Associated production of a Higgs boson decaying into bottom quarks and a weak vector boson decaying leptonically at NNLO in QCD
Journal of High Energy Physics, ISSN: 1029-8479, Vol: 2019, Issue: 10, Page: 2
2019
- 34Citations
- 6Captures
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Example: if you select the 1-year option for an article published in 2019 and a metric category shows 90%, that means that the article or review is performing better than 90% of the other articles/reviews published in that journal in 2019. If you select the 3-year option for the same article published in 2019 and the metric category shows 90%, that means that the article or review is performing better than 90% of the other articles/reviews published in that journal in 2019, 2018 and 2017.
Citation Benchmarking is provided by Scopus and SciVal and is different from the metrics context provided by PlumX Metrics.
Article Description
We present the calculation of next-to-next-to-leading order (NNLO) corrections in perturbative QCD for the production of a Higgs boson decaying into a pair of bottom quarks in association with a leptonically decaying weak vector boson: pp→ VH + X→ ℓ ℓ ¯ b b ¯ + X. We consider the corrections to both the production and decay sub-processes, retaining a fully differential description of the final state including off-shell propagators of the Higgs and vector boson. The calculation is carried out using the antenna subtraction formalism and is implemented in the NNLOjet framework. Clustering and identification of b-jets is performed with the flavour-k algorithm and results for fiducial cross sections and distributions are presented for the LHC at s = 13 TeV. We assess the residual theory uncertainty by varying the production and decay scales independently and provide scale uncertainty bands in our results, yielding percent-level accurate predictions for observables in this Higgs production mode computed at NNLO. Confronting a na¨ıve perturbative expansion of the cross section against the customary re-scaling procedure to a fixed branching ratio reveals that starting from NNLO, the latter could be inadequate in estimating missing higher-order effects through scale variations.
Bibliographic Details
http://www.scopus.com/inward/record.url?partnerID=HzOxMe3b&scp=85073610804&origin=inward; http://dx.doi.org/10.1007/jhep10(2019)002; https://link.springer.com/10.1007/JHEP10(2019)002; https://link.springer.com/content/pdf/10.1007/JHEP10(2019)002.pdf; https://link.springer.com/article/10.1007/JHEP10(2019)002/fulltext.html; http://hdl.handle.net/20.500.11850/372993; https://www.zora.uzh.ch/id/eprint/178404; http://dx.doi.org/10.3929/ethz-b-000372993; https://dx.doi.org/10.3929/ethz-b-000372993; https://www.research-collection.ethz.ch/handle/20.500.11850/372993; http://dx.doi.org/10.5167/uzh-178404; https://dx.doi.org/10.5167/uzh-178404; https://www.zora.uzh.ch/id/eprint/178404/; http://dx.doi.org/10.1007/jhep10%282019%29002; https://dx.doi.org/10.1007/jhep10%282019%29002; https://link.springer.com/article/10.1007/JHEP10(2019)002; https://www.zora.uzh.ch/id/eprint/178404/1/Gauld2019_Article_AssociatedProductionOfAHiggsBo.pdf; https://www.research-collection.ethz.ch/bitstream/20.500.11850/372993/3/Gauld2019_Article_AssociatedProductionOfAHiggsBo.pdf
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