Built on

M. J. Duncan, G. L. Kane, and W. W. Repko, “ W W WW Physics at Future Colliders,” Nucl. Phys
1986
Earlier work this paper cites.
W. Buchmuller and D. Wyler, “Effective Lagrangian Analysis of New Interactions and Flavor Conservation,” Nucl. Phys
1986
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K. Hagiwara, R. D. Peccei, D. Zeppenfeld, and K. Hikasa, “Probing the Weak Boson Sector in e + e − → W + W − e^{+}e^{-}\rightarrow W^{+}W^{-} ,” Nucl. Phys
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Earlier work this paper cites.
L. J. Dixon, Z. Kunszt, and A. Signer, “Vector boson pair production in hadronic collisions at order α s \alpha_{s} : Lepton correlations and anomalous couplings,” Phys. Rev
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Earlier work this paper cites.
J. M. Campbell and R. K. Ellis, “An Update on vector boson pair production at hadron colliders,” Phys. Rev
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P. Nason, “A New method for combining NLO QCD with shower Monte Carlo algorithms,” JHEP
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B. Grzadkowski, M. Iskrzynski, M. Misiak, and J. Rosiek, “Dimension-Six Terms in the Standard Model Lagrangian,” JHEP
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2018

NLO Effects in EFT Fits to $W^+W^-$ Production at the LHC

Baglio, Julien, Dawson, Sally, Lewis, Ian M.

Understand

We study the impact of anomalous gauge boson and fermion couplings on the production of $W^+W^-$ pairs at potential future LHC upgrades and estimate the sensitivity at $\sqrt{S}=14$ TeV with $3~ab^{-1}$ and $\sqrt{S}=27$ TeV with $15~ab^{-1}$.

A general technique for including NLO QCD effects in effective field theory (EFT) fits to kinematic distributions is presented, and numerical results are given for $\sqrt{S}=13$ TeV $W^+W^-$ production.
Our method allows fits to anomalous couplings at NLO accuracy in any EFT basis and has been implemented in a publicly available version of the POWHEG-BOX.
Analytic expressions for the $K$-factors relevant for $13$ TeV total cross sections are given for the HISZ and Warsaw EFT bases and differential $K$-factors can be obtained using the supplemental material.

Built on

M. J. Duncan, G. L. Kane, and W. W. Repko, “ W W WW Physics at Future Colliders,” Nucl. Phys
1986
Earlier work this paper cites.
W. Buchmuller and D. Wyler, “Effective Lagrangian Analysis of New Interactions and Flavor Conservation,” Nucl. Phys
1986
Earlier work this paper cites.
K. Hagiwara, R. D. Peccei, D. Zeppenfeld, and K. Hikasa, “Probing the Weak Boson Sector in e + e − → W + W − e^{+}e^{-}\rightarrow W^{+}W^{-} ,” Nucl. Phys
1987
Earlier work this paper cites.
L. J. Dixon, Z. Kunszt, and A. Signer, “Vector boson pair production in hadronic collisions at order α s \alpha_{s} : Lepton correlations and anomalous couplings,” Phys. Rev
1999
Earlier work this paper cites.
J. M. Campbell and R. K. Ellis, “An Update on vector boson pair production at hadron colliders,” Phys. Rev
1999
Earlier work this paper cites.
P. Nason, “A New method for combining NLO QCD with shower Monte Carlo algorithms,” JHEP
2004
Earlier work this paper cites.
B. Grzadkowski, M. Iskrzynski, M. Misiak, and J. Rosiek, “Dimension-Six Terms in the Standard Model Lagrangian,” JHEP
Original
2010
Earlier work this paper cites.
S. Alioli, P. Nason, C. Oleari, and E. Re, “A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX,” JHEP
Original
2010
Earlier work this paper cites.
J. M. Campbell, R. K. Ellis, and C. Williams, “Vector boson pair production at the LHC,” JHEP
Original
2011
Earlier work this paper cites.
T. Melia, P. Nason, R. Rontsch, and G. Zanderighi, “W+W-, WZ and ZZ production in the POWHEG BOX,” JHEP
Original
2011
Earlier work this paper cites.
DELPHI, OPAL, LEP Electroweak, ALEPH, L3
Original
2013
Earlier work this paper cites.
A. Bierweiler, T. Kasprzik, and J. H. Kuhn, “Vector-boson pair production at the LHC to 𝒪 ⁡ ( α 3 ) \mathcal{O}(\alpha^{3}) accuracy,” JHEP
Original
2013
Earlier work this paper cites.