Rare two-body decays of the top quark into a bottom meson plus an up or charm quark

Abstract

Abstract Rare two-body decays of the top quark into a neutral bottom-quark meson plus an up- or charm-quark: t → B ¯ 0 + u , c ; t → B ¯ s 0 + c , u $$ t\to {\overline{B}}^0+u,\kern0.5em c;t\to {\overline{B}}_s^0+c,\kern0.5em u $$ ; and t → ϒ(nS) + c, u, are studied for the first time. The corresponding partials widths are computed at leading order in the non-relativistic QCD framework. The sums of all two-body branching ratios amount to ℬ t → B ¯ 0 + jet ≈ ℬ t → B ¯ s 0 + jet ≈ 4.2 ⋅ 10 − 5 $$ \mathrm{\mathcal{B}}\left(t\to {\overline{B}}^0+\mathrm{jet}\right)\approx \mathrm{\mathcal{B}}\left(t\to {\overline{B}}_s^0+\mathrm{jet}\right)\approx 4.2\cdot {10}^{-5} $$ and ℬ(t → ϒ(nS) + jet) ≈ 2 ⋅ 10−9, respectively. The feasibility to observe the t → B ¯ s 0 + $$ t\to {\overline{B}}_{(s)}^0+ $$ jet decay is estimated in top- pair events produced in proton-proton collisions at s $$ \sqrt{s} $$ = 14, 100 TeV at the LHC and FCC, respectively. Combining many exclusive hadronic B ¯ s 0 $$ {\overline{B}}_{(s)}^0 $$ decays, with J/ψ or D 0,± final states, about 50 (16 000) events are expected in 3 (20) ab −1 of integrated luminosity at the LHC (FCC), after typical selection criteria, acceptance, and efficiency losses. An observation of the two-body top-quark decay can also be achieved in the interesting t → b(jet) + c(jet) dijet final state, where the B ¯ s 0 $$ {\overline{B}}_{(s)}^0 $$ decay products are reconstructed as a jet, with 5 300 and 1.4 million signal events above backgrounds expected after selection criteria at the LHC and FCC, respectively. Such unique final states provide a new direct method to precisely measure the top-quark mass via simple 2-body invariant mass analyses.

Keywords

• QCD Phenomenology