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Related papers: Light Baryon Spectroscopy using the CLAS Spectrome…

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The Lattice Hadron Physics Collaboration (LHPC) baryon spectroscopy effort is reviewed. To date the LHPC has performed exploratory Lattice QCD calculations of the low-lying spectrum of Nucleon and Delta baryons. These calculations…

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the…

High Energy Physics - Experiment · Physics 2008-11-26 COMPASS Collaboration , P. Abbon

The spectroscopy of light, strange baryons have been an important aspect with still unknown resonances and intrinsic baryonic properties. The present document is focused on the $\Delta$ baryons unlike earlier work, here all the four isospin…

High Energy Physics - Phenomenology · Physics 2022-12-21 Chandni Menapara , Ajay Kumar Rai

Protons and neutrons are the building blocks of matter, glued together in nuclei by strong interactions. They can be excited by pions, real and virtual photons, neutrinos and other probes. These excitations are referred to as light baryon…

Nuclear Theory · Physics 2025-10-16 Michael Döring

Tensions in several phenomenological models grew with experimental results on neutrino/antineutrino oscillations at Short-Baseline (SBL) and with the recent, carefully recomputed, antineutrino fluxes from nuclear reactors. At a refurbished…

Precision measurements in the neutrino sector are becoming increasingly feasible due to the development of relatively high-rate experimental capabilities. These important developments command renewed attention to the systematic corrections…

Nuclear Experiment · Physics 2007-05-23 W. K. Brooks

We study baryon spectroscopy including the effects of pseudoscalar meson exchange and one gluon exchange potentials between quarks, governed by $\alpha_s$. The non-perturbative, hyperspherical method calculations show that one can obtain a…

Nuclear Theory · Physics 2008-11-26 Z. Dziembowski , M. Fabre de la Ripelle , Gerald A. Miller

We study baryon excited states for quark confinement and chiral symmetry breaking. In the first part we discuss spatially deformed baryon excitations. As signals of deformation, we study masses and electromagnetic transitions. Such a study…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Hosaka

The COMPASS experiment at CERN is well designed for light-hadron spectroscopy with emphasis on the detection of new states, in particular the search for $J^{PC}$-exotic states and glueballs. We have collected data with 190 GeV/c charged…

High Energy Physics - Experiment · Physics 2019-08-13 Frank Nerling

We study baryons on the lattice with a special focus on excited states. For that purpose we construct several interpolators which differ in their Dirac structure. These interpolators are built from Jacobi smeared quarks with different…

High Energy Physics - Lattice · Physics 2007-05-23 Tommy Burch , Christof Gattringer , Leonid Ya. Glozman , Christian Hagen , Dieter Hierl , C. B. Lang , Andreas Schaefer

A black hole holographic model is used to mimic the behavior of the quark gluon plasma at finite temperature and density. This model reproduces lattice data at $\mu_B\!=\!0$ and displays critical behavior at large densities. High order…

Nuclear Theory · Physics 2018-03-14 Israel Portillo

We study the conjectured "Insensitivity to Chiral Symmetry Breaking" in the highly excited light baryon spectrum. While the experimental spectrum is being measured at JLab and CBELSA/TAPS, this insensitivity remains to be computed…

High Energy Physics - Phenomenology · Physics 2016-09-14 Pedro Bicudo , Marco Cardoso , Felipe J. Llanes-Estrada , Tim Van Cauteren

The ability to control and modify infrared excitations in condensed matter is of both fundamental and application interests. Here we explore a system supporting low-energy excitations, in particular, mid-infrared localized plasmon modes and…

The physics of electromagnetic excitation of nucleon resonances and of their relevance in nucleon structure studies are discussed. Preliminary data from the CLAS detector on the N-Delta(1232) transition multipoles, the helicity amplitudes…

High Energy Physics - Phenomenology · Physics 2019-08-14 Volker D. Burkert

An overview of the CLAS12 detector is presented and the initial physics program after the energy-doubling of the Jefferson Lab electron accelerator. Construction of the 12 GeV upgrade project has started October 2008. A broad program has…

High Energy Physics - Phenomenology · Physics 2008-11-07 Volker D. Burkert

Precision measurements of the structure of nucleons and nuclei in the regime of strong interaction QCD are now possible with the availability of high current polarized electron beams, polarized targets, and recoil polarimeters, in…

Nuclear Experiment · Physics 2017-08-23 Elton S. Smith

Recent results on studies of the structure of nucleons and nuclei in the regime of strong interaction QCD are discussed. Use of high current polarized electron beams, polarized targets, and recoil polarimeters, in conjunction with modern…

Nuclear Theory · Physics 2008-11-26 Volker D. Burkert

Measurement results of photoproduced excited hyperon states using the CLAS detector at Jefferson Lab are shown. The invariant mass distribution of the Lambda(1405) has recently been shown to be different for each of the three Sigma pi…

Nuclear Experiment · Physics 2015-06-17 Kei Moriya , Reinhard Schumacher

The task of mapping and explaining the spectrum of baryons and the structure of these states in terms of quarks and gluons is a longstanding challenge in hadron physics, which is likely to persist for another decade or more. We review the…

Nuclear Theory · Physics 2019-11-13 J. Segovia , C. Chen , Z. -F. Cui , Y. Lu , C. D. Roberts

Positron beams, both polarized and unpolarized, are identified as essential ingredients for the experimental program at the next generation of lepton accelerators. In the context of the Hadronic Physics program at the Jefferson Laboratory…

Nuclear Experiment · Physics 2019-06-25 A. Afanasev , I. Albayrak , S. Ali , M. Amaryan , A. D'Angelo , J. Annand , J. Arrington , A. Asaturyan , H. Avakian , T. Averett , L. Barion , M. Battaglieri , V. Bellini , V. Berdnikov , J. Bernauer , A. Biselli , M. Boer , M. Bondì , K. -T. Brinkmann , B. Briscoe , V. Burkert , A. Camsonne , T. Cao , L. Cardman , M. Carmignotto , L. Causse , A. Celentano , P. Chatagnon , G. Ciullo , M. Contalbrigo , D. Day , M. Defurne , S. Diehl , B. Dongwi , R. Dupré , D. Dutta , M. Ehrhart , L. Elouadrhiri , R. Ent , I. Fernando , A. Filippi , Y. Furletova , H. Gao , A. Gasparian , D. Gaskell , F. Georges , F. -X. Girod , J. Grames , C. Gu , M. Guidal , D. Hamilton , D. Hasell , D. Higinbotham , M. Hoballah , T. Horn , C. Hyde , A. Italiano , N. Kalantarians , G. Kalicy , D. Keller , C. Keppel , M. Kerver , P. King , E. Kinney , H. -S. Ko , M. Kohl , V. Kubarovsky , L. Lanza , P. Lenisa , N. Liyanage , S. Liuti , J. Mamei , D. Marchand , P. Markowitz , L. Marsicano , M. Mazouz , M. McCaughan , B. McKinnon , M. Mihovilovič , R. Milner , A. Mkrtchyan , H. Mkrtchyan , A. Movsisyan , C. Muñoz Camacho , P. Nadel-Turońs , M. De Napoli , J. Nazeer , S. Niccolai , G. Niculescu , R. Novotny , L. Pappalardo , R. Paremuzyan , E. Pasyuk , T. Patel , I. Pegg , D. Perera , A. Puckett , N. Randazzo , M. Rashad , M. Rathnayake , A. Rizzo , J. Roche , O. Rondon , A. Schmidt , M. Shabestari , Y. Sharabian , S. Širca , D. Sokhan , A. Somov , N. Sparveris , S. Stepanyan , I. Strakovsky , V. Tadevosyan , M. Tiefenback , R. Trotta , R. De Vita , H. Voskanyan , E. Voutier , R. Wang , B. Wojtsekhowski , S. Wood , H. -G. Zaunick , S. Zhamkochyan , J. Zhang , S. Zhao , X. Zheng , C. Zorn