Difference between revisions of "Lojasiewicz inequality"
m (→Commennts) |
m (→Applications) |
||
Line 61: | Line 61: | ||
'''Lemma 4''' | '''Lemma 4''' | ||
− | Assume is open, f: U \to \mathbb R is a C^1 function and x:[0, \infty[\to \mathbb R^n is a solution of \eqref{e:gradient_flow}. Assume the existence of a sequence t_n\to \infty such that x (t_n) converges to a critical point \bar{x} of f which satisfies \eqref{e:Loj2} for some $\ | + | Assume U\subset \mathbb R^n is open, f: U \to \mathbb R is a C^1 function and x:[0, \infty[\to \mathbb R^n is a solution of \eqref{e:gradient_flow}. Assume the existence of a sequence t_n\to \infty such that x (t_n) converges to a critical point \bar{x} of f which satisfies \eqref{e:Loj2} for some $\theta \in ]0,1[ in some neighborhood V$. Then |
\[ | \[ | ||
\lim_{t\to \infty} x(t) = \bar{x}\, . | \lim_{t\to \infty} x(t) = \bar{x}\, . |
Revision as of 11:12, 13 December 2013
2020 Mathematics Subject Classification: Primary: 14P05 [MSN][ZBL]
An inequality on real analytic functions proved by S. Lojasiewicz in [Lo]. One form of the inequality states the following.
Theorem 1 Consider an open set U\subset \mathbb R^n and an analytic function f:\mathbb U \to \mathbb R. Then for every open set V\subset\subset U there is a positive \alpha>0 such that \begin{equation}\label{e:Loj1} {\rm dist}\, (x, Z_f)^\alpha \leq f(x) \qquad \qquad \forall x \in V. \end{equation}
A different form of the inequality is often used in analysis and is also called Lojasiewicz inequality (sometimes Lojasiewicz gradient inequality)
Theorem 2 Let U and f be as above. For every critical point x\in U of f there is a neighborhood V of x, an exponent \theta\in [\frac{1}{2},1[ and a constant C such that \begin{equation}\label{e:Loj2} |f(x)-f(y)|^\theta \leq C |\nabla f (y)| \qquad \qquad \forall y\in V\, . \end{equation}
Commennts
Observe that
- If we know \eqref{e:Loj2}, we can remove the constant C by restricting the inequality to a smaller neighborhood W of V and substituing \theta with a larger exponent. However, the inequality is usually stated as above since in several applications it is convenient to have the smallest possible exponent \theta.
- For n=1 it is very easy to prove both \eqref{e:Loj1} and \eqref{e:Loj2} using the power expansion of f. More precisely, if the function is not constant, then there is a smallest N\geq 1 such that f^{(N)} (x)\neq 0. We can then write
f(y) - f(x) = \sum_{k\geq N} \frac{f^{(k)} (x)}{k!} (y-x)^k for y in a neighborhood of x. Choosing r sufficiently small we easily conclude |f(y) - f(x)| \geq \frac{1}{2}\left|\frac{f^{(N)} (x)}{N!}\right| |y-x|^N \qquad \forall y\in ]x-r, x+r[\, . Next, assuming that f' (x) = 0 (i.e. N>1) we also conclude, for r sufficiently small |f'(y)|\geq \frac{1}{2} \left|\frac{f^{(N)} (x)}{(N-1)!}\right| |y-x|^{N-1} and we conclude \eqref{e:Loj2} with \theta = \frac{N-1}{N} The inequalities are however rather difficult to prove when n>1.
- The classical example of a C^\infty function which is not real analytic shows that the analyticity assumption is necessary. Indeed consider
f(x) =\left\{ \begin{array}{ll} e^{-\frac{1}{|x|}} \qquad&\mbox{for } x\neq 0\\ 0 &\mbox{for } x=0 \end{array}\right. It can be easily checked that f\in C^\infty and that Z_f = \{0\}. It is also obvious that \eqref{e:Loj1} fails in any neighborhood of 0 and that Theorem 2 does not hold at x=0.
Remark 3 Further important remarks:
- By the argument above we draw the important conclusion that, if \nabla f (x) =0, then the exponent \theta in \eqref{e:Loj2} is necessarily larger than \frac{1}{2}.
- The inequality \eqref{e:Loj2} can be shown to hold with \theta = \frac{1}{2} when D^2 f (x) is invertible, i.e. x is a non-degenerate critical point: the inequality is indeed a simple consequence of the Morse lemma and the analyticity assumption is superfluous (f\in C^2 is sufficient to apply the Morse lemma).
Applications
The Lojasiewicz inequality has found rather striking applications in the theory of ordinary and partial differential equations, in particular to gradient flows. In a finite-dimensional context, a gradient flow is sometimes called gradient dynamical system and consists of a system of ordinary differential equations of the form \begin{equation}\label{e:gradient_flow} \dot{x} (t) = - \nabla f (x(t))\, . \end{equation} The following lemma of Lojasiewicz (see [Lo2]) then holds
Lemma 4 Assume U\subset \mathbb R^n is open, f: U \to \mathbb R is a C^1 function and x:[0, \infty[\to \mathbb R^n is a solution of \eqref{e:gradient_flow}. Assume the existence of a sequence t_n\to \infty such that x (t_n) converges to a critical point \bar{x} of f which satisfies \eqref{e:Loj2} for some \theta \in ]0,1[ in some neighborhood V. Then \lim_{t\to \infty} x(t) = \bar{x}\, .
Thus, from the Theorem 2 we conclude the following important corollary
Corollary 5 Assume f:\mathbb R^n \to \mathbb R is real analytic and let x:[0,\infty[\to \mathbb R^n be a solution of \eqref{e:gradient_flow}. Then, either \lim_{t\to\infty} |x(t)| = \infty or there exists \bar{x} critical point of f such that \lim_{t\to\infty} x(t) = \bar{x}\, .
It was realized in a pioneering work of L. Simon (see [Si]) that under appropriate ellipticity assumptions the Lojasiewicz inequality can be extended to an infinite-dimensional setting and used to study
- The asymptotic behavior of solutions to parabolic equations
- The asymptotic behavior of solutions to geometric variational problems near an isolated singular point.
For this reason, suitable infinite-dimensional versions of \eqref{e:Loj2} (which can be reduced to Theorem 2 using a suitable Lyapunov-Schmidt reduction, see [Si2]) are often called Lojasiewicz-Simon inequalities.
Remark 6 Corollary 5 can be shown to fail under the assumption f\in C^\infty. The exponent \theta in \eqref{e:Loj2} is related to the rate of convergence of x(t) to \bar{x} in Lemma 4. In particular, if \theta = \frac{1}{2}, then it can be shown that |x(t) - \bar{x}|\leq e^{\bar{C} t}\, . If \theta > \frac{1}{2}, then it can be shown that |x(t)-\bar{x}| \leq \frac{C}{t^\alpha}\, , where the epxonent \alpha can be explicitely computed from \theta. Cf. [Si2].
References
[Lo] | S. Łojasiewicz, "Ensembles semi-analytiques", preprint IHES, 1965 |
[Lo2] | S. Łojasiewicz, "Sur les trajectoires du gradient d’une fonction analytique", Seminari di Geometria, Bologna (1982/83), Universita' degli Studi di Bologna, Bologna (1984), pp. 115–117 |
[Lo] | S. Łojasiewicz, "Une propriété topologique des sous ensembles analytiques réels", Colloques internationaux du C.N.R.S 117. Les Équations aux Dérivées Partielles, (1963) 87-89 |
[Si] | L. Simon, "Asymptotics for a class of non-linear evolution equations, with applications to geometric problems", Ann. Math. 118 (1983), pp. 525-571 |
[Si1] | L. Simon, "Theorems on regularity and singularity of energy minimizing maps" Lectures in Mathematics. ETH Zürich. Birkhäuser, Basel (1996). |
Lojasiewicz inequality. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Lojasiewicz_inequality&oldid=31064