CERN Accelerating science

 
: $\yb{}$ diagram : $\yt{}$ diagram
: Sample Feynman diagrams for $b \bar b H$ production proportional to \yb{} at tree-level and proportional to \yt{} induced by a top-quark loop. : Caption not extracted
Distribution in the number of $b$-jets without further cuts (left) and in the $\mbbggs{}$ variable defined in \eqn{eq:mbbggs} with fiducial baseline selection cuts applied (right).
Distribution in the number of $b$-jets without further cuts (left) and in the $\mbbggs{}$ variable defined in \eqn{eq:mbbggs} with fiducial baseline selection cuts applied (right).
Distribution in the transverse momentum of the Higgs boson reconstructed from the two photons (left) and of the leading $b$-jet (right), with the fiducial baseline selection cuts applied.
Distribution in the transverse momentum of the Higgs boson reconstructed from the two photons (left) and of the leading $b$-jet (right), with the fiducial baseline selection cuts applied.
Distribution in $m^\star_{2b2\gamma}$ with fiducial selection cuts, for the $y_t^2$ contribution. Predictions at LO and NLO in the 4FS are shown, as well as 5FS results, the latter with and without contributions from $g\to b\bar{b}$ splittings in the shower.
Distribution in the invariant mass of the two hardest $B$ hadrons (left) and in the number of light jets (right) in the 5FS calculation, with and without the contributions from $g\to b\bar{b}$ splittings in the shower, in the fiducial region. The shaded area in the left-hand side plot corresponds to the invariant-mass requirement on the $b$-jets employed in our fiducial cuts.
Distribution in the invariant mass of the two hardest $B$ hadrons (left) and in the number of light jets (right) in the 5FS calculation, with and without the contributions from $g\to b\bar{b}$ splittings in the shower, in the fiducial region. The shaded area in the left-hand side plot corresponds to the invariant-mass requirement on the $b$-jets employed in our fiducial cuts.