disregardthat said:
I don't think there's many physicists with disdain for advanced mathematics that come up with breaktroughs in theoretical physics.
"If all mathematics disappeared, it would set physics back precisely one week."-Feynman
To paraphrase Einstein (i can't find the original quote), "General relativity became unrecognizable after the mathematicians got their hands on it.", implying that he was not particularly fond of (or perhaps just not clever enough to understand) pure mathematics.
A cursory glance at the modern theoretical physics literature would probably further help you to disabuse yourself of this absurd notion. Beware of citing articles in string theory or topological matter, for instance, since neither of these fields constitute breakthroughs yet.
This article does indeed sum up a few of my complaints with mathematics.
What I mean is that not every path integral defines a quantum theory. We only accept a path integral theory as a quantum theory if it has an equivalent Hilbert space (or C* algebra) formulation. If one could write a path integral formulation of a quantum theory which has no Hilbert space formulation, then one can say that the path integral formulation is more fundamental. At this stage, since the Hilbert space formulation is needed to define an acceptable path integral quantum theory, the Hilbert space formulation is more fundamenta
This conception of a quantum theory is so ludicrous that I can only conclude that a mathematician came up with it and not a physicist. It is a definition munged from the Platonist's world view and not from those who just want to figure out how the world works.
But for fermions, the variables are not classical variables, they are Grassmann numbers, and the integral is a brand new object called the Berezin integral. So I would like to know why you think this is more intuitive than the "abstract" Hilbert space formalism. It's abstract enough that Feynman was not able to derive the path integral for fermions.
For field theory the path integral formalism becomes murkier and more difficult to grasp. But it retains its key advantages, such as the fact that it handles Lorentz invariance with much greater ease than the canonical formalism. The fundamental intuitive picture, best communicated in terms of particles, remains elegant, as does the least action principle.
As for the complexity of the mathematical objects involved, my own experience of the Berezin integral and Grassman variables is that the former is barely remarked upon in field theory texts (it is not usually given that name) and important integrals are computed very intuitively; in the latter case, the relevance of Grassman variables is challenging to communicate but the rules which govern them are hardly sophisticated. I would even argue that the canonical formalism is really not that sophisticated as far as pure mathematics is concerned, it's just very slightly more abstract.
Incidentally, it has been conjectured that some quantum theories have no Lagrangian formulation - I don't understand this work at all - just thought I'd bring it up in case someone can explain it.
A reasonable way to define a quantum field theory would be one which actually describes nature. None of the theories you described actually describe nature, so far as we know. Therefore, I am unsure why anybody would be impressed by the fact that they might not admit themselves to a Lagrangian formulation; this may merely be an artifact of faulty assumptions about nature.
Of course if they could compute interesting experimental results, that would make it very interesting indeed!