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Resummation of jet veto logarithms at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">N</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msup><mml:msub><mml:mrow><mml:mi>LL</mml:mi></mml:mrow><mml:mrow><mml:mi>a</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>NNLO</mml:mi></mml:mrow></mml:math> for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mi…
We compute the resummed on-shell ${W}^{+}{W}^{\ensuremath{-}}$ production cross section under a jet veto at the LHC to partial ${\mathrm{N}}^{3}\mathrm{LL}$ order matched to the fixed-order NNLO result. Differential NNLO cross sections are obtained from an implementation of ${q}_{T}$ subtraction in Sherpa. The two-loop virtual corrections to the $q\overline{q}\ensuremath{\rightarrow}{W}^{+}{W}^{\ensuremath{-}}$ amplitude, used in …