Starting from the alternating Abel Plana summation formula (presented here):
$$\sum_{n=0}^\infty (-1)^nf(n) = \frac{f(0)}{2} + i\int_0^\infty\frac{f(iy)−f(−iy)}{2\sinh(πy)} dy \tag{1}$$
and putting $f(t)=\xi\left(\frac12+it\right)$, where $\xi(s)$ is the Riemann $\xi-$function. Since $\xi(s) = \xi(1-s)$ the integral part reduces to zero and we obtain:
$$2\,\sum_{n=0}^\infty (-1)^n\,\xi\left(\frac12+in\right) = \xi\left(\frac12\right) \tag{2}$$
Questions:
Numerically this appears to work fine, but is it formally allowed in terms of the required growth conditions for the Abel Plana formula?
This is rather philosophical, but the series on the LHS "samples" its values at the integer imaginary parts on the critical line. We know that $\xi\left(\frac12+it\right)$ oscillates around $0$ and has its sign changes at the non-trivial zeros. Given the unpredictable nature of these zeros, the signs of the integer samples are expected to fluctuate rather randomly as well. Does this imply that the complexity of the distribution of the non-trivial zeros is fully "encoded" in $\xi\left(\frac12\right)$
ADDED 1:
Numerical evidence strongly suggests that the above could be generalised as follows:
$$\xi(s) = \sum_{n=1}^\infty (-1)^{n+1}\,\big(\xi\left(s+in\right)+\xi\left(1-s+in\right)\big) \qquad s \in \mathbb{C} \tag{3}$$
or after expanding to the $d$-th derivative:
$$\xi^{(d)}(s) = \sum_{n=1}^\infty (-1)^{n+1}\,\big(\xi^{(d)}\left(s+in\right)+(-1)^d\,\xi^{(d)}\left(1-s+in\right)\big) \qquad s \in \mathbb{C} \tag{4}$$
ADDED 2:
Numerical evidence also strongly supports the alternating series with multiplication of $\xi(s)$:
$$\frac12\,\xi(s)^2 = \sum_{n=1}^\infty (-1)^{n+1}\,\xi\left(s+in\right)\,\xi\left(1-s+in\right) \qquad s \in \mathbb{C} \tag{5}$$