Journal
JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 10, Pages -Publisher
SPRINGER
DOI: 10.1007/JHEP10(2021)088
Keywords
QCD Phenomenology
Categories
Funding
- Royal Society [URF\R1\180549]
- Royal Society Enhancement Award [RGF\EA\181033, CEC19\100349]
- European Union's Horizon 2020 research and innovation programme as part of the Marie Sklodowska-Curie Innovative Training Network MCnetITN3 [722104]
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The study aims to investigate the vector and axial-vector dynamics of the produced lepton pair by correlating them in two observables, the transverse momentum q(T) of the lepton pair and its azimuthal separation increment phi.
The production of weak gauge bosons, W-+/- and Z, are at the core of the LHC precision measurement program. Their transverse momentum spectra as well as their pairwise ratios are key theoretical inputs to many high-precision analyses, ranging from the W mass measurement to the determination of parton distribution functions. Owing to the different properties of the W and Z boson and the different accessible fiducial regions for their measurement, a simple one-dimensional correlation is insufficient to capture the differing vector and axial-vector dynamics of the produced lepton pair. We propose to correlate them in two observables, the transverse momentum q(T) of the lepton pair and its azimuthal separation increment phi. Both quantities are purely transverse and therefore accessible in all three processes, either directly or by utilising the missing transverse momentum of the event. We calculate all the single-differential q(T) and increment phi as well as the double-differential (q(T), increment phi) spectra for all three processes at (NLL)-L-3 '+(NLO)-L-2 accuracy, resumming small transverse momentum logarithms in the soft-collinear effective theory approach and including all singlet and non-singlet contributions. Using the double-differential cross sections we build the pairwise ratios Script capital RW+/Z, Script capital RW-/Z, and Script capital RW+/W- and determine their uncertainties assuming fully correlated, partially correlated, and uncorrelated uncertainties in the respective numerators and denominators. In the preferred partially correlated case we find uncertainties of less than 1% in most phase space regions and up to 3% in the lowest q(T) region.
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