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A. Neumaier
A. Neumaier is offline
Feb28-12, 10:44 AM
Sci Advisor
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Quote Quote by rubbergnome View Post
Hello everyone. I have a question regarding algebraic QFT. I read that, in order to avoid ill-defined, divergent expressions like the mode expansions for spacetime-dependent field operators φ(x), one starts from the (Wightman?) axioms, using operator-valued distribution on compact support functions, φ(f), instead. Formally this is achieved by integrating the product f(x)φ(x) which results in a smearing that encodes the uncertainty in spacetime position. This is, I think, to avoid having arbitrairly high frequency modes in the mode expansion in terms of annihilation-creation operators.

The question is: why many people use the spacetime-dependence formalism anyway? Is that because:

1) it's operationally simpler
2) experiments give extremely accurate results anyway
3) renormalization takes care of every divergence
4a) phycisists don't bother that much with quantum fields being well-defined, or
4b) the φ(x) formalism is actually well-defined, and AQFT just wants to better formalize the theory

? I'm confused, because I rarely see people using the algebraic formalism.
All of 1) through 4a). The smeared version is needed only when you want to impose some rigor on what is done, as the field operators are distributions only, so its value at a spacetime point is typically not defined. But the extra baggage in the formulas is of no significant help in actual computations, so most people avoid it.