I am studying the notes of David Tong on Statistical Field Theory (https://www.damtp.cam.ac.uk/user/tong/sft/sft.pdf). I don't understand how to formally get the result after Eq. 2.11, that is the following step: $$ \prod_{\textbf{k}}\Big[\mathcal{N}\int d\phi_{\textbf{k}}d\phi^*_{\textbf{k}}\exp{\Big(-\frac{\beta}{2V}(\gamma k^2+\mu^2)\Big)|\phi_{\textbf{k}}|^2}\Big]=\prod_{\textbf{k}}\mathcal{N}\sqrt{\frac{2\pi TV}{\gamma k^2+\mu^2}}\,, $$ where $\phi_\textbf{k}$ is a variable in a reciprocal lattice, ($\textbf{k}$ is a momentum vector in a discretized space). In particular the author says that since $\phi_{\textbf{k}}$ and $\phi^*_{\textbf{k}}$ are not independent the result is a square root. I don't understand how to compute the integral over two dependent variables.
As I can read here Complex Gaussian integral the result should be without the square root. It seems to me that to have the previous result one should integrate on $d|\phi_\textbf{k}|$ (indeed the presence of $d\phi_\textbf{k}$ is due to a previous step in which the author uses a Dirac delta $\delta^D(k_1+k_2)$ so that $k_2=-k_1$, and rename $k_1$ in $k$).