Can electro-weak unification be tested at CERN?

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SUMMARY

The discussion centers on the potential for testing electroweak unification at CERN's Large Hadron Collider (LHC). It highlights that the LHC operates above the energy threshold necessary for electroweak unification but has not yet provided evidence for massless right and left-handed electrons, or the three massless W bosons and the massless B boson. The conversation also clarifies that unification involves a set of forces described by a single set of equations, and the electroweak phase transition occurs at energy levels above 100 TeV, which the LHC cannot achieve. The complexities of weak and electromagnetic interactions are discussed, emphasizing the need for advanced theoretical frameworks like the Weinberg-Salam theory.

PREREQUISITES
  • Understanding of electroweak interaction and symmetry breaking
  • Familiarity with the Large Hadron Collider (LHC) and its operational energy levels
  • Knowledge of Weinberg-Salam theory and its implications for particle physics
  • Basic concepts of quantum electrodynamics (QED) and weak force interactions
NEXT STEPS
  • Research the implications of the electroweak phase transition in high-energy physics
  • Study the details of Weinberg-Salam theory and its application in particle interactions
  • Explore the role of the LHC in testing theories of particle physics at high energies
  • Investigate the significance of massless particles in the context of quantum field theory
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Physicists, researchers in particle physics, and students interested in the fundamental forces of nature and their unification theories.

Carlos L. Janer
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1.- Electroweak interaction broke its symmetry about 1ps after the Big Bang and two different types of interactions appeared: weak interactions and electrodynamics.

2.- The LHC at Geneva is routinely conducting experiments above the energy threshold of electroweak unification. Could these experiments reproduce (at a very small scale) the state the Universe was at 1ps after the Big Bang?

3.- If so, have they foud any evidence of the massless right and left handed electrons? Have the found any evidence of the three massless W bosons and the massless B boson?

4.- If not, can they? After all, there are no such fields in our frozen Universe. How could all these particles exist without the corresponding vacuum fields from which they could be brought into existence?
 
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Unification doesn't work this way. What unification means is that there is a set of forces (electromagnetic and weak) that can be described by a single set of equations with a single strength. This has been shown to be the case at many times and places, perhaps most elegantly by Hera:

electroweak_unification.jpg


At low energies, there appear to be two different forces with two different strengths (the red and the blue), but at high energies they come together. That's unification.

You seem to be talking about the electroweak phase transition, which happens at a very high temperature (probablly above 100 TeV) and it is a many-body problem. So not only does each individual particle need a lot more energy that the LHC can produce, you need a lot of them.
 
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Carlos L. Janer said:
3.- If so, have they foud any evidence of the massless right and left handed electrons? Have the found any evidence of the three massless W bosons and the massless B boson?

Isn't that the Goldstone boson equivalence theorem?
 
Vanadium 50: I'm not sure if I understood you well. Do you mean that 'weak and electromagnetic interaction unification energy' roughly means that you need to use Weinberg's-Salam theory to achieve accurate results? and at much lower energies you could just use QED and Fermi's model?
Vanadium 50: Did you also mean that 'electroweak phase transition energy' is the energy scale at which QED and weak force running coupling contants merge?
 
Vanadium 50 doesn't seem to be available at the moment. Could anybody tell me if what I understood from his explanation is, at least, a rough simplification of what he actually said? I'm not even a physicist and even a crude aproximation would do for me.
 
Carlos L. Janer said:
Did you also mean that 'electroweak phase transition energy' is the energy scale at which QED and weak force running coupling contants merge?

Current theory says that there is no "QED force" at all. There are two weak forces, one is due to weak isospin SU(2) symmetry, another is due to weak hypercharge U(1) symmetry. These forces have coupling constants g2 and g1. "QED force" is due to existence of linear combination of SU(2) and U(1) generators which leaves our vacuum invariant. This linear combination generates (another) U(1) group. Its coupling constant, "fine structure constant" is 1/4pi * (g1*g2)^2/(g1^2 + g2^2).

Thus, "QED and weak force running coupling contants merge" doesn't even make sense, really.

The transition energy is the energy above which masses of W and Z bosons are insignificant. At those energies, seeing QED/weak interactions as exchange of W+-,Z,gamma bosons is not a useful description. It would be simpler to see it as exchange of W1,W2,W3 and B bosons of original, unbroken symmetries.
 
Carlos L. Janer said:
Vanadium 50: I'm not sure if I understood you well. Do you mean that 'weak and electromagnetic interaction unification energy' roughly means that you need to use Weinberg's-Salam theory to achieve accurate results? and at much lower energies you could just use QED and Fermi's model?
Vanadium 50: Did you also mean that 'electroweak phase transition energy' is the energy scale at which QED and weak force running coupling contants merge?
I cannot read minds, but I guess he meant something like that.
 
Thank you for your interest, mfb!
 

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