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. 2019;79(10):868.
doi: 10.1140/epjc/s10052-019-7324-0. Epub 2019 Oct 22.

The transverse momentum spectrum of weak gauge bosons at N 3 LL + NNLO

Affiliations

The transverse momentum spectrum of weak gauge bosons at N 3 LL + NNLO

Wojciech Bizoń et al. Eur Phys J C Part Fields. 2019.

Abstract

We present accurate QCD predictions for the transverse momentum ( p ) spectrum of electroweak gauge bosons at the LHC for 13 TeV collisions, based on a consistent combination of a NNLO calculation at large p and N 3 LL resummation in the small p limit. The inclusion of higher order corrections leads to substantial changes in the shape of the differential distributions, and the residual perturbative uncertainties are reduced to the few percent level across the whole transverse momentum spectrum. We examine the ratio of p distributions in charged- and neutral-current Drell-Yan production, and study different prescriptions for the estimate of perturbative uncertainties that rely on different degrees of correlation between these processes. We observe an excellent stability of the ratios with respect to the perturbative order, indicating a strong correlation between the corresponding QCD corrections.

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Figures

Fig. 1
Fig. 1
Comparison of the normalised transverse momentum distribution for neutral and charged Drell–Yan pair production at NLL+LO (green, dotted), NNLL + NLO (blue, dashed) and N3LL + NNLO (red, solid) at s=13TeV for the fiducial volume defined in the text. The lower panel shows the ratio to the NNLL + NLO result
Fig. 2
Fig. 2
Comparison of the normalised transverse momentum distribution for neutral and charged Drell–Yan pair production at NNLO (green, dotted), NNLL + NLO (blue, dashed) and N3LL + NNLO (red, solid) at s=13TeV for the fiducial volume defined in the text. For reference, the Pythia8 prediction in the AZ tune is also shown, and the lower panel shows the ratio of each prediction to the Pythia8 result
Fig. 3
Fig. 3
Difference Eq. (13) between the matched and the resummed predictions for the Z (green, dotted), W+ (blue, dashed) and W- (red, solid) normalised distributions. The lower panel shows the ratio of ΔN3LL to the N3LL + NNLO matched result
Fig. 4
Fig. 4
Ratios of Z/W+ and W-/W+ normalised differential distributions at NLL + LO (green, dotted), NNLL+NLO (blue, dashed) and N3LL + NNLO (red, solid) at s=13TeV. The three lower panels show three different prescriptions for the theory uncertainty, as described in the text
Fig. 5
Fig. 5
Ratios of Z/W+ and W-/W+ normalised differential distributions at NNLO (green, dotted), NNLL+NLO (blue, dashed) and N3LL + NNLO (red, solid) at s=13TeV. For reference, the Pythia8 prediction in the AZ tune is also shown, and the lower panels show the ratio of each prediction to the latter

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