Bottom-flavored hadrons from top-quark decay at next-to-leading order in the general-mass variable-flavor-number scheme
From MaRDI portal
Publication:447424
DOI10.1016/J.NUCLPHYSB.2012.05.008zbMath1246.81434arXiv1205.2528OpenAlexW2027361487WikidataQ59869214 ScholiaQ59869214MaRDI QIDQ447424
Gustav Kramer, Bernd A. Kniehl, S. Mohammad Moosavi Nejad
Publication date: 3 September 2012
Published in: Nuclear Physics. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1205.2528
Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05) Nonperturbative methods of renormalization applied to problems in quantum field theory (81T16) Quantum scattering theory (81U99)
Related Items (5)
Charged Higgs production from polarized top-quark decay in the 2HDM considering the general-mass variable-flavor-number scheme ⋮ Next-to-leading order corrections to the spin-dependent energy spectrum of hadrons from polarized top quark decay in the general two Higgs doublet model ⋮ NLO QCD corrections to gluon fragmentation function into \(\eta_b\) and \(\eta_c\) based on the Suzuki's model ⋮ Indirect search for light charged Higgs bosons through the dominant semileptonic decays of top quark \(t \rightarrow b(\rightarrow B/D + X)+H^{+}(\rightarrow \tau^{+}\nu_{\tau})\) ⋮ Spin-dependent energy distribution of B-hadrons from polarized top decays considering the azimuthal correlation rate
This page was built for publication: Bottom-flavored hadrons from top-quark decay at next-to-leading order in the general-mass variable-flavor-number scheme