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相关论文: Scalar Mesons in a Chiral Quark Model with Gluebal…

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In a U(3)x U(3) quark chiral model of the Nambu-Jona-Lasinio type with the 't Hooft interaction, the ground scalar isoscalar mesons and a scalar glueball are described. The glueball (dilaton) is introduced into the effective meson…

高能物理 - 唯象学 · 物理学 2007-05-23 M. Nagy , M. K. Volkov , V. L. Yudichev

An effective meson Lagrangian including a scalar glueball is constructed on the base of $U(3)\times U(3)$ chiral symmetry. The glueball is introduced into the meson Lagrangian by using the principle of scale invariance of an effective…

高能物理 - 唯象学 · 物理学 2008-11-26 M. K. Volkov , V. L. Yudichev

Ground and first radially excited scalar isoscalar meson states and a scalar glueball are described in a nonlocal U(3)xU(3) quark model. The glueball is introduced into the effective meson Lagrangian by means of the dilaton model on the…

高能物理 - 唯象学 · 物理学 2011-07-19 M. K. Volkov , V. L. Yudichev

We present a detailed study of the interactions among scalar and pseudoscalar mesons and glueballs within the framework of the generalized linear sigma model in the SU(3) flavor limit. The basis of our approach is to develop a global…

高能物理 - 唯象学 · 物理学 2021-08-25 Amir H. Fariborz , Mars Lyukova

We study the strong and electromagnetic decay properties of scalar mesons above 1 GeV within a chiral approach. The scalar-isoscalar states are treated as mixed states of quarkonia and glueball configurations. A fit to the experimental mass…

高能物理 - 唯象学 · 物理学 2008-11-26 F. Giacosa , Th. Gutsche , V. E. Lyubovitskij , Amand Faessler

We study the strong and electromagnetic decay properties of scalar mesons above 1 GeV within a chiral approach. The scalar-isoscalar states are treated as mixed states of quarkonia and glueball configurations. A fit to the experimental…

高能物理 - 唯象学 · 物理学 2008-11-26 F. Giacosa , Th. Gutsche , V. E. Lyubovitskij , Amand Faessler

We study the interactions of the pseudoscalar glueball with scalar and pseudoscalar quark-antiquark meson fields and with the nucleon and its chiral partner. In both cases we introduce the corresponding chiral Lagrangian and discuss its…

高能物理 - 唯象学 · 物理学 2012-09-19 Walaa. I. Eshraim , Stanislaus Janowski , Antje Peters , Klaus Neuschwander , Francesco Giacosa

We calculate the mass spectra of the pseudoscalar and scalar meson nonets in the Nambu--Jona-Lasinio model with the 't Hooft interaction. We obtain satisfactory result for the pseudoscalar mesons. For the scalar mesons, the 't Hooft…

高能物理 - 唯象学 · 物理学 2009-10-31 M. K. Volkov , M. Nagy , V. L. Yudichev

A scaled SU(3) Nambu - Jona-Lasinio Lagrangian is used to compute the mass of the nine scalar mesons in the vacuum and the mass of the gluball. It is shown that a suitable choice of the vacuum gluon condensate allows to reproduce the…

核理论 · 物理学 2007-05-23 M. Jaminon , B. Van den Bossche

The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. Two recent lattice results are employed as the starting point; one is the approximate SU(3) symmetry in the scalar sector above 1 GeV for the…

高能物理 - 唯象学 · 物理学 2007-05-23 Hai-Yang Cheng

The mixing angles between scalar isoscalar resonances and a scalar glueball are determined from their decays into two pseudoscalar mesons. For $f_0(1370)$ and $f_0(1500)$, at most a small glueball component is admitted by the data. The…

高能物理 - 唯象学 · 物理学 2022-03-14 Eberhard Klempt , Andrey V. Sarantsev

The highlights of studies of mixing among scalar mesons below and above 1 GeV within a nonlinear chiral Lagrangian framework is briefly presented. Two scalar meson nonets are introduced to explore the mass spectrum and decay properties of…

高能物理 - 唯象学 · 物理学 2008-11-26 Amir H. Fariborz

The isosinglet scalar mesons $f_0(1710)$, $f_0(1500)$, $f_0(1370)$ and their mixing are studied. We employ two recent lattice results as the starting point; one is the isovector scalar meson $a_0(1450)$ which displays an unusual property of…

高能物理 - 唯象学 · 物理学 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua , Keh-Fei Liu

Within a nonlinear chiral Lagrangian framework, the underlying mixings among quark-antiquark, four-quark and glue components of $f_0(1500)$ and $f_0(1710)$ are studied in a global picture that includes all isosinglet scalar mesons below 2…

高能物理 - 唯象学 · 物理学 2016-01-20 Amir H. Fariborz , Azizollah Azizi , Abdorreza Asrar

Within the framework of the generalized linear sigma model, a comprehensive analysis of scalar and pseudoscalar glueballs and their mixing with mesons is presented. The Lagrangian of the model contains two chiral nonets, a quark-antiquark…

高能物理 - 唯象学 · 物理学 2025-08-14 Amir H. Fariborz

We present a generalized linear sigma model that includes both scalar and pseudoscalar glueballs in addition to a quark-antiquark as well as a four-quark chiral nonet. Utilizing the axial and trace anomalies of QCD (at the effective mesonic…

高能物理 - 唯象学 · 物理学 2018-12-05 Amir H. Fariborz , Renata Jora

In a relativistic quark model with linear confinement and an instanton-induced interaction which solves the $\eta$-$\eta'$ puzzle, scalar mesons are found as almost pure SU(3) flavor states. This suggests a new interpretation of the scalar…

高能物理 - 唯象学 · 物理学 2008-11-26 E. Klempt , B. C. Metsch , C. R. Munz , H. R. Petry

Because glueballs are SU(3)_{Flavor} singlets, they are expected to couple equally to u,d, and s quarks, so that equal coupling strengths to \pi^+\pi^- and K^+K^- are predicted. However, we show that chiral symmetry implies the scalar…

高能物理 - 唯象学 · 物理学 2008-11-26 Michael Chanowitz

A chiral invariant Lagrangian describing the tetraquark-quarkonia interaction is considered at the leading and subleading order in the large-$N_{c}$ expansion. Spontaneous chiral symmetry breaking generates mixing of scalar tetraquark and…

高能物理 - 唯象学 · 物理学 2008-11-26 Francesco Giacosa

A chiral Lagrangian containing, besides the usual meson fields, their first radial excitations is constructed. The Lagrangian is derived by bosonization of a Nambu--Jona-Lasinio (NJL) type quark model with separable nonlocal interactions.…

高能物理 - 唯象学 · 物理学 2007-05-23 M. K. Volkov , V. L. Yudichev
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