How was the generalized harmonics number's relation to the hurwitz zeta function derived?
$H_{n,\ m} =\zeta ( m,\ 1) -\zeta ( m,\ n+1),\ \Re(m)>1$
I tried looking at the series representations for both functions, but I couldn't see how they could relate.
$\sum ^{n}_{k=1}\frac{1}{k^{m}} =\sum ^{\infty }_{k=1}\left[\frac{1}{k^{m}} -\frac{1}{( k+n)^{m}}\right]$
Somehow I just can't find a way to show these two series are equal.
I thought to loook at the integral representations, but I couldn't find the representation for the generalized harmonic numbers.
Any help in proving that both series are equal or in providing a derivation for the relation would be greatly appreciated!
Start with Gamma function
$$\Gamma(m)=\int_0^\infty t^{m-1}e^{-t}dt,\quad \Re(m)>1$$
and by subbing $t=-k\ln(x)$ we have
$$\frac1{k^m}=\frac{(-1)^{m-1}}{\Gamma(m)}\int_0^1 x^{k-1}\ln^{m-1}(x)dx,\quad \Re(m)>1$$
sum up both sides over $n$ we have
$$\sum_{k=1}^n\frac1{k^m}=H_n^{(m)}=\frac{(-1)^{m-1}}{\Gamma(m)}\int_0^1\ln^{m-1}(x)\left(\sum_{k=1}^n x^{k-1}\right)dx.$$
Using the geometric series for the inner sum we obtain
$$H_n^{(m)}=\frac{(-1)^{m-1}}{\Gamma(m)}\int_0^1 \frac{\ln^{m-1}(x)(1-x^n)}{1-x}dx$$
By writing $\frac1{1-x}=\sum_{k=1}^\infty x^{k-1}$ we have
$$H_n^{(m)}=\frac{(-1)^{m-1}}{\Gamma(m)}\sum_{k=1}^\infty\int_0^1\ln^{m-1}(x)[x^{k-1}-k^{n+k-1}]dx$$
$$=\frac{(-1)^{m-1}}{\Gamma(m)}\sum_{k=1}^\infty\left(\frac{(-1)^{m-1}\Gamma(m)}{k^m}-\frac{(-1)^{m-1}\Gamma(m)}{(n+k)^m}\right)$$
$$=\sum_{k=1}^\infty\frac{1}{k^m}-\sum_{k=1}^\infty\frac{1}{(n+k)^m}=\zeta(m)-\sum_{k=1}^\infty\frac{1}{(n+k)^m}$$
Different approach:
$$H_n^{(m)}=\sum_{k=1}^n\frac{1}{k^m}=\sum_{k=1}^\infty\frac{1}{k^m}-\sum_{k=n+1}^\infty\frac{1}{k^m}$$
reindex the second sum we have
$$H_n^{(m)}=\sum_{k=1}^\infty\frac{1}{k^m}-\sum_{k=1}^\infty\frac{1}{(n+k)^m}$$
But the problem with this proof is that its valid for only integer $n$ as you can see that from manipulating the sum limits.