Electroweak symmetry breaking without a Higgs

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Discussion Overview

The discussion revolves around a paper by John Moffat proposing a non-local, finite quantum field theory (QFT) that aims to explain electroweak symmetry breaking without the Higgs mechanism. The scope includes theoretical implications, potential experimental evidence at the LHC, and comparisons with existing models such as supersymmetry (SUSY) and technicolor theories.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants suggest that if Moffat's theory holds and the LHC does not find Higgs or top quark condensates, it could lead to significant new research directions.
  • Others argue that the theory is parsimonious, as it only requires the existence of already discovered Standard Model particles, although dark matter remains unexplained.
  • It is noted that the theory undermines a central argument for SUSY related to the hierarchy problem, potentially providing indirect support for new theories.
  • Some participants express that the theory might enhance the prospects for loop quantum gravity (LQG) and preon ribbon models.
  • Concerns are raised regarding the non-locality of the theory, which some view as contrived and problematic.
  • Participants emphasize the importance of having well-motivated theories that respect fundamental symmetries and avoid excessive fine-tuning.
  • Historical context is provided regarding Moffat's previous theories, such as non-symmetric gravitational theory, which faced inconsistencies with established theories.

Areas of Agreement / Disagreement

Participants express a mix of support and skepticism regarding Moffat's theory. While some see potential in its implications, others raise concerns about its non-locality and historical inconsistencies, indicating that the discussion remains unresolved with multiple competing views.

Contextual Notes

Limitations include the theory's reliance on experimental outcomes that have yet to be observed, as well as the challenges posed by its non-local nature and the historical context of Moffat's previous work.

A/4
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Interesting new paper from John Moffat:

http://arxiv.org/abs/0709.4269

Introduces a non-local, finite QFT that dynamically generates boson and fermion masses as loop corrections. Experimental evidence for the theory will be visible in WW scattering at the LHC (coupling goes to zero, which is distinct from various other models with Higgs fields).

Comments?
 
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A/4 said:
Interesting new paper from John Moffat:

http://arxiv.org/abs/0709.4269

Introduces a non-local, finite QFT that dynamically generates boson and fermion masses as loop corrections. Experimental evidence for the theory will be visible in WW scattering at the LHC (coupling goes to zero, which is distinct from various other models with Higgs fields).

Comments?

1- if this paper holds, and if LHC/TEV does NOT find higgs/top quark condensates/technicolor, it will be an impressive first paper in new research directions,
2- it is very parsimonious in that only the already discovered SM particles "exist" although DM remains a mystery. SUSY doubles the # of particles.
3- it undermines a central argument for SUSY (the hierarchy problem), providing indirect support for NEW/TWP
4- it might provide a big boost to LQG preon ribbon style particle physics.

If LHC/TEV does NOT find higgs/top quark condensates/technicolor, and LHC does find WW scattering in according with his predictions, I think he deserves a nobel prize in physics.
 
ensabah6 said:
1- if this paper holds, and if LHC/TEV does NOT find higgs/top quark condensates/technicolor, it will be an impressive first paper in new research directions,
2- it is very parsimonious in that only the already discovered SM particles "exist" although DM remains a mystery. SUSY doubles the # of particles.
3- it undermines a central argument for SUSY (the hierarchy problem), providing indirect support for NEW/TWP
4- it might provide a big boost to LQG preon ribbon style particle physics.

If LHC/TEV does NOT find higgs/top quark condensates/technicolor, and LHC does find WW scattering in according with his predictions, I think he deserves a nobel prize in physics.

Vis-a-vis points 2 and 3, Moffat has historically omitted orthodox predictions in his theories. In certain ways, this is a plus: simplicity is better than complexity. Why have a model that predicts more particles than we have observed? It's a bold move to address the elephant in the room: what if we see nothing out of the LHC?

But, in other ways it creates more problems than it solves. In the 80s and 90s, he was promoting a non-symmetric gravitational theory (NGT), which posited a spacetime metric with off-diagonal terms. Some of the novel predictions included dipole gravitational radiation. Although it encompassed GR in its formulation, it was obviously inconsistent with other theories that required a symmetric metric. I can't remember what the resolution was to this, but it seems that NGT has since faded away.
 
It breaks locality though, so its rather contrived.

In general in phenemonology, people like to have a

1) Well motivated theory (in the sense that there's something more fundamental behind it, or is utilized to solve a particular problem -eg hierarchy)
2) Simple model (so no extra random particles that don't have much use other than to clutter up things)
3) Respect for the usual symmetries and analytic conditions (Gauge invariance, Lorentz invariance, unitarity, etc etc)
4) Natural. In the sense that there's not too much finetunning.

Unfortunately its very rare to find new models that respect those conditions, so people usually relax one or more of the conditions above. But be sure that each such new model tends to be seen as problematic and unlikely.
 

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