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We employ a continuum approach to the three valence-quark bound-state problem in relativistic quantum field theory to predict a range of properties of the proton's radial excitation and thereby unify them with those of numerous other…

The properties of the Roper resonance N(1440) are reviewed. Quark models have long struggled to reproduce its mass relative to its negative-parity partner N(1535). This discrepancy motivated interpretations of the Roper as a dynamically…

Nuclear Experiment · Physics 2025-10-28 Volker Burkert , Eberhard Klempt

The $N(1440)1/2^+$ nucleon resonance, first identified in 1964 by L.D. Roper and collaborators in analyses of $\pi N$ hadroproduction data have continued to provide pivotal insights that serve to advance our understanding of nucleon excited…

Nuclear Experiment · Physics 2025-11-05 V. I. Mokeev , D. S. Carman

In view of the recent results of lattice QCD simulation in the P11 partial wave that has found no clear signal for the three-quark Roper state we investigate a different mechanism for the formation of the Roper resonance in a coupled…

High Energy Physics - Phenomenology · Physics 2018-03-14 B. Golli , H. Osmanović , S. Širca , A. Švarc

Two different descriptions of the existing pion-nucleon scattering data in the region of the Roper resonance are constructed. Both descriptions fit the experimental data very well. In one scenario the resonance is the result of strong…

Nuclear Theory · Physics 2018-06-06 Jia-jun Wu , Derek B. Leinweber , Zhan-wei Liu , Anthony W. Thomas

Recent measurements of nucleon resonance transition form factors with CLAS at Jefferson Lab are discussed. The new data resolve a long-standing puzzle of the nature of the Roper resonance, and confirm the assertion of the symmetric…

Nuclear Experiment · Physics 2014-11-18 Volker D. Burkert

We study the electromagnetic transitions of the Roper N(1440) resonance. Our results, when combined with the previously obtained for the mass and the pionic strong decay widths of the Roper, show that within a non-relativistic constituent…

Nuclear Theory · Physics 2009-10-31 F. Cano , P. Gonzalez

The recently proposed mechanism for the formation of the Roper resonance, in which a dynamically generated state as well as a genuine three-quark resonant state play an equally important role, is confronted with the model proposed almost…

High Energy Physics - Phenomenology · Physics 2018-12-06 B. Golli

The second excitation of the nucleon, the Roper, has properties differentiated from other low-lying nucleon resonances. Their properties challenge our understanding of the structure of the baryons in terms of the degrees of freedom from…

High Energy Physics - Phenomenology · Physics 2026-02-12 G. Ramalho

The Roper resonance is considered as a mixed state of a three-quark core configuration and a hadron molecular component N+sigma. Based on this ansatz we study electroproduction of the Roper resonance. The strong and electromagnetic…

High Energy Physics - Phenomenology · Physics 2011-07-13 Igor T. Obukhovsky , Amand Faessler , Dimitry K. Fedorov , Thomas Gutsche , Valery E. Lyubovitskij

The first baryon resonance was discovered in the early 1950s. The Roper resonance joined the collection ten years later. Today, many baryon resonances are known and more are being discovered. As baryons, these states are the most…

High Energy Physics - Phenomenology · Physics 2025-12-12 Peng Cheng , Langtian Liu , Ya Lu , Craig D. Roberts

A Dyson-Schwinger equation calculation of the light hadron spectrum, which correlates the masses of meson and baryon ground- and excited-states within a single framework, produces a description of the Roper resonance that corresponds…

Nuclear Theory · Physics 2015-05-30 Craig D. Roberts , Ian C. Cloet , Lei Chang , Hannes L. L. Roberts

A relativistic light-front quark model is used to describe both the elastic nucleon and nucleon-Roper transition form factors in a large Q2 range, up to 35 GeV2 for the elastic and up to 12 GeV2 for the resonance case. Relativistic…

High Energy Physics - Phenomenology · Physics 2014-01-28 Igor T. Obukhovsky , Amand Faessler , Thomas Gutsche , Valery E. Lyubovitskij

We discuss a new description for the Roper resonance, the first nucleon excited state of JP = 1/2+, in a model of strong diquark correlations. Treating the scalar-isoscalar and axial-vector--isovector diquarks as independent degrees of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Keitaro Kagata , Atsushi Hosaka

All the time since its discovery the N$^*$(1440) baryon state, commonly known as Roper resonance, has been a state with many question marks - despite of its 4-star ranking in the particle data book. One reason is that it does not produce…

We describe the electroproduction of the N(1440) Roper resonance in soft-wall AdS/QCD. The Roper resonance is identified as the first radially excited state of the nucleon, where higher-Fock states in addition to the three-quark component…

High Energy Physics - Phenomenology · Physics 2013-03-04 Thomas Gutsche , Valery E. Lyubovitskij , Ivan Schmidt , Alfredo Vega

The Roper resonance, the first excited state of the nucleon, Is one of the best-established baryon resonances. Yet, its properties have not been consistently explained by effective models of QCD, such as the non-relativistic quark model. In…

High Energy Physics - Phenomenology · Physics 2022-07-27 Daisuke Fujii , Akihiro Iwanaka , Atsushi Hosaka

The electroexcitation of the ${\cal N}^*(1440)$ Roper resonance, which defines the first radially excited state of the nucleon, is examined within the soft-wall AdS/QCD model. Such excited Fock states are characterized by the leading…

High Energy Physics - Phenomenology · Physics 2024-03-14 G. Karapetyan

Studies of the nucleon resonance electroexcitation amplitudes in a wide range of photon virtualities offer unique information on many facets of strong QCD behind the generation of all prominent excited nucleon states. Advances in the…

Nuclear Experiment · Physics 2022-10-19 Victor I. Mokeev

Using the constrained curve fitting method and overlap fermions with the lowest pion mass at $180 {\rm MeV}$, we observe that the masses of the first positive and negative parity excited states of the nucleon tend to cross over as the quark…

High Energy Physics - Phenomenology · Physics 2016-08-16 N. Mathur , Y. Chen , S. J. Dong , T. Draper , I. Horváth , F. X. Lee , K. F. Liu , J. B. Zhang
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