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Related papers: Scalar meson exchange in phi->P0P0gamma decays

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We make a theoretical study of the $\J$ decays into $\omega\pi\pi$, $\phi\pi\pi$, $\omega K \bar{K}$ and $\phi K\bar{K}$ using the techniques of the chiral unitary approach stressing the important role of the scalar resonances dynamically…

High Energy Physics - Phenomenology · Physics 2009-11-10 L. Roca , J. E. Palomar , E. Oset , H. C. Chiang

The following topics are considered. 1. Confinement, chiral dynamics and light scalar mesons. 2. $\phi$-meson radiative decays about nature of light scalar resonances. Arguments in favor of the four-quark model of the $a_0(980)$ and…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. N. Achasov

Radiative decays of the $\phi$ meson have been studied using a data sample of about 19 million $\phi$ decays collected by the CMD-2 detector at VEPP-2M collider in Novosibirsk. From selected $e^+e^-\to\pi^{0}\pi^{0}\gamma$ and…

High Energy Physics - Experiment · Physics 2008-11-26 2 Collaboration

New high statistics Belle data on the $\gamma\gamma\to\pi^+\pi^-$ reaction cross section measured in the range of pion-pair invariant masses $\sqrt{s}$ between 0.8 GeV and 1.5 GeV are analyzed to clarify the current situation around the…

High Energy Physics - Phenomenology · Physics 2008-11-26 N. N. Achasov , G. N. Shestakov

We calculate low-energy meson decay processes and pion-pion scattering lengths in a globally chirally invariant two-flavour linear sigma model exploring the quark content of the scalar mesons f(0)(600) and a(0)(980), as well as f(0)(1370)…

High Energy Physics - Phenomenology · Physics 2010-04-28 Denis Parganlija , Francesco Giacosa , Dirk H. Rischke

Two photon decay widths of the $J^P = O^+$ scalar mesons $a_{0} (980)$, $f_{0}(980)$, $f_{0}(1370)$ and $\chi_{c0}$ are calculated in a covariant model which is characterized by the quark - antiquark structure. Previously such models were…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Fajfer , D. Horvatic , D. Tadic , S. Zganec

A phenomenological analysis of the scalar meson f0(980) is performed that relies on the quasi-two body decays D and Ds -> f0(980)P, with P=pi, K. The two-body branching ratios are deduced from experimental data on D or Ds -> pi pi pi, K…

High Energy Physics - Phenomenology · Physics 2009-04-22 B. El-Bennich , O. Leitner , J. -P. Dedonder , B. Loiseau

We present a general framework for the model-independent decomposition of the fully differential cross section of the reactions e+e- -> gamma* -> (pi0 pi0 gamma) and e+e- -> gamma* -> (pi0 eta gamma), which can provide important information…

High Energy Physics - Phenomenology · Physics 2010-09-21 S. Eidelman , S. Ivashyn , A. Korchin , G. Pancheri , O. Shekhovtsova

We analyze the electromagnetic and strong decay properties of the light scalars a0(980) and f0(980) within a hadronic molecule interpretation. Both scalars are discussed within a covariant and gauge invariant model which also allows for…

High Energy Physics - Phenomenology · Physics 2008-12-18 Tanja Branz , Thomas Gutsche , Valery E. Lyubovitskij

Rare radiative decay $\phi\to\eta\pi^0\gamma$ was studied with SND detector at {VEPP-2M} electron-positron collider and its branching ratio was measured: $B(\phi\to\eta\pi^0\gamma)=(0.88\pm0.14\pm0.09)\cdot 10^{-4}$. Significant…

We work out the Linear Sigma Model (LSM) predictions for the 2 gamma decay rates of the a_0(980),f_0(980) mesons under the assumption that they are respectively the I=1 and I=0 members of the bar q q scalar nonet. Agreement with…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. L. Lucio Martinez , M. Napsuciale Mendivil

Using the chiral unitary approach in coupled channels and $SU(3)$ symmetry we describe the production of $f_0(500)$, $f_0(980)$ and $a_0(980)$ in the $\chi_{c1} \to \eta \pi^+ \pi^-$ reaction, recently performed by the BESIII collaboration.…

High Energy Physics - Phenomenology · Physics 2018-04-03 V. R. Debastiani , Wei-Hong Liang , Ju-Jun Xie , E. Oset

The scalar meson f_0(1370) - indicated in particular in the low energy p\bar p \to 3 body reactions - is a crucial element in certain schemes of the scalar meson spectroscopy including glueballs. The most definitive results can be obtained…

High Energy Physics - Phenomenology · Physics 2015-05-18 Wolfgang Ochs

We review how a certain effective chiral Lagrangian approach to pi pi scattering, pi K scattering and eta-prime decay to eta pi pi provides evidence for the existence of light scalars sigma(550) and kappa(900) as well as describing the…

High Energy Physics - Phenomenology · Physics 2010-12-13 Deirdre Black , Amir H. Fariborz , Joseph Schechter

We reexamine the $\omega \to \pi^{0} \pi^{0} \gamma $ decay, adding the effect of $\omega-\rho$ mixing to the amplitude calculated with the aid of chiral perturbation theory and vector meson dominance. We predict the neutral decay to occur…

High Energy Physics - Phenomenology · Physics 2009-10-31 Dafne Guetta , Paul Singer

The role of light scalar meson `$f_0 (600)$' is investigated in nuclear matter in an Effective chiral model in the mean-field approach. For the purpose, we scan the properties of the matter at various saturation densities imposing…

Nuclear Theory · Physics 2009-06-01 T. K. Jha

The potentialities of the production of the $a_0(980)$ and $f_0(980)$ mesons in the $\phi$ radiative decays are considered.

High Energy Physics - Phenomenology · Physics 2007-05-23 N. N. Achasov , V. V. Gubin

In the SND experiment at the VEPP-2M electron-positron collider the PHI(1020)--->PI0+PI0+GAMMA decay was studied. The branching ratio B(PHI--->PI0+PI0+GAMMA)=(1.14+-0.10+-0.12)x10^{-4} was measured. It was shown, that the F0(980)GAMMA…

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

We analyze the experimental data for $\phi\to f_0(980)\gamma$, $\phi\to a_0(980)\gamma$, $f_0(980)\to\gamma\gamma$ and $a_0(980)\to\gamma\gamma$ decay widths in a framework where $f_0(980)$ and $a_0(980)$ are assumed to be mainly…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Teshima , I. Kitamura , N. Morisita
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