Symmetry breaking and the ground state of a quantum field theory.

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Discussion Overview

The discussion revolves around the concept of symmetry breaking in quantum field theory, particularly focusing on the implications for ground states and the stability of these states under perturbations. Participants explore the nature of different ground states, the role of Goldstone bosons, and the distinctions between true symmetries and gauge symmetries.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant questions why the ground state does not change with slight perturbations, suggesting that the production of Goldstone bosons could lead to different ground states.
  • Another participant emphasizes the need to differentiate between true symmetries and gauge symmetries, stating that only true symmetry breaking leads to multiple ground states.
  • Concerns are raised about the stability of different vacuum expectation values (vevs) and their implications for the naturalness and triviality of certain theories.
  • Some participants suggest that the stability of ground states is influenced by macroscopic scale symmetry breaking, while local experiments may not fully capture this effect.

Areas of Agreement / Disagreement

Participants express differing views on the nature of symmetry breaking, particularly regarding the distinction between true and gauge symmetries. There is no consensus on the implications of these distinctions for ground state stability and the behavior of vevs.

Contextual Notes

The discussion includes assumptions about the definitions of true and gauge symmetries, as well as the implications of vacuum stability, which remain unresolved.

alemsalem
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when a continuous symmetry is broken, we say that the ground state is just one of the possible ground states, and there is no energy cost in moving from one to the other..
why doesn't the state keep changing with the slightest perturbation (production of goldstone boson).
why don't we have a different ground state every time we do an experiment.
and what if we had different possible ground states that are not symmetric (but equal in energy),, then every time we have a phase transition we could get a field with a different mass.

sorry for the question being unclear, I barely understand this.
thanks!
 
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To begin with I think one should differentiate whether the symmetry broken is a "true" symmetry or merely a gauge symmetry.
I the latter case, there is only but one ground state.
In the first case (e.g. broken rotational symmetry in a magnet or broken translational symmetry in a crystal) there are different ground states which owe their stability to the ground state being broken on a macroscopic scale, while all (or most ) of the experiments we are doing only act locally.
 
Different vacuum expectation values (vevs) may disrupt the vacuum stability. One can not choose arbitrary or multiple vevs. that's the reason why some theories (ex:Technicolor) have been discredited. Furthermore, it may effect the naturalness and triviality of your theory.
 
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