Undergrad Why do we require locality in quantum field theory?

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Locality in quantum field theory (QFT) requires that the Lagrangian density is a functional of fields and a finite number of their derivatives at a single spacetime point, ensuring that the physical state at that point depends only on its immediate surroundings. This principle prevents direct interactions between fields at different spacetime points, avoiding action at a distance and maintaining causality. The cluster decomposition property supports this by allowing fields to be prepared independently at spacelike points. Local interactions and causal commutation relations are essential for ensuring relativistic consistency in QFT predictions. Ultimately, locality is crucial for constructing theories that align with both intuition and empirical observations.
  • #31
vanhees71 said:
I think what Schwartz discusses there is the realization of an Abelian massive vector field as a gauge field. This is a remarkable model, because it shows that in the Abelian case, i.e., gauge group U(1), you can formulate a gauge-symmetric renormalizable model with massive gauge bosons without the Higgs mechanism. This construct does not work for the non-Abelian case. There you need the Higgs mechanism to consistently describe massive gauge bosons and/or fermions for chiral gauge groups as in the electroweak sector of the Standard Model.
Would this also be true for a non-compact gauge group?
 
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  • #32
Non-compact gauge groups are pretty evil. The prime example for that is the notorious trouble the quantization of gravity (general relativity) provides. For the mathematical reasons, why for the local gauge symmetry we have to assume compact semisimple gauge groups (or direct products of such groups and U(1)'s as in the Standard Model), see Weinberg, Quantum Theory of Fields, vol. 2, Sect. 15.2.
 

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