利用者:Muraken/翻訳/Ricci flow

In differential geometry, the Ricci flow (named after Gregorio Ricci-Curbastro) is a process which deforms the metric of a Riemannian manifold in a manner formally analogous to the diffusion of heat.

Mathematical definition

Given a Riemannian manifold with metric tensor $g_{ab}$, we can compute the Ricci tensor $R_{ab}$, which collects averages of sectional curvatures into a kind of "trace" of the Riemann curvature tensor. If we consider the metric tensor (and the associated Ricci tensor) to be functions of a variable which is usually called "time" (but which may have nothing to do with any physical time), then the Ricci flow may be defined by the geometric evolution equation

$\partial _{t}g_{ij}=-2R_{ij}$

The normalized Ricci flow is the equation

$\partial _{t}g_{ij}=-2R_{ij}+{\frac {2}{n}}R_{avg}g_{ij}$

where $R_{avg}$ is the average (mean) of the scalar curvature (which is obtained from the Ricci tensor by taking the trace) and $n$ is the dimension of the manifold. This normalized equation preserves the volume of the metric.

Relationship to uniformization and geometrization

The Ricci flow was introduced by Richard Hamilton in 1981 in order to gain insight into the geometrization conjecture of William Thurston, which concerns the topological classification of three-dimensional smooth manifolds. Hamilton's idea was to define a kind of nonlinear diffusion equation which would tend to smooth out irregularities in the metric. Then, by placing an arbitrary metric g on a given smooth manifold M and evolving the metric by the Ricci flow, the metric should approach a particularly nice metric, which might constitute a canonical form for M. Suitable canonical forms had already been identified by Thurston; the possibilities, called Thurston model geometries, include the three-sphere S³, three-dimensional Euclidean space E³, three-dimensional hyperbolic space H³, which are homogeneous and isotropic, and five slightly more exotic Riemannian manifolds, which are homogeneous but not isotropic. (This list is closely related to, but not identical with, the well-known Bianchi classification of the three-dimensional real Lie algebras into nine isomorphism classes .) Hamilton's idea was that these special metrics should behave like fixed points of the Ricci flow, and that if, for a given manifold, globally only one Thurston geometry was admissible, this might even act like an attractor under the flow.

Hamilton succeeded in proving that any smooth closed three-manifold which admits a metric of positive Ricci curvature also admits a unique Thurston geometry, namely a spherical metric, which does indeed act like an attracting fixed point under the Ricci flow. This doesn't prove the full geometrization conjecture because the most difficult case turns out to concern manifolds with negative Ricci curvature and more specifically those with negative sectional curvature. (A strange and interesting fact is that all closed three-manifolds admit metrics with negative Ricci curvatures! This was proved by L. Zhiyong Gao and Shing-Tung Yau in 1986.) In this case, mathematicians expect that the Ricci flow should evolve an arbitrary negatively curved three-manifold into one which is locally isometric to H³. Indeed, a triumph of nineteenth century geometry was the proof of the uniformization theorem, the analogous topological classification of smooth two-manifolds, where Hamilton showed that the Ricci flow does indeed evolve a negative curved two-manifold into a two-dimensional multi-holed torus which is locally isometric to the hyperbolic plane. This topic is closely related to important topics in analysis, number theory, dynamical systems, mathematical physics, and even cosmology.

Note that the term "uniformization" correctly suggests a kind of smoothing away of irregularities in the geometry, while the term "geometrization" correctly suggests placing a geometry on a smooth manifold. Geometry is being used here in a precise manner akin to Klein's notion of geometry (see Geometrization conjecture for further details). In particular, the result of geometrization may be a geometry that is not isotropic. In most cases including the cases of constant curvature, the geometry is unique. An important theme in this area is the interplay between real and complex formulations. In particular, many discussions of uniformization speak of complex curves rather than real two-manifolds.

It is possible to construct a kind of superspace of n-dimensional Riemannian manifolds, and then the Ricci flow really does give a flow (in the intuitive sense of particles flowing along flowlines) in this superspace.

Relation to diffusion

To see why the evolution equation defining the Ricci flow is indeed a kind of nonlinear diffusion equation, we can consider the special case of (real) two-manifolds in more detail. Any metric tensor on a two-manifold can be written with respect to an exponential isothermal coordinate chart in the form

$ds^{2}=\exp(2\,p(x,y))\,\left(dx^{2}+dy^{2}\right)$

(These coordinates provide an example of a conformal coordinate chart, because angles, but not distances, are correctly represented.)

The easiest way to compute the Ricci tensor and Laplace-Beltrami operator for our Riemannian two-manifold is to use the differential forms method of Élie Cartan. Take the coframe field

$\sigma ^{1}=\exp(p)\,dx,\;\;\sigma ^{2}=\exp(p)\,dy$

so that metric tensor becomes

$\sigma ^{1}\otimes \sigma ^{1}+\sigma ^{2}\otimes \sigma ^{2}=\exp(2p)\,\left(dx\otimes dx+dy\otimes dy\right)$

Next, given an arbitrary smooth function $h(x,y)$, compute the exterior derivative

$dh=h_{x}dx+h_{y}dy=\exp(-p)h_{x}\,\sigma ^{1}+\exp(-p)h_{y}\,\sigma ^{2}$

Take the Hodge dual

$\star dh=-\exp(-p)h_{y}\,\sigma ^{1}+\exp(-p)h_{x}\,\sigma ^{2}=-h_{y}\,dx+h_{x}\,dy$

Take another exterior derivative

$d\star dh=-h_{yy}\,dy\wedge dx+h_{xx}\,dx\wedge dy=\left(h_{xx}+h_{yy}\right)\,dx\wedge dy$

(where we used the anti-commutative property of the exterior product). That is,

$d\star dh=\exp(-2p)\,\left(h_{xx}+h_{yy}\right)\,\sigma ^{1}\wedge \sigma ^{2}$

Taking another Hodge dual gives

$\Delta h=\star d\star dh=\exp(-2p)\,\left(h_{xx}+h_{yy}\right)$

which gives the desired expression for the Laplace/Beltrami operator

$\Delta =\exp(-2\,p(x,y))\left(D_{x}^{2}+D_{y}^{2}\right)$

To compute the curvature tensor, we take the exterior derivative of the covector fields making up our coframe:

$d\sigma ^{1}=p_{y}\exp(p)dy\wedge dx=-\left(p_{y}dx\right)\wedge \sigma ^{2}=-{\omega ^{1}}_{2}\wedge \sigma ^{2}$

$d\sigma ^{2}=p_{x}\exp(p)dx\wedge dy=-\left(p_{x}dy\right)\wedge \sigma ^{1}=-{\omega ^{2}}_{1}\wedge \sigma ^{1}$

From these expressions, we can read off the only independent connection one-form

${\omega ^{1}}_{2}=p_{y}dx-p_{x}dy$

Take another exterior derivative

$d{\omega ^{1}}_{2}=p_{yy}dy\wedge dx-p_{xx}dx\wedge dy=-\left(p_{xx}+p_{yy}\right)\,dx\wedge dy$

This gives the curvature two-form

${\Omega ^{1}}_{2}=-\exp(-2p)\left(p_{xx}+p_{yy}\right)\,\sigma ^{1}\wedge \sigma ^{2}=-\Delta p\,\sigma ^{1}\wedge \sigma ^{2}$

from which we can read off the only linearly independent component of the Riemann tensor using

${\Omega ^{1}}_{2}={R^{1}}_{212}\,\sigma ^{1}\wedge \sigma ^{2}$

Namely

${R^{1}}_{212}=-\Delta p$

from which the only nonzero components of the Ricci tensor are

$R_{22}=R_{11}=-\Delta p$

From this, we find components with respect to the coordinate cobasis, namely

$R_{xx}=R_{yy}=-\left(p_{xx}+p_{yy}\right)$

But the metric tensor is also diagonal, with

$g_{xx}=g_{yy}=\exp(2p)$

and after some elementary manipulation, we obtain an elegant expression for the Ricci flow:

${\frac {\partial \log p}{\partial t}}=\Delta \log p$

This is manifestly analogous to the best known of all diffusion equations, the heat equation

${\frac {\partial u}{\partial t}}=\Delta u$

where now $\Delta =D_{x}^{2}+D_{y}^{2}$ is the usual Laplacian on the Euclidean plane. The reader may object that the heat equation is of course a linear partial differential equation--- where is the promised nonlinearity in the p.d.e. defining the Ricci flow?

The answer is that nonlinearity enters because the Laplace-Beltrami operator depends upon the same function p which we used to define the metric. But notice that the flat Euclidean plane is given by taking $p(x,y)=0$. So if $p$ is small in magnitude, we can consider it to define small deviations from the geometry of a flat plane, and if we retain only first order terms in computing the exponential, the Ricci flow on our two-dimensional almost flat Riemannian manifold becomes the usual two dimensional heat equation. This computation suggests that, just as (according to the heat equation) an irregular temperature distribution in a hot plate tends to become more homogeneous over time, so too (according to the Ricci flow) an almost flat Riemannian manifold will tend to flatten out the same way that heat can be carried off "to infinity" in an infinite flat plate. But if our hot plate is finite in size, and has no boundary where heat can be carried off, we can expect to homogenize the temperature, but clearly we cannot expect to reduce it to zero. In the same way, we expect that the Ricci flow, applied to a distorted round sphere, will tend to round out the geometry over time, but not to turn it into a flat Euclidean geometry.

Recent developments

The Ricci flow has been intensively studied since 1981. Some recent work has focused on the question of precisely how higher dimensional Riemannian manifolds evolve under the Ricci flow, and in particular, what types of parametric singularities may form. For instance, a certain class of solutions to the Ricci flow demonstrates that neckpinch singularities will form on an evolving n-dimensional metric Riemannian manifold having a certain topological property (positive Euler characteristic), as the flow approaches some characteristic time $t_{0}$. In certain cases such neckpinches will produce manifolds called Ricci solitons.

Many variants of the Ricci flow have also been studied:

• Various curvature flows defined using either an extrinsic curvature, which describes how a curve or surface is embedded in a higher dimensional flat space, or an intrinsic curvature, which describes the internal geometry of some Riemannian manifold,
• Various flows which extremalize some quantity mathematically analogous to an energy or entropy,
• Various flows controlled by a p.d.e. which is a higher order analog of a nonlinear diffusion equation.

Some of the most interesting variants are examples of all of these possibilities. In particular, the Calabi flow, which, like the Ricci flow, is an intrinsic curvature flow. This flow tends to smooth out deviations from roundness in a manner formally analogous to the way that the two-dimensional vibration equation damps and propagates away transverse mechanical vibrations in a thin plate, and it extremalizes a certain intrinsic curvature functional. The Calabi flow is important in the study of Calabi-Yau manifolds and also in the study of Robinson-Trautman spacetimes in general relativity. An intriguing observation is that the underlying Calabi equation appears to be completely integrable, which would give a direct link with the theory of solitons.

Curvature flows may or may not preserve volume. The Calabi flow does; the Ricci flow does not, so to be more careful in applying the Ricci flow to uniformization we'd need to normalize the Ricci flow to obtain a flow which preserves volume. If we fail to do this, the problem is that (for example) instead of evolving a given three-dimensional manifold into one Thurston's canonical forms, we might just shrink its size.

See also

• Ricci curvature
• uniformization theorem
• geometrization conjecture
• Fuchsian group
• automorphic function
• Falting's theorem
• calculus of variations
• Kähler manifold
• Yamabe flow

References

• Bakas, I.. “The algebraic structure of geometric flows in two dimensions”. arXiv eprint server. July 28閲覧。

• Chow, Bennet and Knopf, Dan (2004). The Ricci Flow: an introduction. American Mathematical Society. ISBN 0821835157 .

• Weeks, Jeffrey R. (1985). The Shape of Space: how to visualize surfaces and three-dimensional manifolds. New York: Marcel Dekker. ISBN 0-824-77437-X . A superb popular book which aims to explain the background for the Thurston classification programme.