On the Higgs boson pair production at the LHC
By J. Grigo, J. Hoff, K. Melnikov, Matthias Steinhauser. 2013
158 citations recorded by the source corpus.
We compute the production cross section of a pair of Standard Model Higgs bosons at the LHC at next-to-leading order in QCD, including corrections in inverse powers of the top quark mass. We calculate these power corrections through O(1/Mt8) and study their relevance for phenomenology of the double Higgs production. We find that power corrections are significant, even for moderate values of partonic center-of-mass energies, and that convergence of the 1/Mt1/Mt expansion can be dramatically improved by factorizing the leading order cross section with full MtMt-dependence.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/86f6fd79db349f95c3fc7f8da5669c1c9df43c05
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In Nuclear and High Energy Physics
- Atlas Collaboration
- Cms Collaboration
- Gudrun Heinrich
- M. Schönherr
- Stefan Dittmaier
- Ansgar Denner
- Fabio Maltoni
- F. Krauss
Citations in the corpus
- Higgs boson pair production in the D = 6 extension of the SM (2014, background): “We choose 30% as a conservative estimate of the uncertainty, incorporating scale (O(10%) at NNLO [38]), PDF plus strong coupling constant (also O(10%) [38]) as well as heavy top mass approximation uncertainties (another O(10%) [40]).”
- Top-quark mass effects in double and triple Higgs production in gluon-gluon fusion at NLO (2014, methodology): “[57] an attempt was made by combining the exact Born cross section with the 1/m(2)t expanded K−factors, as a “taming” technique for the expansion.”
- Les Houches 2015: Physics at TeV Colliders Standard Model Working Group Report (2016, background): “Finite top mass corrections are very important here and power corrections to O(1/m(8)t ) have been computed [148,149].”
- Physics at a 100 TeV pp collider: Higgs and EW symmetry breaking studies (2016, methodology): “[209, 210] the analysis was performed through the computation of subleading terms in the 1/mt expansion.”
- Higgs pair production at next-to-next-to-leading logarithmic accuracy at the LHC (2015, methodology): “[35] through the computation of subleading terms in the 1/Mt expansion, and in ref.”
- Les Houches 2013: Physics at TeV Colliders: Standard Model Working Group Report (2014, methodology): “Double-Higgs production via gluon fusion, used to measure the triple-Higgs coupling, is known at LO QCD with full top mass dependence, including the leading finite-mass effects at NLO QCD [52,53] and at NNLO QCD in the infinite-mt limit [54].”
- Mass effects in the Higgs-gluon coupling: boosted vs. off-shell production (2014, background): “On the other hand, the same description fails spectacularly once the process becomes sensitive to specific kinematic features, for instance for Higgs pair production [49–51].”
- Les Houches 2017: Physics at TeV Colliders Standard Model Working Group Report (2017, methodology): “Power corrections to the NLO and NNLO cross sections in the mt → ∞ limit have been computed [274, 275].”
- FIRE5: A C++ implementation of Feynman Integral REduction (2014, background): “It was successfully applied in [12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26] as well as in several pending projects.”