Gedanken Worlds without Higgs: QCD-Induced Electroweak Symmetry Breaking
Chris Quigg, Robert Shrock

TL;DR
This paper explores toy models where electroweak symmetry breaking arises solely from QCD dynamics without Higgs fields, offering insights into alternative mechanisms and their implications for particle physics.
Contribution
It introduces and analyzes Higgs-free models with various gauge symmetries where QCD induces electroweak symmetry breaking, providing new perspectives on symmetry breaking mechanisms.
Findings
QCD can induce electroweak symmetry breaking in Higgsless models
Models show the weak interaction strength can be comparable to strong interactions
Insights into field theory applications without Higgs fields
Abstract
To illuminate how electroweak symmetry breaking shapes the physical world, we investigate toy models in which no Higgs fields or other constructs are introduced to induce spontaneous symmetry breaking. Two models incorporate the standard SU(3)_c x SU(2)_L x U(1)_Y gauge symmetry and fermion content similar to that of the standard model. The first class--like the standard electroweak theory--contains no bare mass terms, so the spontaneous breaking of chiral symmetry within quantum chromodynamics is the only source of electroweak symmetry breaking. The second class adds bare fermion masses sufficiently small that QCD remains the dominant source of electroweak symmetry breaking and the model can serve as a well-behaved low-energy effective field theory to energies somewhat above the hadronic scale. A third class of models is based on the left-right--symmetric SU(3)_c x SU(2)_L x SU(2)_R x…
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