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Proof of Clarkson's Inequalities 📂Lebesgue Spaces

Proof of Clarkson's Inequalities

Theorem1

Let’s say that ΩRn\Omega \subset \mathbb{R}^{n} is an open set.

Let’s say that u,vLp(Ω)u,v\in {L}^{p}(\Omega). Also, let’s say it satisfies 1p+1p=1\frac{1}{p}+\frac{1}{p^{\prime}}=1. If 2p<2 \le p \lt \infty, then the following two inequalities hold.

u+v2pp+uv2pp12upp+12vpp \begin{equation} \left\| \frac{u+v}{2}\right\|_{p}^{p}+ \left\| \frac{u-v}{2} \right\|_{p}^{p} \le \frac{1}{2}\left\| u \right\|_{p}^{p} + \frac{1}{2}\left\| v \right\|_{p}^{p} \end{equation}

u+v2pp+uv2pp(12upp+12vpp)p1 \begin{equation} \left\| \frac{u+v}{2}\right\|_{p}^{p^{\prime}}+ \left\| \frac{u-v}{2} \right\|_{p}^{p^{\prime}} \ge \left( \frac{1}{2}\left\| u \right\|_{p}^{p} + \frac{1}{2}\left\| v \right\|_{p}^{p}\right)^{p^{\prime}-1} \end{equation}

If 1<p21 \lt p \le 2, then the following two inequalities hold.

u+v2pp+uv2pp12upp+12vpp \begin{equation} \left\| \frac{u+v}{2}\right\|_{p}^{p}+ \left\| \frac{u-v}{2} \right\|_{p}^{p} \ge \frac{1}{2}\left\| u \right\|_{p}^{p} + \frac{1}{2}\left\| v \right\|_{p}^{p} \end{equation}

u+v2pp+uv2pp(12upp+12vpp)p1 \begin{equation} \left\| \frac{u+v}{2}\right\|_{p}^{p^{\prime}}+ \left\| \frac{u-v}{2} \right\|_{p}^{p^{\prime}} \le \left( \frac{1}{2}\left\| u \right\|_{p}^{p} + \frac{1}{2}\left\| v \right\|_{p}^{p}\right)^{p^{\prime}-1} \end{equation}

Explanation

This is called Clarkson’s inequalities.

(1)(1) and (3)(3), (2)(2) and (4)(4) have opposite sign directions in the same equation.

As with many inequalities, rather than having significant meaning by themselves, they are handy in proving other important theorems. As there are many auxiliary theorems and formulas needed for the proof, we will organize them in advance. Since 1p+1p=1\frac{1}{p}+\frac{1}{p^{\prime}}=1, we can obtain the following formulas when organized well.

(a) p=p(p1),(b) p=p(p1),(c) pp=p1(d) pp=p1,(e)1p1=p1(5) \begin{array}{c} \displaystyle (a)\ p^{\prime}=p(p^{\prime}-1),\quad (b)\ p=p^{\prime}(p-1),\quad (c)\ \frac{p}{p^{\prime}}=p-1 \\ \displaystyle (d)\ \frac{p^{\prime}}{p}=p^{\prime}-1,\quad (e)\frac{1}{p-1}=p^{\prime}-1\end{array} \quad \cdots (5)

Also, using the definition of a norm, it is easy to see that the following formula holds for uLpu\in {L}^{p}.

upp= upp1(6) \| u \|_{p}^{p^{\prime}}=|\ |u|^{p^{\prime}} |_{p-1}\quad \cdots (6)


Auxiliary Theorem

Let’s say z,wCz,w \in \mathbb{C} and 1p+1p=1\frac{1}{p}+\frac{1}{p^{\prime}}=1. If 1<p21<p \le 2, then the following inequality holds.

z+w2p+zw2p(12zp+12wp)1p1(7) \left| \frac{z+w}{2} \right|^{p^{\prime}} + \left| \frac{z-w}{2} \right|^{p^{\prime}} \le \left( \frac{1}{2}|z|^{p} + \frac{1}{2}|w|^{p} \right)^{\frac{1}{p-1}}\quad \cdots (7)

If 2p<2 \le p <\infty, then the following inequality holds.

z+w2p+zw2p12zp+12wp(8) \left| \frac{z+w}{2} \right|^{p} + \left| \frac{z-w}{2} \right|^{p} \le \frac{1}{2}|z|^{p} + \frac{1}{2}|w|^{p} \quad \cdots (8)


Minkowski’s inequality

Let’s say 1p<1 \le p<\infty. If u,vLpu,v\in {L}^{ p}, then the following inequality holds.

u+vpup+vp | u+v|_{p} \le \| u \|_{p}+\left\| v \right\|_{p}

Reverse Minkowski’s inequality

Let’s say 0<p10<p \le 1. If u,vLpu,v\in {L}^{ p}, then the following inequality holds.

 u+v pup+vp | \ |u|+|v| \ |_{p} \ge \| u \|_{p}+\left\| v \right\|_{p}

Proof

(1)

Assuming 2p<2 \le p <\infty. Inserting z=u(x)z=u(x), w=v(x)w=v(x) into (8)(8) and taking the integral, we directly get (1)(1).

Ω(u+v2p+uv2p)dxΩ(12up+12vp)dx \int_{\Omega} \left( \left| \frac{u+v}{2} \right|^{p}+ \left| \frac{u-v}{2} \right|^{p} \right) dx \le \int_{\Omega} \left( \frac{1}{2}|u|^{p} +\frac{1}{2}|v|^{p} \right) dx

    Ωu+v2pdx+Ωuv2pdx12Ωupdx+12Ωvpdx \implies \int_{\Omega} \left| \frac{u+v}{2} \right|^{p}dx+ \int_{\Omega} \left| \frac{u-v}{2} \right|^{p} dx \le \frac{1}{2}\int_{\Omega} |u|^{p}dx +\frac{1}{2}\int_{\Omega} |v|^{p} dx

    u+v2pp+uv2pp12upp+12vpp \implies \left\| \frac{u+v}{2} \right\|_{p}^{p} + \left\| \frac{u-v}{2} \right\|_{p}^{p} \le \frac{1}{2}\| u \|_{p}^{p} + \frac{1}{2} \left\| v \right\|_{p}^{p}

(2)

Assuming 2p<2 \le p <\infty. Then 1<p21<p^{\prime}\le 2 and 1p1\le p. Using the results organized above for calculation

u+v2pp+u+v2pp=  u+v2pp1+ uv2pp1 u+v2p+uv2pp1= (Ω u+v2p+uv2pp1dx)1p1(Ω(12up+12vp)dx)1p1= (12Ωupdx+12Ωvpdx)1p1= (12upp+12vpp)p1 \begin{align*} \left\| \frac{u+v}{2} \right\|_{p}^{p^{\prime}}+\left\| \frac{u+v}{2} \right\|_{p}^{p^{\prime}} =&\ \left\| \ \left| \frac{u+v}{2}\right|^{p^{\prime}} \right\|_{p-1}+\left\| \ \left| \frac{u-v}{2}\right|^{p^{\prime}} \right\|_{p-1} \\ \ge& \left\| \ \left|\frac{u+v}{2}\right|^{p^{\prime}} + \left| \frac{u-v}{2}\right|^{p^{\prime}} \right\|_{p-1} \\ =&\ \left( \int_{\Omega} \left| \ \left|\frac{u+v}{2}\right|^{p^{\prime}} + \left| \frac{u-v}{2}\right|^{p^{\prime}} \right|^{p-1} dx \right)^{\frac{1}{p-1}} \\ \ge& \left( \int_{\Omega} \left( \frac{1}{2} \left| u \right|^{p} + \frac{1}{2}\left| v \right|^{p} \right) dx \right)^{\frac{1}{p-1}} \\ =&\ \left( \frac{1}{2}\int_{\Omega} \left| u \right|^{p} dx + \frac{1}{2} \int_{\Omega} \left| v \right|^{p} dx \right)^{\frac{1}{p-1}} \\ =&\ \left( \frac{1}{2} \left\| u \right\|_{p}^{p} + \frac{1}{2} \left\| v \right\|_{p}^{p} \right)^{p^{\prime}-1} \end{align*}

The first line holds by (6)(6). The second line holds by the Minkowski inequality because of 1p11\le p-1. The third line is the direct application of the definition of p1p-1 norm. More calculation is needed to prove the fourth line holds.

  • Additional calculation Since 1<p21<p^{\prime}\le 2, inserting p=pp=p^{\prime}, z=u+vz=u+v, w=uvw=u-v into (7)(7)

    up+vp(12u+vp+12uvp)1p1 \left| u \right|^{p} + \left| v \right|^{p} \le \left( \frac{1}{2}|u+v|^{p^{\prime}} + \frac{1}{2}|u-v|^{p^{\prime}} \right)^{\frac{1}{p^{\prime}-1}}

    Multiplying both sides by 12\frac{1}{2}

    12up+12vp12(12u+vp+12uvp)1p1= (12)p11p1(12u+vp+12uvp)p1= (12)(p1)(p1)(12u+vp+12uvp)p1= (12pu+vp+12puvp)p1= (u+v2p+uv2p)p1(9) \begin{align*} \frac{1}{2}\left| u \right|^{p} + \frac{1}{2}\left| v \right|^{p} \le& \frac{1}{2}\left( \frac{1}{2}|u+v|^{p^{\prime}} + \frac{1}{2}|u-v|^{p^{\prime}} \right)^{\frac{1}{p^{\prime}-1}} \\ =&\ \left(\frac{1}{2}\right)^{{p^{\prime}-1} \frac{1}{p^{\prime}-1}} \left( \frac{1}{2}|u+v|^{p^{\prime}} + \frac{1}{2}|u-v|^{p^{\prime}} \right)^{p-1} \\ =&\ \left(\frac{1}{2}\right)^{(p^{\prime}-1) (p-1)} \left( \frac{1}{2}|u+v|^{p^{\prime}} + \frac{1}{2}|u-v|^{p^{\prime}} \right)^{p-1} \\ =&\ \left(\frac{1}{2^{p^{\prime}}}|u+v|^{p^{\prime}} + \frac{1}{2^{p^{\prime}}}|u-v|^{p^{\prime}} \right)^{p-1} \\ =&\ \left(\frac{u+v}{2}|^{p^{\prime}} + |\frac{u-v}{2}|^{p^{\prime}} \right)^{p- 1} \end{align*} \quad \cdots (9)

    The third line holds by (5)(e)(5)(e). The fourth line holds by (9)(9). By organizing and using the definition of the norm and applying (5)(e)(5)(e), the last line holds.

(4)

Let’s say 1<p21<p\le 2.

u+v2pp+u+v2pp=  u+v2pp1+ uv2pp1 u+v2p+uv2pp1= (Ω u+v2p+uv2pp1dx)1p1(Ω(12up+12vp)1p1p1dx)1p1= (12Ωupdx+12Ωvpdx)p1= (12upp+12vpp)p1 \begin{align*} \left\| \frac{u+v}{2} \right\|_{p}^{p^{\prime}}+\left\| \frac{u+v}{2} \right\|_{p}^{p^{\prime}} =&\ \left\| \ \left| \frac{u+v}{2}\right|^{p^{\prime}} \right\|_{p-1}+\left\| \ \left| \frac{u-v}{2}\right|^{p^{\prime}} \right\|_{p-1} \\ \le& \left\| \ \left|\frac{u+v}{2}\right|^{p^{\prime}} + \left| \frac{u-v}{2}\right|^{p^{\prime}} \right\|_{p-1} \\ =&\ \left( \int_{\Omega} \left|\ \left|\frac{u+v}{2}\right|^{p^{\prime}} + \left| \frac{u-v}{2}\right|^{p^{\prime}} \right|^{p-1} dx \right)^{\frac{1}{p-1}} \\ \le& \left( \int_{\Omega} \left| \left( \frac{1}{2} \left| u \right|^{p} + \frac{1}{2}\left| v \right|^{p}\right)^{\frac{1}{p-1}} \right|^{p-1} dx \right)^{\frac{1}{p-1}} \\ =&\ \left( \frac{1}{2}\int_{\Omega} \left| u \right|^{p} dx + \frac{1}{2} \int_{\Omega} \left| v \right|^{p} dx \right)^{p^{\prime}-1} \\ =&\ \left( \frac{1}{2} \left\| u \right\|_{p}^{p} + \frac{1}{2} \left\| v \right\|_{p}^{p} \right)^{p^{\prime}-1} \end{align*}

The first line holds by (6)(6). The second line holds by the reverse Minkowski inequality because of 0<p110<p-1\le 1. The fourth line holds by (7)(7). Using the definition of the norm and (5)(e)(5)(e), the last line holds.


  1. Robert A. Adams and John J. F. Foutnier, Sobolev Space (2nd Edition, 2003), p44-45 ↩︎