I am working in the appendix to Section II.6 in Zee's QFT book, 2nd Ed. I am trying to compute the cross section for a meson to decay to two mesons as $\varphi\to\eta+\xi$ with three respective momenta $k,p,q$. To simplify the problem, I have imposed the big box condition which quantizes the $k,p,q$. I have computed the probability amplitude
$$ \mathcal{A}\propto \big(2\pi)^4\delta^{(4)}(p+q-k) ~~, $$
where "$\propto $" means "is proportional to." Now I need to square $\mathcal{A}$ to get the probability. I substitute the integral form of the $\delta$-function so
$$ |\mathcal{A}|^2\propto \left[\big(2\pi)^4\delta^{(4)}(p+q-k)\right ]^2=\big(2\pi)^4\delta^{(4)}(p+q-k)\int\!d^4x\,e^{ix(p+q-k )}~~. $$
Zee simplifies this to
$$ |\mathcal{A}|^2\propto\big(2\pi)^4\delta^{(4)}(p+q-k)\int\!d^4x =\big(2\pi)^4\delta^{(4)}(p+q-k)VT~~,$$
where $VT$ is the 4-volume of spacetime in the box we have chosen. Zee cites as motivation for the approximation $e^{ix(p+q-k )}=1$ the fact we are using the big box normalization instead of considering all of spacetime. I do not see why the big box normalization which imposes quantization on the momenta $k,p,q$ allows us to approximate the integrand as being equal to one. How does he do this? We have used the box to quantize momenta so I do not see what it does for the present integral over $d^4x$.