ポリガンマ関数同士の差の極限
ポリガンマ関数同士の差の極限
\[ \lim_{z\rightarrow0}\left(\psi^{\left(n\right)}\left(z-m\right)-\psi^{\left(n\right)}\left(z\right)\right)=n!H_{m,n+1} \]
\[ \lim_{z\rightarrow0}\left(\frac{\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z\right)}{\Gamma^{n+1}\left(z\right)}\right)=\left(-1\right)^{n}n! \]
\(H_{n,m}\)は一般化調和数
(1)
\(n,m\in\mathbb{N}_{0}\)とする。\[ \lim_{z\rightarrow0}\left(\psi^{\left(n\right)}\left(z-m\right)-\psi^{\left(n\right)}\left(z\right)\right)=n!H_{m,n+1} \]
(2)
\(n\in\mathbb{N}_{0}\)とする。\[ \lim_{z\rightarrow0}\left(\frac{\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z\right)}{\Gamma^{n+1}\left(z\right)}\right)=\left(-1\right)^{n}n! \]
-
\(\psi\left(x\right)\)はポリガンマ関数\(H_{n,m}\)は一般化調和数
(1)
\begin{align*} \lim_{z\rightarrow0}\left(\psi^{\left(n\right)}\left(z-m\right)-\psi^{\left(n\right)}\left(z\right)\right) & =\lim_{z\rightarrow0}\left(\psi^{\left(n\right)}\left(z-m\right)-\psi^{\left(n\right)}\left(z+1\right)+\frac{\left(-1\right)^{n}n!}{z^{n+1}}\right)\\ & =\lim_{z\rightarrow0}\left(\psi^{\left(n\right)}\left(z+1\right)+\left(-1\right)^{n}n!\sum_{k=1}^{-m-1}\frac{1}{\left(z+k\right)^{n+1}}-\psi^{\left(n\right)}\left(z+1\right)+\frac{\left(-1\right)^{n}n!}{z^{n+1}}\right)\\ & =\lim_{z\rightarrow0}\left(-\left(-1\right)^{n}n!\sum_{k=-m}^{0}\frac{1}{\left(z+k\right)^{n+1}}+\frac{\left(-1\right)^{n}n!}{z^{n+1}}\right)\\ & =-\left(-1\right)^{n}n!\sum_{k=-m}^{-1}\frac{1}{k^{n+1}}\\ & =-\left(-1\right)^{n}n!\sum_{k=1}^{m}\frac{1}{\left(-k\right)^{n+1}}\\ & =n!\sum_{k=1}^{m}\frac{1}{k^{n+1}}\\ & =n!H_{m,n+1} \end{align*}(2)
\(n\in\mathbb{N}_{0}\)とする。\begin{align*} \lim_{z\rightarrow0}\left(\frac{\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z\right)}{\Gamma^{n+1}\left(z\right)}\right) & =\lim_{z\rightarrow0}\left(\frac{\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z+1\right)+\frac{\left(-1\right)^{n}n!}{z^{n+1}}}{\Gamma^{n+1}\left(z\right)}\right)\\ & =\lim_{z\rightarrow0}\left(\frac{z^{n+1}\left(\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z+1\right)\right)+\left(-1\right)^{n}n!}{z^{n+1}\Gamma^{n+1}\left(z\right)}\right)\\ & =\lim_{z\rightarrow0}\left(\frac{z^{n+1}\left(\psi^{\left(n\right)}\left(z+\alpha\right)-\psi^{\left(n\right)}\left(z+1\right)\right)+\left(-1\right)^{n}n!}{\Gamma^{n+1}\left(z+1\right)}\right)\\ & =\frac{\left(-1\right)^{n}n!}{\Gamma^{n+1}\left(1\right)}\\ & =\left(-1\right)^{n}n! \end{align*}
ページ情報
| タイトル | ポリガンマ関数同士の差の極限 |
| URL | https://www.nomuramath.com/hmva3swl/ |
| SNSボタン |
不完全ガンマ関数とガンマ関数との関係
\[
\gamma\left(a,x\right)+\Gamma\left(a,x\right)=\Gamma\left(a\right)
\]
ガンマ関数を含む極限
\[
\lim_{n\rightarrow\infty}\sqrt{n}\frac{\Gamma\left(n\right)}{\Gamma\left(n+\frac{1}{2}\right)}=1
\]
ガンマ関数の非正整数近傍での値
\[
\lim_{\epsilon\rightarrow\pm0}\Gamma\left(-\epsilon\right)=-\lim_{\epsilon\rightarrow\pm0}\Gamma\left(\epsilon\right)
\]
ガンマ関数のハンケル積分表示
\[
\Gamma\left(z\right)=\frac{i}{2\sin\left(\pi z\right)}\int_{C}\left(-\tau\right)^{z-1}e^{-\tau}d\tau
\]