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The extrapolation of the decay amplitudes of the pseudoscalar mesons into two photons from the soft meson limit where it is obtained from the axial-anomaly to the mass shell involves the contribution of the 0^ - continuum. These chiral…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Nasrallah

The scalar and vector meson exchange contributions to the doubly radiative decays $\eta^{(\prime)}\to\pi^0\gamma\gamma$ and $\eta^\prime\to\eta\gamma\gamma$ are analysed within the Linear Sigma Model and Vector Meson Dominance frameworks,…

High Energy Physics - Phenomenology · Physics 2020-09-02 Rafel Escribano , Sergi Gonzàlez-Solís , Renata Jora , Emilio Royo

Motivated by recent experimental advancements in the study of radiative decays of charmed mesons, we investigate the magnetic (transition) moments of vector mesons by applying the effective mass scheme, obtained from the one-gluon exchange…

High Energy Physics - Phenomenology · Physics 2025-09-03 Binesh Mohan , Christas Mony A. , Rohit Dhir

We study the medium modifications of the spectral functions as well as production cross-sections of the strange vector mesons ($\phi$, $K^*$ and $\bar {K^*}$) in isospin asymmetric strange hadronic matter. These are obtained from the…

Nuclear Theory · Physics 2021-04-14 Amruta Mishra , S. P. Misra

We have studied the $P\to\gamma^\star\gamma^\star$ form factor in Resonance Chiral Theory, with $P = \pi^0\eta\eta'$, to compute the contribution of the pseudoscalar pole to the hadronic light-by-light piece of the anomalous magnetic moment…

High Energy Physics - Phenomenology · Physics 2019-09-04 Adolfo Guevara , Juan José Sanz Cillero , Pablo Roig

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

Cabibbo-allowed charmed meson decays into a pseudoscalar meson and an axial-vector meson are studied. The charm to axial-vector meson transition form factors are evaluated in the Isgur-Scora-Grinstein-Wise quark model. The dipole momentum…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hai-Yang Cheng

The recent precise measurements of the $e^+e^-\to K_SK_L$ and $e^+e^-\to K^+K^-$ cross sections and the hadronic spectral function of the $\tau^-\to K^-K_S\nu_\tau$ decay are used to extract the isoscalar and isovector electromagnetic kaon…

High Energy Physics - Phenomenology · Physics 2020-01-08 K. I. Beloborodov , V. P. Druzhinin , S. I. Serednyakov

The light axial-vector resonances $a_1(1260)$ and $b_1(1235)$ are explored in Nf=2 lattice QCD by simulating the corresponding scattering channels $\rho\pi$ and $\omega\pi$. Interpolating fields $\bar{q} q$ and $\rho\pi$ or $\omega\pi$ are…

High Energy Physics - Lattice · Physics 2014-06-02 C. B. Lang , Luka Leskovec , Daniel Mohler , Sasa Prelovsek

We analyze charm meson semileptonic decays using the measured ratios $\Gamma_L/\Gamma_T$ and $\Gamma_{+}/\Gamma_{-}$ from $D\to {\bar K}^{*}$ and the branching ratios for $D \to {\bar K}^{*}$ and $D \to {\bar K}$. First we introduce the…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Bajc , S. Fajfer , R. J. Oakes

We relate here the vacuum structure of chiral symmetry breaking to a wide class of low energy hadronic properties to examine consistency with experimental results. Phase transition of chiral symmetry breaking is described through explicit…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. P. Misra

The recent measurement of the tau -> Ks pion nu_tau spectrum by the Belle Collaboration provides the frame to set forth a theoretical description of the decay, which is based on the contributing vector F_+(s) and scalar F_0(s) form factors.…

High Energy Physics - Phenomenology · Physics 2009-04-30 J. Portoles

In this talk we study the low-energy effective couplings generated by strongly-coupled electroweak models that contain heavy composite resonances. Invariance under $SU(2)_L\times SU(2)_R$ is a key ingredient in the construction of the…

High Energy Physics - Phenomenology · Physics 2015-11-13 J. J. Sanz-Cillero

We perform a theoretical study of the $\chi_{cJ} \to \phi K^* \bar K \to \phi K\pi \bar K$ reaction taking into account the $K^* \bar K$ final state interaction, which in the chiral unitary approach is responsible, together with its coupled…

High Energy Physics - Phenomenology · Physics 2019-08-14 Sheng-Juan Jiang , S. Sakai , Wei-Hong Liang , E. Oset

The charged $K_{\ell 4}$ decay, $K^+\to\pi^+\pi^-\ell^+\nu_{\ell}$ is studied in the framework of chiral perturbation theory based on the effective Lagrangian including mesons, photons, and leptons. We give analytic expressions for the two…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Cuplov , A. Nehme

Hadronic electromagnetic form factors and radiative decay properties offer a crucial window into the nonperturbative dynamics of Quantum chromodynamics (QCD). In this work, we employ the light-cone sum rules (LCSR) method to systematically…

High Energy Physics - Phenomenology · Physics 2026-05-11 Zhi Jun Wang , Di Gao , Kai Kai Zhang , Yuan Yuan Ma , Yan Jun Sun

It is pointed out that the radiative decays of a $\phi$ meson, $\phirho$ and $\phiom$, receive dominant contributions from the pseudoscalar ($P = \eta, \eta^{'}$) exchanges. Using the vector meson dominance model, we find that $B (\phirho)…

High Energy Physics - Phenomenology · Physics 2009-10-28 Pyungwon Ko , Jungil Lee , H. S. Song

It is shown that a chiral quark model of the Nambu--Jona-Lasinio type can be used to describe "soft"-momenta parts of the amplitudes with large momentum transfer. As a sample, the processes \gamma^* --> \gamma (\pi,\eta,\eta') where one of…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. E. Dorokhov , M. K. Volkov , V. L. Yudichev

We present a phenomenological study of the $\gamma\gamma^*\to K\bar{K}^*(892)$ process by including the $s$-channel production of the $\eta(1475)$ and $f_1(1420)$ resonances. The non-resonant channel via $K$- and $K^*$-exchanges is…

High Energy Physics - Phenomenology · Physics 2024-08-22 Xiu-Lei Ren , Igor Danilkin , Marc Vanderhaeghen
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