Analysis of the strong <i>D</i><sub>2</sub>* (2460)<SUP>0</SUP> → <i>D</i><SUP>+</SUP> π<SUP>-</SUP> and D<sub>s2</sub>*(2573)<SUP>+</SUP> → <i>D</i><SUP>+</SUP> <i>K</i><SUP>0</SUP> transitions via QCD sum rules
dc.authorid | Azizi, Kazem/0000-0003-3741-2167 | |
dc.authorscopusid | 17345170000 | |
dc.authorscopusid | 24391488900 | |
dc.authorscopusid | 6508230150 | |
dc.authorwosid | Sundu, Hayriye/A-5128-2018 | |
dc.authorwosid | Sarac, Yasemin/AAN-1696-2020 | |
dc.authorwosid | Azizi, Kazem/ABE-4757-2021 | |
dc.contributor.author | Azizi, K. | |
dc.contributor.author | Sarac, Y. | |
dc.contributor.author | Sundu, H. | |
dc.contributor.other | Physics Group | |
dc.date.accessioned | 2024-07-05T14:26:53Z | |
dc.date.available | 2024-07-05T14:26:53Z | |
dc.date.issued | 2014 | |
dc.department | Atılım University | en_US |
dc.department-temp | [Azizi, K.] Dogus Univ, Dept Phys, Acibadem Kadikoy, TR-34722 Istanbul, Turkey; [Sarac, Y.] Atilim Univ, Elect & Elect Engn Dept, TR-06836 Ankara, Turkey; [Sundu, H.] Kocaeli Univ, Dept Phys, TR-41380 Izmit, Turkey | en_US |
dc.description | Azizi, Kazem/0000-0003-3741-2167 | en_US |
dc.description.abstract | The strong D-2* (2460)(0) -> D+ pi(-) and D-s2* (2573)(+) -> D+ K-0 transitions are analyzed via three-point QCD sum rules. First we calculate the corresponding strong coupling constants g(D2)*D pi and g(Ds2)*DK. Then we use them to calculate the corresponding decay widths and branching ratios. Making use of the existing experimental data on the ratio of the decay width in the pseudoscalar D channel to that of the vector D* channel, finally, we estimate the decay width and branching ratio of the strong D-2(*) (2460)(0) -> D*(2010)(+)pi(-) transition. | en_US |
dc.description.sponsorship | Scientific and Technological Research Council of Turkey (TUBITAK) [114F018] | en_US |
dc.description.sponsorship | This work has been supported in part by the Scientific and Technological Research Council of Turkey (TUBITAK) under the research project 114F018. | en_US |
dc.identifier.citation | 10 | |
dc.identifier.doi | 10.1140/epjc/s10052-014-3106-x | |
dc.identifier.issn | 1434-6044 | |
dc.identifier.issn | 1434-6052 | |
dc.identifier.issue | 10 | en_US |
dc.identifier.scopus | 2-s2.0-84919926755 | |
dc.identifier.scopusquality | Q1 | |
dc.identifier.uri | https://doi.org/10.1140/epjc/s10052-014-3106-x | |
dc.identifier.uri | https://hdl.handle.net/20.500.14411/193 | |
dc.identifier.volume | 74 | en_US |
dc.identifier.wos | WOS:000346524900001 | |
dc.identifier.wosquality | Q2 | |
dc.institutionauthor | Saraç Oymak, Yasemin | |
dc.language.iso | en | en_US |
dc.publisher | Springer | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/openAccess | en_US |
dc.subject | [No Keyword Available] | en_US |
dc.title | Analysis of the strong <i>D</i><sub>2</sub>* (2460)<SUP>0</SUP> → <i>D</i><SUP>+</SUP> π<SUP>-</SUP> and D<sub>s2</sub>*(2573)<SUP>+</SUP> → <i>D</i><SUP>+</SUP> <i>K</i><SUP>0</SUP> transitions via QCD sum rules | en_US |
dc.type | Article | en_US |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | 76c2e6e0-40bb-4e6f-b776-53c925ab44d4 | |
relation.isAuthorOfPublication.latestForDiscovery | 76c2e6e0-40bb-4e6f-b776-53c925ab44d4 | |
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