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An Exactly Solvable Model for Dimension Six Higgs Operators and $h \to γγ$

Aneesh V. Manohar

Abstract

An exactly solvable large $N$ model is constructed which reduces at low energies to the Standard Model plus the dimension six Higgs-gauge operators $g_1^2 H^\dagger H B_{μν} B^{μν}$, $g_2^2 H^\dagger H W^a_{μν} W^{aμν}$, $g_1 g_2 H^\dagger τ^a H W^a_{μν} B^{μν}$, and $ε^{abc} W^a_μ{}^νW^b_ν{}^ρW^c_ρ{}^μ$. All other dimension six operators are suppressed by powers of $1/N$. The Higgs-gauge operators lead to deviations from the Standard Model $h \to γγ$ and $h \to γZ$ rates. A simple variant of the model can be used to also generate the Higgs-gluon operator $g_3^2 H^\dagger H G^A_{μν} G^{Aμν}$ which contributes to the Higgs production rate via gluon fusion.

An Exactly Solvable Model for Dimension Six Higgs Operators and $h \to γγ$

Abstract

An exactly solvable large model is constructed which reduces at low energies to the Standard Model plus the dimension six Higgs-gauge operators , , , and . All other dimension six operators are suppressed by powers of . The Higgs-gauge operators lead to deviations from the Standard Model and rates. A simple variant of the model can be used to also generate the Higgs-gluon operator which contributes to the Higgs production rate via gluon fusion.

Paper Structure

This paper contains 31 equations, 2 figures.

Figures (2)

  • Figure 1: Graphs contributing to the dimension six effective action. The internal lines are $S_\alpha$ scalar fields. The external lines are $\Phi$, $\Psi^a$ and gauge fields.
  • Figure 2: Graph generating the $h \to \gamma \gamma$ amplitude.