$B^0 \to ωη^{(\prime)}$ and $ϕη^{(\prime)}$ decays in the perturbative QCD approach
| dc.creator | Guo, Dong-Qin | |
| dc.creator | Chen, Xin-Fen | |
| dc.creator | Xiao, Zhen-Jun | |
| dc.date | 2007-02-11 | |
| dc.date | 2007-03-07 | |
| dc.date.accessioned | 2026-07-07T11:59:03Z | |
| dc.date.available | 2026-07-07T11:59:03Z | |
| dc.description | We calculate the branching ratios and CP-violating asymmetries for $B^0 \toωη$, $ωη^\prime$, $ϕη$ and $ϕη^\prime$ decays in the perturbative QCD (pQCD) factorization approach. The pQCD predictions for the CP-averaged branching ratios are $Br(B^0 \to ωη) = \left (2.7 ^{+1.1}_{-1.0})\times 10^{-7}$, $Br(B^0 \to ωη^\prime) = \left (0.75 ^{+0.37}_{-0.33}) \times 10^{-7}$, and $Br(B^0 \to ϕη) = \left (6.3 ^{+3.3}_{-1.9}) \times 10^{-9}$, $Br(B^0 \to ϕη^{\prime}) = \left (7.3^{+3.5}_{-2.6}) \times 10^{-9}$ which are consistent with currently available experimental upper limits. The inclusion of the gluonic contribution can change the branching ratios of $B \to ω(ϕ) η^\prime$ decays by about 10%. The direct CP-violating asymmetries for $B^0 \to ωη$ and $ωη^\prime$ decays are generally large in size. | |
| dc.description | 23 pages, 4 ps/eps figures, RevTex, typos removed, minor corrections | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0702110 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0702110 | |
| dc.identifier | Phys.Rev.D75:054033,2007 | |
| dc.identifier | doi:10.1103/PhysRevD.75.054033 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/206433 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | $B^0 \to ωη^{(\prime)}$ and $ϕη^{(\prime)}$ decays in the perturbative QCD approach | |
| dc.type | text |