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mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, the Poincaré inequality is a result in the theory of Sobolev spaces, named after the French
mathematician A mathematician is someone who uses an extensive knowledge of mathematics in their work, typically to solve mathematical problems. Mathematicians are concerned with numbers, data, quantity, mathematical structure, structure, space, Mathematica ...
Henri Poincaré Jules Henri Poincaré (, ; ; 29 April 185417 July 1912) was a French mathematician, Theoretical physics, theoretical physicist, engineer, and philosophy of science, philosopher of science. He is often described as a polymath, and in mathemati ...
. The inequality allows one to obtain bounds on a function using bounds on its derivatives and the geometry of its domain of definition. Such bounds are of great importance in the modern, direct methods of the calculus of variations. A very closely related result is Friedrichs' inequality.


Statement


The classical Poincaré inequality

Let ''p'', so that 1 ≤ ''p'' < ∞ and Ω a subset bounded at least in one direction. Then there exists a constant ''C'', depending only on Ω and ''p'', so that, for every function ''u'' of the Sobolev space ''W''01,''p''(Ω) of zero- trace (a.k.a. zero on the boundary) functions, :\, u \, _ \leq C \, \nabla u \, _.


Poincaré–Wirtinger inequality

Assume that 1 ≤ ''p'' ≤ ∞ and that Ω is a bounded connected
open subset In mathematics, an open set is a generalization of an open interval in the real line. In a metric space (a set with a distance defined between every two points), an open set is a set that, with every point in it, contains all points of the met ...
of the ''n''-
dimension In physics and mathematics, the dimension of a mathematical space (or object) is informally defined as the minimum number of coordinates needed to specify any point within it. Thus, a line has a dimension of one (1D) because only one coo ...
al
Euclidean space Euclidean space is the fundamental space of geometry, intended to represent physical space. Originally, in Euclid's ''Elements'', it was the three-dimensional space of Euclidean geometry, but in modern mathematics there are ''Euclidean spaces ...
\mathbb^ with a Lipschitz boundary (i.e., Ω is a Lipschitz domain). Then there exists a constant ''C'', depending only on Ω and ''p'', such that for every function ''u'' in the Sobolev space , \, u - u_ \, _ \leq C \, \nabla u \, _, where u_ = \frac \int_ u(y) \, \mathrm y is the average value of ''u'' over Ω, with , Ω, standing for the
Lebesgue measure In measure theory, a branch of mathematics, the Lebesgue measure, named after French mathematician Henri Lebesgue, is the standard way of assigning a measure to subsets of higher dimensional Euclidean '-spaces. For lower dimensions or , it c ...
of the domain Ω. When Ω is a ball, the above inequality is called a -Poincaré inequality; for more general domains Ω, the above is more familiarly known as a Sobolev inequality. The necessity to subtract the average value can be seen by considering constant functions for which the derivative is zero while, without subtracting the average, we can have the integral of the function as large as we wish. There are other conditions instead of subtracting the average that we can require in order to deal with this issue with constant functions, for example, requiring trace zero, or subtracting the average over some proper subset of the domain. The constant ''C'' in the Poincaré inequality may be different from condition to condition. Also note that the issue is not just the constant functions, because it is the same as saying that adding a constant value to a function can increase its integral while the integral of its derivative remains the same. So, simply excluding the constant functions will not solve the issue.


Generalizations

In the context of metric measure spaces, the definition of a Poincaré inequality is slightly different. One definition is: a metric measure space supports a (q,p)-Poincare inequality for some 1\le q,p<\infty if there are constants ''C'' and so that for each ball B in the space, \mu(B)^ \left \, u-u_B \right \, _\le C \operatorname(B) \mu(B)^ \, \nabla u\, _. Here we have an enlarged ball in the right hand side. In the context of metric measure spaces, \, \nabla u\, is the minimal p-weak upper gradient of u in the sense of Heinonen and Koskela. Whether a space supports a Poincaré inequality has turned out to have deep connections to the geometry and analysis of the space. For example, Cheeger has shown that a doubling space satisfying a Poincaré inequality admits a notion of differentiation. Such spaces include sub-Riemannian manifolds and Laakso spaces. There exist other generalizations of the Poincaré inequality to other Sobolev spaces. For example, consider the Sobolev space ''H''1/2(T2), i.e. the space of functions ''u'' in the ''L''2 space of the unit
torus In geometry, a torus (: tori or toruses) is a surface of revolution generated by revolving a circle in three-dimensional space one full revolution about an axis that is coplanarity, coplanar with the circle. The main types of toruses inclu ...
T2 with
Fourier transform In mathematics, the Fourier transform (FT) is an integral transform that takes a function as input then outputs another function that describes the extent to which various frequencies are present in the original function. The output of the tr ...
''û'' satisfying ^2 = \sum_ , k , \left , \hat (k) \right , ^2 < + \infty. In this context, the Poincaré inequality says: there exists a constant ''C'' such that, for every with ''u'' identically zero on an open set , \int_ , u(x) , ^2 \, \mathrm x \leq C \left( 1 + \frac1 \right) u ^2, where denotes the harmonic capacity of when thought of as a subset of \mathbb^. Yet another generalization involves weighted Poincaré inequalities where the Lebesgue measure is replaced by a weighted version.


The Poincaré constant

The optimal constant ''C'' in the Poincaré inequality is sometimes known as the Poincaré constant for the domain Ω. Determining the Poincaré constant is, in general, a very hard task that depends upon the value of ''p'' and the geometry of the domain Ω. Certain special cases are tractable, however. For example, if Ω is a bounded,
convex Convex or convexity may refer to: Science and technology * Convex lens, in optics Mathematics * Convex set, containing the whole line segment that joins points ** Convex polygon, a polygon which encloses a convex set of points ** Convex polytop ...
, Lipschitz domain with
diameter In geometry, a diameter of a circle is any straight line segment that passes through the centre of the circle and whose endpoints lie on the circle. It can also be defined as the longest Chord (geometry), chord of the circle. Both definitions a ...
''d'', then the Poincaré constant is at most ''d''/2 for , d/\pi for , and this is the best possible estimate on the Poincaré constant in terms of the diameter alone. For smooth functions, this can be understood as an application of the isoperimetric inequality to the function's level sets. In one dimension, this is Wirtinger's inequality for functions. However, in some special cases the constant ''C'' can be determined concretely. For example, for ''p'' = 2, it is well known that over the domain of unit isosceles right triangle, ''C'' = 1/π ( < ''d''/π where d=\sqrt). Furthermore, for a smooth, bounded domain , since the Rayleigh quotient for the
Laplace operator In mathematics, the Laplace operator or Laplacian is a differential operator given by the divergence of the gradient of a Scalar field, scalar function on Euclidean space. It is usually denoted by the symbols \nabla\cdot\nabla, \nabla^2 (where \ ...
in the space W^_0(\Omega) is minimized by the eigenfunction corresponding to the minimal eigenvalue of the (negative) Laplacian, it is a simple consequence that, for any u\in W^_0(\Omega), \, u\, _^2\leq \lambda_1^ \left \, \nabla u\right \, _^2 and furthermore, that the constant λ1 is optimal.


Poincaré inequality on metric-measure spaces

Since the 90s there have been several fruitful ways to make sense of Sobolev functions on general metric measure spaces (metric spaces equipped with a measure that is often compatible with the metric in certain senses). For example, the approach based on "upper gradients" leads to Newtonian-Sobolev space of functions. Thus, it makes sense to say that a space "supports a Poincare inequality". It turns out that whether a space supports any Poincare inequality and if so, the critical exponent for which it does, is tied closely to the geometry of the space. For example, a space that supports a Poincare inequality must be path connected. Indeed, between any pair of points there must exist a rectifiable path with length comparable to the distance of the points. Much deeper connections have been found, e.g. through the notion of modulus of path families. A good and rather recent reference is the monograph "Sobolev Spaces on Metric Measure Spaces, an approach based on upper gradients" written by Heinonen et al.


Sobolev–Slobodeckij spaces

Given 0 < s < 1 and p \in , \infty), the Sobolev–Slobodeckij space W^(\Omega) is defined as the set of all functions u such that u \in L^p(\Omega) and the seminorm is finite, where is defined by: : = \left( \int_\Omega \int_\Omega \frac \, dx \, dy \right)^ The Poincaré inequality in this context can be generalized as follows: : \, u - u_\Omega\, _ \leq C where u_\Omega is the average of u over \Omega and C is a constant dependent on s, p, and \Omega. This inequality holds for every bounded \Omega.


Proof of the Poincaré inequality

The proof follows that of Irene Drelichman and Ricardo G. Durán. Let f_\Omega = \frac \int_\Omega f(x) \, dx. By applying Jensen's inequality, we obtain: : \, f - f_\Omega\, ^p_ = \left\, \frac \int_\Omega (f(y) - f(x)) \, dx \right\, ^p_ = \int_\Omega \left, \frac \int_\Omega f(y) - f(x) \, dy \^p \, dx : \leq \frac \int_\Omega \int_\Omega , f(y) - f(x), ^p \, dy \, dx By exploiting the boundedness of \Omega and further estimates: : \frac \int_\Omega \int_\Omega , f(y) - f(x), ^p \, dy \, dx : \leq \frac \int_\Omega \int_\Omega \frac \, dy \, dx It follows that the constant C is given as C = \frac; however, the reference with Theorem 1 indicates that this is not the optimal constant.


Poincaré on balls

We can derive a growth constant for Balls in a manner similar to previous cases. The relationship is given by the following inequality: : \, u - u_\Omega\, _ \leq C R^s The proof proceeds similarly to the classical one, by using the scaling u_R(x) = u(Rx). Then, by using a form of chain rule for the fractional derivative, we get R^s as a result.


See also

* Friedrichs' inequality * Korn's inequality * Spectral gap


References

* * Leoni, Giovanni (2009),
A First Course in Sobolev Spaces
', Graduate Studies in Mathematics, American Mathematical Society, pp. xvi+607 , ,
MAA
{{DEFAULTSORT:Poincare inequality Theorems in mathematical analysis Inequalities (mathematics) Sobolev spaces Inequality