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It works heuristically, but not necessarily mathematically.atyy said:Why does the wrong derivation work (I think I've read that it reproduces the right derivation term by term)?
Being constructively inclined, I prefer those other methods, i.e. a non-perturbative analysis. I would even go as far to say that mathematically speaking a non-perturbative analysis is necessary in order to prove existence at all since perturbation theory is known to break down for many classes of problems, including many which are asymptotic, not convergent.DarMM said:You just can't use that expansion method directly in the continuum. If you want to prove the relation directly in the continuum there are other methods but they are much more mathematically involved.
The failure of those doing the perturbative expansion is then essentially caused by them not realizing that they are expanding the power series by assuming ad hoc that the independent variable is fixed purely in order to be able to make an empirical comparison i.e. making a mathematically illegitimate assumption which is in a specific sense completely independent of experiment!
The 'some theories' for which this can be proved require both linearity of the space of solutions as well as linearity of the equations; if one or both of these assumptions fail, then perturbation theory - beyond an initial small semi-accurate range of validity - will quickly fail once the independent variables aren't ad hoc assumed to be fixed anymore. In this sense, perturbation theory is obviously just a more sophisticated version of a heuristic technique such as the small angle approximation.DarMM said:There is one side effect of the fact that they are disjoint that shows up when using the free theory to compute the terms. The need to renormalize the terms.
The perturbative series ends up being only asymptotic of course, not convergent. Though that happens in NRQM as well. In lower dimensions for some theories you can use the Borel transform to sum the series and thus existence of the interacting theory can be proved directly from perturbation theory.
In 4D but also for Yang Mills in lower dimensions there are poles in the Borel plane preventing resummation. The poles mean one has to take a contour around them to obtain the interacting theory, but there are infinite such contours introducing an ambiguity of order ##\mathcal{O}\left(e^{-\frac{1}{\lambda}}\right)##.
