This question is not so much related to the physics as it is the integral itself. In terms of the canonical coherent states, $|z\rangle$, one encounters a resolution of the identity of the form:
$$\hat{I}=\displaystyle\int \dfrac{d^2z}{\pi} |z\rangle\langle{z}|$$
Where the integral is taken over the entire complex plane. My question is, often this is re-expressed in the forms:
$$\displaystyle\int \dfrac{dzd\bar{z}}{2\pi i}|z\rangle\langle{z}|$$
$$\displaystyle\int \dfrac{dxdy}{\pi} |z\rangle\langle{z}| \qquad \text{where } x=\Re z, \ y=\Im z$$
How does one show that the $z-\bar{z}$ integral is equivalent to $x-y$ integral? How does one show that either of these are equivalent to the original integral? I presume this has something to do with the properties of differential forms inducing the area element but I'm unsure how to formulate these in terms of differential forms (and back again) in the first place.
For instance, it's clear to me that IF I assume that I can assume a correspondence of the form:
$$\int dzd\bar{z} = \int dz \wedge d\bar{z}$$
Then I could use the standard properties of the exterior product to come to the relation $dz \wedge d\bar{z} = -2idx \wedge dy$. Whilst close, this is still not quite right even if one were to use the above unjustified correspondence to return to the element $dxdy$. I presume this issue is related to orientation, but I have yet to see a satisfactory explanation for what's going on here.
How does one relate the area element $dzd\bar{z}$ to the differential 2-form $dz\wedge d\bar{z}$ in the context of the integral? Why is this a valid step to take?
Thanks in advance!