quantum field theory - Understanding Measure in Path integrals

I know this is still a current topic of study, so my question is less about mathematical underpinnings, and more about the transition from the "sum-over-all-possible-intermediate-points" measure $$\mathcal{Dx} = \lim_{N\to\infty} \prod_{i=0}^{N} dx_{i}$$

to the "sum-over-all-possible-field-configurations" measure found in the non-abelian partition function for Yang-Mills, which I've been told has the form:

$$\mathcal{D}[A] = \lim_{N\to\infty} \prod_{i=0}^{N} \prod_{\mu=0}^{3} \prod_{c=0}^{N_{c}} dA_{\mu}^{c}(x_i) $$

where $N_{c}$ is the is the dimension of gauge group. The relevant passages I found in Peskin and Schroeder glossed over the topic. (p.294 Eq. (9.50) begins the discussion, but it is for Abelian groups, where I imagine we can treat each component of Aμ as a scalar field, so the product makes sense to me (and the color product isn't present of course). I've yet to find a proper expansion/derivation of the same measure for non-abelian gauge configurations. There seems to be a brief mention of the functional integral measure around p. 665 Eq. (19.67) as well, but not quite what I'm looking to understand.)

Answer

Forget about gauge fields. Consider a scalar field $\phi:V\subseteq \mathbb{R}^4\to \mathbb{R}$ for simplicity. The relevant equation in Peskin & Schroeder is instead $$ {\cal D}\phi ~=~\prod_i d\phi(x_i). \tag{9.20}$$ Here $x_i$ is a point of a square lattice with a lattice spacing $\epsilon$, and $i$ runs over all lattice points. In other words, the discretized path integral measure is $$ {\cal D}\phi~=~\prod_{n\in \mathbb{Z}^4}^{\epsilon n\in V} d\phi(\epsilon n). \tag{9.20'}$$ Does this help? Ultimately, we are interested in the continuum limit $\epsilon\to 0^+$.