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.authoridAzizi, Kazem/0000-0003-3741-2167
dc.authorscopusid17345170000
dc.authorscopusid24391488900
dc.authorscopusid6508230150
dc.authorwosidSundu, Hayriye/A-5128-2018
dc.authorwosidSarac, Yasemin/AAN-1696-2020
dc.authorwosidAzizi, Kazem/ABE-4757-2021
dc.contributor.authorAzizi, K.
dc.contributor.authorSarac, Y.
dc.contributor.authorSundu, H.
dc.contributor.otherPhysics Group
dc.date.accessioned2024-07-05T14:26:53Z
dc.date.available2024-07-05T14:26:53Z
dc.date.issued2014
dc.departmentAtılım Universityen_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, Turkeyen_US
dc.descriptionAzizi, Kazem/0000-0003-3741-2167en_US
dc.description.abstractThe 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.sponsorshipScientific and Technological Research Council of Turkey (TUBITAK) [114F018]en_US
dc.description.sponsorshipThis 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.citation10
dc.identifier.doi10.1140/epjc/s10052-014-3106-x
dc.identifier.issn1434-6044
dc.identifier.issn1434-6052
dc.identifier.issue10en_US
dc.identifier.scopus2-s2.0-84919926755
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1140/epjc/s10052-014-3106-x
dc.identifier.urihttps://hdl.handle.net/20.500.14411/193
dc.identifier.volume74en_US
dc.identifier.wosWOS:000346524900001
dc.identifier.wosqualityQ2
dc.institutionauthorSaraç Oymak, Yasemin
dc.language.isoenen_US
dc.publisherSpringeren_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subject[No Keyword Available]en_US
dc.titleAnalysis 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 rulesen_US
dc.typeArticleen_US
dspace.entity.typePublication
relation.isAuthorOfPublication76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isAuthorOfPublication.latestForDiscovery76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isOrgUnitOfPublication2682824b-512d-4a4e-8498-5b5719f606fe
relation.isOrgUnitOfPublication.latestForDiscovery2682824b-512d-4a4e-8498-5b5719f606fe

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