確率変数の変数変換 Z=X/Y
Z=X/Y
$$
\begin{eqnarray}
p_{X/Y}(z)
&=&\int \int \delta\left(z-\frac{x}{y}\right)f(x)g(y)\mathrm{d}x\mathrm{d}y
\\&&\;\cdots\;\href{https://shikitenkai.blogspot.com/2020/09/delta-function.html}{\int_{-\infty}^{\infty}\delta(x)f(x)\mathrm{d}x=f(0)}
\\&&\;\cdots\;X=x,Y=yの同時確率f(x)g(x)のうちz-\left(\frac{x}{y}\right)=0を満たすものだけを足し合わせる.
\\&=&\int \int \left|y\right|\delta\left(x-yz\right)\;f\left(x\right)g(y)\mathrm{d}x\mathrm{d}y
\\&&\;\cdots\;\href{https://shikitenkai.blogspot.com/2020/09/delta-function.html}{\delta(u(x))=\sum_{\alpha\in u^{-1}(0)}\frac{1}{\left|u^{\prime}(\alpha)\right|}\delta\left(x-\alpha\right)}
\\&&\;\cdots\;u(x)=z-\frac{x}{y}
\\&&\;\cdots\;u(x=\alpha)=0,\;\alpha=yz
\\&&\;\cdots\;u^\prime=\frac{\mathrm{d}u}{\mathrm{d}x}=\frac{\mathrm{d}}{\mathrm{d}x}(z-\frac{x}{y})=-\frac{1}{y}
\\&&\;\cdots\;\delta\left(z-\frac{x}{y}\right)
=\frac{1}{|u^\prime(\alpha)|}\delta\left(x-\alpha\right)
=\frac{1}{\left|-\frac{1}{y}\right|}\delta\left(x-yz\right)
=\frac{1}{\left|\frac{1}{y}\right|}\delta\left(x-yz\right)
=\left|y\right|\delta\left(x-yz\right)
\\&=&\int |y|\delta\left(yz-yz\right)f\left(yz\right)g(y)\mathrm{d}y
\;\cdots\;z=\frac{x}{y},x=yz
\\&=&\int |y|\delta\left(0\right)f\left(yz\right)g(y)\mathrm{d}y
\\&=&\int |y|f(yz)g(y)\mathrm{d}y
\;\cdots\;\delta凾数の引数が全域で0なので,全域で|y|f(yz)g(y)を足し合わせる積分になる.
\end{eqnarray}
$$
標準正規分布同士の例
$$
\begin{eqnarray}
f_X(x)&=&\frac{1}{\sqrt{2\pi}}e^{-\frac{x^2}{2}}
\;\cdots\;N(0,1)\;(標準正規分布)
\\g_Y(y)&=&\frac{1}{\sqrt{2\pi}}e^{-\frac{y^2}{2}}
\;\cdots\;N(0,1)\;(標準正規分布)
\\p_{X/Y}(z)&=&\int \int \delta(z-\frac{x}{y})f_X(x)g_Y(y)\mathrm{d}x\mathrm{d}y
\\&=&\int \int \delta(z-\frac{x}{y})\frac{1}{\sqrt{2\pi}}e^{-\frac{x^2}{2}}\frac{1}{\sqrt{2\pi}}e^{-\frac{y^2}{2}}\mathrm{d}x\mathrm{d}y
\\&=&\int_{-\infty}^{\infty} \left|y\right| \frac{1}{\sqrt{2\pi}}e^{-\frac{\left(yz\right)^2}{2}}\frac{1}{\sqrt{2\pi}}e^{-\frac{y^2}{2}} \mathrm{d}y
\;\cdots\;z=\frac{x}{y},x=yz
\\&=&\frac{1}{2\pi}\int_{-\infty}^{\infty} \left|y\right| e^{-\frac{\left(yz\right)^2}{2}}e^{-\frac{y^2}{2}} \mathrm{d}y
\;\cdots\;\int c f(x) \mathrm{d}x = c \int f(x) \mathrm{d}x
\\&=&\frac{1}{2\pi}\int_{-\infty}^{\infty} \left|y\right| e^{-\frac{\left(yz\right)^2}{2}-\frac{y^2}{2}} \mathrm{d}y
\;\cdots\;A^BA^C=A^{B+C}
\\&=&\frac{1}{2\pi}\int_{-\infty}^{\infty} \left|y\right| e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
\\&=&\frac{1}{2\pi}\left\{
\int_{-\infty}^{0} \left|y\right| e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
+ \int_{0}^{\infty} \left|y\right| e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
\right\}
\\&&\;\cdots\;\int_{A}^{B} f(x)\mathrm{d}x=\int_{A}^{C} f(x)\mathrm{d}x+\int_{C}^{B} f(x)\mathrm{d}x\;(ただしA\leq C \leq B)
\\&=&\frac{1}{2\pi}\left\{
\int_{-\infty}^{0} -y e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
+ \int_{0}^{\infty} y e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
\right\}
\;\cdots\;\left|A\right|=\left\{
\begin{array}
\\A&(A\geq0)
\\-A&(A\lt0)
\end{array}
\right.
\\&=&\frac{1}{2\pi}2\int_{0}^{\infty} y e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
\\&&\;\cdots\;y=xが奇凾数でy=e^{-\frac{x^2\left(z^2+1\right)}{2}}が偶凾数なのでその積は奇凾数.
\\&&\;\cdots\;負の区間(-\infty,0)と正の区間(0,\infty)で符号が逆なので全体としては偶凾数と同じに扱える.
\\&&\;\cdots\;-f_{奇凾数(-\infty,0)}(x) + f_{奇凾数(0,\infty)}(x) = f_{偶凾数}(x)\mathrm{d}x
\\&&\;\cdots\;偶凾数の(-a,a)での積分は正の区間(0,a)の2倍として計算できる.
\\&&\;\cdots\;\int_{-a}^a f_{奇凾数}(x) \mathrm{d}x=2\int_0^a f_{偶凾数}(x)\mathrm{d}x
\\&=&\frac{1}{\pi}\int_{0}^{\infty} y e^{-\frac{y^2\left(z^2+1\right)}{2}} \mathrm{d}y
\\&=&\frac{1}{\pi}\int_{0}^{\infty} \color{red}{y} e^{-t}\cdot\frac{1}{\left(z^2+1\right)\color{red}{y}}\mathrm{d}t
\\&&\;\cdots\;t=\frac{y^2\left(z^2+1\right)}{2},\frac{\mathrm{d}t}{\mathrm{d}y}=\frac{\left(z^2+1\right)}{2}2y=\left(z^2+1\right)y,\mathrm{d}y=\frac{1}{\left(z^2+1\right)y}\mathrm{d}t
\\&=&\frac{1}{\pi}\frac{1}{\left(z^2+1\right)}\int_{0}^{\infty} e^{-t} \mathrm{d}t
\;\cdots\;\int c f(x) \mathrm{d}x = c \int f(x) \mathrm{d}x
\\&=&\frac{1}{\pi}\frac{1}{\left(z^2+1\right)}\cdot1
\;\cdots\;\int_{0}^{\infty} e^{-t} \mathrm{d}t=\left[-e^{-t}\right]_{0}^{\infty}=\left[\left(-e^{-\infty}\right)-\left(-e^0\right)\right]=\left[0+1\right]=1
\\&=&\frac{1}{\pi}\frac{1}{\left(z^2+1\right)}\;\cdots\;標準コーシー分布に等しい.
\\f(x;x_0, \gamma)&=&\frac{1}{\pi}\frac{\gamma}{(x-x_0)^2+\gamma^2}\;\cdots\;コーシー分布(Cauchy\;distribution)の確率密度凾数
\\f(x;0, 1)&=&\frac{1}{\pi}\frac{1}{(x-0)^2+1^2}\;\cdots\;標準コーシー分布の確率密度凾数
\\&=&\frac{1}{\pi}\frac{1}{x^2+1}
\end{eqnarray}
$$
指数分布同士の例
$$
\begin{eqnarray}
f_X(x)&=&\lambda e^{-\lambda x} (x \geq 0, \lambda \gt 0)
\\g_Y(y)&=&\lambda e^{-\lambda y} (x \geq 0, \lambda \gt 0)
\\p_{X/Y}(z)&=&\int \int \delta(x-\frac{z}{y})f_X(x)g_Y(y)\mathrm{d}x\mathrm{d}y
\\&=&\int \int \delta(x-\frac{z}{y})\lambda e^{-\lambda x} \lambda e^{-\lambda y} \mathrm{d}x\mathrm{d}y
\\&=&\int_0^{\infty} \left|y\right|\lambda e^{-\lambda yz} \lambda e^{-\lambda y}\mathrm{d}y
\;\cdots\;z=\frac{x}{y},x=yz
\\&=&\lambda^2 \int_0^{\infty} \left|y\right|e^{-\lambda yz} e^{-\lambda y}\mathrm{d}y
\;\cdots\;\int c f(x) \mathrm{d}x = c \int f(x) \mathrm{d}x
\\&=&\lambda^2 \int_0^{\infty} \left|y\right|e^{-\lambda yz-\lambda y}\mathrm{d}y
\;\cdots\;A^BA^C=A^{B+C}
\\&=&\lambda^2 \int_0^{\infty} \left|y\right|e^{-\lambda y\left(z+1\right)}\mathrm{d}y
\\&=&\lambda^2 \int_0^{\infty} ye^{-\lambda y\left(z+1\right)}\mathrm{d}y
\;\cdots\;y \gt 0\;(積分範囲より)
\\&=&\lambda^2 \int_0^{\infty} \frac{t}{\lambda\left(z+1\right)}e^{-t}\frac{1}{\lambda\left(z+1\right)}\mathrm{d}t
\\&&\;\cdots\;t=\lambda\left(z+1\right)y, y=\frac{t}{\lambda\left(z+1\right)}
\\&&\;\cdots\;\frac{\mathrm{d}t}{\mathrm{d}y}=\lambda\left(z+1\right),\mathrm{d}y=\frac{1}{\lambda\left(z+1\right)}\mathrm{d}t
\\&=&\lambda^2 \left\{\frac{1}{\lambda\left(z+1\right)}\right\}^2\int_0^{\infty} te^{-t}\mathrm{d}t
\;\cdots\;\int c f(x) \mathrm{d}x = c \int f(x) \mathrm{d}x
\\&=&\frac{1}{\left(z+1\right)^2}\int_0^{\infty} te^{-t}\mathrm{d}t
\\&=&\frac{1}{\left(z+1\right)^2}\int_0^{\infty} t\left(-e^{-t}\right)^\prime\mathrm{d}t
\;\cdots\;\left(-e^{-t}\right)^\prime=e^{-t}
\\&=&\frac{1}{\left(z+1\right)^2}\left\{\left[-te^{-t}\right]_0^{\infty}-\int_0^{\infty} -e^{-t}\mathrm{d}t\right\}
\;\cdots\;\int_a^b f^\prime(x)g(x) \mathrm{d}x=\left[f(x)g(x)\right]_a^b -\int_a^b f(x)g^\prime(x)\mathrm{d}x
\\&=&\frac{1}{\left(z+1\right)^2}\left\{\left[-(\infty)e^{-\infty}-\left(-0e^{-0}\right)\right]+\int_0^{\infty} e^{-t}\mathrm{d}t\right\}
\\&=&\frac{1}{\left(z+1\right)^2}\left(0+1\right)
\;\cdots\;\int_{0}^{\infty} e^{-t} \mathrm{d}t=\left[-e^{-t}\right]_{0}^{\infty}=\left[\left(-e^{-\infty}\right)-\left(-e^0\right)\right]=\left[0+1\right]=1
\\&=&\frac{1}{\left(z+1\right)^2}
\end{eqnarray}
$$
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