ZaidAlyafey said:
There is no thing to evaluate since we have
$$\psi(z+1) = -\gamma + \sum \frac{z}{n(n+z)}$$
Putting $z=0$ we get $\psi(1) = -\gamma$.
No problem. Ok, we arrived at the following
$$\sum_{n=1}^\infty \frac{z^{2n}}{n} = -\log(1-z^2)$$
Divide by $z^2$
$$\sum_{n=1}^\infty \frac{z^{2n-2}}{n} = -\frac{\log(1-z^2)}{z^2}$$
Integrate with respect to $z$
$$\sum_{n=1}^\infty \frac{z^{2n-1}}{n(2n-1)} = -\int^z_0\frac{\log(1-x^2)}{x^2}\,dx$$
Put $z=1$
$$\sum_{n=1}^\infty \frac{1}{n(2n-1)} = -\int^1_0\frac{\log(1-x^2)}{x^2}\,dx$$Can you evaluate the integral on the right ?
Thank you very much @ZaidAlyafey, kudos to you, and I really appreciate this; the method is much clearer this way as I can understand better, and as I read carefully, all at once. So thank you ZaidAlyafey, I can't thank you enough! I owe you =)
The INTEGRAL:
----------------------
$$-\int^1_0\frac{\log(1-x^2)}{x^2}\,dx$$
$$B(a, b) = \int_{0}^{1} {t}^{a-1}{(1-t)}^{(b-1)} \,dt$$
Let's differentiate with respect to $b$
$$B_b(a, b) = \int_{0}^{1} {t}^{a-1}{(1-t)}^{(b-1)}\ln(1-t) \,dt$$
Let $t = x^2 \implies dt = 2x dx$
$$B_b(a,b) = (2) \int_{0}^{1} {x}^{2a-1}{(1-x^2)}^{(b-1)}\ln(1-x^2) \,dx$$
We need $b - 1 = 0 \implies b = 1$
We need $2a - 1 = -2 \implies a = -1/2$
$$B_b((-1/2),1) = (2) \int_{0}^{1} {x}^{-2}\ln(1-x^2) \,dx$$
Darn... We still can't do anything =(
$$B_b(a, b) = B(a, b)(\psi(b) - \psi(a + b))$$
Let $\psi(1/2) = u$
$$I = 1/2B_b(-1/2, 1) = 1/2B(-1/2, 1)(-\gamma - u)$$
The sum is $u = \psi(1/2)$ so
$$u = (-1/2)B(-1/2, 1)\gamma - (1/2)B(-1/2, 1)(u)$$
It is
very surprising.
I couldn't compute it but how in the world is $B(-1/2, 1) = -2$? I computed it on WolframAlpha, but I am stumped.
$$u = \gamma + u$$
$$0 = \gamma$$
Some error happened unfortunately.