Understanding the GUT Scale: Merging Fundamental Forces at High Energies

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SUMMARY

The discussion centers on the Grand Unified Theory (GUT) scale, specifically the merging of fundamental forces at high energies. Participants clarify that while all forces may exhibit equal strength at high energies, this does not imply they are the same force. The electroweak force serves as a prime example, where the SU(2) symmetry breaks into distinct phenomena at lower energies, resulting in W± bosons and photons. The conversation emphasizes the importance of understanding electroweak symmetry breaking and the implications of unbroken SU(2) and U(1) forces.

PREREQUISITES
  • Understanding of fundamental forces in physics
  • Familiarity with electroweak theory and SU(2) symmetry
  • Knowledge of high-energy physics concepts
  • Basic comprehension of particle physics terminology
NEXT STEPS
  • Research the implications of electroweak symmetry breaking in particle physics
  • Study the characteristics of unbroken SU(2) and U(1) forces
  • Explore the concept of Grand Unified Theories (GUTs) in high-energy physics
  • Examine the role of W± bosons and their interactions in the Standard Model
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Physicists, students of particle physics, and anyone interested in the unification of fundamental forces and high-energy theoretical frameworks.

nolxiii
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So I've heard it talked about how how at high energies all the strength of all fundamental forces are expected to merge together to single force, but don't quite get how you get from "all the forces have the same strength at high energies" to "all the forces are really the same force."

Couldn't they have the same strength but still act differently? And if they acted the same at high energies wouldn't their behavior at low energies still differentiate them into separate phenomenon?
 
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nolxiii said:
So I've heard it talked about how how at high energies all the strength of all fundamental forces are expected to merge together to single force, but don't quite get how you get from "all the forces have the same strength at high energies" to "all the forces are really the same force."

You are right, it does not follow. It's just a "maybe", a hint from the data that maybe it's one force.

And if they acted the same at high energies wouldn't their behavior at low energies still differentiate them into separate phenomenon?

We have an example. Electroweak SU(2) force is one force, but at low energies it "breaks" into two seemingly completely different things: W+- bosons are quite different from that part of SU(2) which is part of photons.
 
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Right on. Still struggling somewhat to build a mental model of how the electroweak symmetry breaking works, the link below I think helped a bit though. Am I understanding this right that if the symmetry just happened to break in such a way that W bosons were (nearly?) massless that the weak and electromagnetic forces would still behave more or less identically?

http://hyperphysics.phy-astr.gsu.edu/hbase/Forces/unify.html
 
An unbroken SU(2) force would not be identical to electromagnetism.
An unbroken U(1) force is identical to electromagnetism.
 
nikkkom said:
An unbroken SU(2) force would not be identical to electromagnetism.
An unbroken U(1) force is identical to electromagnetism.

what would this unbroken SU(2) force look like?
 
It would be a long-range force, IIRC attractive for any SU(2) charges (unlike electricity, where like charges repel).
 

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