Abstract

We have calculated the $W$-loop contribution to the amplitude of the decay $H\rightarrow Z+\gamma$ in two different methods: 1) in the $R_\xi$-gauge using dimensional regularization (DimReg), and 2) in the unitary gauge through the dispersion method. Using the dispersion method we have followed two approaches: i) without subtraction and ii) with subtraction, the subtraction constant being determined adopting the Goldstone boson equivalence theorem (GBET) at the limit $M_W\to 0$. The results of the calculations in $R_\xi$-gauge with DimReg and the dispersion method with the GBET completely coincide, which shows that DimReg is compatible with the dispersion method obeying the GBET.

Highlights

  • The calculation of the Higgs decay rate into two photons through the W-loop has become the subject of a controversy

  • We have calculated the W-loop contribution to the amplitude of the decay H → Z þ γ in two different methods: (1) in the Rξ-gauge using dimensional regularization (DimReg), and (2) in the unitary gauge through the dispersion method

  • The problem with the dispersion method is that it determines the amplitude merely up to an additive subtraction constant

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Summary

INTRODUCTION

The calculation of the Higgs decay rate into two photons through the W-loop has become the subject of a controversy. Responding to a criticism, [7], which points out that the delicate cancellation of divergences is ambiguous and one needs a regularization, the result of [5] was confirmed in [8] by applying unsubtracted dispersion relations in a calculation that deals only with absolutely convergent integrals. Before we go into the details it shall be mentioned that in this study we have used a couple of helpful Mathematica packages, [18,19,20,21,22,23]

THE FEYNMAN DIAGRAMS
ABSORPTIVE PART OF THE AMPLITUDE
REAL PART OF THE AMPLITUDE
The charged ghost contribution and the constant CðaÞ
CONCLUDING REMARKS
D1D2D3
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