In this paper we develop a theory for oscillatory integrals with complex
phases. When , we evaluate this phase function
on the basic character of ${\mathbb
C} \simeq {\mathbb R}^2z = x+iy \in {\mathbb C}z = (x,y) \in
{\mathbb R}^2$ I \ =
\int_{{\mathbb C}^n} {\rm e}(f({\underline{z}})) , \phi({\underline{z}}) ,
d{\underline{z}} $\phi \in C^{\infty}_c({\mathbb C}^n)$.
Unfortunately basic scale-invariant bounds for the oscillatory integrals
do not hold in the generality that they do in the real setting. Our main effort
is to develop a perspective and arguments to locate scale-invariant bounds in
(necessarily) less generality than we are accustomed to in the real setting.

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