Physics often deals with classical models where the dynamical variables are a collection of functions {ÃÂ<sup>ñ</sup>}<sub>ñ</sub> over a d-dimensional space/spacetime manifold M where ñ is the "flavor" index. This involves functionals over the ÃÂs, functional derivatives, functional integrals, etc. From a functional point of view this is equivalent to working with an infinite-dimensional smooth manifold where its points are an assignment of a function for each ñ, and the procedure is in analogy with differential geometry where the coordinates for a point x of the manifold M are ÃÂ<sup>ñ</sup>(x).
In the DeWitt notation (named after theoretical physicist Bryce DeWitt), ÃÂ<sup>ñ</sup>(x) is written as ÃÂ<sup>i</sup> where i is now understood as an index covering both ñ and x.
So, given a smooth functional A, A<sub>,i</sub> stands for the functional derivative
as a functional of ÃÂ. In other words, a "1-form" field over the infinite dimensional "functional manifold".
In integrals, the Einstein summation convention is used. Alternatively,