Abstract

In the production of the Higgs through a bottom-quark loop, the transverse momentum distribution of the Higgs at large $P_T$ is complicated by its dependence on two other important scales: the bottom quark mass $m_b$ and the Higgs mass $m_H$. A strategy for simplifying the calculation of the cross section at large $P_T$ is to calculate only the leading terms in its expansion in $m_b^2/P_T^2$. In this paper, we consider the bottom-quark-loop contribution to the parton process $q\bar{q}\to H+g$ at leading order in $\alpha_s$. We show that the leading power of $1/P_T^2$ can be expressed in the form of a factorization formula that separates the large scale $P_T$ from the scale of the masses. All the dependence on $m_b$ and $m_H$ can be factorized into a distribution amplitude for $b \bar b$ in the Higgs, a distribution amplitude for $b \bar b$ in a real gluon, and an endpoint contribution. The factorization formula can be used to organize the calculation of the leading terms in the expansion in $m_b^2/P_T^2$ so that every calculation involves at most two scales.

Highlights

  • The discovery of the Higgs boson in the year 2012 completed the Standard Model (SM) of particle physics [1,2]

  • In Ref. [42], we showed that the top-quark-loop contribution to the LP form factor for gà → H þ g at leading order (LO) can be expressed in terms of a factorization formula that separates the hard scale Q from the masses mt and mH

  • We applied factorization methods developed for QCD to the amplitude for Higgs production at large transverse momentum through a bottom-quark loop

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Summary

INTRODUCTION

The discovery of the Higgs boson in the year 2012 completed the Standard Model (SM) of particle physics [1,2]. Since the high-lminosity LHC may be able to measure the Higgs PT distribution with a few percent accuracy, it is important to understand the bottom-quark-loop contribution to the same level of precision This requires calculating the process to higher orders in αs and resumming large logarithms to all orders. The mb → 0 limit can be calculated by solving the differential equations for master integrals in this limit [7] This method has been used by Mueller and Öztürk to calculate bottom-quark-loop contributions to the inclusive cross section for Higgs production to NLO [7]. The bottom-quark-loop contribution to the matrix elements for gq → H þ q and gq → H þ qat LO can be expressed in terms of the same function F as the form factor for qq → H þ g but with the positive Mandelstam variable sreplaced by a negative Mandelstam variablet. If the form factor F for qq → H þ g is expressed in terms of the complex variable sþ iε, it can be applied to gq → H þ q and gq → H þ qby analytic continuation

LP form factor pffiffi
Leading-power regions
Factorization formula
REGULARIZED FACTORIZATION FORMULA
Rapidity regularization and zero-bin subtraction
Hard contribution
Higgs collinear contribution
Gluon collinear contribution
Soft contribution
LP form factor
RENORMALIZED FACTORIZATION FORMULA
Improved mass dependence
COMPARISON WITH FULL FORM FACTOR
Findings
SUMMARY AND OUTLOOK
Full Text
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