Orlicz space

In mathematical analysis, and especially in real, harmonic analysis and functional analysis, an Orlicz space is a type of function space which generalizes the L^p spaces. Like the L^p spaces, they are Banach spaces. The spaces are named for Władysław Orlicz, who was the first to define them in 1932.

Besides the L^p spaces, a variety of function spaces arising naturally in analysis are Orlicz spaces. One such space L log⁺ L, which arises in the study of Hardy–Littlewood maximal functions, consists of measurable functions f such that the integral

${\displaystyle \int _{\mathbb {R} ^{n}}|f(x)|\log ^{+}|f(x)|\,dx<\infty .}$

Here log⁺ is the positive part of the logarithm. Also included in the class of Orlicz spaces are many of the most important Sobolev spaces.

Terminology[]

These spaces are called Orlicz spaces by an overwhelming majority of mathematicians and by all monographies studying them, because Władysław Orlicz was the first who introduced them, in 1932.^[1] Some mathematicians, including Wojbor Woyczyński, Edwin Hewitt and Vladimir Mazya, include the name of Zygmunt Birnbaum as well, referring to his earlier joint work with Władysław Orlicz. However in the Birnbaum–Orlicz paper the Orlicz space is not introduced, neither explicitly nor implicitly, hence the name Orlicz space is preferred. By the same reasons this convention has been also openly criticized by another mathematician (and an expert in the history of Orlicz spaces), Lech Maligranda.^[2] Orlicz was confirmed as the person who introduced Orlicz spaces already by Stefan Banach in his 1932 monograph.^[3]

Formal definition[]

Suppose that μ is a σ-finite measure on a set X, and Φ : [0, ∞) → [0, ∞) is a , i.e., a convex function such that

${\displaystyle {\frac {\Phi (x)}{x}}\to \infty ,\quad {\text{as }}x\to \infty ,}$

${\displaystyle {\frac {\Phi (x)}{x}}\to 0,\quad {\text{as }}x\to 0.}$

Let ${\displaystyle L_{\Phi }^{\dagger }}$ be the set of measurable functions f : X → R such that the integral

${\displaystyle \int _{X}\Phi (|f|)\,d\mu }$

is finite, where, as usual, functions that agree almost everywhere are identified.

This might not be a vector space (i.e., it might fail to be closed under scalar multiplication). The vector space of functions spanned by ${\displaystyle L_{\Phi }^{\dagger }}$ is the Orlicz space, denoted ${\displaystyle L_{\Phi }}$.

To define a norm on ${\displaystyle L_{\Phi }}$, let Ψ be the Young complement of Φ; that is,

${\displaystyle \Psi (x)=\int _{0}^{x}(\Phi ')^{-1}(t)\,dt.}$

Note that Young's inequality for products holds:

${\displaystyle ab\leq \Phi (a)+\Psi (b).}$

The norm is then given by

${\displaystyle \|f\|_{\Phi }=\sup \left\{\|fg\|_{1}\mid \int \Psi \circ |g|\,d\mu \leq 1\right\}.}$

Furthermore, the space ${\displaystyle L_{\Phi }}$ is precisely the space of measurable functions for which this norm is finite.

An equivalent norm,^[4]: §3.3 called the Luxemburg norm, is defined on L_Φ by

${\displaystyle \|f\|'_{\Phi }=\inf \left\{k\in (0,\infty )\mid \int _{X}\Phi (|f|/k)\,d\mu \leq 1\right\},}$

and likewise L_Φ(μ) is the space of all measurable functions for which this norm is finite.

Example[]

Here is an example where ${\displaystyle L_{\Phi }^{\dagger }}$ is not a vector space and is strictly smaller than ${\displaystyle L_{\Phi }}$. Suppose that X is the open unit interval (0,1), Φ(x) = exp(x) – 1 – x, and f(x) = log(x). Then af is in the space ${\displaystyle L_{\Phi }}$ but is only in the set ${\displaystyle L_{\Phi }^{\dagger }}$ if |a| < 1.

Properties[]

• Orlicz spaces generalize L^p spaces (for ${\displaystyle 1<p<\infty }$) in the sense that if ${\displaystyle \varphi (t)=t^{p}}$, then ${\displaystyle \|u\|_{L^{\varphi }(X)}=\|u\|_{L^{p}(X)}}$, so ${\displaystyle L^{\varphi }(X)=L^{p}(X)}$.
• The Orlicz space ${\displaystyle L^{\varphi }(X)}$ is a Banach space — a complete normed vector space.

Relations to Sobolev spaces[]

Certain Sobolev spaces are embedded in Orlicz spaces: for ${\displaystyle n>1}$ and ${\displaystyle X\subseteq \mathbb {R} ^{n}}$ open and bounded with Lipschitz boundary ${\displaystyle \partial X}$, we have

${\displaystyle W_{0}^{1,n}(X)\subseteq L^{\varphi }(X)}$

for

${\displaystyle \varphi (t):=\exp \left(|t|^{n/(n-1)}\right)-1.}$

This is the analytical content of the Trudinger inequality: For ${\displaystyle X\subseteq \mathbb {R} ^{n}}$ open and bounded with Lipschitz boundary ${\displaystyle \partial X}$, consider the space ${\displaystyle W_{0}^{k,p}(X)}$ with ${\displaystyle kp=n}$ and ${\displaystyle p>1}$. Then there exist constants ${\displaystyle C_{1},C_{2}>0}$ such that

${\displaystyle \int _{X}\exp \left(\left({\frac {|u(x)|}{C_{1}\|\mathrm {D} ^{k}u\|_{L^{p}(X)}}}\right)^{n/(n-k)}\right)\,\mathrm {d} x\leq C_{2}|X|.}$

Orlicz norm of a random variable[]

Similarly, the Orlicz norm of a random variable characterizes it as follows:

${\displaystyle \|X\|_{\Psi }\triangleq \inf \left\{k\in (0,\infty )\mid \operatorname {E} [\Psi (|X|/k)]\leq 1\right\}.}$

This norm is homogeneous and is defined only when this set is non-empty.

When ${\displaystyle \Psi (x)=x^{p}}$, this coincides with the p-th moment of the random variable. Other special cases in the exponential family are taken with respect to the functions ${\displaystyle \Psi _{q}(x)=\exp(x^{q})-1}$ (for ${\displaystyle q\geq 1}$). A random variable with finite ${\displaystyle \Psi _{2}}$ norm is said to be "sub-Gaussian" and a random variable with finite ${\displaystyle \Psi _{1}}$ norm is said to be "sub-exponential". Indeed, the boundedness of the ${\displaystyle \Psi _{p}}$ norm characterizes the limiting behavior of the probability density function:

${\displaystyle \|X\|_{\Psi _{p}}=c\rightarrow \lim _{x\rightarrow \infty }f_{X}(x)\exp(|x/c|^{p})=0,}$

so that the tail of this probability density function asymptotically resembles, and is bounded above by ${\displaystyle \exp(-|x/c|^{p})}$.

The ${\displaystyle \Psi _{1}}$ norm may be easily computed from a strictly monotonic moment-generating function. For example, the moment-generating function of a chi-squared random variable X with K degrees of freedom is ${\displaystyle M_{X}(t)=(1-2t)^{-K/2}}$, so that the reciprocal of the ${\displaystyle \Psi _{1}}$ norm is related to the functional inverse of the moment-generating function:

${\displaystyle \|X\|_{\Psi _{1}}^{-1}=M_{X}^{-1}(2)=(1-4^{-1/K})/2.}$

References[]

Further reading[]

• Birnbaum, Z. W.; Orlicz, W. (1931), "Über die Verallgemeinerung des Begriffes der zueinander Konjugierten Potenzen", Studia Mathematica, 3: 1–67 PDF.
• Bund, Iracema (1975), "Birnbaum–Orlicz spaces of functions on groups", Pacific Mathematics Journal, 58 (2): 351–359.
• Hewitt, Edwin; Stromberg, Karl, Real and abstract analysis, Springer-Verlag.
• Krasnosel'skii, M.A.; Rutickii, Ya.B. (1961), Convex Functions and Orlicz Spaces, Groningen: P.Noordhoff Ltd.
• Zygmund, Antoni, "Chapter IV: Classes of functions and Fourier series", Trigonometric Series, Volume 1 (3rd ed.), Cambridge University Press.
• Ledoux, Michel; Talagrand, Michel, Probability in Banach Spaces, Springer-Verlag.

External links[]

• "Orlicz space", Encyclopedia of Mathematics, EMS Press, 2001 [1994]