English
 
Help Privacy Policy Disclaimer
  Advanced SearchBrowse
  1. View item / 
  2. Item Summary

Item

ITEM ACTIONSEXPORT
Add to Basket
  Local TagsRelease HistoryDetailsSummary

Released
Journal Article

Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects

MPS-Authors

Heinrich,  G.
Max Planck Institute for Physics, Max Planck Society and Cooperation Partners;

Jones,  S.P.
Max Planck Institute for Physics, Max Planck Society and Cooperation Partners;

Kerner,  M.
Max Planck Institute for Physics, Max Planck Society and Cooperation Partners;

Luisoni,  G.
Max Planck Institute for Physics, Max Planck Society and Cooperation Partners;

Scyboz,  L.
Max Planck Institute for Physics, Max Planck Society and Cooperation Partners;

External Resource
No external resources are shared
Fulltext (restricted access)
There are currently no full texts shared for your IP range.
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available
Citation

Heinrich, G., Jones, S., Kerner, M., Luisoni, G., & Scyboz, L. (2019). Probing the trilinear Higgs boson coupling in di-Higgs production at NLO QCD including parton shower effects. Journal of High Energy Physics, 1906, 066. Retrieved from https://publications.mppmu.mpg.de/?action=search&mpi=MPP-2019-50.


Cite as: https://hdl.handle.net/21.11116/0000-0005-D717-F
Abstract
We present results for Higgs boson pair production with variations of the trilinear Higgs boson self-coupling at next-to-leading order (NLO) in QCD including the full top quark mass dependence. Differential results at 14 TeV are presented, and we discuss the implications of anomalous trilinear couplings as well as differences between the PYTHIA 8.2 and HERWIG 7.1 parton showers in combination with POWHEG. The implementation of the NLO QCD calculation with variable Higgs boson self-coupling is made publicly available in the POWHEG-BOX-V2 Monte Carlo framework. A simple method for using the new implementation to study also variations of the top quark Yukawa coupling is described.