We now begin using the theory established in the last two lectures to rigorously extract an asymptotic gradient shrinking soliton from the scaling limit of any given \kappa-solution. This will require a number of new tools, including the notion of a geometric limit of pointed Ricci flows t \mapsto (M, g(t), p), which can be viewed as the analogue of the Gromov-Hausdorff limit in the category of smooth Riemannian flows. A key result here is Hamilton’s compactness theorem: a sequence of complete pointed non-collapsed Ricci flows with uniform bounds on curvature will have a subsequence which converges geometrically to another Ricci flow. This result, which one can view as an analogue of the Arzelá-Ascoli theorem for Ricci flows, relies on some parabolic regularity estimates for Ricci flow due to Shi.

Next, we use the estimates on reduced length from the Harnack inequality analysis in Lecture 13 to locate some good regions of spacetime of a \kappa-solution in which to do the asymptotic analysis. Rescaling these regions and applying Hamilton’s compactness theorem (relying heavily here on the \kappa-noncollapsed nature of such solutions) we extract a limit. Formally, the reduced volume is now constant and so Lecture 14 suggests that this limit is a gradient soliton; however, some care is required to make this argument rigorous. In the next section we shall study such solitons, which will then reveal important information about the original \kappa-solution.

Our treatment here is primarily based on Morgan-Tian’s book and the notes of Ye. Other treatments can be found in Perelman’s original paper, the notes of Kleiner-Lott, and the paper of Cao-Zhu. See also the foundational papers of Shi and Hamilton, as well as the book of Chow, Lu, and Ni.

– Geometric limits –

To develop the theory of geometric limits for pointed Ricci flows t \mapsto (M,g(t),p), we begin by studying such limits in the simpler context of pointed Riemannian manifolds (M,g,p), i.e. a Riemannian manifold (M,g) together with a point p \in M, which we shall call the origin or distinguished point of the manifold. To simplify the discussion, let us restrict attention to complete Riemannian manifolds (though for later analysis we will eventually have to deal with incomplete manifolds).

Definition 1. (Geometric limits) A sequence (M_n,g_n,p_n) of pointed d-dimensional connected complete Riemannian manifolds is said to converge geometrically to another pointed d-dimensional connected complete Riemannian manifold (M_\infty,g_\infty,p_\infty) if there exists a sequence V_1 \subset V_2 \subset \ldots of connected neighbourhoods of p_\infty increasing to M_\infty (i.e. \bigcup_n V_n = M_\infty) and a sequence of smooth embeddings \phi_n: V_n \to M_n mapping p_\infty to p_n such that

  1. The closure of each V_n is compact and contained in V_{n+1} (note that this implies that every compact subset of M_\infty will be contained in V_n for sufficiently large n);
  2. The pullback metric \phi_n^* g_n converges in the C^\infty_{loc}(M_\infty) topology to g_\infty (i.e. all derivatives of the metric converge uniformly on compact sets).

Example 1. The pointed round d-sphere of radius R converges geometrically to the pointed Euclidean space {\Bbb R}^d as R \to \infty. Note how this example shows that the geometric limit of compact manifolds can be non-compact. \diamond

Example 2. If (M,g) is Hamilton’s cigar (Example 3 from Lecture 8), and p_n is a sequence on M tending to infinity, then (M,g,p_n) converges geometrically to the pointed round 2-cylinder. \diamond

Example 3. The d-torus of length 1/n does not converge to a geometric limit as n \to \infty, despite being flat. More generally, the sequence needs to be locally uniformly non-collapsed in order to have a geometric limit. \diamond

Exercise 1. Show that the geometric limit (M_\infty,g_\infty,p_\infty) of a sequence (M_n,g_n,p_n), if it exists, is unique up to (pointed) isometry. \diamond

Geometric limits, as their name suggests, tend to preserve all (local) “geometric” or “intrinsic” information about the manifold, although global information of this type can be lost. Here is a typical example:

Exercise 2. Suppose that (M_n,g_n,p_n) converges geometrically to (M_\infty,g_\infty,p_\infty). Show that \hbox{Vol}_{g_\infty}(B_{g_\infty}(p_\infty,r)) = \lim_{n \to \infty} \hbox{Vol}_{g_n}(B_{g_n}(p_n,r)) for every 0 < r < \infty, and that we have the Fatou-type inequality \hbox{Vol}_{g_\infty}(M_\infty) \leq \lim\inf_{n \to \infty} \hbox{Vol}_{g_n}(M_n). Give an example to show that the latter inequality can be strict. \diamond

Here is the basic compactness theorem for such limits.

Theorem 1. (Compactness theorem) Let (M_n,g_n,p_n) be a sequence of connected complete Riemannian d-dimensional manifolds. Assume that

  1. (Uniform bounds on curvature and derivatives) For all k, r_0 \geq 0, one has the pointwise bound |\nabla^k \hbox{Riem}_n|_{g_n} \leq C_{k,r_0} on the ball B_n(p_n,r_0) for all sufficiently large n and some constant C_{k,r_0}.
  2. (Uniform non-collapsing) For every r_0 > 0 there exists \delta, \kappa > 0 such that \hbox{Vol}_n(x,r) \geq \kappa r^d for all x \in B_n(p_n,r_0) and 0 < r \leq \delta, and all sufficiently large n.

Then, after passing to a subsequence if necessary, the sequence (M_n,g_n,p_n) has a geometric limit.

Proof. (Sketch) Let r_0 > 0 be an arbitrary radius. From Cheeger’s lemma (Theorem 1 from Lecture 7) and hypothesis 2, we know that the injectivity radius on B_n(p_n,2r_0) is bounded from below by some small \delta > 0 for sufficiently large n. Also, from the curvature bounds and Bishop-Gromov comparison geometry (Lemma 1 from Lecture 9) we know that the volume of B_n(p_n,2r_0) is uniformly bounded from above for sufficiently large n.

Now find a maximal \delta/4-net x_{n,1},\ldots,x_{n,k} of B_n(p_n,r_0), thus the balls B_n(x_{n,1},\delta/8), \ldots, B_n(x_{n,k},\delta/8) are disjoint and the balls B_n(x_{n,1},\delta/4), \ldots, B_n(x_{n,k},\delta/4) cover B_n(p_n,r_0). Volume counting shows that k is bounded for all sufficiently large n; by passing to a subsequence we may assume that it is constant. Similarly we may assume that all the distances d_n(x_{n,i},x_{n,j}) converge to a limit. Using the exponential map and some arbitrary identification of tangent spaces with {\Bbb R}^d, we can identify each ball B_n(x_{n,i},\delta/2) with the standard Euclidean ball of radius \delta/2. Any pair x_{n,i}, x_{n,j} of separation less than \delta/2 induces a smooth transition map from the Euclidean ball of radius \delta/2 into some subset of {\Bbb R}^d, which can be shown by comparison geometry to be uniformly bounded in C^\infty norms; applying the (C^\infty version of the) Arzelá-Ascoli theorem we may thus pass to a subsequence and assume that all these transition maps converge in C^\infty to a limit. It is then a routine matter to glue together all the limit transition maps to fashion an incomplete manifold to which the balls B_n(p_0,r_0) converge geometrically (up to errors of O(\delta) at the boundary). Furthermore, as one increases r_0, one can show (by a modification of Exercise 1) that these limits are compatible. Now letting r_0 go to infinity (and using the usual diagonalisation trick on all the subsequences obtained), and then gluing together all the incomplete limits obtained, one can create the full geometric limit. \Box

Remark 1. One could use ultrafilters here in place of subsequences, but this does not significantly affect any of the arguments. \diamond

Now we turn to geometric limits of pointed Ricci flows (Ricci flows t \mapsto (M,g(t)) with a specified origin p \in M).

Definition 2. Let t \mapsto (M_n,g_n(t),p_n) be a sequence of pointed d-dimensional complete connected Ricci flows, each on its own time interval I_n. We say that a pointed d-dimensional complete connected Ricci flow t \mapsto (M_\infty,g_\infty(t),p_\infty) on a time interval I is a geometric limit of this sequence if

  1. Every compact subinterval of I is contained in I_n for all sufficiently large n.
  2. There exists neighbourhoods V_n of p_\infty as in Definition 1, compact time intervals J_n \subset I increasing to I, and smooth embeddings \phi_n: V_n \to M_n preserving the origin such that the pullback of the flow g_n to J_n \times V_n converges in spacetime C^\infty_{loc} to g_\infty.

Exercise 3. Show that if a sequence of \kappa-noncollapsed Ricci flows (with a uniform value of \kappa) converges geometrically to another Ricci flow, then the limit flow is also \kappa-noncollapsed. \diamond

Now we present Hamilton’s compactness theorem for Ricci flows, which requires less regularity hypotheses than Theorem 1 due to the parabolic smoothing effects of Ricci flow (as captured by Shi’s estimates, see Theorem 3).

Theorem 2. (Hamilton compactness theorem) Let t \mapsto (M_n,g_n(t),p_n) and I_n be as in Definition 2, and let I be an open interval obeying hypothesis 1 of that definition. Let t_0 \in I be a time. Suppose that

  1. For every compact subinterval J of I containing t_0 and every r > 0, one has the curvature bound |\hbox{Riem}_n|_{g_n} \leq K on the cylinder J \times B_{g_n(t_0)}(p_n,r) for some K = K(J,r) and all sufficiently large n; and
  2. One has the non-collapsing bound \hbox{Vol}_{g_n(t_0)}(B_{g_n(t_0)}(p_n,r)) \geq \kappa r^d for some r > 0 and \kappa > 0, and all sufficiently large n.
  3. (Uniform lower bound on curvature)  For any compact J, there is a K such that for any r>0, one has the curvature lower bound \hbox{Ric}_n(g_n) \geq -K on J \times B_{g_n(t_0)}(p_n,r) for all sufficiently large n.  (This is not quite implied by 1. because the curvature bound K there is allowed to depend on r, whereas here we require that K is independent of r.)

Then some subsequence of t \mapsto (M_n,g_n(t),p_n) converges geometrically to a limit t \mapsto (M_\infty,g_\infty(t),p_\infty) on I.

Condition 3 is technical (and was erroneously omitted in some of the literature), but it was recently observed by Topping that the claim fails without some hypothesis of this form.  Fortunately, in the applications to the Poincare conjecture one always has a uniform lower bound on Ricci curvature, and so Condition 3 is not difficult to verify in practice.

Proof. By Shi’s estimates (Theorem 3) we can upgrade the bound on curvature in hypothesis 1 to bounds on derivatives of curvature. Indeed, these estimates imply that for any J, r as in that hypothesis, and any k \geq 0, we have |\nabla^k \hbox{Riem}_n|_{g_n} \leq K for some K = K(J,r,k) and sufficiently large n.

Now we restrict to the time slice t=t_0 and apply Theorem 1. Passing to a subsequence, we can assume that (M_n,g_n(t_0),p_n) converges geometrically to a limit (M_\infty,g_\infty(t_0),p_\infty).

For any radius r and any compact J in I containing t_0, we can pull back the flow t \mapsto (M_n,g_n(t),p_n) to a (spatially incomplete) flow t \mapsto (B_{g_\infty(t_0)}(p_\infty,r), \tilde g_n(t), p_\infty) on the cylinder J \times B_{g_\infty(t_0)}(p_\infty,r) for sufficiently large n. By construction, \tilde g_n(t_0) converges in C^\infty_{loc}(B_{g_\infty(t_0)}(p_\infty,r)) norm to g_\infty(t_0); in particular, it is uniformly bounded in each of the seminorms of this space. Also, each t \mapsto \tilde g_n(t) is a Ricci flow with uniform bounds on any derivative of curvature for sufficiently large n.

Exercise 4. Using these facts, show that the sequence of flows t \mapsto \tilde g_n is uniformly bounded in each of the seminorms of C^\infty_{loc}(J \times B_{g_\infty(t_0)}(p_\infty,r)) for each fixed J, r, and for n sufficiently large. \diamond

By using the Arzelá-Ascoli theorem as before, we may thus pass to a further subsequence and assume that t \mapsto \tilde g_n(t) converges in C^\infty_{loc}(J \times B_{g_\infty(t_0)}(p_\infty,r)) to a limiting flow t \mapsto g_\infty(t). Clearly this limit is a Ricci flow. Letting r \to \infty and pasting together the resulting limits one obtains the desired geometric limit. (One has to verify that every geodesic in (M_\infty,g_\infty(t),p_\infty) starting from p_\infty can be extended to any desired length, thus establishing completeness by the Hopf-Rinow theorem, but this is easy to establish given all the uniform bounds on the metric and curvature, and their derivatives. It is here that hypothesis 3 is used to prevent the metric from shrinking too rapidly as one goes backwards in time. ) \Box

– Locating an asymptotic gradient shrinking soliton –

We now return to the study of \kappa-solutions t \mapsto (M,g(t)). We pick an arbitrary point x_0 \in M and consider the reduced length function l = l_{(0,x_0)}. Recall (see equation (18) from Lecture 11) that we had

\inf_{x \in M} l(t,x) < d/2 (1)

for every t < 0. (This bound was obtained from the parabolic inequality \partial_\tau l \geq \Delta l + \frac{l-(d/2)}{\tau} and the maximum principle.) Thus we can find a sequence (-\tau_n, x_n) \in (-\infty,0] \times M with \tau_n \to \infty such that

l(-\tau_n,x_n) = O(1). (2)

Now recall that as a consequence of Hamilton’s Harnack inequality, we have the pointwise estimates

\displaystyle 0 \leq |\nabla l|^2 + R \leq \frac{3l}{\tau} (3)

and

\displaystyle -\frac{2l}{\tau} \leq \partial_t l \leq \frac{l}{\tau} (4)

(see equations (37), (38) from Lecture 13). From these bounds and Gronwall’s inequality, one easily sees that we can extend (2) to say that

l(-\tau,x) = O_r(1) (5)

for any (-\tau,x) in the cylinder {}[-\tau_n/r, -r\tau_n] \times B_{g(-\tau')}(x_n,r\sqrt{\tau_n}) and any r \geq 1 and \tau_n/r \leq \tau' \leq r\tau_n. Applying (3) once more, together with the hypothesis of non-negative curvature more, we also obtain bounded normalised curvature on this cylinder:

|\hbox{Riem}(-\tau,x)|_g = O_r( \tau^{-1} ) (6).

If we thus introduce the rescaled flow t \mapsto (M_n, g_n(t), p_n) by setting M_n := M, p_n := x_n, and g_n(t) := t_n g(t t_n), we see that these flows obey hypothesis 1 of Theorem 2. Also, since the original \kappa-solutions are \kappa-noncollapsed, so are their rescalings, which (in conjunction with hypothesis 1) gives us hypothesis 2. We can thus invoke Theorem 2 and assume (after passing to a subsequence) that the rescaled flows converge geometrically to an ancient Ricci flow t \mapsto (M_\infty, g_\infty(t), p_\infty) on the time interval t \in (-\infty,0). From Exercise 3 we see that this limit is also \kappa-noncollapsed. Since the rescaled flows have non-negative curvature, the limit flow has non-negative curvature also. (Note however that we do not expect in general that (M_\infty,g_\infty(t)) has bounded curvature (for instance, if the original \kappa-solution was a round shrinking sphere terminating at the unit radius sphere, the limit object would be a round shrinking sphere terminating at a point). In particular we do not expect (M_\infty,g_\infty) to be a \kappa-solution.)

Let l_n: (-\infty,0) \times M_n \to {\Bbb R} be the rescaled length function, thus l_n(t,x) := l(t t_n, x). From (5) we see that l_n is uniformly bounded on compact subsets of (-\infty,0) \times M_\infty for n sufficiently large (where we identify compact subsets of M_\infty with subsets of M_n for n large enough). By the rescaled versions of (4) and (5) we also see that |\nabla l_n|_{g_\infty}, |\partial_t l_n| is also uniformly bounded on such compact sets for sufficiently large n; thus the l_n are uniformly Lipschitz on each compact set. Applying the Arzelá-Ascoli theorem and passing to a subsequence, we may thus assume that the l_n converge uniformly on compact sets to some limit l_\infty, which is then locally Lipschitz.

Remark 2. We do not attempt to interpret l_\infty as a reduced length function arising from some point at time t=0; indeed we expect the limiting flow to develop a singularity at this time. \diamond

We know that the reduced volume \int_M \tau^{-d/2} e^{-l}\ d\mu is non-increasing in \tau and ranges between 0 and (4\pi)^{d/2}, and so converges to a limit \tilde V(-\infty) between 0 and (4\pi)^{d/2}. This limit cannot equal (4\pi)^{d/2} since this would mean that the \kappa-solution is flat (by Theorem 1 from Lecture 14), which is absurd. The limit cannot be zero either, since the bounds (5) and the non-collapsing ensure a uniform lower bound on the reduced volume. By rescaling, we conclude that

\int_{M_n} \tau^{-d/2} e^{-l_n}\ d\mu_n \to \tilde V(-\infty) (7)

for each fixed \tau > 0.

Let us now argue informally, and then return to make the argument rigorous later. Formally taking limits in (7), we conclude that

\int_{M_\infty} \tau^{-d/2} e^{-l_\infty}\ d\mu_\infty = \tilde V(-\infty). (8)

On the other hand, from the proof of the monotonicity of reduced volume from Lecture 10 we have (formally, at least)

\displaystyle \partial_{\tau} l - \Delta l + |\nabla l|_g^2 - R + \frac{d}{2\tau} \geq 0 (9)

and hence by rescaling

\displaystyle \partial_{\tau} l_n - \Delta l_n + |\nabla l_n|_{g_n}^2 - R + \frac{d}{2\tau} \geq 0. (10)

Formally taking limits, we obtain

\displaystyle \partial_{\tau} l_\infty - \Delta l_\infty + |\nabla l_\infty|_{g_\infty}^2 - R_\infty + \frac{d}{2\tau} \geq 0. (11)

We can rewrite this as the assertion that \tau^{-d/2} e^{-l_\infty} is a subsolution of the backwards heat equation:

(\partial_\tau - \Delta_{g_\infty} - R_\infty) ( \tau^{-d/2} e^{-l_\infty} ) \leq 0. (12)

This (formally) implies that the left-hand side of (8) is non-increasing in \tau. On the other hand, this quantity is constant in \tau; and so (12) must be obeyed with equality, and thus

\displaystyle \partial_{\tau} l_\infty - \Delta l_\infty + |\nabla l_\infty|^2 - R_\infty + \frac{d}{2\tau} = 0. (13)

Also, recall from Lecture 10 that

\displaystyle \partial_\tau l = \frac{1}{2} R - \frac{1}{2} |\nabla l|_g^2 - \frac{1}{2\tau} l. (14)

Rescaling and taking limits, we formally conclude that the same is true for l_\infty;

\displaystyle \partial_\tau l_\infty = \frac{1}{2} R_\infty - \frac{1}{2} |\nabla l_\infty|_{g_\infty}^2 - \frac{1}{2\tau} l_\infty. (15)

From (14) and (15) we obtain that the Perelman {\mathcal W}-functional

\displaystyle {\mathcal W}(M_\infty,g_\infty(t),l_\infty,\tau) =

\displaystyle \int_{M _\infty}(\tau(|\nabla l_\infty|^2 + R_\infty) + l_\infty - d) (4\pi\tau)^{-d/2} e^{-l_\infty}\ d\mu_\infty (16)

vanishes (cf. the last section of Lecture 11). In particular, it is constant. On the other hand, by (13) and the monotonicity formula for this functional (see Exercise 9 of Lecture 8) we have

\displaystyle \frac{\partial}{\partial \tau} {\mathcal W}(M_\infty,g_\infty(t),l_\infty,\tau) =

\displaystyle - \int_M 2\tau |\hbox{Ric}_\infty + \hbox{Hess}(l_\infty)- \frac{1}{2\tau} g_\infty|_{g_\infty}^2 (4\pi \tau)^{-d/2} e^{-l_\infty}\ d\mu_\infty. (17)

Combining this with the vanishing of (16) we thus conclude that

\hbox{Ric}_\infty + \hbox{Hess}(l_\infty)- \frac{1}{2\tau} g_\infty = 0 (18)

and thus t \mapsto (M_\infty,g_\infty(t)) is a gradient shrinking soliton as desired.

– Making the argument rigorous I. Spatial localisation –

Now we turn to the (surprisingly delicate) task of justifying the steps from (7) to (18).

The first task is to deduce (8) from (7). From the dominated convergence theorem it is not difficult to show that

\int_{B_n(p_n,r)} \tau^{-d/2} e^{-l_n}\ d\mu_n \to \int_{B_\infty(p_\infty,r)} \tau^{-d/2} e^{-l_\infty}\ d\mu_\infty (19)

for any fixed \tau and r; the difficulty is to prevent the escape of mass of e^{-l_n} to spatial infinity. (Fatou’s lemma will tell us that the left-hand side of (8) is less than or equal to the right, but this is not enough for our application.)

In order to prevent such an escape, one needs a lower bound on l_n(-\tau,x) when d_{g_n(-\tau)}(x_n,x) is large. (Note that estimates such as (3), (4) only provide upper bounds on l_n(-\tau,x).) The problem is equivalent to that of upper bounding d_{g_n(-\tau)}(x_n,x) in terms of l_n(-\tau,x). To do this we need some control on quantities related to the distance function at extremely large distances. Remarkably, such bounds are possible. We begin with a lemma of Perelman (related to an earlier argument of Hamilton).

Lemma 1. Let (M,g) be a d-dimensional Riemannian manifold, let x, y \in M, and let r > 0. Suppose that \hbox{Ric} \leq K on the balls B(x,r) and B(y,r). Then for any minimising geodesic \gamma connecting x and y, we have \int_\gamma \hbox{Ric}(X,X) \leq O_d( K r + r^{-1} ), where X := \gamma' is the velocity field.

Proof. We may assume that d(x,y) \geq 2r, since the claim is trivial otherwise. We recall the second variation formula

\frac{d^2}{ds^2} E(\gamma) = \int_\gamma |\nabla_X Y|^2 - g(\hbox{Riem}(X,Y) X, Y) (20)

whenever one deforms a geodesic \gamma along a vector field Y (see equation (17) of Lecture 10). Since \gamma is minimising, the left-hand side of (20) is non-negative when Y vanishes at the endpoints of \gamma. Now let v be any unit vector at x, transported by parallel transport along \gamma. Setting Y(t) to equal tv/r when 0 \leq t \leq r, equal to v when r \leq t \leq d(x,y)-r, and equal to (d(x,y)-t)v/r when d(x,y)-r \leq t \leq d(x,y), we conclude that

\int_\gamma g(\hbox{Riem}(X,Y) X, Y) \leq O( r^{-1} ). (21)

Letting v vary over an orthonormal frame and summing, we soon obtain the claim. \Box

The above lemma, combined with the Ricci flow equation, gives an upper bound as to how rapidly the distance function can grow as one goes backwards in time.

Corollary 1. Let t \mapsto (M,g(t)) be a d-dimensional Ricci flow, let x,y \in M, let t be a time, and let r > 0. Suppose that \hbox{Ric} \leq K on B_{g(t)}(x,r) and on B_{g(t)}(y,r). Then \frac{d}{d\tau} d_{g(t)}(x,y) \leq O_d( K r + r^{-1} ) (in the sense of forward difference quotients).

Using this estimate, we can now obtain a bound on distance in terms of reduced length.

Proposition 1. Let t \mapsto (M,g(t)) be a d-dimensional \kappa-solution, let x_0, p, p' \in M, and \tau_1 > 0. Then

\displaystyle \frac{d_{g(-\tau_1)}(p,p')^2}{\tau_1} \leq O_d( 1 + l_{(0,x_0)}(-\tau_1,p) +l_{(0,x_0)}(-\tau_1,p') ). (22)

Proof. We use an argument of Ye. Write A for the expression inside the O_d() on the right-hand side, and let \gamma, \gamma': [0,\tau_1] \to M be minimising {\mathcal L}-geodesics from x_0 to p, p’ respectively. By the fundamental theorem of calculus, we have

d_{g(-\tau_1)}(p,p') = \int_0^{\tau_1} \frac{d}{d\tau} d_{g(-\tau)}( \gamma(-\tau), \gamma'(-\tau) )\ d\tau. (24)

Using (3) and the {\mathcal L}-Gauss lemma \nabla l = X we see that \gamma, \gamma' move at speed O(A^{1/2}/\tau^{1/2}), and that all curvature tensors are O( A / \tau ) in a O( \tau^{1/2}/A^{1/2} )-neighbourhood of either curve. Applying Corollary 1, the chain rule, and the Gauss lemma we conclude that

\frac{d}{d\tau} d_{g(-\tau)}( \gamma(-\tau), \gamma'(-\tau) ) \leq O_d(A^{1/2}/\tau^{1/2}); (25)

inserting this into (24) we obtain the claim. \Box

Combining this with (5) and rescaling we see that we have a bound of the form

l_n( -\tau, x ) \geq c d_{g_n(-\tau)}(p_n,x)^2 / \tau - O_d(1) (26)

for all x and some c = c_d > 0; taking limits we also obtain

l_\infty( -\tau, x ) \geq c d_{g_\infty(-\tau)}(p_\infty,x)^2/\tau - O_d(1). (27)

On the other hand, from the Bishop-Gromov inequality we know that balls of radius r in either (M_n, g_n(-\tau)) or (M_\infty, g_\infty(-\tau)) have volume O_d(r^d). These facts are enough to establish that the portion of (7) or (8) outside of the ball of radius r decays exponentially fast in r, uniformly in n, and this allows us to take limits in (19) as r \to \infty to deduce (8) from (7).

– Making the argument rigorous II. Parabolic inequality for l_\infty

The next major task in making the previous arguments rigorous is to justify the passage from (10) to (11). First of all, because of the {\mathcal L}-cut locus, (10) is only valid in the sense of distributions. We would like to take limits and conclude that (11) holds in the sense of distributions as well. There is no difficulty taking limits with the linear terms \partial_\tau l_n - \Delta l_n in (10), or in the zeroth order terms -R_n + \frac{d}{\tau}; the only problem is in justifying the limit from |\nabla l_n|_{g_n}^2 to |\nabla l_\infty|_{g_n}^2. We know that the l_n are uniformly locally Lipschitz, and converge locally uniformly to l_\infty; but this is unfortunately not enough to ensure that |\nabla l_n|_{g_n}^2 converges in the sense of distributions to |\nabla l_\infty|_{g_n}^2, due to possible high frequency oscillations in l_n. To give a toy counterexample, the one-dimensional functions l_n(x) := \frac{1}{n} \sin(nx) are uniformly Lipschitz and converge uniformly to zero, but |\frac{d}{dx} l_n|^2 = \cos^2(nx) converges in the distributional sense to \frac{1}{2} rather than zero.

Since \nabla l_n - \nabla l_\infty is bounded and converges distributionally to zero, it will be locally asymptotically orthogonal l_\infty. From this and Pythagoras’ theorem we obtain

\lim_{n \to \infty} |\nabla l_n|_{g_n}^2 = |\nabla l_\infty|_g^2 + \lim_{n \to \infty} |\nabla l_\infty - \nabla l_n|_{g_n}^2 (28)

in the sense of distributions, where we pass to a subsequence in order to make the limits on both sides exist. (Note that g_n converges locally uniformly to g and so there is no difficulty passing back and forth between those metrics.) The task is now to show that there is not enough oscillation to cause the second term on the right-hand side to be non-vanishing.

To do this, we observe that (10) provides an upper bound on \Delta_{g_n} l_n; indeed on any fixed compact set in (-\infty,0) \times M_\infty, we have \Delta_{g_n} l_n \leq O(1). This one-sided bound on the Laplacian is enough to rule out the oscillation problem. Indeed, as l_n converges locally uniformly to l_\infty, we see that

\displaystyle \limsup_{n \to \infty} \int_{M_\infty} \phi (l_\infty - l_n + \varepsilon_n) \Delta_{g_n} l_n\ d\mu_n \leq 0 (29)

for any non-negative bump function \phi and \varepsilon_n \to 0 chosen so that l_\infty - l_n + \varepsilon_n \geq 0 on the support of \phi. Integrating by parts and disposing of a lower order term, we conclude that

\displaystyle \limsup_{n \to \infty} \int_{M_\infty} \phi \langle \nabla (l_n-l_\infty), \nabla l_n \rangle_{g_n}\ d\mu_n \leq 0. (30)

On the other hand, since \nabla (l_n - l_\infty) is bounded converges weakly to zero, one has

\displaystyle \limsup_{n \to \infty} \int_M \phi \langle \nabla (l_n-l_\infty), \nabla l_\infty \rangle_{g_\infty}\ d\mu_\infty \to 0. (31)

One can easily replace g_\infty and \mu_\infty here by g_n and \mu_n. Combining (30) and (31) we conclude that the second term on the RHS of (28) is non-positive in the sense of distributions. But it is clearly also non-negative, and so it vanishes as required.

This gives (11); as a by-product of the argument we have also established the useful fact

\lim_{n \to \infty} |\nabla l_n|_{g_n}^2 = |\nabla l_\infty|_g^2 (32)

in the sense of distributions. Combining this with the growth bounds (26), (27) on l_n and $l_\infty$ from the previous section (which give exponential decay bounds on e^{-l_n}, e^{-l_\infty} and their first derivatives), it is not too difficult to then justify the remaining steps (12)-(18) of the argument rigorously; see Section 9.2 of Morgan-Tian for full details. (Note that once one reaches (13), one has a nonlinear heat equation for l_\infty, and it is not difficult to use the smoothing effects of the heat kernel to then show that the locally Lipschitz function l_\infty is in fact smooth.)

– The asymptotic gradient shrinking soliton is not flat –

Finally, we show that the asymptotic gradient shrinking soliton t \mapsto (M_\infty, g_\infty(t)) is non-trivial in the sense that its curvature is not identically zero at some time. For if the curvature did vanish everywhere at time t, then the equation (18) simplifies to \hbox{Hess}(l_\infty) = \frac{1}{2\tau} g_\infty. On the other hand, being flat, (M_\infty,g_\infty(t)) is the quotient of Euclidean space {\Bbb R}^d by some discrete subgroup. Lifting l_\infty up to this space, we thus see that f is quadratic, and more precisely is equal to |x|^2/4\tau plus an affine-linear function. Thus f has no periodicity whatsoever and so the above-mentioned discrete subgroup is trivial. If we now apply (8) we see that \tilde V(-\tau) = (4\pi)^{d/2}. But on the other hand, as the original \kappa-solution was not flat, its reduced volume was strictly less than (4\pi)^{d/2} by Theorem 1 from Lecture 14, a contradiction. Thus the asymptotic gradient soliton is not flat.

– Appendix: Shi’s derivative estimates –

The purpose of this appendix is to prove the following estimate of Shi.

Theorem 3. Suppose that t \mapsto (M,g(t)) is a complete d-dimensional Ricci flow on the time interval {}[0,T], and that on the cylinder {}[0,T] \times B_{g(0)}(x_0,r_0) one has the pointwise curvature bound |\hbox{Riem}|_g \leq K. Then on any slightly smaller cylinder {}(0,T] \times B_{g(0)}(x_0,(1-\varepsilon)r_0) one has the curvature bounds |\nabla^k \hbox{Riem}|_g = O( t^{-k/2} ) for any k \geq 0, where the implied constant depend on d, T, r_0, K, \varepsilon, k.

Proof. (Sketch) We induct on k. The case k = 0 is trivial, so suppose that k \geq 1 and that the claim has already been proven for all smaller values of k. We allow all implied constants in the O() notation to depend on d, T, r_0, K, \varepsilon, k. We refer to {}[0,T] \times B_{g(0)}(x_0,r_0) and {}(0,T] \times B_{g(0)}(x_0,(1-\varepsilon)r_0) as the “large cylinder” and “small cylinder” respectively.

We make some reductions. It is easy to see that we can take r_0 and T to be small.

Since |\dot g|_g = 2 |\hbox{Ric}| = O(1) on the cylinder, we see that the metric at later times of the large cylinder is comparable to the initial metric up to multiplicative constants. The curvature bound tells us that if r_0 is small, then we are inside the conjugacy radius; pulling back under the exponential map, we may thus assume that the exponential map from x_0 is injective on the large cylinder. Let r = d_{g(t)}(x_0,x) be the time-varying radial coordinate; observe that the annulus \{ (1-2\varepsilon/3)r_0 \leq r \leq (1-\varepsilon/3)r_0 \} will be contained between the large cylinder and small cylinder for T small enough.

Exercise 5. Show that if r_0 and T are small enough, then |\hbox{Hess}(r)|_g = O(1/r) on the large cylinder. \diamond

Let \eta = \eta(r) be a smooth non-negative radial cutoff to the large cylinder that equals 1 on the small cylinder. From the above exercise, the Gauss lemma, and the chain rule, we see that |\nabla \eta|_g, |\partial_t \eta|, |\hbox{Hess} \eta|_g, \Delta \eta = O(1).

Now we study the heat equation obeyed by the “energy densities” |\nabla^m \hbox{Riem}|_g^2 for various m.

Exercise 6. (Bochner-Weitzenböck type estimate) For any m \geq 0, show that

(\partial_t - \Delta) |\nabla^m \hbox{Riem}|_g^2 \leq O(\sum_{j=0}^m |\nabla^j \hbox{Riem}|_g |\nabla^{m-j} \hbox{Riem}|_g |\nabla^m \hbox{Riem}|_g)

- 2 |\nabla^{m+1} \hbox{Riem}|_g^2. (33)

(Hint: start with the equation \partial_t \hbox{Riem} = \Delta \hbox{Riem} + {\mathcal O}( g^{-1} \hbox{Riem}^2 ) and use the product rule and the definition of curvature repeatedly.) \diamond

From this exercise and the induction hypothesis we see that

(\partial_t - \Delta) [\eta^{2m+2} t^m |\nabla^m \hbox{Riem}|_g^2] \leq O(1) + O(\eta^{2m} t^{m-1} |\nabla^m \hbox{Riem}|_g^2)

- 2 \eta^{2m+2} t^m |\nabla^{m+1} \hbox{Riem}|_g^2 (34)

for all 0 \leq m \leq k, with the understanding that the second term on the right-hand side is absent when m=0. Telescoping this, we can thus find an expression

E := \sum_{m=0}^k C^{-m} \eta^{2m+2} t^m |\nabla^m \hbox{Riem}|_g^2 (35)

for some sufficiently large positive constant C, which obeys the heat equation (\partial_t - \Delta) E \leq O(1). Also, by hypothesis we have E=O(1) at time zero. Applying the maximum principle, we obtain the claim. \Box

Exercise 6. Suppose that in the hypotheses of Shi’s theorem that we also have |\nabla^j \hbox{Riem}|=O(1) for 0 \leq j \leq m on the large cylinder at time zero. Conclude that we have |\nabla^j \hbox{Riem}|=O( 1 + t^{-(j-m)/2} ) on the small cylinder for all j. \diamond

Exercise 7. Let (M,g) be a smooth compact manifold, and let u: [0,T] \times M \to {\Bbb R} be a bounded solution to the heat equation \partial_t u = \Delta u which obeys a pointwise bound |u(0)| \leq K at time zero. Establish the bounds |\nabla^k u|_g = O( t^{-k/2} ) on the spacetime {}[0,T] \times M and all k \geq 0, where the implied constant depends on (M,g), K, T, and k. \diamond

(Update, June 2: some corrections.)

(Update, Oct 18 2011: A recently discovered issue with the Hamilton compactness theorem in the case where the curvature bound is not uniform in r has been addressed.)