Breaking of a local symmetry is impossible, so what about global symmetry....

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SUMMARY

The discussion centers on the impossibility of breaking local symmetry within the context of the Higgs mechanism in quantum field theory. It clarifies that while local gauge symmetry cannot be spontaneously broken, a global symmetry can undergo spontaneous symmetry-breaking after gauge fixing. The conversation references the works of Dominic Else and Greiter, emphasizing that the distinction between local and global symmetry is crucial for understanding the implications of the Higgs mechanism. The participants agree that the local symmetry remains intact, while a global subgroup may exhibit symmetry breaking.

PREREQUISITES
  • Understanding of gauge theory and its implications in quantum field theory.
  • Familiarity with the Higgs mechanism and its role in the Standard Model.
  • Knowledge of spontaneous symmetry breaking (SSB) and its distinction from explicit symmetry breaking.
  • Basic grasp of Noether's theorem and its relation to conserved quantities in field theories.
NEXT STEPS
  • Study the implications of gauge fixing in quantum field theories.
  • Explore the concept of spontaneous symmetry breaking in the context of the Higgs mechanism.
  • Review the differences between local and global symmetries in classical and quantum field theories.
  • Investigate the role of the Z2 lattice gauge theory in understanding ground states and symmetry breaking.
USEFUL FOR

Physicists, particularly those specializing in quantum field theory, particle physics, and theoretical physics, will benefit from this discussion. It is also relevant for students and researchers interested in the nuances of gauge symmetry and the Higgs mechanism.

jakob1111
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Breaking of a local symmetry is impossible. It is often said that therefore the role of the Higgs mechanism in the standard model is a different one.

Namely,

Once a gauge is fixed, however, to remove the redundant degrees of freedom, the remaining (discrete!) global symmetry may undergo spontaneous symmetry-breaking exactly along the lines discussed in the previous chapter. The phrase "spontaneous breaking of local gauge symmetry" is therefore in some sense a misnomer, but a convenient one, if we think of it as a short circumlocution for "spontaneous breaking of remnant global symmetry after removal of redundant gauge degrees of freedom by appropriate gauge fixing".

Or here's a similar statement from a different source:

But is the gauge symmetry actually broken spontaneously? In the above exposition of the Higgs mechanism, there were two instances when a symmetry was broken. First, when we selected one minimum out of infinite amount of equivalent minima, a spontaneous breaking indeed took place, but only of a global symmetry. This minimum represents a vacuum, and in order to perturbatively describe the quantum field theory, we need to quantize the fields. Quantization of gauge field theories requires introduction of a gauge-fixing procedure, and during this procedure we break the gauge symmetry by hand, explicitly, not spontaneously. Thus, the two notions, EWSB and SSB, are in certain sense correct, but they do not refer to the same symmetry. [...] As Englert says in his Nobel lecture [54]: “… The vacuum is no more degenerate and strictly speaking there is no spontaneous symmetry breaking of a local symmetry. The reason why the phase with nonvanishing scalar expectation value is often labeled SSB is that one uses perturbation theory to select at zero coupling with the gauge fields a scalar field configuration from global SSB; but this preferred choice is only a convenient one.

What global symmetry are they referring to? (I find it extremely strange that they don't specify the allegedly broken global symmetry.)
 
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vanhees71 said:
Here is a very nice and simple non-technical explanation:

http://web.physics.ucsb.edu/~d_else/gauge_rant.pdf

Thanks, however the author does not mention that there is actually symmetry breaking. The local symmetry is not and can not be broken. However, a global subgroup of it is actually broken I think, and in this sense there is symmetry breaking in the Higgs mechanism happening.
 
jakob1111 said:
Thanks, however the author does not mention that there is actually symmetry breaking. The local symmetry is not and can not be broken. However, a global subgroup of it is actually broken I think, and in this sense there is symmetry breaking in the Higgs mechanism happening.

Actually I think I agree with the author (who I assume is Dominic Else based on the URL and the similarity to the answer here). In contrast, the Greiter article I posted makes some comments about breaking of global symmetry.

I think the issue is with the very different role "gauge symmetry" plays in classical field theory. In a classical action with gauge invariance, you still have a Noether theorem which gives you some conserved charge. This also implies conservation laws and Ward identities. However, in the quantum gauge theory the actual states in the Hilbert space do not transform under the gauge symmetry (including the "global part" of it). Dominic is correct that the Higgs phase of the Z2 lattice gauge theory has a unique ground state, which clearly cannot be true is there exists a spontaneously broken global symmetry.

In particular, in the gauge-fixed model (the traverse field Ising model), the two ground states of the ordered phase should not be taken to be separate states - the global Z2 symmetry connecting them is not physical.
 

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