B^0 \to \omega\eta^{(\prime)}$ and $\phi\eta^{(\prime)}$ decays in the perturbative QCD approach

Phys.Rev.D75:054033,2007 We calculate the branching ratios and CP-violating asymmetries for $B^0 \to\omega \eta $, $\omega \eta^\prime$, $\phi \eta$ and $\phi \eta^\prime$ decays in the perturbative QCD (pQCD) factorization approach. The pQCD predictions for the CP-averaged branching ratios are $Br(...

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description Phys.Rev.D75:054033,2007 We calculate the branching ratios and CP-violating asymmetries for $B^0 \to\omega \eta $, $\omega \eta^\prime$, $\phi \eta$ and $\phi \eta^\prime$ decays in the perturbative QCD (pQCD) factorization approach. The pQCD predictions for the CP-averaged branching ratios are $Br(B^0 \to \omega\eta) = \left (2.7 ^{+1.1}_{-1.0})\times 10^{-7}$, $Br(B^0 \to \omega \eta^\prime) = \left (0.75 ^{+0.37}_{-0.33}) \times 10^{-7}$, and $Br(B^0 \to \phi\eta) = \left (6.3 ^{+3.3}_{-1.9}) \times 10^{-9}$, $Br(B^0 \to \phi\eta^{\prime}) = \left (7.3^{+3.5}_{-2.6}) \times 10^{-9}$ which are consistent with currently available experimental upper limits. The inclusion of the gluonic contribution can change the branching ratios of $B \to \omega(\phi) \eta^\prime$ decays by about 10%. The direct CP-violating asymmetries for $B^0 \to \omega \eta$ and $\omega \eta^\prime$ decays are generally large in size.
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The pQCD predictions for the CP-averaged branching ratios are $Br(B^0 \to \omega\eta) = \left (2.7 ^{+1.1}_{-1.0})\times 10^{-7}$, $Br(B^0 \to \omega \eta^\prime) = \left (0.75 ^{+0.37}_{-0.33}) \times 10^{-7}$, and $Br(B^0 \to \phi\eta) = \left (6.3 ^{+3.3}_{-1.9}) \times 10^{-9}$, $Br(B^0 \to \phi\eta^{\prime}) = \left (7.3^{+3.5}_{-2.6}) \times 10^{-9}$ which are consistent with currently available experimental upper limits. The inclusion of the gluonic contribution can change the branching ratios of $B \to \omega(\phi) \eta^\prime$ decays by about 10%. The direct CP-violating asymmetries for $B^0 \to \omega \eta$ and $\omega \eta^\prime$ decays are generally large in size.</description><identifier>DOI: 10.48550/arxiv.hep-ph/0702110</identifier><language>eng</language><subject>Physics - High Energy Physics - Phenomenology</subject><creationdate>2007-02</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/hep-ph/0702110$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.1103/PhysRevD.75.054033$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.hep-ph/0702110$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Guo, Dong-Qin</creatorcontrib><creatorcontrib>Chen, Xin-Fen</creatorcontrib><creatorcontrib>Xiao, Zhen-Jun</creatorcontrib><title>B^0 \to \omega\eta^{(\prime)}$ and $\phi\eta^{(\prime)}$ decays in the perturbative QCD approach</title><description>Phys.Rev.D75:054033,2007 We calculate the branching ratios and CP-violating asymmetries for $B^0 \to\omega \eta $, $\omega \eta^\prime$, $\phi \eta$ and $\phi \eta^\prime$ decays in the perturbative QCD (pQCD) factorization approach. The pQCD predictions for the CP-averaged branching ratios are $Br(B^0 \to \omega\eta) = \left (2.7 ^{+1.1}_{-1.0})\times 10^{-7}$, $Br(B^0 \to \omega \eta^\prime) = \left (0.75 ^{+0.37}_{-0.33}) \times 10^{-7}$, and $Br(B^0 \to \phi\eta) = \left (6.3 ^{+3.3}_{-1.9}) \times 10^{-9}$, $Br(B^0 \to \phi\eta^{\prime}) = \left (7.3^{+3.5}_{-2.6}) \times 10^{-9}$ which are consistent with currently available experimental upper limits. The inclusion of the gluonic contribution can change the branching ratios of $B \to \omega(\phi) \eta^\prime$ decays by about 10%. The direct CP-violating asymmetries for $B^0 \to \omega \eta$ and $\omega \eta^\prime$ decays are generally large in size.</description><subject>Physics - High Energy Physics - Phenomenology</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA1NNAzsTA1NdBPLKrILNPLSC3QLcjQNzA3MDI0NOBkSHCKM1CIKclXiMnPTU1PjEktSYyr1ogpKMrMTdWsVVFIzEtRUIkpyMjEkElJTU6sLFbIzFMoyUhVKEgtKiktSkosySxLVQh0dlFILCgoyk9MzuBhYE1LzClO5YXS3AzKbq4hzh66YPfEg4xLLKqMB7orviAjHuouY-JUAQBq2Ub8</recordid><startdate>20070211</startdate><enddate>20070211</enddate><creator>Guo, Dong-Qin</creator><creator>Chen, Xin-Fen</creator><creator>Xiao, Zhen-Jun</creator><scope>GOX</scope></search><sort><creationdate>20070211</creationdate><title>B^0 \to \omega\eta^{(\prime)}$ and $\phi\eta^{(\prime)}$ decays in the perturbative QCD approach</title><author>Guo, Dong-Qin ; Chen, Xin-Fen ; Xiao, Zhen-Jun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_hep_ph_07021103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Physics - High Energy Physics - Phenomenology</topic><toplevel>online_resources</toplevel><creatorcontrib>Guo, Dong-Qin</creatorcontrib><creatorcontrib>Chen, Xin-Fen</creatorcontrib><creatorcontrib>Xiao, Zhen-Jun</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Guo, Dong-Qin</au><au>Chen, Xin-Fen</au><au>Xiao, Zhen-Jun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>B^0 \to \omega\eta^{(\prime)}$ and $\phi\eta^{(\prime)}$ decays in the perturbative QCD approach</atitle><date>2007-02-11</date><risdate>2007</risdate><abstract>Phys.Rev.D75:054033,2007 We calculate the branching ratios and CP-violating asymmetries for $B^0 \to\omega \eta $, $\omega \eta^\prime$, $\phi \eta$ and $\phi \eta^\prime$ decays in the perturbative QCD (pQCD) factorization approach. The pQCD predictions for the CP-averaged branching ratios are $Br(B^0 \to \omega\eta) = \left (2.7 ^{+1.1}_{-1.0})\times 10^{-7}$, $Br(B^0 \to \omega \eta^\prime) = \left (0.75 ^{+0.37}_{-0.33}) \times 10^{-7}$, and $Br(B^0 \to \phi\eta) = \left (6.3 ^{+3.3}_{-1.9}) \times 10^{-9}$, $Br(B^0 \to \phi\eta^{\prime}) = \left (7.3^{+3.5}_{-2.6}) \times 10^{-9}$ which are consistent with currently available experimental upper limits. The inclusion of the gluonic contribution can change the branching ratios of $B \to \omega(\phi) \eta^\prime$ decays by about 10%. The direct CP-violating asymmetries for $B^0 \to \omega \eta$ and $\omega \eta^\prime$ decays are generally large in size.</abstract><doi>10.48550/arxiv.hep-ph/0702110</doi><oa>free_for_read</oa></addata></record>
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title B^0 \to \omega\eta^{(\prime)}$ and $\phi\eta^{(\prime)}$ decays in the perturbative QCD approach
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