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The Little Higgs from a Simple Group

David E. Kaplan, Martin Schmaltz

Abstract

We present a model of electroweak symmetry breaking in which the Higgs boson is a pseudo-Nambu-Goldstone boson. By embedding the standard model SU(2) x U(1) into an SU(4) x U(1) gauge group, one-loop quadratic divergences to the Higgs mass from gauge and top loops are canceled automatically with the minimal particle content. The potential contains a Higgs quartic coupling which does not introduce one-loop quadratic divergences. Our theory is weakly coupled at the electroweak scale, it has new weakly coupled particles at the TeV scale and a cutoff above 10 TeV, all without fine tuning. We discuss the spectrum of the model and estimate the constraints from electroweak precision measurements.

The Little Higgs from a Simple Group

Abstract

We present a model of electroweak symmetry breaking in which the Higgs boson is a pseudo-Nambu-Goldstone boson. By embedding the standard model SU(2) x U(1) into an SU(4) x U(1) gauge group, one-loop quadratic divergences to the Higgs mass from gauge and top loops are canceled automatically with the minimal particle content. The potential contains a Higgs quartic coupling which does not introduce one-loop quadratic divergences. Our theory is weakly coupled at the electroweak scale, it has new weakly coupled particles at the TeV scale and a cutoff above 10 TeV, all without fine tuning. We discuss the spectrum of the model and estimate the constraints from electroweak precision measurements.

Paper Structure

This paper contains 11 sections, 56 equations, 5 figures.

Figures (5)

  • Figure 1: Quadratically divergent contributions to the Higgs mass in the Standard model: top loop, $SU(2)\times U(1)$ gauge boson loops and Higgs loop.
  • Figure 2: $SU(3)$ gauge boson loop corrections to the ${\bf \Phi}$ mass.
  • Figure 3: Gauge boson contributions to the ${\bf \Phi}$ potential in $\partial_\mu A^\mu =0$ gauge.
  • Figure 4: The top loop contribution to the Higgs mass in sigma model formalism.
  • Figure 5: The canceling top and $\chi$-loops in component form.