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The predictions of the hypercentral Consituent Quark Model for the nucleon helicity amplitudes are briefly reported. Some future perspectives are also discussed.

Nuclear Theory · Physics 2015-06-22 M. M. Giannini

A constituent quark model based on the spectator formalism is applied to the gamma N -> N* transition for the three cases, where N* is the nucleon, the Delta and the Roper resonance. The model is covariant, and therefore can be used for the…

High Energy Physics - Phenomenology · Physics 2017-08-23 G. Ramalho , Franz Gross , M. T. Pena , K. Tsushima

It is shown that the helicity amplitudes A_1/2 and S_1/2 in the gamma N -> N(1535) reaction, can be well related by S_1/2 = -\frac{\sqrt{1+\tau}}{\sqrt{2}} \frac{M_S^2-M^2}{2 M_S Q} A_1/2 in the region Q^2 > 2 GeV^2, where M and M_S are the…

High Energy Physics - Phenomenology · Physics 2011-09-29 G. Ramalho , K. Tsushima

We develop a covariant model for the $\gamma^\ast N \to N(1535)$ transition in the timelike kinematical region, the region where the square momentum transfer $q^2$ is positive. Our starting point is the covariant spectator quark model…

High Energy Physics - Phenomenology · Physics 2020-06-16 G. Ramalho , M. T. Peña

Recent experimental and theoretical advancements have led to significant progress in our understanding of the electromagnetic structure of nucleons ($N$), nucleon excitations ($N^\ast$), and other baryons. These breakthroughs have been made…

High Energy Physics - Phenomenology · Physics 2024-03-12 G. Ramalho , M. T. Peña

In the nucleon electroexcitation reactions, $\gamma^\ast N \to R$, where $R$ is a nucleon resonance ($N^\ast$), the electric amplitude $E$, and the longitudinal amplitude $S_{1/2}$, are related by $E \propto \frac{\omega}{|{\bf…

High Energy Physics - Phenomenology · Physics 2016-06-17 G. Ramalho

In this work, we will evaluate the nucleon helicity flip form factor at the limit of large momentum transfer. Hereby, we will study the exchange of one and two virtual photons separately. For the calculation of the scattering amplitudes and…

High Energy Physics - Phenomenology · Physics 2011-11-09 Thorsten Sachs , Patrick Sturm

The helicity amplitudes for the transitions $N-S_{11}$ and $N-S_{31}$ are presented. The amplitudes have been obtained within our front-form CQM model, based on hadron eigenstates of a relativistic mass operator and CQ current with Dirac…

Nuclear Theory · Physics 2011-04-15 E. Pace , G. Salme` , S. Simula

The form factors, as well as the helicity amplitudes for the $\gamma^\ast N \to N(1535)$ transition are calculated in framework of the QCD light cone sum rules. The contamination coming from diagonal transition is eliminated by considering…

High Energy Physics - Phenomenology · Physics 2013-09-24 T. M. Aliev , M. Savci

We report on the determination of the electrocouplings for the transition from the proton to the $N(1675){\frac{5}{2}}^-$ resonance state using recent differential cross section data on $e p \rightarrow e\pi^+ n$ by the CLAS collaboration…

Nuclear Theory · Physics 2015-07-15 I. G. Aznauryan , V. D. Burkert

The covariant spectator quark model, tested before in a variety of electromagnetic baryon excitations, is applied here to the $\gamma^\ast N \to N^\ast(1520)$ reaction in the timelike regime. The transition form factors are first…

Nuclear Theory · Physics 2017-01-10 G. Ramalho , M. T. Peña

We discuss how electromagnetic properties provide useful tests of the nature of resonances, and we study these properties for the N*(1535) which appears dynamically generated from the strong interaction of mesons and baryons. Within this…

Nuclear Theory · Physics 2008-11-26 D. Jido , M. Doering , E. Oset

We apply the perturbative chiral quark model to the gamma N -> Delta transition. The four momentum dependence of the respective transverse helicity amplitudes A(1/2) and A(3/2) is determined at one loop in the pseudoscalar Goldstone boson…

High Energy Physics - Phenomenology · Physics 2009-11-10 K. Pumsa-ard , V. E. Lyubovitskij , Th. Gutsche , Amand Faessler , S. Cheedket

The unitary isobar model MAID has been extended and used for a partial wave analysis of pion photo- and electroproduction in the resonance region W < 2 GeV. Older data from the world data base and more recent experimental results from…

Nuclear Theory · Physics 2015-06-26 L. Tiator , D. Drechsel , S. Kamalov , M. M. Giannini , E. Santopinto , A. Vassallo

We present results for the invariant and helicity amplitudes in the transitions $\Lambda_b\to\Lambda^{(\ast)}(J^P)+J/\psi$ where the $\Lambda^{(\ast)}(J^P)$ are $\Lambda(sud)$-type ground and excited states with $J^P$ quantum numbers…

High Energy Physics - Phenomenology · Physics 2017-11-30 Mikhail A. Ivanov

We report on the recent results of the hypercentral constituent quark model. The model contains a spin independent three-quark interaction which is inspired by QCD lattice calculations and reproduces the average energy values of the SU(6)…

Nuclear Theory · Physics 2017-08-23 M. M. Giannini , E. Santopinto , A. Vassallo

A covariant spectator quark model is applied to estimate the valence quark contributions to the$ F1*(Q2) and F2*(Q2) transition form factors for the gamma N -> P11(1440) reaction. The Roper resonance, P11(1440), is assumed to be the first…

High Energy Physics - Phenomenology · Physics 2015-05-20 G. Ramalho , K. Tsushima

The Roper resonance is described in a chiral version of the chromodielectric model as a cluster of three quarks in radial-orbital configuration (1s)$^2$(2s)$^1$, surrounded by $\pi$ and $\sigma$-meson clouds and by a chromodielectric field…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. Alberto , M. Fiolhais , B. Golli , J. Marques

We present a study of the $N^*(1535)$ resonance electroexcitation in a soft-wall AdS/QCD model. Both the transverse $A_{1/2}^p$ and longitudinal $S_{1/2}^p$ helicity amplitudes are calculated resulting in good agreement with data and with…

High Energy Physics - Phenomenology · Physics 2020-02-26 Thomas Gutsche , Valery E. Lyubovitskij , Ivan Schmidt

We present an alternative approach for calculating helicity amplitudes for processes involving both massless and massive fermions. With this method one can easily obtain covariant expressions for the helicity amplitudes. The final…

High Energy Physics - Phenomenology · Physics 2014-11-17 R. Vega , J. Wudka