Massive gauge boson pair production at the LHC: A next-to-leading order story
By Julien Baglio, Le Duc Ninh, M. Weber. 2013
196 citations recorded by the source corpus.
Electroweak gauge boson pair production is one of the most important Standard Model processes at the LHC, not only because it is a benchmark process but also by its ability to probe the electroweak interaction directly. We present full next-to-leading order predictions for the production cross sections and distributions of on-shell massive gauge boson pair production in the Standard Model. This includes the QCD and electroweak (EW) corrections. We study the hierarchy between the different channels when looking at the size of the QCD gluon-induced processes and the EW photon-induced processes and provide the first comprehensive explanation of this hierarchy thanks to analytical leading-logarithmic results. We also provide a detailed study of the theoretical uncertainties affecting the total cross section predictions that stem from scale variation, parton distribution function and $\alpha_s$ errors. We then compare with the present LHC data.
View Paper: https://www.semanticscholar.org/paper/7595f1ff2f9b0163a36e5ee125a98525d9c88856
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
- M. Grazzini
- Stefan Kallweit
- Gudrun Heinrich
- Cms Collaboration
- Ansgar Denner
- Valentin Hirschi
- M. Wiesemann
- D. Pagani
Citations in the corpus
- Next-to-leading-order electroweak corrections to the production of four charged leptons at the LHC (2016, background): “5% [39], respectively ∼ −4% [40] in a slightly different setup.”
- The automation of next-to-leading order electroweak calculations (2018, background): “ production In the left panel of g.8we present the transverse momentum of the hardest vector boson in triple vector boson production. This class of processes has been considered previously e.g. refs. [132,133] for discussions on this point. 38The presence of resonant contributions does not constitut”
- W±Z production at the LHC: fiducial cross sections and distributions in NNLO QCD (2016, background): “bles 2, 3, 4 and 6) are expected to provide the correct order of magnitude of yet uncalculated higher-order contributions. EW corrections would aect the ducial cross sections at the 1% level or less [16,17], but are expected to become relevant in the tails of the distributions, which will be potenti”
- W+W− production at the LHC: fiducial cross sections and distributions in NNLO QCD (2015, background): “EW corrections would affect the fiducial cross sections at the 1% level or less [16, 17], but are expected to become relevant in the tails of the distributions, which will be potentially important for new-physics searches.”
- Electroweak radiative corrections for collider physics (2019, unknown): “Typical examples for enhanced γγ contributions are the channels γγ → l+l− [421–423] and γγ → W+W− [355–357, 424, 425], where the γγ channels comprise more than 10% of the differential cross sections in certain regions of phase space.”