An oscillatory phase is a real-valued Φ(t,x)\Phi(t,x) appearing in a factor eiκΦ(t,x)e^{i\kappa\Phi(t,x)}, with a fixed nonzero frequency parameter κ\kappa. Smooth phases permit differentiation by the chain rule. The exponential depends on κΦ\kappa\Phi modulo 2π2\pi.

Locally defined phases

On a periodic domain the exponential can be globally defined even when a real-valued phase exists only in local charts. Two local phases give the same exponential on an overlap if their difference lies in (2π/κ)Z(2\pi/\kappa)\mathbb Z. For continuous lifts on a connected overlap this integer difference is constant.

is a separate composition operation. Averaging in independent auxiliary variables before this composition need not equal averaging the composed physical field.