Thanks @cardinal for the definition.
Simplifying on both sides of the $=$ sign, we get
$$ \frac{\bar{F}_1(\delta x) \bar{F}_2(\delta x)}{\bar{F}_1((1-\delta) x) + \bar{F}_2((1-\delta) x)} = o(1), $$
which means that it tends to 0 (as $x \rightarrow \infty$ since you specified it).
Is your question about the meaning of $o(1)$ or how to prove this inequality? If it is the first case, the small $o$ Landau notation $f(x) = o(g(x))$, $x\to a$ sometimes said "$f$ is negligible compared to $g$ in the neighborhood of $a$", means that the function $f$ is such that
$$ \lim_{x\to a} \frac{f(x)}{g(x)} = 0, $$
so $o(1)$ means that $f$ tends to 0.
If your question is actually the second one, I feel we miss some information, like can $\delta$ be greater than 1 (in which case the limit is trivially true)?
EDIT: with the new assumptions you can prove it as follows:
$$ \frac{\bar{F}_1(\delta x) \bar{F}_2(\delta x)}{\bar{F}_1((1-\delta) x) + \bar{F}_2((1-\delta) x)} = \frac{(\delta x)^{-2\alpha}L_1(\delta x)L_2(\delta x)}{((1 - \delta)x)^{-\alpha} (L_1((1-\delta) x) + L_2((1-\delta) x))}. $$
Dividing numerator and denominator by $L_1(x)L_2(x)$ and taking the limit, the whole things is equivalent to
EDIT:
$$\frac{(\delta x)^{-2\alpha}}{((1 - \delta)x)^{-\alpha}(\frac{1}{L_2(x)} + \frac{1}{L_1(x)})}.$$
By hypothesis $L_i(x) = o(x^\alpha)$, in the limit $\frac{1}{L_i(x)} > x^{-\alpha}$ so the denominator is bounded and the ration tends to 0.