Quantum loop effects amplify the effective binding force in top quark condensation, allowing a weaker new force to produce the observed Higgs boson with a composite scale near 6 TeV.
Quantum Aspects of Natural Top Quark Condensation
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abstract
In top quark condensation the Brout-Englert-Higgs (BEH) boson is a $\bar{t}t$ bound state. With a UV completion of a single coloron exchange interaction, a recent semiclassical treatment gave a novel theory of the BEH boson as an extended object with composite scale $M_0\sim 6$ TeV. Presently we obtain the semiclassical theory as an effective action, using the source/Legendre transformation techniques of Jackiw, \etal, and fermion loop effects in the large-$N_c$ limit by deploying an auxiliary field to implement the sum of leading fermion loop diagrams. The theory remains natural at the loop level, with fine tuning at the level of a few \%, and the effective coupling of the 4-fermion interaction, $\bar{g}_0^2$, is significantly enhanced by quantum loops over the fundamental coloron coupling, $g_0^2$. Hence a relatively weaker ``topcolor'' theory can produce critical coupling in the effective BEH bound state theory.
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Quantum Aspects of Natural Top Quark Condensation
Quantum loop effects amplify the effective binding force in top quark condensation, allowing a weaker new force to produce the observed Higgs boson with a composite scale near 6 TeV.