$\newcommand{\+}{^{\dagger}} \newcommand{\angles}[1]{\left\langle\, #1 \,\right\rangle} \newcommand{\braces}[1]{\left\lbrace\, #1 \,\right\rbrace} \newcommand{\bracks}[1]{\left\lbrack\, #1 \,\right\rbrack} \newcommand{\ceil}[1]{\,\left\lceil\, #1 \,\right\rceil\,} \newcommand{\dd}{{\rm d}} \newcommand{\down}{\downarrow} \newcommand{\ds}[1]{\displaystyle{#1}} \newcommand{\expo}[1]{\,{\rm e}^{#1}\,} \newcommand{\fermi}{\,{\rm f}} \newcommand{\floor}[1]{\,\left\lfloor #1 \right\rfloor\,} \newcommand{\half}{{1 \over 2}} \newcommand{\ic}{{\rm i}} \newcommand{\iff}{\Longleftrightarrow} \newcommand{\imp}{\Longrightarrow} \newcommand{\isdiv}{\,\left.\right\vert\,} \newcommand{\ket}[1]{\left\vert #1\right\rangle} \newcommand{\ol}[1]{\overline{#1}} \newcommand{\pars}[1]{\left(\, #1 \,\right)} \newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}} \newcommand{\pp}{{\cal P}} \newcommand{\root}[2][]{\,\sqrt[#1]{\vphantom{\large A}\,#2\,}\,} \newcommand{\sech}{\,{\rm sech}} \newcommand{\sgn}{\,{\rm sgn}} \newcommand{\totald}[3][]{\frac{{\rm d}^{#1} #2}{{\rm d} #3^{#1}}} \newcommand{\ul}[1]{\underline{#1}} \newcommand{\verts}[1]{\left\vert\, #1 \,\right\vert} \newcommand{\wt}[1]{\widetilde{#1}}$ Con $\ds{\mu > 0}$ : \begin{align} &\color{#00f}{{\ds{\int_{0}^{\infty}x^{9}\expo{-x^{2}}\,\dd x} \over \ds{\int_{0}^{\infty}x^{7}\expo{-x^{2}}\,\dd x}}} =\left.-\,\partiald{}{\mu}\ln\pars{\int_{0}^{\infty}x^{7}\expo{-\mu x^{2}}\,\dd x} \right\vert_{\mu\ =\ 1} \\[3mm]&=\left.-\,\partiald{}{\mu}\ln\pars{\mu^{-4}\int_{0}^{\infty}x^{7} \expo{-x^{2}}\,\dd x}\right\vert_{\mu\ =\ 1} =\left.-\,\partiald{\ln\pars{\mu^{-4}}}{\mu}\right\vert_{\mu\ =\ 1} =\left.{4 \over \mu}\right\vert_{\mu\ =\ 1} =\color{#00f}{\Large 4} \end{align}