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L infinity space 📂Lebesgue Spaces

L infinity space

Definitions1

  • Let ΩRn\Omega \subset \mathbb{R}^{n} be called an open set. For a measurable function uu on Ω\Omega, if there exists a constant KK that satisfies the following condition for uu, then uu is said to be essentially bounded on Ω\Omega.

    u(x)K a.e. on Ω \left| u(x) \right| \le K \text{ a.e. on } \Omega

    Here, a.e.\text{a.e.} means almost everywhere.

  • The supremum of such KK is called the essential supremum of u\left| u \right| and is denoted as follows.

    ess supxΩu(x):=inf{K:u(x)K a.e. on Ω} \underset{x\in \Omega}{\text{ess sup}}\left| u(x) \right| := \inf \left\{ K : \left| u(x) \right| \le K \text{ a.e. on } \Omega \right\}

  • The set of all functions uu that are essentially bounded on Ω\Omega is defined as L(Ω)L^{\infty}(\Omega).

    L(Ω):={u:u is essentially bounded on Ω} L^{\infty}(\Omega) := \left\{ u : u \text{ is essentially bounded on } \Omega \right\}

Explanation

LL^{\infty} space is read as L infinity space.

‘Saying almost everywhere bounded’ essentially means ‘frankly bounded’, ‘putting it plainly bounded’, so it makes sense to say ’essentially bounded’. Especially in the space LpL^{p}, since it’s about integration, if it’s bounded almost everywhere, it’s essentially bounded literally.

Meanwhile, the LL^{\infty} space becomes a norm space, and the defined essential supremum can be used as is.

u=ess supxΩu(x),uL(Ω) \left\| u \right\|_{\infty} = \underset{x\in \Omega}{\text{ess sup}}\left| u(x) \right|, \quad u \in L^{\infty}(\Omega)

It is not difficult to verify this actually being a norm. The important fact is, as you can guess from the notation, that this really is the same as the limit of up\left\| u \right\|_{p}. If for p<p \lt \infty, uLLpu \in L^{\infty} \cap L^{p} then

u=limpup \left\| u \right\|_{\infty} = \lim \limits_{p \to \infty} \left\| u \right\|_{p}

Moreover, the Hölder’s inequality and its corollaries that were valid for 1<p,p<1 \lt p, p^{\prime} \lt \infty are extended to hold for p=1,p=p = 1, p^{\prime} = \infty and p=,p=1p = \infty, p^{\prime} = 1 respectively.

Hölder’s Inequality

Consider two constants 1p,1p1 \le p \le \infty, 1 \le p^{\prime} \le \infty satisfying the following expression.

1p+1p=1(or p=pp1) \dfrac{1}{p}+\dfrac{1}{p^{\prime}} = 1 \left(\text{or } p^{\prime} = \frac{p}{p-1} \right)

If uLp(Ω)u \in L^p(\Omega), vLp(Ω)v\in L^{p^{\prime}}(\Omega) then uvL1(Ω)uv \in L^1(\Omega) and the inequality below holds.

uv1=Ωu(x)v(x)dxupvp \| uv \|_{1} = \int_{\Omega} |u(x)v(x)| dx \le \| u \|_{p} \| v \|_{p^{\prime}}


  1. Robert A. Adams and John J. F. Foutnier, Sobolev Space (2nd Edition, 2003), p27 ↩︎