Alpha decay: $(Z,A) \rightarrow (Z-2,A-4)+ ^4_2He $
According to the book: "Nuclear and particle physics" by Williams, $Q_\alpha$ is the measure of available energy to permit an alpha decay.
It is defined as:
$$ Q_\alpha = M(Z,A)-M(Z-2,A-4)-M(2,4)$$
(in natural units)
where M is the nuclear mass, defined as: $M(Z,A) = Zm_p+Am_n-BE(Z,A) $
where BE is the binding energy.
Since the number of protons and neutrons doesn't change (in this case), $Q_\alpha$ can be written as:
$$ Q_\alpha = BE_{f}-BE_{i}=\Delta BE$$
If $Q_\alpha >0$ then the reaction is possible.
I am having difficulties to interpret the $Q_\alpha$-value in alpha decays. I will explain my reasoning hoping that someone can point out my mistake.
My reasoning:
If $Q_\alpha = \Delta BE > 0$ then it means that the energy of the system increased, and therefore energy from somewhere would be needed to make the reaction possible. Then $Q_\alpha $ wouldn't be the energy available for the reaction to happen, but the extra energy needed for the reaction to happen.