Quantum numbers of a field acquiring vacuum expectation value

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SUMMARY

The discussion centers on the requirement for fields acquiring vacuum expectation values (v.e.v.) to maintain the same quantum numbers as the vacuum, particularly in the context of the Standard Model. It asserts that symmetries such as local Lorentz invariance and neutrality must be preserved when introducing these fields. The conversation highlights that while scalar mesons, like pions, are compatible with these symmetries, vector mesons pose a challenge as their existence could imply a violation of Lorentz invariance due to potential symmetry-breaking. This leads to the conclusion that only scalar mesons should exist under these constraints.

PREREQUISITES
  • Understanding of vacuum expectation values (v.e.v.) in quantum field theory
  • Familiarity with the Standard Model of particle physics
  • Knowledge of Lorentz invariance and its implications
  • Basic concepts of scalar and vector mesons
NEXT STEPS
  • Research the role of vacuum expectation values in quantum field theory
  • Study the implications of Lorentz invariance in particle physics
  • Explore the properties and classifications of scalar and vector mesons
  • Investigate symmetry-breaking mechanisms in the Standard Model
USEFUL FOR

This discussion is beneficial for theoretical physicists, particle physicists, and students studying quantum field theory, particularly those interested in the implications of symmetries and vacuum states in the Standard Model.

krishna mohan
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Why should symmetries require a field that acquires vacuum expectation value to have the same quantum numbers as the vacuum? Please give me a reference also..if possible...
 
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If the vacuum (without the v.e.v. of the field) has certain symmetries dictated be observation, such as local Lorentz invariance and lack of electric charge, then the presence of the field v.e.v. should not ruin these properties. Otherwise you wouldn't have demanded those symmetries of the original vacuum. That's why condensations of neutral scalars and neutral, Lorentz-scalar groupings of fermions are allowed in the Standard Model.
 
javierR said:
That's why condensations of neutral scalars and neutral, Lorentz-scalar groupings of fermions are allowed in the Standard Model.

So how does one explain the vector meson?

Scalar mesons, such as the pion, are condensations of a colorless, Lorentz-invariant, quark/antiquark composite fields.

If there is a similar condensation (i.e., symmetry-breaking) that leads to a vector meson, then Lorentz-invariance would be broken.

So it seems that only scalar mesons should exist, and vector mesons violate Lorentz invariance because they would spontaneously break it?
 

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