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# A relation between Hilbert and Carlson inequalities

Journal of Inequalities and Applications20122012:277

https://doi.org/10.1186/1029-242X-2012-277

• Received: 13 February 2012
• Accepted: 7 November 2012
• Published:

## Abstract

In this paper, we introduce some new inequalities with a best constant factor. As an application, we obtain a sharper form of Hilbert’s inequality. Some inequalities of Carlson type are also considered.

MSC:26D15.

## Keywords

• Hilbert’s inequality
• Carlson’s inequality
• Cauchy’s inequality
• sharper form

## 1 Introduction

If $f\left(x\right),g\left(x\right)\ge 0$, $0<{\int }_{0}^{\mathrm{\infty }}{f}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, and $0<{\int }_{0}^{\mathrm{\infty }}{g}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, then (see )
${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{f\left(x\right)g\left(y\right)}{x+y}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy<\pi {\left\{{\int }_{0}^{\mathrm{\infty }}{f}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{2}}{\left\{{\int }_{0}^{\mathrm{\infty }}{g}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{2}}.$
(1.1)
Inequality (1.1) is called Hilbert’s integral inequality, which has been extended by Hardy  as: if $p>1$, $\frac{1}{p}+\frac{1}{q}=1$, $f\left(x\right),g\left(x\right)>0$, $0<{\int }_{0}^{\mathrm{\infty }}{f}^{p}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, and $0<{\int }_{0}^{\mathrm{\infty }}{g}^{q}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, then
${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{f\left(x\right)g\left(y\right)}{x+y}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy<\frac{\pi }{sin\frac{\pi }{p}}{\left\{{\int }_{0}^{\mathrm{\infty }}{f}^{p}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{p}}{\left\{{\int }_{0}^{\mathrm{\infty }}{g}^{q}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{q}}.$
(1.2)
The corresponding inequalities in the discrete case are (${a}_{m},{b}_{n}>0$):
provided that the series on the right-hand side of (1.3) and (1.4) are convergent. The constant factor π is the best possible in both (1.1) and (1.3), and the constant $\frac{\pi }{sin\frac{\pi }{p}}$ is the best possible in (1.2) and (1.4). The following general inequality was given in :
where $k\left(p{A}_{2}\right)={\int }_{0}^{\mathrm{\infty }}K\left(1,t\right){t}^{-p{A}_{2}}\phantom{\rule{0.2em}{0ex}}dt$ is the best possible constant, $K\left(x,y\right)\ge 0$ is a homogeneous function of degree −λ ($\lambda >0$), ${A}_{1}\in \left(\frac{1-\lambda }{q},\frac{1}{q}\right)$, ${A}_{2}\in \left(\frac{1-\lambda }{p},\frac{1}{p}\right)$, and $p{A}_{2}+q{A}_{1}=2-\lambda$. Moreover, in  the following is proved:
$\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}K\left(m,n\right){a}_{m}{b}_{n}
(1.6)
here $K\left(x,y\right)\ge 0$ is a homogeneous function of degree −λ ($\lambda >0$) strictly decreasing in both parameters x and y, ${A}_{1}\in \left(max\left\{\frac{1-\lambda }{q},0\right\},\frac{1}{q}\right)$, ${A}_{2}\in \left(max\left\{\frac{1-\lambda }{p},0\right\},\frac{1}{p}\right)$, and $p{A}_{2}+q{A}_{1}=2-\lambda$. In particular, if we set $K\left(x,y\right)=\frac{1}{\alpha x+\beta y}$ and $K\left(m,n\right)=\frac{1}{\alpha m+\beta n}$ ($\alpha ,\beta >0$) respectively in (1.5) and (1.6) for $\lambda =1$, we have
where $B\left(s,t\right)$ is the beta function, ${A}_{1}\in \left(0,\frac{1}{q}\right)$, ${A}_{2}\in \left(0,\frac{1}{p}\right)$, and $p{A}_{2}+q{A}_{1}=1$. We need the following formula for the beta function:
$B\left(s,t+1\right)=\frac{t}{s+t}B\left(s,t\right).$
(1.9)
For the sequence of real numbers $\left({a}_{n}\right)$, Carlson’s inequality is given as
$\sum _{n=1}^{\mathrm{\infty }}{a}_{n}<\sqrt{\pi }{\left(\sum _{n=1}^{\mathrm{\infty }}{a}_{n}^{2}\right)}^{\frac{1}{4}}{\left(\sum _{n=1}^{\mathrm{\infty }}{n}^{2}{a}_{n}^{2}\right)}^{\frac{1}{4}},$
(1.10)
the constant $\sqrt{\pi }$ is the best possible. The continuous version of (1.10) is
${\int }_{0}^{\mathrm{\infty }}f\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\le \sqrt{\pi }{\left({\int }_{0}^{\mathrm{\infty }}{f}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right)}^{\frac{1}{4}}{\left({\int }_{0}^{\mathrm{\infty }}{x}^{2}{f}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right)}^{\frac{1}{4}},$
(1.11)

the constant $\sqrt{\pi }$ is sharp. Regarding these inequalities and their extensions, we refer the reader to the book .

In this paper, we introduce two new inequalities with a best constant factor which gives an upper estimate for the double series ${\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}{\sigma }_{n,m}$ and the double integral ${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}G\left(x,y\right)\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy$, where ${\sigma }_{n,m}$ is a double sequence of positive numbers and $G\left(x,y\right)$ is a positive function on $\left(0,\mathrm{\infty }\right)×\left(0,\mathrm{\infty }\right)$. As an application, we obtain a sharper form of the Hilbert inequality. Some examples of Carlson type inequalities are also considered. The proof of the inequalities depends on inequalities (1.7), (1.8) and Hardy’s idea in proving Carlson’s inequality.

## 2 Discrete case

Theorem 2.1 Let $p>1$, $\frac{1}{p}+\frac{1}{q}=1$, ${a}_{n}$ and ${b}_{n}$ be two sequences of positive numbers such that $0<{\sum }_{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}<\mathrm{\infty }$, $0<{\sum }_{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}<\mathrm{\infty }$. Let ${\sigma }_{n,m}$ be a double sequence of positive numbers such that ${\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{m{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}<\mathrm{\infty }$ and ${\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{n{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}<\mathrm{\infty }$, then the following inequality holds:
$\begin{array}{rcl}{\left[\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}{\sigma }_{n,m}\right]}^{2}& <& L{\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}\\ ×{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}\right\}}^{q{A}_{1}}{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}\right\}}^{p{A}_{2}},\end{array}$
(2.1)

here ${A}_{1}\in \left(0,\frac{1}{q}\right)$, ${A}_{2}\in \left(0,\frac{1}{p}\right)$, $p{A}_{2}+q{A}_{1}=1$, and the constant $L=\frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\left(p{A}_{2}\right)}^{p{A}_{2}}{\left(q{A}_{1}\right)}^{q{A}_{1}}}$ is the best possible.

Proof Let $\alpha ,\beta >0$, using Cauchy’s inequality and then applying (1.8), we get
$\begin{array}{rcl}{\left[\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}{\sigma }_{n,m}\right]}^{2}& =& {\left[\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\left\{\frac{\sqrt{{a}_{m}{b}_{n}}}{\sqrt{\alpha m+\beta n}}\right\}\left\{\frac{\sqrt{\alpha m+\beta n}}{\sqrt{{a}_{m}{b}_{n}}}{\sigma }_{n,m}\right\}\right]}^{2}\\ \le & \sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{\alpha m+\beta n}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{\alpha m+\beta n}{{a}_{m}{b}_{n}}{\sigma }_{n,m}^{2}\\ <& \frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\alpha }^{1-q{A}_{1}}{\beta }^{1-p{A}_{2}}}{\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}\\ ×\left[\alpha \sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}+\beta \sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}\right]\\ =& B\left(p{A}_{2},1-p{A}_{2}\right){\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}\\ ×\left[{\left(\frac{\alpha }{\beta }\right)}^{q{A}_{1}}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}+{\left(\frac{\beta }{\alpha }\right)}^{p{A}_{2}}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}\right].\end{array}$

Set $T={\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{m{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}$, $S={\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{n{\sigma }_{n,m}^{2}}{{a}_{m}{b}_{n}}$, $t=\frac{\alpha }{\beta }$ and consider the function $h\left(t\right)={t}^{q{A}_{1}}T+{t}^{-p{A}_{2}}S$. Since ${h}^{\mathrm{\prime }}\left(t\right)=\frac{1}{{t}^{p{A}_{2}}}\left(q{A}_{1}T-\frac{p{A}_{2}S}{t}\right)$, we conclude that the minimum of this function attains for $t=\frac{p{A}_{2}S}{q{A}_{1}T}$. Therefore, if we let $\alpha =p{A}_{2}S$ and $\beta =q{A}_{1}T$, we get (2.1).

It remains to show that the constant L in (2.1) is the best possible. To do that, suppose that there exists a positive constant $C such that (2.1) is still valid if we replace L by C. For $0<\epsilon , setting ${\stackrel{˜}{a}}_{m}$ and ${\stackrel{˜}{b}}_{n}$ as ${\stackrel{˜}{a}}_{m}={m}^{-q{A}_{1}-\frac{\epsilon }{p}}$, $\stackrel{˜}{{b}_{n}}={n}^{-p{A}_{2}-\frac{\epsilon }{q}}$, and ${\stackrel{˜}{\sigma }}_{n,m}=\frac{{\stackrel{˜}{a}}_{m}{\stackrel{˜}{b}}_{n}}{m+n}$, we have ${\sum }_{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{\stackrel{˜}{a}}_{m}^{p}={\sum }_{m=1}^{\mathrm{\infty }}\frac{1}{{m}^{1+\epsilon }}=1+{\sum }_{m=2}^{\mathrm{\infty }}\frac{1}{{m}^{1+\epsilon }}<1+{\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }\phantom{\rule{0.2em}{0ex}}dx=1+\frac{1}{\epsilon }$; similarly, we obtain ${\sum }_{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{\stackrel{˜}{b}}_{n}^{q}<1+\frac{1}{\epsilon }$. Moreover,
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{\stackrel{˜}{\sigma }}_{n,m}^{2}}{{\stackrel{˜}{a}}_{m}{\stackrel{˜}{b}}_{n}}& =& \sum _{n=1}^{\mathrm{\infty }}{n}^{1-p{A}_{2}-\frac{\epsilon }{q}}\sum _{m=1}^{\mathrm{\infty }}\frac{{m}^{-q{A}_{1}-\frac{\epsilon }{p}}}{{\left(m+n\right)}^{2}}\\ <& \sum _{n=1}^{\mathrm{\infty }}{n}^{1-p{A}_{2}-\frac{\epsilon }{q}}{\int }_{0}^{\mathrm{\infty }}\frac{{x}^{-q{A}_{1}-\frac{\epsilon }{p}}}{{\left(n+x\right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\\ =& \sum _{n=1}^{\mathrm{\infty }}{n}^{-1-\epsilon }{\int }_{0}^{\mathrm{\infty }}\frac{{u}^{-q{A}_{1}-\frac{\epsilon }{p}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du=\left[B\left(1-q{A}_{1},1+q{A}_{1}\right)+o\left(1\right)\right]\sum _{n=1}^{\mathrm{\infty }}{n}^{-1-\epsilon }\\ <& \frac{\epsilon +1}{\epsilon }\left[B\left(1-q{A}_{1},1+q{A}_{1}\right)+o\left(1\right)\right].\end{array}$
Similarly,
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{\stackrel{˜}{\sigma }}_{n,m}^{2}}{{\stackrel{˜}{a}}_{m}{\stackrel{˜}{b}}_{n}}& =& \sum _{m=1}^{\mathrm{\infty }}{m}^{1-q{A}_{1}-\frac{\epsilon }{p}}\sum _{n=1}^{\mathrm{\infty }}\frac{{m}^{-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(m+n\right)}^{2}}<\sum _{m=1}^{\mathrm{\infty }}{m}^{1-q{A}_{1}-\frac{\epsilon }{p}}{\int }_{0}^{\mathrm{\infty }}\frac{{x}^{-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(m+x\right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\\ =& \sum _{m=1}^{\mathrm{\infty }}{m}^{-1-\epsilon }{\int }_{0}^{\mathrm{\infty }}\frac{{u}^{-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du=\left[B\left(1-p{A}_{2},1+p{A}_{2}\right)+o\left(1\right)\right]\sum _{m=1}^{\mathrm{\infty }}{m}^{-1-\epsilon }\\ <& \frac{\epsilon +1}{\epsilon }\left[B\left(1-p{A}_{2},1+p{A}_{2}\right)+o\left(1\right)\right].\end{array}$
On the other hand,
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}{\stackrel{˜}{\sigma }}_{n,m}& =& \sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{m}^{-q{A}_{1}-\frac{\epsilon }{p}}{n}^{-p{A}_{2}-\frac{\epsilon }{q}}}{m+n}>{\int }_{1}^{\mathrm{\infty }}{\int }_{1}^{\mathrm{\infty }}\frac{{x}^{-q{A}_{1}-\frac{\epsilon }{p}}{y}^{-p{A}_{2}-\frac{\epsilon }{q}}}{x+y}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy\\ >& \frac{1}{\epsilon }\left[B\left(p{A}_{2},1-p{A}_{2}\right)+o\left(1\right)\right]-O\left(1\right).\end{array}$
Multiplying inequality (2.2) by ${\epsilon }^{2}$ ($\epsilon ={\epsilon }^{q{A}_{1}}{\epsilon }^{p{A}_{2}}$) and then letting $\epsilon \to {0}^{+}$, we have
${B}^{2}\left(p{A}_{2},1-p{A}_{2}\right)\le C{B}^{q{A}_{1}}\left(1-q{A}_{1},1+q{A}_{1}\right){B}^{p{A}_{2}}\left(1-p{A}_{2},1+p{A}_{2}\right).$
(2.3)
Using (1.9), we find
$\begin{array}{rcl}{B}^{q{A}_{1}}\left(1-q{A}_{1},1+q{A}_{1}\right)& =& {\left(q{A}_{1}\right)}^{q{A}_{1}}{B}^{q{A}_{1}}\left(1-q{A}_{1},q{A}_{1}\right)\\ =& {\left(q{A}_{1}\right)}^{q{A}_{1}}{B}^{q{A}_{1}}\left(p{A}_{2},1-p{A}_{2}\right),\end{array}$
(2.4)
and
${B}^{p{A}_{2}}\left(1-p{A}_{2},1+p{A}_{2}\right)={\left(p{A}_{2}\right)}^{p{A}_{2}}{B}^{p{A}_{2}}\left(1-p{A}_{2},p{A}_{2}\right).$
(2.5)

Substituting (2.4) and (2.5) in (2.3), we obtain the contradiction $C\ge L=\frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\left(p{A}_{2}\right)}^{p{A}_{2}}{\left(q{A}_{1}\right)}^{q{A}_{1}}}$. The theorem is proved. □

### 2.1 Some applications

1. 1.
If ${\sigma }_{n,m}=\frac{{a}_{m}{b}_{n}}{m+n}$ in (2.1), then we have the following form of Hilbert’s inequality:
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}& <& \sqrt{L}{\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{2p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{2q}}\\ ×{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}\right\}}^{\frac{q{A}_{1}}{2}}{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}\right\}}^{\frac{p{A}_{2}}{2}}.\end{array}$
(2.6)

Inequality (2.6) is a sharper form of (1.8). To see that, let us rewrite (2.6) in the following form:
${\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}\right\}}^{2}<\frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\left(p{A}_{2}\right)}^{p{A}_{2}}{\left(q{A}_{1}\right)}^{q{A}_{1}}}{\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}{S}^{q{A}_{1}}{T}^{p{A}_{2}},$
where $S={\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{n{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}$ and $T={\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{m{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}$. Since we may write ${\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}=T+S$, dividing both sides of the last inequality by ${\sum }_{n=1}^{\mathrm{\infty }}{\sum }_{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}$, we get
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}& <& B\left(p{A}_{2},1-p{A}_{2}\right){\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}\\ ×\frac{{\left(\frac{S}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{T}{p{A}_{2}}\right)}^{p{A}_{2}}}{T+S}.\end{array}$
(2.7)
Applying Young’s inequality (${x}^{\theta }{y}^{\mu }\le \theta x+\mu y$, $\theta +\mu =1$) to the product ${\left(\frac{S}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{T}{p{A}_{2}}\right)}^{p{A}_{2}}$ with $x=\frac{S}{q{A}_{1}}$ and $y=\frac{T}{p{A}_{2}}$, we obtain
$\frac{{\left(\frac{S}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{T}{p{A}_{2}}\right)}^{p{A}_{2}}}{T+S}\le \frac{T+S}{T+S}=1.$
Therefore, inequality (2.6) is a sharper form of (1.8). In particular, if we set $p=q=2$, ${A}_{1}=\frac{1}{4}={A}_{2}$ in (2.6), we obtain the following sharper form of the classical Hilbert inequality (1.3):
$\begin{array}{rcl}{\left[\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n}\right]}^{2}& <& 2\pi {\left\{\sum _{m=1}^{\mathrm{\infty }}{a}_{m}^{2}\right\}}^{\frac{1}{2}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{b}_{n}^{2}\right\}}^{\frac{1}{2}}\\ ×{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{n{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}\right\}}^{\frac{1}{2}}{\left\{\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{m{a}_{m}{b}_{n}}{{\left(m+n\right)}^{2}}\right\}}^{\frac{1}{2}}.\end{array}$
(2.8)
Note that we may obtain the Hilbert inequality from (2.8) by applying the AG inequality $\sqrt{ST}\le \frac{S+T}{2}$ to the right-hand side of (2.8).
1. 2.
The more accurate Hilbert inequality is given as
$\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n+1}<\frac{\pi }{sin\frac{\pi }{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{a}_{n}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{b}_{n}^{q}\right\}}^{\frac{1}{q}}.$
(2.9)

If we put ${\sigma }_{n,m}=\frac{{a}_{m}{b}_{n}}{m+n+\mu }$ ($\mu >0$) in (2.1), then we have
we obtain
$\begin{array}{rcl}\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n+\mu }& <& B\left(p{A}_{2},1-p{A}_{2}\right){\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{pq{A}_{1}-1}{a}_{m}^{p}\right\}}^{\frac{1}{p}}{\left\{\sum _{n=1}^{\mathrm{\infty }}{n}^{pq{A}_{2}-1}{b}_{n}^{q}\right\}}^{\frac{1}{q}}\\ ×\frac{{\left(\frac{{S}_{1}}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{{S}_{2}}{p{A}_{2}}\right)}^{p{A}_{2}}}{{S}_{1}+{S}_{2}+{S}_{3}}.\end{array}$
Applying Young’s inequality, we get $\frac{{\left(\frac{{S}_{1}}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{{S}_{2}}{p{A}_{2}}\right)}^{p{A}_{2}}}{{S}_{1}+{S}_{2}+{S}_{3}}\le \frac{{S}_{1}+{S}_{2}}{{S}_{1}+{S}_{2}+{S}_{3}}<1$, thus we arrive at
$\sum _{n=1}^{\mathrm{\infty }}\sum _{m=1}^{\mathrm{\infty }}\frac{{a}_{m}{b}_{n}}{m+n+\mu }
In particular, if $\mu =1$, ${A}_{1}=\frac{1}{pq}={A}_{2}$, then we have (2.9).
1. 3.
For $\alpha >1$, set ${a}_{m}={m}^{-\frac{\alpha }{p}}$, ${b}_{n}={n}^{-\frac{\alpha }{q}}$, and ${A}_{1}={A}_{2}=\frac{1}{pq}$ in (2.1), then we get

where $\zeta \left(\alpha \right)$ is the Riemann zeta function. In particular, if $\alpha =2$ and if ${\sigma }_{n,m}={c}_{m}{c}_{n}$, then we get the following Carlson type inequality:
$\sum _{m=1}^{\mathrm{\infty }}{c}_{m}<{\left(\frac{{\pi }^{3}}{3}\right)}^{\frac{1}{4}}{\left\{\sum _{m=1}^{\mathrm{\infty }}m{c}_{m}^{2}\right\}}^{\frac{1}{4}}{\left\{\sum _{m=1}^{\mathrm{\infty }}{m}^{2}{c}_{m}^{2}\right\}}^{\frac{1}{4}}.$
1. 4.
If we let ${\sigma }_{n,m}={a}_{m}{a}_{n}$ and ${b}_{n}={a}_{n}$, $p=q=2$, ${A}_{1}={A}_{2}=\frac{1}{4}$, we get
$\sum _{m=1}^{\mathrm{\infty }}{a}_{m}<{\left(2\pi \right)}^{\frac{1}{3}}{\left\{\sum _{m=1}^{\mathrm{\infty }}m{a}_{m}\right\}}^{\frac{1}{3}}{\left\{\sum _{m=1}^{\mathrm{\infty }}{a}_{m}^{2}\right\}}^{\frac{1}{3}}.$

## 3 Integral case

Theorem 3.1 If $p>1$, $\frac{1}{p}+\frac{1}{q}=1$, $f\left(x\right),g\left(x\right)>0$ such that $0<{\int }_{0}^{\mathrm{\infty }}{x}^{pq{A}_{1}-1}{f}^{p}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, $0<{\int }_{0}^{\mathrm{\infty }}{x}^{pq{A}_{1}-1}{g}^{q}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<\mathrm{\infty }$, suppose also that the function $G\left(x,y\right)$ is positive on $\left(0,\mathrm{\infty }\right)×\left(0,\mathrm{\infty }\right)$ and that ${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{x{G}^{2}\left(x,y\right)}{f\left(x\right)g\left(y\right)}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy<\mathrm{\infty }$, ${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{y{G}^{2}\left(x,y\right)}{f\left(x\right)g\left(y\right)}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy<\mathrm{\infty }$, then the following inequality holds:

where ${A}_{1}\in \left(0,\frac{1}{q}\right)$, ${A}_{2}\in \left(0,\frac{1}{p}\right)$, $p{A}_{2}+q{A}_{1}=1$, and the constant $L=\frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\left(p{A}_{2}\right)}^{p{A}_{2}}{\left(q{A}_{1}\right)}^{q{A}_{1}}}$ is the best possible.

Proof By Cauchy’s inequality, taking into account (1.7), we get ($\alpha ,\beta >0$)
As in the proof of Theorem 2.1, if we set ${I}_{1}={\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{x{G}^{2}\left(x,y\right)}{f\left(x\right)g\left(y\right)}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy$, ${I}_{2}={\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{y{G}^{2}\left(x,y\right)}{f\left(x\right)g\left(y\right)}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy$, $t=\frac{\alpha }{\beta }$ and consider the function $h\left(t\right)={t}^{q{A}_{1}}{I}_{1}+{t}^{-p{A}_{2}}{I}_{2}$, we find that the minimum of this function attains for $t=\frac{p{A}_{2}{I}_{2}}{q{A}_{1}{I}_{1}}$. Thus, if we let $\alpha =p{A}_{2}{I}_{2}$ and $\beta =q{A}_{1}{I}_{1}$, we get (3.1). If the constant factor L is not the best possible, then there exists a positive constant M (with $M), thus (3.1) is still valid if we replace L by M. For $0<\epsilon , setting $\stackrel{˜}{f}$ and $\stackrel{˜}{g}$ as $\stackrel{˜}{f}\left(x\right)=\stackrel{˜}{g}\left(x\right)=0$ for $x\in \left(0,1\right)$, $\stackrel{˜}{f}\left(x\right)={x}^{-q{A}_{1-}\frac{\epsilon }{p}}$, $\stackrel{˜}{g}\left(x\right)={x}^{-p{A}_{2-}\frac{\epsilon }{q}}$ for $x\in \left[1,\mathrm{\infty }\right)$, and setting $\stackrel{˜}{G}\left(x,y\right)=\frac{\stackrel{˜}{f}\left(x\right)\stackrel{˜}{g}\left(y\right)}{x+y}$, we have
$\begin{array}{rcl}{I}^{2}& :=& {\left[{\int }_{1}^{\mathrm{\infty }}{\int }_{1}^{\mathrm{\infty }}\stackrel{˜}{G}\left(x,y\right)\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy\right]}^{2}\\ <& M{\left({\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }\phantom{\rule{0.2em}{0ex}}dx\right)}^{\frac{1}{p}}{\left({\int }_{1}^{\mathrm{\infty }}{y}^{-1-\epsilon }\phantom{\rule{0.2em}{0ex}}dy\right)}^{\frac{1}{q}}{\left\{{\int }_{1}^{\mathrm{\infty }}{\int }_{1}^{\mathrm{\infty }}\frac{{x}^{1-q{A}_{1}-\frac{\epsilon }{p}}{y}^{-p{A}_{2-}\frac{\epsilon }{q}}}{{\left(x+y\right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy\right\}}^{p{A}_{2}}\\ ×{\left\{{\int }_{1}^{\mathrm{\infty }}{\int }_{1}^{\mathrm{\infty }}\frac{{y}^{1-p{A}_{2-}\frac{\epsilon }{q}}{x}^{-q{A}_{1}-\frac{\epsilon }{p}}}{{\left(x+y\right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy\right\}}^{q{A}_{1}}\\ =& \frac{M}{\epsilon }{\left({I}_{1}\right)}^{p{A}_{2}}{\left({I}_{2}\right)}^{q{A}_{1}}.\end{array}$
(3.2)
Let $y=ux$, then we have
$\begin{array}{rcl}{I}_{1}& =& {\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }{\int }_{1/x}^{\mathrm{\infty }}\frac{{u}^{-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du\phantom{\rule{0.2em}{0ex}}dx<{\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }{\int }_{0}^{\mathrm{\infty }}\frac{{u}^{-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du\phantom{\rule{0.2em}{0ex}}dx\\ =& \frac{1}{\epsilon }\left[B\left(1-p{A}_{2},1+p{A}_{2}\right)+o\left(1\right)\right].\end{array}$
Similarly,
$\begin{array}{rcl}{I}_{2}& =& {\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }{\int }_{1/x}^{\mathrm{\infty }}\frac{{u}^{1-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du\phantom{\rule{0.2em}{0ex}}dy<{\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }{\int }_{0}^{\mathrm{\infty }}\frac{{u}^{1-p{A}_{2}-\frac{\epsilon }{q}}}{{\left(1+u\right)}^{2}}\phantom{\rule{0.2em}{0ex}}du\phantom{\rule{0.2em}{0ex}}dx\\ =& \frac{1}{\epsilon }\left[B\left(p{A}_{2},2-p{A}_{2}\right)+o\left(1\right)\right].\end{array}$
Finally,
$\begin{array}{rcl}I& =& {\int }_{1}^{\mathrm{\infty }}{x}^{-1-\epsilon }{\int }_{1/x}^{\mathrm{\infty }}\frac{{u}^{-p{A}_{2}-\frac{\epsilon }{q}}}{1+u}\phantom{\rule{0.2em}{0ex}}du\phantom{\rule{0.2em}{0ex}}dx\\ >& \frac{1}{\epsilon }\left[B\left(1-p{A}_{2},p{A}_{2}\right)+o\left(1\right)\right]-O\left(1\right).\end{array}$

Substituting the above estimates in (3.2) and then letting $\epsilon \to {0}^{+}$, we find $M\ge \frac{B\left(p{A}_{2},1-p{A}_{2}\right)}{{\alpha }^{1-q{A}_{1}}{\beta }^{1-p{A}_{2}}}$. The theorem is proved. □

### 3.1 Some applications

1. 1.
Putting $G\left(x,y\right)=\frac{f\left(x\right)g\left(y\right)}{x+y}$ in inequality (3.1), we get

We may prove that inequality (3.3) is sharper than inequality (1.7) as we did in the discrete case, or we may do that by using (1.5) in the following way: set $K\left(x,y\right)=\frac{x}{{\left(x+y\right)}^{2}}$ and $K\left(x,y\right)=\frac{y}{{\left(x+y\right)}^{2}}$ respectively in (1.5), then we have
Using these two inequalities in (3.3), we get (1.7). In particular, if we set $p=q=2$, ${A}_{1}=\frac{1}{4}={A}_{2}$ in (3.3), we obtain the following sharper form of the Hilbert inequality (1.1):
1. 2.
Assuming $G\left(x,y\right)=\frac{f\left(x\right)g\left(y\right)}{x+y+\mu }$ ($\mu >0$) in inequality (3.1), we get

Since we may write ${\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{f\left(x\right)g\left(y\right)}{x+y+\mu }\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy={\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{xf\left(x\right)g\left(y\right)}{{\left(x+y+\mu \right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy+{\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{yf\left(x\right)g\left(y\right)}{{\left(x+y+\mu \right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy+{\int }_{0}^{\mathrm{\infty }}{\int }_{0}^{\mathrm{\infty }}\frac{\mu f\left(x\right)g\left(y\right)}{{\left(x+y+\mu \right)}^{2}}\phantom{\rule{0.2em}{0ex}}dx\phantom{\rule{0.2em}{0ex}}dy={I}_{1}+{I}_{2}+{I}_{3}$,
the quotient $\frac{{\left(\frac{{I}_{1}}{q{A}_{1}}\right)}^{q{A}_{1}}{\left(\frac{{I}_{2}}{p{A}_{2}}\right)}^{p{A}_{2}}}{{I}_{1}+{I}_{2}+{I}_{3}}\le 1$, thus we have the following inequality:
1. 3.
Put $f\left(x\right)={e}^{-x}$ and $g\left(y\right)={e}^{-y}$ in (3.1), ${A}_{1}=\frac{1}{pq}={A}_{2}$, then we get the following Carlson type inequality for functions of two variables:

Moreover, if we assume $G\left(x,y\right)=\phi \left(x\right)\phi \left(y\right)$ in (3.4), we get ($p=2$)
${\int }_{0}^{\mathrm{\infty }}\phi \left(x\right)\phantom{\rule{0.2em}{0ex}}dx<{\pi }^{\frac{1}{4}}{\left\{{\int }_{0}^{\mathrm{\infty }}x{e}^{x}{\phi }^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{4}}{\left\{{\int }_{0}^{\mathrm{\infty }}{e}^{x}{\phi }^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{4}},$
which is a sharper form of Carlson’s inequality (1.11).
1. 4.
Let $G\left(x,y\right)=f\left(x\right)f\left(y\right)$, $f\left(x\right)=g\left(x\right)$ in (3.1), then we obtain the following Carlson type inequality:
${\int }_{0}^{\mathrm{\infty }}f\left(x\right)\phantom{\rule{0.2em}{0ex}}dx<{\left(2\pi \right)}^{\frac{1}{3}}{\left\{{\int }_{0}^{\mathrm{\infty }}xf\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{3}}{\left\{{\int }_{0}^{\mathrm{\infty }}{f}^{2}\left(x\right)\phantom{\rule{0.2em}{0ex}}dx\right\}}^{\frac{1}{3}}.$

## Authors’ Affiliations

(1)
Department of Mathematics, Al al-Bayt University, P.O. Box 130095, Mafraq, Jordan

## References 