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Lp Spaces, Lebesgue Spaces 📂Lebesgue Spaces

Lp Spaces, Lebesgue Spaces

Definition1 2 3

Let ΩRn\Omega \subset \mathbb{R}^{n} be an open set, and pp be a positive real number.

For all measurable functions ff defined on Ω\Omega, define set Lp(Ω)L^{p}(\Omega) as follows.

Lp(Ω):={f:Ωf(x)pdx<} L^{p}(\Omega) := \left\{ f : \int_{\Omega} \left| f(x) \right|^{p} dx < \infty \right\}

This is called the Lp space or Lebesgue space and is briefly denoted as LpL^{p}. Typically, textbooks on functional analysis describe it as above, while measure theory and real analysis textbooks describe it as follows.

Given a measure space (X,E,μ)(X, \mathcal{E}, \mu), for measurable functions ff defined on XX, define set Lp(X,E,μ)L^{p}(X, \mathcal{E},\mu) as follows.

Lp(X,E,μ):={f:fpdμ<} L^{p}(X, \mathcal{E}, \mu) := \left\{ f : \int \left| f \right|^{p} d \mu < \infty \right\}

Here, μ\mu is the measure. It is simply denoted as Lp(μ),Lp(X)L^{p}(\mu), L^{p}(X) and so on.

Properties

  1. LpL^{p} is a vector space.
  2. For 1p1 \le p \le \infty, LpL^{p} is a normed space.
  3. LpL^{p} is a complete space.
  4. For EXE\subset X, if 1pq1 \le p \le q \le \infty and μ(E)<    Lq(E)Lp(E)\mu (E) < \infty \implies L^{q} (E) \subset L^{p} (E)

Explanation

2. If p<1p \lt 1, then p\left\| \cdot \right\|_{p} does not satisfy the triangle inequality and is not a norm. However, if p=p = \infty, then LpL^{p} space becomes a normed space.

A complete normed vector space is specifically called a Banach space. Therefore, LpL^{p} space is a Banach space. LpL^{p} is especially important as a space where the Hölder inequality and the Minkowski inequality hold.

A vector space on which an inner product is defined is called an inner product space. A complete inner product space is specifically called a Hilbert space. For L2L^{2} space, an inner product can be defined as follows.

(f(x)2dx)12=(f(x)f(x)dx)12=f,f12 \left( \int |f(x)|^2 dx\right)^{\frac{1}{2}} = \left( \int f(x)\overline{f(x)}dx \right) ^{\frac{1}{2}} = \langle f,f \rangle ^{\frac{1}{2}}

Therefore, L2L^{2} space is a Hilbert space.

4. Let’s focus on the condition μ(E)<\mu (E) < \infty. If the integration range is not bounded, then L1(E)L^{1} (E) and L2(E)L^{2} (E) do not have any inclusion relation. For certain conditions that 1p<q<r1 \le p \lt q \lt r meets, uLpLr    uLq{u \in L^{p} \cap L^{r} \implies u \in L^{q}} can also be satisfied.

Proof

2.

For 1p<1\le p <\infty, define p\| \cdot \|_{p} as follows.

fp:=(Ωf(x)pdx)1/p,fLp(Ω) \left\| f \right\|_{p} := \left( \int_{\Omega} \left| f(x) \right|^{p} dx \right)^{1/p},\quad f\in L^{p}(\Omega)

Then p\| \cdot \|_{p} becomes the norm of LpL^{p} space. (When 0<p<10<p<1, it does not become a norm.) It is obvious that fp0\| f \|_{p} \ge 0, and it is also obvious that fp=0    f=0\| f \|_{p}=0 \iff f=0. It can also be shown that for cCc \in \mathbb{C}, cfp=cfp\| cf \|_{p} = \left| c \right| \left\| f \right\|_{p} holds as follows.

cfp=(Ωcf(x)pdx)1/p=(cpΩf(x)pdx)1/p=c(Ωf(x)pdx)1/p=cfp \begin{align*} \left\| cf \right\|_{p} =& \left( \int_{\Omega} \left| cf(x) \right|^{p} dx \right)^{1/p} \\ =& \left( \left| c \right|^{p} \int_{\Omega} \left| f(x) \right|^{p} dx \right)^{1/p} \\ =& \left| c \right| \left( \int_{\Omega} \left| f(x) \right|^{p} dx \right)^{1/p} \\ =& \left| c \right| \left\| f \right\|_{p} \end{align*}

For f,gLpf,g \in L^{p}, f+gpfp+gp\left\| f + g \right\|_{p} \le \| f \|_{p} + \| g \|_{p} also holds, and this is known as the Minkowski inequality.

3.

Strategy: Almost everything is solved by Fatou’s lemma.


Given a Cauchy sequence fnf_{n}, a subsequence fnkf_{n_{k}} that satisfies fnfnkp<12k\left\| f_{n} - f_{n_{k}} \right\|_{p} < \dfrac{1}{2^{k}} can be found. For all kNk \in \mathbb{N},

gk:=i=1kfni+1fnig:=limkgk=i=1fni+1fni \begin{align*} g_{k} :=& \sum_{i=1}^{k} \left| f_{n_{i+1}} - f_{n_{i}} \right| \\ g :=& \lim_{k \to \infty} g_{k} = \sum_{i=1}^{\infty} \left| f_{n_{i+1}} - f_{n_{i}} \right| \end{align*}

by defining it, the triangle inequality provides

gkpik12i<1 \left\| g_{k} \right\|_{p} \le \sum_{i}^{k} \dfrac{1}{2^{i}} < 1

Fatou’s Lemma

For a sequence of non-negative measurable functions {fn}\left\{ f_{n} \right\},

(lim infnfn)dμlim infnfndμ \int \left( \liminf_{n \to \infty} f_{n} \right) d \mu \le \liminf_{n \to \infty} \int f_{n} d \mu

According to Fatou’s lemma,

gpplimngkpdμlim infkgkpdμ1 \left\| g \right\|_{p}^{p} \le \int \lim_{n \to \infty} g_{k}^{p} d \mu \le \liminf_{k \to \infty} \int g_{k}^{p} d \mu \le 1

Since gg is finite almost everywhere,

fnk=fn1(x)+i=1k[fni(x)fni1(x)] f_{n_{k}} = f_{n_{1}}(x) + \sum_{i=1}^{ k } \left[ f_{n_{i}} (x) - f_{n_{i-1}} (x) \right]

converges almost everywhere. If we define f:=limkfnkf := \lim\limits_{k \to \infty} f_{n_{k}}, then by Fatou’s lemma,

ffmp=ffmpdμlim infkfnkfmpdμεp \left\| f - f_{m} \right\|_{p} = \int |f - f_{m}|^{p} d \mu \le \liminf_{k \to \infty} \int | f_{n_{k}} - f_{m}|^{p} d \mu \le \varepsilon^{p}

Therefore, ffmLpf - f_{m} \in L^{p} and f=fm+(ffm)Lpf = f_{m} + (f - f_{m} ) \in L^{p}. Since every Cauchy sequence in LpL^{p} converges to an element in LpL^{p}, LpL^{p} is a complete space.

4.

Strategy: Showing the inequality f(x)p1+f(x)q|f(x)|^{p} \le 1 + |f(x)|^{q} is sufficient; the rest follows from the properties of Lebesgue integration.


Let’s assume fLqf \in L^{q}. Then the following equation holds.

f(x)1    f(x)p11f(x)    f(x)pf(x)q \begin{align*} | f(x) | \le 1 \implies& |f(x) |^{p} \le 1 \\ 1 \le |f(x)| \implies& |f(x)|^{p} \le |f(x)|^{q} \end{align*}

Hence, whether f(x)| f(x) | is larger or smaller than 11, the following holds.

f(x)p1+f(x)q |f(x)|^{p} \le 1 + |f(x)|^{q}

Taking the Lebesgue integral Edμ\displaystyle \int_{E} d \mu results in

EfpdμE1dμ+Efqdμ=m(E)+Efqdμ< \int_{E} |f|^{p} d \mu \le \int_{E} 1 d \mu + \int_{E} |f|^{q} d \mu = m(E) + \int_{E} |f|^{q} d \mu < \infty

Since m(E)<m(E) < \infty and Efqdμ<\displaystyle \int_{E} |f|^{q} d \mu < \infty, the following holds.

Efpdμ< \int_{E} |f|^{p} d \mu < \infty

In other words, since fLq    fLpf \in L^{q} \implies f \in L^{p},

Lq(E)Lp(E) L^{q} (E) \subset L^{p} (E)

See Also


  1. Capinski, Measure, Integral and Probability (1999), p140 ↩︎

  2. Robert A. Adams and John J. F. Foutnier, Sobolev Space (2nd Edition, 2003), p23 ↩︎

  3. Gerald B. Folland, Real Analysis: Modern Techniques and Their Applications (2nd Edition, 1999), p181 ↩︎