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200 papers

We explain how an analytic continuation we have developed recently is applied to determine the residues of the nucleon resonance poles within a dynamical coupled-channel model of meson-baron reactions. A procedure for evaluating the…

Nuclear Theory · Physics 2009-10-12 N. Suzuki , T. Sato , T. -S. H. Lee

A brief overview of the recent activity in the measurement of the elastic electromagnetic proton and neutron form factors is presented. It is discussed how the quality of the data has been greatly improved by performing double polarization…

Nuclear Theory · Physics 2008-11-26 Marc Vanderhaeghen

We report a new extraction of nucleon resonance couplings using pi- photoproduction cross sections on the neutron. The world database for the process gamma n --> pi- p above 1 GeV has quadrupled with the addition of new differential cross…

High Energy Physics - Phenomenology · Physics 2013-05-30 W. Chen , H. Gao , W. J. Briscoe , D. Dutta , A. E. Kudryavtsev , M. Mirazita , M. Paris , P. Rossi , S. Stepanyan , I. I. Strakovsky , V. E. Tarasov , R. L. Workman

The search for undiscovered excited states of the nucleon continues to be a focus of experiments at Jefferson Lab.Recent LQCD calculations have confirmed long-standing quark-model predictions of many more states than have so far been…

Nuclear Experiment · Physics 2015-06-18 Natalie K. Walford , Franz J. Klein

Longitudinal and transverse transition form factors for most of the four-star nucleon resonances have been obtained from high-quality cross section data and polarization observables measured at MAMI, ELSA, BATES, GRAAL and CEBAF. As an…

Nuclear Theory · Physics 2015-06-11 Lothar Tiator

Inclusive electron scattering cross sections off a hydrogen target at a beam energy of 10.6 GeV have been measured with data collected from the CLAS12 spectrometer at Jefferson Laboratory. These first absolute cross sections from CLAS12…

High Energy Physics - Experiment · Physics 2025-01-28 V. Klimenko , D. S. Carman , R. W. Gothe , K. Joo , N. Markov , V. I. Mokeev , G. Niculescu , P. Achenbach , J. S. Alvarado , W. Armstrong , H. Atac , H. Avakian , L. Baashen , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , F. Benmokhtar , A. Bianconi , A. S. Biselli , S. Boiarinov , F. Bossu , K. -Th. Brinkmann , W. J. Briscoe , W. K. Brooks , V. D. Burkert , S. Bueltmann , R. Capobianco , J. Carvajal , A. Celentano , P. Chatagnon , G. Ciullo , A. D Angelo , N. Dashyan , M. Defurne , R. De Vita , A. Deur , S. Diehl , C. Dilks , C. Djalali , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , I. P. Fernando , A. Filippi , G. Gavalian , G. P. Gilfoyle , D. I. Glazier , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , T. B. Hayward , D. Heddle , A. N. Hiller Blin , A. Hobart , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , S. Joosten , T. Kageya , D. Keller , A. Kim , W. Kim , H. T. Klest , A. Kripko , V. Kubarovsky , S. E. Kuhn , L. Lanza , S. Lee , P. Lenisa , K. Livingston , I. J. D. MacGregor , D. Marchand , D. Martiryan , V. Mascagna , D. Matamoris , B. McKinnon , T. Mineeva , M. Mirazita , C. Munoz Camacho , P. Nadel Turonski , T. Nagorna , K. Neupane , S. Niccolai , M. Osipenko , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , S. Polcher Rafael , J. W. Price , Y. Prok , B. A. Raue , J. Richards , M. Ripani , J. Ritman , P. Rossi , A. A. Rusova , C. Salgado , S. Schadmand , A. Schmidt , Y. G. Sharabian , E. V. Shirokov , S. Shrestha , N. Sparveris , M. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , J. A Tan , M. Tenorio , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , T. Vittorini , H. Voskanyan , E. Voutier , D. P. Watts , U. Weerasinghe , X. Wei , M. H. Wood , L. Xu , N. Zachariou , Z. W. Zhao , M. Zurek , V. Klimenko , D. S. Carman , R. W. Gothe , K. Joo , N. Markov , V. I. Mokeev , G. Niculescu , P. Achenbach , J. S. Alvarado , W. Armstrong , H. Atac , H. Avakian , L. Baashen , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , F. Benmokhtar , A. Bianconi , A. S. Biselli , S. Boiarinov , F. Bossu , K. -Th. Brinkmann , W. J. Briscoe , W. K. Brooks , V. D. Burkert , S. Bueltmann , R. Capobianco , J. Carvajal , A. Celentano , P. Chatagnon , G. Ciullo , A. D Angelo , N. Dashyan , M. Defurne , R. De Vita , A. Deur , S. Diehl , C. Dilks , C. Djalali , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , I. P. Fernando , A. Filippi , G. Gavalian , G. P. Gilfoyle , D. I. Glazier , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , T. B. Hayward , D. Heddle , A. N. Hiller Blin , A. Hobart , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , S. Joosten , T. Kageya , D. Keller , A. Kim , W. Kim , H. T. Klest , A. Kripko , V. Kubarovsky , S. E. Kuhn , L. Lanza , S. Lee , P. Lenisa , K. Livingston , I. J. D. MacGregor , D. Marchand , D. Martiryan , V. Mascagna , D. Matamoris , B. McKinnon , T. Mineeva , M. Mirazita , C. Munoz Camacho , P. Nadel Turonski , T. Nagorna , K. Neupane , S. Niccolai , M. Osipenko , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , S. Polcher Rafael , J. W. Price , Y. Prok , B. A. Raue , J. Richards , M. Ripani , J. Ritman , P. Rossi , A. A. Rusova , C. Salgado , S. Schadmand , A. Schmidt , Y. G. Sharabian , E. V. Shirokov , S. Shresth , N. Sparveris , M. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , J. A Tan , M. Tenorio , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , T. Vittorini , H. Voskanyan , E. Voutier , D. P. Watts , U. Weerasinghe , X. Wei , M. H. Wood , L. Xu , N. Zachariou , Z. W. Zhao , M. Zurek

Proton and neutron electric and magnetic form factors are the primary characteristics of their spatial structure and have been studied extensively over the past half-century. At large values of the momentum transfer $Q^2$ they should reveal…

High Energy Physics - Lattice · Physics 2025-02-25 S. Syritsyn , M. Engelhardt , S. Krieg , J. Negele , A. Pochinsky

We compute nucleon and Roper e.m. elastic and transition form factors using a symmetry-preserving treatment of a contact-interaction. Obtained thereby, the e.m. interactions of baryons are typically described by hard form factors. In…

Nuclear Theory · Physics 2015-06-03 D. J. Wilson , I. C. Cloet , L. Chang , C. D. Roberts

Parity-conserving and -violating response functions are computed for the inclusive electroexcitation of the N*(1440)(Roper) resonance in nuclear matter modeled as a relativistic Fermi gas. Using various empirical parameterizations and…

Nuclear Theory · Physics 2009-11-10 L. Alvarez-Ruso , M. B. Barbaro , T. W. Donnelly , A. Molinari

Radiative transitions gamma + Delta(1232) -> N^* are discussed in the nonrelativistic quark model with spin-orbit corrections for the 70-plet L^P=1^- nucleon resonances N^*. The reaction gamma + N -> gamma + Delta is considered as a tool to…

Nuclear Theory · Physics 2017-08-23 A. I. L'vov

We present some predictions for the $\gamma^\ast N \to N^\ast$ transition amplitudes, where $N$ is the nucleon, and $N^\ast$ is a nucleon excitation from the third resonance region. First we estimate the transition amplitudes associated…

High Energy Physics - Phenomenology · Physics 2016-09-27 G. Ramalho

We discuss recent results from CLAS on electromagnetic resonance transition amplitudes and their dependence on the distance scale ($Q^2$). From the comparison of these results with most advanced theoretical calculations within QCD-based…

Nuclear Experiment · Physics 2015-10-12 I. G. Aznauryan , V. D. Burkert , V. I. Mokeev

Differential cross sections of the exclusive process $e p \to e^\prime \pi^+ n$ were measured with good precision in the range of the photon virtuality $Q^2 = 1.8 - 4.5$ GeV$^2$, and the invariant mass range of the $\pi^+ n$ final state W =…

Nuclear Experiment · Physics 2015-04-22 K. Park , I. G. Aznauryan , V. D. Burkert , the CLAS collaboration

The simplest models might describe the nucleon as 3 light quarks, but this description would be incomplete without inclusion of the sea of glue and q-qbar pairs which binds it. Early indications of a particularly large contribution from…

Nuclear Experiment · Physics 2011-10-18 Kent Paschke , Anthony Thomas , Robert Michaels , David Armstrong

Over the past decade measurements of unpolarized structure functions at Jefferson Lab with unprecedented precision have significantly advanced our knowledge of nucleon structure. These have for the first time allowed quantitative tests of…

Nuclear Experiment · Physics 2015-05-27 M. E. Christy , W. Melnitchouk

The momentum distributions of the constituent quarks inside the nucleon and the prominent electroproduced nucleon resonances are investigated in the two most sophisticated, available quark potential models, based respectively on the…

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

The study of nucleon resonances in electromagnetic meson production with the CLAS detector is discussed. The electromagnetic interaction is complementary to pion scattering in the exploration of the nucleon excitation spectrum. Higher mass…

Nuclear Experiment · Physics 2017-08-23 Volker D. Burkert

A Poincar\'e-covariant continuum approach to the three valence-quark bound-state problem in quantum field theory is used to perform a detailed analysis of the nucleon's ground and first excited states: the so-called $N(940)\frac{1}{2}^+$…

Nuclear Theory · Physics 2019-05-22 Jorge Segovia

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…

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