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Underlying mixing of scalar mesons is studied in $\eta'\rightarrow \eta\pi\pi$ decay within a generalized linear sigma model of low-energy QCD which contains two nonets of scalar mesons and two nonets of pseudoscalar mesons (a…

High Energy Physics - Phenomenology · Physics 2015-06-22 Amir H. Fariborz , Joseph Schechter , Soodeh Zarepour , Mohammad Zebarjad

Based on the recently proposed Roy-Steiner equations for pion-nucleon scattering, we derive a system of coupled integral equations for the pi pi --> N-bar N and K-bar K --> N-bar N S-waves. These equations take the form of a two-channel…

High Energy Physics - Phenomenology · Physics 2012-06-13 M. Hoferichter , C. Ditsche , B. Kubis , U. -G. Meißner

First I review some previous work on the lightest scalars below 1.5 GeV, and how these scalars can be understood as unitarized nonet states. The bare scalars are strongly distorted by hadronic mass shifts, and the lightest I=0 state becomes…

High Energy Physics - Phenomenology · Physics 2016-09-06 Nils A. Tornqvist

Within a linear sigma model framework, possible mixing between two chiral nonets (a two quark nonet, and a four quark nonet) below 2 GeV is studied. Incorporating the U(1)$_A$ behavior of the underlying QCD, and working in the isospin…

High Energy Physics - Phenomenology · Physics 2007-05-23 Amir H. Fariborz , Renata Jora , Joseph Schechter

We first review the work of the Syracuse group, which uses an effective chiral Lagrangian approach, on meson-meson scattering. An illustration providing evidence for the existence of a strange scalar resonance of mass around 900 MeV is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Deirdre Black , Amir H. Fariborz , Joseph Schechter

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…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amir H. Fariborz

We consider mixing of the antidecuplet with three J^P=1/2^+ octets (the ground-state octet, the octet containing N(1440), \Lambda(1600), \Sigma(1660) and \Xi(1690) and the octet containing N(1710), \Lambda(1800), \Sigma(1880) and \Xi(1950))…

High Energy Physics - Phenomenology · Physics 2009-11-11 V. Guzey , M. V. Polyakov

We show that the application of Regge phenomenology to SU(4) meson multiplets leads to a new Gell-Mann-Okubo mass-mixing formula in the SU(3) sector, 3m_1^2 + (cos theta)^2 m_0^2 + (sin theta)^2 m_{0'}^2 + sqrt{2} sin(2theta) (m_0^2 -…

High Energy Physics - Phenomenology · Physics 2007-05-23 L. Burakovsky , T. Goldman

Our method of analysis, which led to existence of sigma and kappa mesons, is reviewed and examined from a viewpoint of general S-matrix. It is shown that the method is consistent with the constraints from chiral symmetry and unitarity.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Muneyuki Ishida , Shin Ishida

We enforce chiral Ward identities on the vertices of the linear sigma model to take into account the width of the scalar sigma, considered as a true physical resonance. We consider pion scattering at very low energies and, from a fit to the…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. L. Lucio , M. Napsuciale , M. Ruiz-Altaba

We study the feasibility of having the $\Sigma^*(1430)$ state, predicted within the chiral unitary approach and recently reported by the Belle Collaboration, as corresponding to a state of non-molecular nature. Starting from this…

High Energy Physics - Phenomenology · Physics 2025-05-22 Jia-Xin Lin , Jing Song , Miguel Albaladejo , Albert Feijoo , Eulogio Oset

The radiative $\phi\to\pi^0\eta\gamma$ decay is discussed emphasizing the effects of the $a_0$(980) scalar resonance which dominates the high values of the $\pi^0\eta$ invariant mass spectrum. In its lowest part, the proposed amplitude…

High Energy Physics - Phenomenology · Physics 2009-09-24 A. Bramon , R. Escribano , J. L. Lucio M. , M. Napsuciale , G. Pancheri

Scalar-isoscalar mesons are studied using an unitary model in three channels: pi-pi, K-anti K and an effective 2pi-2pi. All the solutions, fitted to the pi-pi and K-anti K data, exhibit a wide f0(500), a narrow f0(980) and two relatively…

High Energy Physics - Phenomenology · Physics 2016-09-06 R. Kaminski , L. Lesniak , B. Loiseau

We present that there should exist a light strange-scalar meson kappa', in addition to the kappa(800), which has a mass around 1.1-1.2 GeV, a rather narrow width, and couples strongly to kappa(800)sigma(600) (Kpipipi) but weakly to Kpi,…

High Energy Physics - Phenomenology · Physics 2007-12-06 Kenji Yamada , Tomohito Maeda

The formulae needed to parametrise sigma, kappa, a0(980) and f0(980) are reviewed. For sigma and kappa, the Adler zero due to Chiral Symmetry Breaking plays a crucial role. The f0(980) and a0(980) are locked to the KK threshold by a cusp…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. V. Bugg

The complementarity between Chiral Perturbation Theory and the Linear Sigma Model in the scalar channel is exploited to study $\pi^0\pi^0$ production in $\rho$ and $\omega$ radiative decays, where the effects of a low mass scalar resonance…

High Energy Physics - Phenomenology · Physics 2009-09-24 A. Bramon , R. Escribano , J. L. Lucio M. , M. Napsuciale

We investigate the $a_0(980)$ resonance within chiral effective field theory through a three-coupled-channel analysis, namely $\pi\eta$, $K\bar{K}$ and $\pi\eta'$. A global fit to recent lattice finite-volume energy levels from $\pi\eta$…

High Energy Physics - Phenomenology · Physics 2017-03-15 Zhi-Hui Guo , Liuming Liu , Ulf-G. Meißner , J. A. Oller , A. Rusetsky

A consistent description of the pi0 pi0 invariant mass distribution in the phi(1020) -> f0(980) gamma -> pi0 pi0 gamma decay and the pi0 eta in phi(1020) -> a0(980) gamma -> pi0 eta gamma is suggested. A search for the consequences of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Ivashyn , A. Korchin

In the I=0 sector there are more scalar mesons than can fit in one $q{\bar q}$ nonet. Consequently, many have claimed that there is in fact more than one multiplet, perhaps both $q{\bar q}$ and $qq{\bar {qq}}$. Such proposals require the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. N. Cherry , M. R. Pennington

A novel, nonperturbative, way to generate chiral symmetry breaking within the linear sigma model for 3 flavours is discussed. After spontaneous chiral symmetry breaking in the vacuum at the tree level the scalar nonet obtains mass, while…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nils A. Tornqvist