The method of dimensional regularization in QFT comes with a few definitions which are crucial to evaluating integrals of this type. Following Zinn-Justin, they are the properties of these integrals under the following:
- Translations:
$$
\int d^d p \, F(p + q) = \int d^d p \, F(p)
$$
- Dilatations:
$$
\int d^d p \, F(\lambda p) = |\lambda|^{-d} \int d^d p \, F(p)
$$
- Factorizations:
$$
\int d^d p \, d^{d'}q \, F(p) G(q) = \left( \int d^d p \, F(p) \right) \left( \int d^{d'}q \, G(q) \right)
$$
From these properties, you can already address some of the integrals you have mentioned. In particular, the first two properties immediately imply the "identity"
$$
\int \frac{d^d p}{(2 \pi)^d} \frac{1}{(p + q)^{2\alpha}} = 0,
$$
for all $d$ and $\alpha$.
In the comments, you have also mentioned the integral
$$
\int_{\mathbb{C}} \frac{d^2 z}{(z - z_i)(\bar{z} - \bar{z}_j)}.
$$
You can consider applying dimensional regularization to this integral, either by introducing multiple copies of $\mathbb{C}$ or writing it as an integral over $\mathbb{R}^2$ and then generalizing to an integration over $\mathbb{R}^d$. You'll find that if $z_j = z_i$, the integral is zero in dimensional regularization, but if $z_j \neq z_i$, I see no reason why it should vanish.