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Transverse-Momentum Resummation for Gauge Boson Pair Production at the Hadron Collider

Yan Wang, Chong Sheng Li, Ze Long Liu, Ding Yu Shao, Hai Tao Li

TL;DR

This work develops NNLL transverse-momentum resummation for gauge-boson pair production (W^+W^-, ZZ, and the first NNLL treatment of WZ) at the LHC using soft-collinear effective theory. The formalism factorizes the q_T spectrum into a hard function, TMD-like PDFs with a collinear anomaly, and RG evolution, and it is matched to NLO fixed-order results to include non-singular contributions. Numerical results show reduced scale dependence and modest non-perturbative effects, with predictions that agree with CMS ZZ 8 TeV data and quantified PDF uncertainties. The study enhances SM predictions for gauge-boson kinematics and provides robust backgrounds for Higgs and new-physics searches at current and future hadron colliders.

Abstract

We perform the transverse-momentum resummation for $W^{+}W^{-}$, $ZZ$, and $W^{\pm}Z$ pair productions at the next-to-next-to-leading logarithmic accuracy using soft-collinear effective theory for $\sqrt{S}=8 \text{TeV}$ and $\sqrt{S}=14 \text{TeV}$ at the LHC, respectively. Especially, this is the first calculation of $W^{\pm}Z$ transverse-momentum resummation. We also include the non-perturbative effects and discussions on the PDF uncertainties. Comparing with the next-to-leading logarithmic results, the next-to-next-to-leading logarithmic resummation can reduce the dependence of the transverse-momentum distribution on the factorization scales significantly. Finally, we find that our numerical results are consistent with data measured by CMS collaboration for the $ZZ$ production, which have been only reported by the LHC experiments for the unfolded transverse-momentum distribution of the gauge boson pair production so far, within theoretical and experimental uncertainties.

Transverse-Momentum Resummation for Gauge Boson Pair Production at the Hadron Collider

TL;DR

This work develops NNLL transverse-momentum resummation for gauge-boson pair production (W^+W^-, ZZ, and the first NNLL treatment of WZ) at the LHC using soft-collinear effective theory. The formalism factorizes the q_T spectrum into a hard function, TMD-like PDFs with a collinear anomaly, and RG evolution, and it is matched to NLO fixed-order results to include non-singular contributions. Numerical results show reduced scale dependence and modest non-perturbative effects, with predictions that agree with CMS ZZ 8 TeV data and quantified PDF uncertainties. The study enhances SM predictions for gauge-boson kinematics and provides robust backgrounds for Higgs and new-physics searches at current and future hadron colliders.

Abstract

We perform the transverse-momentum resummation for , , and pair productions at the next-to-next-to-leading logarithmic accuracy using soft-collinear effective theory for and at the LHC, respectively. Especially, this is the first calculation of transverse-momentum resummation. We also include the non-perturbative effects and discussions on the PDF uncertainties. Comparing with the next-to-leading logarithmic results, the next-to-next-to-leading logarithmic resummation can reduce the dependence of the transverse-momentum distribution on the factorization scales significantly. Finally, we find that our numerical results are consistent with data measured by CMS collaboration for the production, which have been only reported by the LHC experiments for the unfolded transverse-momentum distribution of the gauge boson pair production so far, within theoretical and experimental uncertainties.

Paper Structure

This paper contains 11 sections, 55 equations, 6 figures.

Figures (6)

  • Figure 1: Comparison of the leading singular (red) and the exact NLO (black) distributions in the small $q_T$ region.
  • Figure 2: The non-perturbative effects on the differential cross sections of gauge boson pair production with $\sqrt{S}=14~\text{TeV}$, respectively.
  • Figure 3: Up: the $q_T$ distributions with scale uncertainties for gauge boson pair productions at the LHC with $\sqrt{S}=8~\text{TeV}$ and $\sqrt{S}=14~\text{TeV}$. Down: NNLL + NLO results normalized to NLO.
  • Figure 4: The PDF uncertainties of NNLL order resummed transverse-momentum for gauge boson pair production, where the bands represent 2$\sigma$ deviation.
  • Figure 5: Comparison of NNLL + NLO resummed $q_T$ distribution for $W^+W^-$ and $ZZ$ distributions in the SCET and CSS frame at $\sqrt{S}=14~\text{TeV}$ with MRST2002NLO PDF set.
  • ...and 1 more figures