Γ G(k) = #{g G l k and g i1,, g il Γ s.t. g = g ±1 i 1 g ±1 i l }. Definition 2.3. Let G be finitely generated, and Γ is a finite set that generates G. We say that G is of (at most) polynomial growth if N Γ G(k) ck n for some constant c depending only on G, Γ. Similarly we say G is of (at least) exponential growth if N Γ G(k) ce k. Remark. Note that if Γ is another finite set of generators, then there exists integers c 1, c 2 so that any element of Γ can be represented via at most c 1 elements of Γ, and any element of Γ can be represented via at most c 2 elements of Γ. It follows that N Γ G(k) N Γ G (c 1 k), N Γ G (k) N Γ G(c 2 k). So the conception of polynomial/exponential growth is independent of the choice of the generating set. Remark. A celebrated theorem of Gromov: If G is finitely generated and has polynomial growth, then G is virtually nilpotent, i.e. G contains a nilpotent subgroup of finite index. Coming back to Riemannian manifolds. If (M, g) is a compact Riemannian manifold, and M its universal covering endowed with the pull-back metric. Then the fundamental group π 1 (M) acts isometrically on M as the group of deck transformations. Some known results:

LECTURE 24: THE BISHOP-GROMOV VOLUME COMPARISON THEOREM AND ITS APPLICATIONS7 If M is compact, then π 1 (M) is finitely generated. [c.f. Munkres, Topology, Exercise at the end of chapter 13.][See also Allen Hatcher, Algebraic Topology, page 529.] (Schwarz 1957) The rate of volume growth of M is equal to the rate of growth of π 1 (M). (Gromov) If K 0, then the set of generates can be choose to be no more than c(m) for some constant c depending only on m. A similar results holds for manifolds with K k 2 and diam(m, g) D. (The proof uses Toporogov comparison theorem. The first part was proved earlier in this course.) (Milnor) If Ric 0, then NG Γ(k) ckm ; if K < 0, then NG Γ(k) cek. (The proof uses volume comparison theorem. See the following theorem for the first part.) For non-compact Riemannian manifolds, the fundamental group might be not finitely generated in general. However, we have Theorem 2.4 (Milnor). Let M be a complete Riemannian manifold with Ric 0 and let G π 1 (M) be any finitely generated subgroup. Then there exists a constant c depending only on M and the chosen finite generating set Γ of G so that N Γ (k) ck m. Proof. Let Γ be a finite set of generators of G. Fix a point p M and let l = max{dist( p, g i p) g i Γ}. Then by triangle inequality, for any g = g i1 g ik Γ k G, dist( p, g p) kl. On the other hand side, we can pick ε = 1 min{dist( p, g p) e g G} > 0 3 so that the balls B ε (g p) are all disjoint for g G. It follows B kl+ε ( p) g Γ kb ε (g p) and thus Vol(B kl+ε ( p)) NGVol(B Γ ε (p)). Applying the Bishop-Gromov s volume comparison theorem, we get N Γ G Vol(B kl+ε( p)) Vol(B ε (p)) (kl + ε)m ε m ck m. We end this part of our course by stating the following major conjecture in Riemannian geometry: Conjecture (Milnor). Let M be a complete Riemannian manifold with Ric 0, then π 1 (M) is finitely generated.