A brief introduction to Functional Calculus

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Let be a functional of the functions y(x) and z(x).

Then this functional, S, can be expanded in a Taylor series



Or the finite difference is



where it is understood that we evaluate S using the functions

We can change notation so that and and get



The first variation of S, labeled , which is called the first functional derivative of S, is the linear part of the Taylor expansion, or



and the term with second power in and is called the second variation or second functional derivative, or



and similarly for higher order variations,

And with this notation,




What is ?





But y(x) and z(x) do not depend on one another, so terms like are obviously zero.

And with terms like we have that is a function of x and is independent of y. So they go to zero as well. What is left is



But this last part was exactly how  was defined. So we have

So what is the variation of a composite functional? If , then what is ?

Remember from post 10,



But we know from calculus that,

   and    

So that,





Or,



Now if,



then,




So that,



commutes with

Then,



And keeping only the first approximation linear terms on both sides of the equation,



commutes with

And if



Then





So we see here that commutes with

But also,





Then keeping first approximation linear terms on each side of the equation we see



Or,

Many text use the integral definition of a functional, in its development. I suppose they do this because it makes it easier to justify taking only the linear terms inside the integral since differentials approach zero more naturally in the process of integration.

It's easy to see that variation commutes with any number of integral signs since a difference outside the integral is translated to a difference inside the integral signs. Or,





So following a similar procedure of keeping only linear terms,



This means that the variation of the integration of the path integral gets passed inside all the infinite number of integrations to taking the variation of the exponent of the action.

 

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