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Related papers: Roper resonance in a quark-diquark model

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The standard description of the nucleon in the non-relativistic quark model is an $1S,L=0$ state without orbital motion. Yet, there are several indications from phenomenology that an admixture of states with nonzero orbital motion maybe…

High Energy Physics - Phenomenology · Physics 2025-03-18 Nicholas Miesch , Edward Shuryak , Ismail Zahed

Analyses of the three valence-quark bound-state problem in relativistic quantum field theory predict that the nucleon may be understood primarily as a Borromean bound-state, in which binding arises mainly from two separate effects. One…

Nuclear Theory · Physics 2015-09-30 Jorge Segovia , Craig D. Roberts , Sebastian M. Schmidt

In a relativistic quark model we study the structure of the $N(1710)$ resonance, and the $\gamma^\ast N \to N(1710)$ reaction focusing on the high momentum transfer region, where the valence quark degrees of freedom are expected to be…

High Energy Physics - Phenomenology · Physics 2014-04-14 G. Ramalho , K. Tsushima

The $\rho(770)$ vector resonance, its radial recurrences, and the corresponding P-wave $\pi\pi$ phase shifts are investigated in an unquenched quark model with all classes of relevant decay channels included, viz. pseudoscalar-pseudoscalar,…

High Energy Physics - Phenomenology · Physics 2015-12-09 Susana Coito , George Rupp , Eef van Beveren

We develop a formally covariant quark-diquark model of the nucleon. The nucleon is treated as a bound state of a constituent quark and a diquark interacting via a quark exchange. We include both scalar and axial-vector diquarks. The…

Nuclear Theory · Physics 2007-05-23 Volker Keiner

Treating the quark and diquark as elementary particles, the Bethe-Salpeter equation for the nucleon is solved numerically. The dependence of the mass on the diquark mass and on the coupling constants is investigated. The resulting…

Nuclear Theory · Physics 2009-10-28 H. Meyer

In this paper we develop a theoretical framework which allows us to study excitations of the nucleon. Assuming an effective two-body interaction as a model for low-energy QCD, we derive a relativistic TDHF equation for a many-body system of…

High Energy Physics - Phenomenology · Physics 2016-09-01 S. Hardt , J. Geiss , H. Lenske , U. Mosel

In this work, the spectrum of ground state and excited baryons (N, {\Delta}, , , and {\Omega} particles) has been investigated by using a non-relativistic quantum mechanics under the Killingbeck plus isotonic oscillator potentials. Using…

Nuclear Theory · Physics 2016-09-06 Nasrin Salehi

Vibrations of the Jeffcott rotor are modelled by a three degree of freedom system including coupling between lateral and torsional modes. The crack in a rotating shaft of the rotor is introduced via time dependent stiffness with off…

Chaotic Dynamics · Physics 2015-05-13 Grzegorz Litak , Jerzy T. Sawicki

A new mechanism for the pp --> pp pi0 reaction close to threshold is suggested coming from the isoscalar excitation of the Roper and its decay into N(pi pi)S-wave, with one of the pi0 emitted and the other one reabsorbed on the second…

Nuclear Theory · Physics 2009-10-31 E. Hernandez , E. Oset

We introduce diquarks as separable correlations in the two-quark Green's function to facilitate the description of baryons as relativistic three-quark bound states. These states then emerge as solutions of Bethe-Salpeter equations for…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Oettel

We propose a four-quark structure for some of the excited states of heavy mesons containing a single charm or bottom quark. The four-quark wave functions are constructed based on a diquark-antidiquark form under the constraint that they…

High Energy Physics - Phenomenology · Physics 2015-06-22 Hungchong Kim , Myung-Ki Cheoun , Yongseok Oh

Masses of the ground and excited (1P, 2S, 1D, 2P, 3S) states of the fully-heavy tetraquarks, composed of charm ($c$) and bottom ($b$) quarks and antiquarks, are calculated in the diquark-antidiquark picture within the relativistic quark…

High Energy Physics - Phenomenology · Physics 2022-12-14 R. N. Faustov , V. O. Galkin , E. M. Savchenko

We study positive and negative parity nucleons on the lattice using the chirally improved lattice Dirac operator. Our analysis is based on a set of three operators chi_i with the nucleon quantum numbers but in different representations of…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dirk Broemmel , Peter Crompton , Christof Gattringer , Leonid Ya. Glozman , C. B. Lang , Stefan Schaefer , Andreas Schaefer

The chromomagnetic interaction, with proper account for flavour-symmetry breaking, is shown to explain the mass and coupling properties of the X(3872) resonance as a $J^{PC}$ = 1$^{++}$ state consisting of a heavy quark-antiquark pair and a…

High Energy Physics - Phenomenology · Physics 2009-08-21 H. Hogaasen , J. M. Richard , P. Sorba

The firm understanding of standard quark-antiquark states (including excited states) is necessary to search for non-conventional mesons with the same quantum numbers. In this work, we study the phenomenology of two nonets of excited vector…

High Energy Physics - Phenomenology · Physics 2018-08-29 Milena Piotrowska , Francesco Giacosa

Assuming four-quark structure for the $X$ resonances in low-lying region, we calculate their masses using the color-spin interaction. In specific, the hyperfine masses of the color-spin interaction are calculated for the possible states in…

High Energy Physics - Phenomenology · Physics 2016-07-20 Hungchong Kim , K. S. Kim , Myung-Ki Cheoun , Daisuke Jido , Makoto Oka

We look for $\Delta\Delta$ and $N\Delta$ resonances by calculating $NN$ scattering phase shifts of two interacting baryon clusters of quarks with explicit coupling to these dibaryon channels. Two phenomenological nonrelativistic chiral…

Nuclear Theory · Physics 2009-11-13 J. L. Ping , H. X. Huang , H. R. Pang , Fan Wang , C. W. Wong

We investigate the $P$-wave states $T^-_{bb}$ in the isospin singlet and three excited modes [excitation occurring in the diquark $[bb]^{s_1}_{c_1}$ ($\rho $-mode), antidiquark $[\bar{u}\bar{d}]^{s_2}_{c_2}$ ($r$-mode) or between them…

High Energy Physics - Phenomenology · Physics 2024-03-08 Zu-Hang Lin , Chun-Sheng An , Cheng-Rong Deng

A chiral Lagrangian containing, besides the usual meson fields, their first radial excitations is constructed. The Lagrangian is derived by bosonization of a Nambu--Jona-Lasinio (NJL) type quark model with separable nonlocal interactions.…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. K. Volkov , V. L. Yudichev
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