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Related papers: Comparing the Broken U3xU3 Linear Sigma Model with…

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The quark-level linear sigma model is revisited, in particular concerning the identification of the f_0(400-1200) (or \sigma(600)) scalar meson as the chiral partner of the pion. We demonstrate the predictive power of the linear sigma model…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eef van Beveren , Frieder Kleefeld , George Rupp , Michael D. Scadron

The suggestion by Jaffe that if $\sigma$ is a light $q^{2}\bar{q}^{2}$ state $0^{++}$ then even the fundamental chiral transformation properties of the $\sigma$ becomes {\bf unclear}, has stimulated much interest. Adler pointed out that in…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. F. Tuan

By analyzing the meson spectra obtained in the constituent quark model, we find that the pseudoscalar mesons $\eta'(2^1S_0)$, $\eta(4^1S_0)$, $\eta'(3^1S_0)$ and $\eta'(4^1S_0)$ are the possible candidates of $\eta(1760)$, X(1835), X(2120)…

High Energy Physics - Phenomenology · Physics 2011-11-16 Shaona Chen , Jialun Ping

The SU(3) linear sigma model is dynamically generated in loop-order using the nonstrange-strange basis. Only self-consistent logarithmic divergent graphs are needed, with quadratic divergent graphs replaced by SU(3) mass-shell equal…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dalibor Kekez , Dubravko Klabucar , Michael D. Scadron

In the SU(3) symmetry limit, the ratio $R\equiv\frac{{\cal B}(D^+\to f_0l^+\nu)+ {\cal B}(D^+\to \sigma l^+\nu)}{{\cal B}(D^+\to a_0^0l^+\nu)}$ is equal to 1 if the scalar mesons are $\bar qq$ states, while it is 3 if these mesons are…

High Energy Physics - Phenomenology · Physics 2014-11-21 Cai-Dian Lu , Wei Wang

The available data on the a0(980), f0(980), f0(1300) and K*0(1430) mesons are fitted as a distorted 0++ nonet using only 6 parameters and a very general model. This includes all light two-pseudoscalar thresholds, constraints from Adler…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nils Tornqvist

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

Although eta-eta' mixing is qualitatively well understood as a consequence of the U(1)_A anomaly in QCD together with a broken SU(3) flavor symmetry, until recently the values of decay and mixing parameters of the eta and eta' were only…

High Energy Physics - Phenomenology · Physics 2009-10-31 Thorsten Feldmann

Within the increasing experimental evidence of the existence of the I=0 scalar low mass and wide \sigma meson, we review the {\it first} analysis of its quark and gluon substructure from QCD spectral sum rules and some low-energy theorems.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stephan Narison

The eta to 3 pion decays are a valuable source of information on low energy QCD. Yet they were not used for an extraction of the chiral symmetry breaking order parameters until now. We use a bayesian approach in the framework of resummed…

High Energy Physics - Phenomenology · Physics 2014-09-12 Marian Kolesar , Jiri Novotny

Non--resonant decays of charmed mesons into three pseudoscalars are analyzed in a weak gauged $U(4)_L \otimes U(4)_R$ chiral lagrangian model. The calculation is free of unknown parameters and only requires the masses of pseudoscalar mesons…

High Energy Physics - Phenomenology · Physics 2009-10-28 F. J. Botella , S. Noguera , J. Portoles

We consider how the recent CMS measurements of the masses and quantum numbers of $X(6600)$, $X(6900)$ and $X(7100)$ can help to reveal the internal structure of these apparent $cc\bar{c}\bar{c}$ tetraquark states. The measured $J^{PC} =…

High Energy Physics - Phenomenology · Physics 2026-05-06 Muhammad Naeem Anwar , Timothy J. Burns

Recently in arXiv:hep-ph/0510321 has been proposed a GUT model for fermion masses and mixings with spontaneously broken S3 discrete flavor symmetry, where S_3 is the permutation group of three objects. The S3 breaking pattern in the quark…

High Energy Physics - Phenomenology · Physics 2015-06-25 Stefano Morisi

Taken by itself, the interference with the etaprime appears to strongly affect the amplitude of the transition eta->3 pi. I point out that this effect is fictitious and also occurs in the mass spectrum of the pseudoscalars. Chiral symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-28 H. Leutwyler

We compute masses, trilinear self-couplings and decay widths into weak bosons of the scalar composite bosons in the case of the Minimal and Ultraminimal technicolor models. The masses, computed via the Bethe-Salpeter equation, turn out to…

High Energy Physics - Phenomenology · Physics 2014-11-20 A. Doff , A. A. Natale

We investigate three classes of supersymmetric models which can be obtained by breaking the chiral SU(2k+3) gauge theories with one antisymmetric tensor and 2k-1 antifundamentals. For N=3, the chiral SU(2k)$\times$SU(3)$\times$U(1) theories…

High Energy Physics - Theory · Physics 2009-10-30 Chih-Lung Chou

The sector of decay constants of the octet of light pseudoscalar mesons in the framework of 'resummed' $SU(3)$ chiral perturbation theory is investigated. A theoretical prediction for the decay constant of $\eta$-meson is compared to a…

High Energy Physics - Phenomenology · Physics 2024-01-30 Marián Kolesár , Jaroslav Říha

We present the latest preliminary results of the MILC collaboration's analysis of the light pseudoscalar meson sector. The analysis includes data from new ensembles with smaller lattice spacings, smaller light quark masses and…

The same, well known, det(Sigma)+ h.c. term in effective theories, which 't Hooft showed is generated by instantons in QCD and which resolves the UA(1) problem giving mass, in particular to the $\eta'$ is for three light flavors shown to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Nils A. Tornqvist

We study the role of a possible nonet of light scalar mesons in the still interesting $\eta \to 3\pi$ decay process, with the primary motivation of learning more about the scalars themselves. The framework is a conventional non-linear…

High Energy Physics - Phenomenology · Physics 2008-11-26 Abdou M. Abdel-Rehim , Deirdre Black , Amir H. Fariborz , Joseph Schechter