NLO QCD and EW corrections to vector-boson scattering into ${\mathrm{W}}^{+}{\mathrm{W}}^{-}$ at the LHC

Abstract

We present the full next-to-leading-order electroweak and QCD corrections to vector-boson scattering into a pair of off-shell opposite-sign W bosons decaying into leptons of different flavour at the LHC. We include full leading-order predictions for the irreducible background. Explicitly, we investigate the process $\mathrm{pp}\to {\mathrm{e}}^{+}\hat{\mathrm{I}}{½}_{\mathrm{e}}\hat{\mathrm{I}}{¼}^{-}\overline{\hat{\mathrm{I}}}{½}_{\hat{\mathrm{I}}}¼\mathrm{jj}+X$ at leading orders $O(\hat{I}{\pm }^6)$, $O(\hat{\mathrm{I}}{\pm }_{\mathrm{s}}\hat{\mathrm{I}}{\pm }^5)$, $O(\hat{\mathrm{I}}{\pm }_{\mathrm{s}}^2\hat{\mathrm{I}}{\pm }^4)$, supplemented by the loop-induced $O(\hat{\mathrm{I}}{\pm }_{\mathrm{s}}^4\hat{\mathrm{I}}{\pm }^4)$ contribution, and at next-to-leading orders $O(\hat{I}{\pm }^7)$ and $O(\hat{\mathrm{I}}{\pm }_{\mathrm{s}}\hat{\mathrm{I}}{\pm }^6)$ in two setups providing fiducial cross sections as well as differential distributions. We take full account of photon-induced next-to-leading-order contributions, which prove to be non negligible. With $-11.4\%$ and $-6.7\%$ in the two setups, the electroweak corrections are smaller than for other vector-boson-scattering processes. This can be traced back to the presence of the Higgs-boson resonance in the fiducial phase space, whose effects we analyse within an additional unphysical, but manifestly gauge-invariant setup. The QCD corrections amount to $-5.1\%$ and $-21.6\%$ in the two setups. The large size of the latter correction, compared to other vector-boson scattering processes, is explained by a very restrictive definition of its fiducial phase space.

34 pages, 29 pdf figure files, some extra comments added, version that appeared in JHEP