Isospin-violating strong decays of scalar single-heavy tetraquarks / Th. Gutsche [et al.]

Уровень набора: Physical Review D, particles, fields, gravitation, and cosmology = 1970-Альтернативный автор-лицо: Gutsche, Th., Thomas;Ivanov, M. A., Mikhail Alekseevich;Korner, J. G., Jurgen;Lyubovitskiy (Lyubovitskij), V. E., physicist, Professor of Tomsk Polytechnic University, Doctor of physical and mathematical sciences, Professor of the University of Tubingen (Germany), 1963-, Valery EfimovichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет (ТПУ), Физико-технический институт (ФТИ), Кафедра высшей математики и математической физики (ВММФ)Язык: английский.Страна: .Резюме или реферат: We present a study of the isospin-violating one-pion strong decays of single heavy tetraquarks XQ=X(sqq¯Q¯), Q=c, b, and q=u, d with spin-parity JP=0+. We assume that the tetraquarks have the configuration of a color diquark and an antidiquark. Three mechanisms of isospin violation can contribute to the decay rate: (1) mixing of the X(suu¯Q¯) and X(sdd¯Q¯) tetraquark currents, (2) an explicit md−mu quark mass difference in the quark diagrams describing the corresponding decay transitions, and (3) π0−η mixing in the final state. Our main results are as follows: (1) It is quite likely that the investigated tetraquark states are isosinglet states with a small admixture of an isotriplet component; (2) The first isospin-breaking mechanism affects the decay rather more significantly than the others; (3) Our calculations contain a size parameter ΛXQ, characterizing the distribution of the quarks in the tetraquark state XQ. Absolute decay rates depend very much on the choice of ΛXQ, varied from 1 to 2 GeV, reflecting the compactness of the multiquark system..Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | изоспин | нарушение | распады Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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We present a study of the isospin-violating one-pion strong decays of single heavy tetraquarks XQ=X(sqq¯Q¯), Q=c, b, and q=u, d with spin-parity JP=0+. We assume that the tetraquarks have the configuration of a color diquark and an antidiquark. Three mechanisms of isospin violation can contribute to the decay rate: (1) mixing of the X(suu¯Q¯) and X(sdd¯Q¯) tetraquark currents, (2) an explicit md−mu quark mass difference in the quark diagrams describing the corresponding decay transitions, and (3) π0−η mixing in the final state. Our main results are as follows: (1) It is quite likely that the investigated tetraquark states are isosinglet states with a small admixture of an isotriplet component; (2) The first isospin-breaking mechanism affects the decay rather more significantly than the others; (3) Our calculations contain a size parameter ΛXQ, characterizing the distribution of the quarks in the tetraquark state XQ. Absolute decay rates depend very much on the choice of ΛXQ, varied from 1 to 2 GeV, reflecting the compactness of the multiquark system.

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