zoukankan      html  css  js  c++  java
  • Euler Sums系列(一)

    [Largesum_{n=1}^{infty} frac{H_{n}}{2^nn^4} ]


    (Largemathbf{Solution:})
    Let

    [mathcal{S}=sum^infty_{n=1}frac{H_n}{n^42^n} ]

    We first consider a slightly different yet related sum. The main idea is to solve this sum with two different methods, one of which involves the sum in question. This then allows us to determine the value of the desired sum.

    [egin{align*} &sum^infty_{n=1}frac{(-1)^nH_n}{n^4} =frac{1}{6}sum^infty_{n=1}(-1)^{n-1}H_nint^1_0x^{n-1}ln^3{x} { m d}x =frac{1}{6}int^1_0frac{ln^3{x}ln(1+x)}{x(1+x)}{ m d}x\ =&frac{1}{6}int^1_0frac{ln^3{x}ln(1+x)}{x}{ m d}x-frac{1}{6}int^1_0frac{ln^3{x}ln(1+x)}{1+x}{ m d}x =frac{1}{6}sum^infty_{n=1}frac{(-1)^{n-1}}{n}int^1_0x^{n-1}ln^3{x} { m d}x\ -&frac{1}{6}int^2_1frac{ln{x}ln^3(x-1)}{x}{ m d}x =sum^infty_{n=1}frac{(-1)^{n}}{n^5}+int^1_{frac{1}{2}}frac{ln{x}ln^3(1-x)}{6x}-int^1_{frac{1}{2}}frac{ln^2{x}ln^2(1-x)}{2x}{ m d}x\+&int^1_{frac{1}{2}}frac{ln^3{x}ln(1-x)}{2x}{ m d}x-int^1_{frac{1}{2}}frac{ln^4{x}}{6x}{ m d}x =-frac{15}{16}zeta(5)+mathcal{I}_1-mathcal{I}_2+mathcal{I}_3-mathcal{I}_4 end{align*}]

    Starting with the easiest integral,

    [egin{align*} mathcal{I}_4=frac{1}{30}ln^5{2} end{align*}]

    For (mathcal{I}_3),

    [egin{align*} mathcal{I}_3 =&-frac{1}{2}sum^infty_{n=1}frac{1}{n}int^1_{frac{1}{2}}x^{n-1}ln^3{x} { m d}x =-frac{1}{2}sum^infty_{n=1}frac{1}{n}frac{partial^3}{partial n^3}left(frac{1}{n}-frac{1}{n2^n} ight)\ =&sum^infty_{n=1}left(frac{3}{n^5}-frac{3}{n^52^n}-frac{3ln{2}}{n^42^n}-frac{3ln^2{2}}{n^32^{n+1}}-frac{ln^3{2}}{n^22^{n+1}} ight)\ =&3zeta(5)-3{ m Li}_5left(dfrac{1}{2} ight)-3{ m Li}_4left(dfrac{1}{2} ight)ln{2}-frac{3}{2}ln^2{2}left(frac{7}{8}zeta(3)-frac{pi^2}{12}ln{2}+frac{1}{6}ln^3{2} ight)\&-frac{1}{2}ln^3{2}left(frac{pi^2}{12}-frac{1}{2}ln^2{2} ight)\ =&3zeta(5)-3{ m Li}_5left(dfrac{1}{2} ight)-3{ m Li}_4left(dfrac{1}{2} ight)ln{2}-frac{21}{16}zeta(3)ln^2{2}+frac{pi^2}{12}ln^3{2} end{align*}]

    For (mathcal{I}_2),

    [egin{align*} mathcal{I}_2 =&frac{1}{6}ln^5{2}+frac{1}{3}int^1_{frac{1}{2}}frac{ln^3{x}ln(1-x)}{1-x}{ m d}x =frac{1}{6}ln^5{2}-frac{1}{3}sum^infty_{n=1}H_nfrac{partial^3}{partial n^3}left(frac{1}{n+1}-frac{1}{(n+1)2^{n+1}} ight)\ =&frac{1}{6}ln^5{2}+sum^infty_{n=1}frac{2H_n}{(n+1)^4}-sum^infty_{n=1}frac{2H_n}{(n+1)^42^{n+1}}-sum^infty_{n=1}frac{2ln{2}H_n}{(n+1)^32^{n+1}}\ &-sum^infty_{n=1}frac{ln^2{2}H_n}{(n+1)^22^{n+1}}-sum^infty_{n=1}frac{ln^3{2}H_n}{3(n+1)2^{n+1}}\ =&frac{1}{6}ln^5{2}+4zeta(5)-frac{pi^2}{3}zeta(3)-2mathcal{S}+2{ m Li}_5left(dfrac{1}{2} ight)-frac{pi^4}{360}ln{2}+frac{1}{4}zeta(3)ln^2{2}-frac{1}{12}ln^5{2}\ &-frac{1}{8}zeta(3)ln^2{2}+frac{1}{6}ln^5{2}-frac{1}{6}ln^5{2}\ =&-2mathcal{S}+2{ m Li}_5left(dfrac{1}{2} ight)+4zeta(5)-frac{pi^4}{360}ln{2}+frac{1}{8}zeta(3)ln^2{2}-frac{pi^2}{3}zeta(3)+frac{1}{12}ln^5{2} end{align*}]

    For (mathcal{I}_1),

    [egin{align*} mathcal{I}_1 =&frac{1}{6}int^{frac{1}{2}}_0frac{ln^3{x}ln(1-x)}{1-x}{ m d}x =-frac{1}{6}sum^infty_{n=1}H_nfrac{partial^3}{partial n^3}left(frac{1}{(n+1)2^{n+1}} ight)\ =&sum^infty_{n=1}frac{H_n}{(n+1)^42^{n+1}}+sum^infty_{n=1}frac{ln{2}H_n}{(n+1)^32^{n+1}}+sum^infty_{n=1}frac{ln^2{2}H_n}{2(n+1)^22^{n+1}}+sum^infty_{n=1}frac{ln^3{2}H_n}{6(n+1)2^{n+1}}\ =&mathcal{S}-{ m Li}_5left(dfrac{1}{2} ight)+frac{pi^4}{720}ln{2}-frac{1}{16}zeta(3)ln^2{2}+frac{1}{24}ln^5{2} end{align*}]

    Combining these four integrals as (mathcal{I}_1-mathcal{I}_2+mathcal{I}_3-mathcal{I}_4) and (displaystyle -dfrac{15}{16}zeta(5)) gives

    [egin{align*} sum^infty_{n=1}frac{(-1)^nH_n}{n^4} =&3mathcal{S}-6{ m Li}_5left(dfrac{1}{2} ight)-frac{31}{16}zeta(5)-3{ m Li}_4left(dfrac{1}{2} ight)ln{2}+frac{pi^4}{240}ln{2}\&-frac{3}{2}zeta(3)ln^2{2}+frac{pi^2}{3}zeta(3)+frac{pi^2}{12}ln^3{2}-frac{3}{40}ln^5{2} end{align*}]

    But consider (displaystyle f(z)=frac{picsc(pi z)(gamma+psi_0(-z))}{z^4}). At the positive integers,

    [sum^infty_{n=1}{ m Res}(f,n)=sum^infty_{n=1}operatorname*{Res}_{z=n}left[frac{(-1)^n}{z^4(z-n)^2}+frac{(-1)^nH_n}{z^4(z-n)} ight]=sum^infty_{n=1}frac{(-1)^nH_n}{n^4}+frac{15}{4}zeta(5) ]

    At (z=0),

    [egin{align*} { m Res}(f,0) &=[z^3]left(frac{1}{z}+frac{pi^2}{6}z+frac{7pi^4}{360}z^3 ight)left(frac{1}{z}-frac{pi^2}{6}z-zeta(3)z^2-frac{pi^4}{90}z^3-zeta(5)z^4 ight)\ &=-zeta(5)-frac{pi^2}{6}zeta(3) end{align*}]

    At the negative integers,

    [egin{align*} sum^infty_{n=1}{ m Res}(f,-n) &=sum^infty_{n=1}frac{(-1)^nH_n}{n^4}+frac{15}{16}zeta(5) end{align*}]

    Since the sum of the residues is zero,

    [sum^infty_{n=1}frac{(-1)^nH_n}{n^4}=-frac{59}{32}zeta(5)+frac{pi^2}{12}zeta(3) ]

    Hence,

    [egin{align*} -frac{59}{32}zeta(5)+frac{pi^2}{12}zeta(3) =&3mathcal{S}-6{ m Li}_5left(dfrac{1}{2} ight)-frac{31}{16}zeta(5)-3{ m Li}_4left(dfrac{1}{2} ight)ln{2}+frac{pi^4}{240}ln{2}\&-frac{3}{2}zeta(3)ln^2{2}+frac{pi^2}{3}zeta(3)+frac{pi^2}{12}ln^3{2}-frac{3}{40}ln^5{2} end{align*}]

    This implies that

    [oxed{egin{align*} {sum^infty_{n=1}frac{H_n}{n^42^n}} {=}&color{blue}{2{ m Li}_5left(dfrac{1}{2} ight)+frac{1}{32}zeta(5)+{ m Li}_4left(dfrac{1}{2} ight)ln{2}-frac{pi^4}{720}ln{2}+frac{1}{2}zeta(3)ln^2{2}}\&color{blue}{-frac{pi^2}{12}zeta(3)-frac{pi^2}{36}ln^3{2}+frac{1}{40}ln^5{2}} end{align*}}]

  • 相关阅读:
    【转】Install libimobiledevice on Mac OSX
    【转】Mac端包管理工具——Homebrew简介及安装
    Appium的安装-Mac平台(命令行 & dmg)
    【转】NO.3、python+appium+ios,遍历真机元素,得到webview
    【转】NO.2、Appium之IOS第一个demo
    【转】NO.1、 appium之ios环境搭建
    如何在 iOS 真机运行 Appium
    【转】adb shell dumpsys 命令
    Mac下抓包工具charles及破解方法
    2017.08 笔记
  • 原文地址:https://www.cnblogs.com/Renascence-5/p/5436454.html
Copyright © 2011-2022 走看看