What is the exact sum of $$\sum_{n=1}^{\infty}(-1)^n\frac{\ln n}{n}$$
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1Why do you think there is a simpler way to write this number? – GEdgar Jan 10 '13 at 20:33
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1According to Mathematica, $\gamma\log 2-(\log2)^2/2\approx .1599$. – Eckhard Jan 10 '13 at 20:33
3 Answers
Define $$\eta(s) = \sum_{n=1}^\infty \frac{(-1)^n}{n^s}$$ convergent $\Re(s)>0$, but we shall only use $\eta(s)$ for $\Re(s)>1$. Then the quantity of interest is $$ -\lim_{s \downarrow 1} \frac{\mathrm{d}}{\mathrm{d}s} \eta(s) $$ Now, for $\Re(s)>1$ we can evaluate $\eta(s)$ as follows: $$ \eta(s) + \zeta(s) = \sum_{n=1}^\infty \frac{(-1)^n}{n^s} + \sum_{n=1}^\infty \frac{1}{n^s} = 2 \sum_{m=1}^\infty \frac{1}{(2m)^s} = 2^{1-s} \zeta(s) $$ Hence $$ \eta(s) = \zeta(s) \left(2^{1-s} - 1 \right) $$ Keeping in mind that Riemann function has a pole at $s=1$, $\zeta(s) = \frac{1}{s-1} + \gamma + \mathcal{o}(1)$, where $\gamma$ denotes the Euler-Mascheroni constant we arrive at: $$ \begin{eqnarray} -\lim_{s \downarrow 1} \frac{\mathrm{d}}{\mathrm{d}s} \eta(s) &=& \lim_{s \downarrow 1} \frac{\mathrm{d}}{\mathrm{d}s} \zeta(s) \left(1-2^{1-s} \right) \\ &=& \lim_{s \downarrow 1} \frac{\mathrm{d}}{\mathrm{d}s} \left( \frac{1}{s-1} + \gamma + \mathcal{o}(1) \right) \left(\log(2) (s-1) - \frac{\log^2(2)}{2} (s-1)^2 + \mathcal{o}\left((s-1)^2\right) \right) \\ &=& -\frac{1}{2} \log^2(2) + \log(2) \gamma \end{eqnarray} $$
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$$\begin{eqnarray}\sum_{k=1}^{2n}(-1)^k\frac{\log(k)}{k} &=& -\sum_{k=1}^{2n}\frac{\log(k)}{k} + \sum_{k=1}^n \frac{\log(2k)}{k}\\ &=& \log(2)\sum_{k=1}^n\frac{1}{k} -\sum_{k=1}^n \frac{\log(n+k)}{n+k}\\ &=& \log(2)\sum_{k=1}^n\frac{1}{k} -\frac{\log(n)}{n}\sum_{k=1}^n \frac{1}{1+\frac{k}{n}}- \frac{1}{n}\sum_{k=1}^n\frac{\log(1+\frac{k}{n})}{1+\frac{k}{n}}\\ \end{eqnarray}$$
Now we can recognize two Riemann sums:
$$\frac{1}{n}\sum_{k=1}^n \frac{1}{1+\frac{k}{n}}=\int_1^2\frac{dt}{t} + O(\frac{1}{n}) = \log(2)+O(\frac{1}{n})$$
and
$$\lim_{n\to\infty}\frac{1}{n}\sum_{k=1}^n\frac{\log(1+\frac{k}{n})}{1+\frac{k}{n}} =\int_1^2\frac{\log(t)}{t}dt = \frac{1}{2}\log(2)^2.$$
Combining all this gives
$$\begin{eqnarray} \sum_{k=1}^{\infty}(-1)^k\frac{\log(k)}{k}&=&-\frac{1}{2}\log(2)^2+\log(2) \lim_{n\to\infty}\left( \sum_{k=1}^n\frac{1}{k} -\log(n)\right)\\ &=& -\frac{1}{2}\log(2)^2+\log(2)\,\gamma. \end{eqnarray}$$
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\begin{align*} S_{n} &:= \sum_{k=1}^{n}(-1)^k\frac{\ln k}{k} \\ (-1)^k &\frac{\ln k}{k} \sum_{k=1}^{\infty}(-1)^k\frac{\ln k}{k} &= \lim_{n\to+\infty}S_{2n}. \end{align*}
\text{Now:}
\begin{align*} S_{2n} &= \sum_{k=1}^{n}\frac{\ln2k}{2k}-\sum_{k=1}^{n}\frac{\ln(2k-1)}{2k-1} \\ &= \frac{\ln2}{2}\sum_{k=1}^{n}\frac{1}{k}+\frac{1}{2}\sum_{k=1}^{n}\frac{\ln k}{k}-\left(\sum_{k=1}^{2n}\frac{\ln k}{k}-\sum_{k=1}^{n}\frac{\ln2k}{2k}\right) \\ &= \ln2H_{n}+\sum_{k=1}^{n}\frac{\ln k}{k}-\sum_{k=1}^{2n}\frac{\ln k}{k} \\ &= \ln2H_{n}-\sum_{k=1}^{n}\frac{\ln(n+k)}{n+k} \\ &= \ln2H_{n}-\sum_{k=1} ^{n}\frac{\ln n+\ln(1+k/n)}{n+k} \\ &= \ln2H_{n}-\ln n(H_{2n}-H_{n})-\frac{ 1}{n}\sum_{k=1}^{n}\frac{\ln(1+k/n)}{1+k/n} \\ &= H_{n}\ln(2n)-H_{2n}\ln n-\frac{1}{n}\sum_{k=1}^{n}\frac{\ln(1+k/ n)}{1+k/n}\stackrel{H_{n}=\ln n+\gamma+\mathcal O(1/n)}{=}\gamma\ln2+\mathcal O(1/n)-\frac {1}{n}\sum_{k=1}^{n}\frac{\ln(1+k/n)}{1+k/n} \\ &\to\gamma\ln2-\int_{0}^ {1}\frac{\ln(1+x)}{1+x}\,dx \\ &=\gamma\ln2-\frac{\ln^22}{2}. \end{align*}
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