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战巡
发表于 2016-3-27 04:10
回复 1# dim
注意到
\[\Gamma'(x)=\frac{\partial}{\partial x}\int_0^{+\infty}t^{x-1}e^{-t}dt=\int_0^{+\infty}t^{x-1}\ln(x)e^{-t}dt\]
有
\[\int_0^{+\infty}x^{-\frac{1}{2}}\ln(x)e^{-x}dx=\Gamma'(\frac{1}{2})=\psi(\frac{1}{2})\Gamma(\frac{1}{2})=\sqrt{\pi}\psi(\frac{1}{2})\]
其中$\psi(x)$为双伽马函数,有
\[\psi(x)=\frac{\Gamma'(x)}{\Gamma(x)}\]
而双伽马函数有如下性质
\[\psi(x+1)=-\gamma+\int_0^1\frac{1-t^x}{1-t}dt\]
\[\psi(\frac{1}{2})=-\gamma+\int_0^1\frac{1-t^{-\frac{1}{2}}}{1-t}dt=-\gamma-2\ln(1+\sqrt{t})|_0^1=-\gamma-\ln(4)\]
\[原式=\sqrt{\pi}\psi(\frac{1}{2})=-\sqrt{\pi}(\gamma+\ln(4))\] |
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