On the interference of and Higgs production mechanisms and the determination of charm Yukawa coupling at the LHC
arXiv:2102.04242 · doi:10.1007/JHEP06(2021)107
Abstract
Higgs boson production in association with a charm-quark jet proceeds through two different mechanisms - one that involves the charm Yukawa coupling and the other that involves direct Higgs coupling to gluons. The interference of the two contributions requires a helicity flip and, therefore, cannot be computed with massless charm quarks. In this paper, we consider QCD corrections to the interference contribution starting from charm-gluon collisions with massive charm quarks and taking the massless limit, . The behavior of QCD cross sections in that limit differs from expectations based on the canonical QCD factorization. This implies that QCD corrections to the interference term necessarily involve logarithms of the ratio whose resummation is currently unknown. Although the explicit next-to-leading order QCD computation does confirm the presence of up to two powers of in the interference contribution, their overall impact on the magnitude of QCD corrections to the interference turns out to be moderate due to a cancellation between double and single logarithmic terms.
28 pages, 4 figures
References in corpus (9)
- LHAPDF6: parton density access in the LHC precision era
- An Exclusive Window onto Higgs Yukawa Couplings
- Analytic results for color-singlet production at NNLO QCD with the nested soft-collinear subtraction scheme
- Factorization at Subleading Power and Endpoint Divergences in Decay: II. Renormalization and Scale Evolution
- Towards all-order factorization of QED amplitudes at next-to-leading power
- Higgs decay into massive b-quarks at NNLO QCD in the nested soft-collinear subtraction scheme
- Analytic results for deep-inelastic scattering at NNLO QCD with the nested soft-collinear subtraction scheme
- On the non-cancellation of infrared singularities in collisions of massive quarks
- Quark Masses and Resummation in Precision QCD Theory