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Related papers: Excited Baryon Structure Using Exclusive Reactions…

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Variational analysis techniques in lattice QCD are powerful tools that give access to the full spectrum of QCD. At zero momentum, these techniques are well established and can cleanly isolate energy eigenstates of either positive or…

High Energy Physics - Lattice · Physics 2017-11-20 Finn M. Stokes , Waseem Kamleh , Derek B. Leinweber , Benjamin J. Owen

We present a new method for extracting excited states from a single two-point correlation function calculated on the lattice. Our method simply combines the correlation function evaluated at different time slices so as to ``subtract'' the…

High Energy Physics - Lattice · Physics 2009-11-10 D. Guadagnoli , M. Papinutto , S. Simula

Excited states of the $^{203}$Po ($Z = 84, N = 119$) have been investigated after populating them through $^{194}$Pt($^{13}$C,4n) fusion-evaporation reaction at E$_{beam}$ = 74 MeV and using a large array of Compton suppressed HPGe clover…

We show that excited baryons in large N_c QCD form multiplets, within which masses are first split at O(1/N_c). The dominant couplings of resonances to various mesons are highly constrained: The N(1535) decays at leading 1/N_c order…

High Energy Physics - Phenomenology · Physics 2009-11-10 Thomas D. Cohen , Richard F. Lebed

The spectrum of baryons containing three b quarks is calculated in nonperturbative QCD, using the lattice regularization. The energies of ten excited bbb states with J^P = 1/2^+, 3/2^+, 5/2^+, 7/2^+, 1/2^-, and 3/2^- are determined with…

High Energy Physics - Lattice · Physics 2012-06-27 Stefan Meinel

For further decoding the inner structure of the two excited $\Xi_b$ states observed by LHCb, we perform a systematical study of the strong decays of the low-lying $1D$-wave $\Xi_b$ and $\Xi_b'$ excitations using the quark pair creation…

High Energy Physics - Phenomenology · Physics 2023-09-26 Yu-Hui Zhou , Wen-Jia Wang , Li-Ye Xiao , Xian-Hui Zhong

A possibility of the construction of a periodic table for the excited baryon spectrum is shown in the frame of a relativistic chiral quark model based on selection rules derived from the one-pion exchange mechanism. It is shown that all the…

High Energy Physics - Phenomenology · Physics 2011-10-31 E. M. Tursunov

We report measurements of the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from an unpolarized proton target using the CLAS detector at the Thomas Jefferson National Accelerator Facility. The separated…

Nuclear Experiment · Physics 2013-03-14 D. S. Carman , K. Park , B. A. Raue , CLAS Collaboration

Excited state contributions represent a formidable challenge for hadron structure calculations in lattice QCD. For physical systems that exhibit an exponential signal-to-noise problem they often hinder the extraction of ground state matrix…

High Energy Physics - Lattice · Physics 2021-03-31 Konstantin Ottnad

We collected notes and simple estimates about putative narrow nucleon N*(1685) - the candidate for the non-strange member of the exotic anti-decuplet of baryons. In particular, we consider the recent high precision data on eta…

High Energy Physics - Phenomenology · Physics 2015-05-27 V. Kuznetsov , M. V. Polyakov , M. Thuermann

We present organization and solutions for a new analysis of all $\pi N$ elastic and the major inelastic channels to extract detailed characteristics of the contributing baryon resonances. This work is based on the work of R. Cutkosky and…

Nuclear Theory · Physics 2008-02-03 S. A. Dytman , T. P. Vrana , T. S. H. Lee

Two reactions, pp->ppX and pp->p\pi^+X, are used to study the 1.47<M<1.68 GeV baryonic mass range. Three different final states are considered in the invariant masses: N^* or \Delta^+, p\pi^0, and p\eta. The last two channels are defined by…

We present results on the electroexcitation of the low mass resonances Delta(1232)P33, N(1440)P11, N(1520)D13, and N(1535)S11 in a wide range of Q2. The results were obtained in the comprehensive analysis of JLab-CLAS data on differential…

Nuclear Experiment · Physics 2010-04-06 I. G. Aznauryan , V. D. Burkert , the CLAS Collaboration

The doubly-strange Xi baryons provide an effective way to study a puzzle called the missing-baryons problem, where both quark models and lattice gauge theory predict more baryon excited states than are seen experimentally. However, few of…

Nuclear Experiment · Physics 2019-01-02 J. T. Goetz , K. Hicks , M. C. Kunkel , J. W. Price , D. P. Weygand , the CLAS Collaboration

The exclusive electroproduction process $ep \rightarrow e'p'\pi^{0}$ was measured in the range of photon virtualities $Q^{2} = 0.4 - 1.0$~GeV$^{2}$ and the invariant mass range of the $p\pi^{0}$ system of $W = 1.1 - 1.8$~GeV. These…

Nuclear Experiment · Physics 2020-01-29 N. Markov , K. Joo , V. D. Burkert , V. I. Mokeev , L. C. Smith , M. Ungaro , S. Adhikari , M. J. ~Amaryan , G. Angelini , H. ~Atac , H. ~Avakian , C. Ayerbe Gayoso , N. A. ~Baltzell , L. Barion , M. ~Battaglieri , I. ~Bedlinskiy , I. ~Bedlinskiy , F. Benmokhtar , A. S. ~Biselli , F. ~Bossù , S. ~Boiarinov , W. J. ~Briscoe , W. K. ~Brooks , D. S. ~Carman , J. C. ~Carvajal , A. ~Celentano , P. ~Chatagnon , T. Chetry , P. L. ~Cole , M. ~Contalbrigo , V. ~Crede , G. Ciullo , A. ~D'Angelo , N. ~Dashyan , R. ~De~Vita , E. ~De~Sanctis , M. Defurne , A. ~Deur , S. Diehl , C. ~Djalali , R. ~Dupre , M. ~Ehrhart , A. ~El~Alaoui , L. ~El~Fassi , P. ~Eugenio , C. ~Evans , A. ~Filippi , Y. ~Ghandilyan , F. X. ~Girod , E. ~Golovatch , R. W. ~Gothe , K. A. ~Griffioen , M. ~Guidal , K. ~Hafidi , H. ~Hakobyan , M. ~Hattawy , T. B. ~Hayward , K. ~Hicks , M. ~Holtrop , Y. ~Ilieva , D. G. ~Ireland , B. S. ~Ishkhanov , E. L. ~Isupov , D. ~Jenkins , H. S. ~Jo , D. ~Keller , M. ~Khachatryan , A. ~Khanal , M. ~Khandaker , A. ~Kim , C. W. ~Kim , W. ~Kim , F. J. ~Klein , V. ~Kubarovsky , L. Lanza , M. ~Leali , K. ~Livingston , I . J . D. ~MacGregor , D. ~Marchand , V. ~Mascagna , B. ~McKinnon , T. ~Mineeva , M. ~Mirazita , P. ~Nadel-Turonski , S. ~Nanda , S. ~Niccolai , G. ~Niculescu , M. ~Osipenko , M. ~Paolone , L. L. ~Pappalardo , R. ~Paremuzyan , K. ~Park , E. ~Pasyuk , W. ~Phelps , O. ~Pogorelko , J. W. ~Price , Y. ~Prok , D. ~Protopopescu , M. ~Ripani , D. Riser , A. ~Rizzo , J. ~Rowley , F. ~Sabatié , C. ~Salgado , R. A. ~Schumacher , Y. G. ~Sharabian , U. ~Shrestha , D. ~Sokhan , O. ~Soto , N. ~Sparveris , S. ~Stepanyan , P. ~Stoler , I. I. ~Strakovsky , S. ~Strauch , M. ~Taiuti , J. A. ~Tan , N. ~Tyler , L. ~Venturelli , H. ~Voskanyan , E. ~Voutier , R. Wang , X. ~Wei , M. H. ~Wood , N. ~Zachariou

We present the results of a search for the production of an excited state of the electron, e*, in proton-antiproton collisions at sqrt(s) = 1.96 TeV. The data were collected with the D0 experiment at the Fermilab Tevatron Collider and…

High Energy Physics - Experiment · Physics 2008-11-26 D0 Collaboration , V. Abazov

New results for the exclusive and quasi-free cross sections off neutrons bound in deuterium ${\gamma}_vn(p) \rightarrow p{\pi}^{-} (p)$ are presented over a wide final state hadron angle range with a kinematic coverage of the invariant mass…

Nuclear Experiment · Physics 2023-01-18 Y. Tian , R. W. Gothe , V. I. Mokeev , G. Hollis , M. J. Amaryan , W. R. Armstrong , H. Atac , H. Avakian , L. Barion , M. Battaglieri , I. Bedlinskiy , B. Benkel , F. Benmokhtar , A. Bianconi , L. Biondo , A. Biselli , F. Bossù , S. Boiarinov , M. Bondì , K. T. Brinkmann , W. J. Briscoe , S. Bueltmann , D. Bulumulla , V. D. Burkert , R. Capobianco , D. S. Carman , J. C. Carvajal , A. Celentano , V. Chesnokov , T. Chetry , G. Ciullo , G. Clash , P. L. Cole , M. Contalbrigo , G. Costantini , A. D'Angelo , N. Dashyan , R. De Vita , M. Defurne , A. Deur , S. Diehl , C. Djalali , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , P. Eugenio , S. Fegan , A. Filippi , G. Gavalian , G. P. Gilfoyle , F. X. Girod , A. A. Golubenko , G. Gosta , K. Griffioen , M. Guidal , H. Hakobyan , M. Hattawy , T. B. Hayward , A. Hobart , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , D. Jenkins , H. S. Jo , K. Joo , S. Joosten , D. Keller , A. Khanal , M. Khandaker , A. Kim , W. Kim , F. J. Klein , A. Kripko , V. Kubarovsky , V. Lagerquist , L. Lanza , M. Leali , P. Lenisa , K. Livingston , I. . J . D. MacGregor , D. Marchand , L. Marsicano , V. Mascagna , B. McKinnon , S. Migliorati , T. Mineeva , M. Mirazita , C. Munoz Camacho , P. Nadel-Turonski , P. Naidoo , K. Neupane , J. Newton , S. Niccolai , M. Nicol , G. Niculescu , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , K. Park , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , D. Počanić , O. Pogorelko , J. Poudel , J. W. Price , Y. Prok , T. Reed , M. Ripani , J. Ritman , A. Rizzo , G. Rosner , F. Sabatié , C. Salgado , S. Schadmand , A. Schmidt , R. A. Schumacher , E. V. Shirokov , U. Shrestha , P. Simmerling , D. Sokhan , N. Sparveris , S. Stepanyan , I. I. Strakovsky , S. Strauch , R. Tyson , M. Ungaro , L. Venturelli , H. Voskanyan , E. Voutier , D. P. Watts , K. Wei , X. Wei , M. H. Wood , B. Yale , N. Zachariou , J. Zhang

Using the polarisation labelling spectroscopy, we performed the detailed analysis of the level structure of excited electronic states of the $^{39}$KCs molecule in the excitation energy interval between 17500~cm$^{-1}$ and 18600~cm$^{-1}$…

We present a study of excited charm-strange baryon states produced in $e^+e^-$ annihilations at or near a center-of-mass energy of $10.58\mathrm{Ge\kern -0.1em V}$, in a data sample with an integrated luminosity of $384 fb^{-1}$ recorded…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

Beam-recoil transferred polarizations for the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from an unpolarized proton target have been measured using the CLAS12 spectrometer at Jefferson Laboratory. The…

Nuclear Experiment · Physics 2022-06-15 D. S. Carman , A. D'Angelo , L. Lanza , V. I. Mokeev , K. P. Adhikari , M. J. Amaryan , W. R. Armstrong , H. Atac , H. Avakian , C. Ayerbe Gayoso , N. A. Baltzell , L. Barion , M. Battaglieri , I. Bedlinskiy , B. Benkel , A. Bianconi , A. S. Biselli , M. Bondi , S. Boiarinov , F. Bossu , W. J. Briscoe , S. Bueltmann , D. Bulumulla , V. D. Burkert , R. Capobianco , J. C. Carvajal , A. Celentano , P. Chatagnon , V. Chesnokov , T. Chetry , G. Ciullo , L. Clark , P. L. Cole , M. Contalbrigo , G. Costantini , V. Crede , N. Dashyan , R. De Vita , M. Defurne , A. Deur , S. Diehl , C. Djalali , R. Dupre , M. Ehrhart , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , A. Filippi , G. Gavalian , Y. Ghandilyan , G. P. Gilfoyle , F. X. Girod , D. I. Glazier , A. A. Golubenko , R. W. Gothe , Y. Gotra , K. A. Griffioen , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , T. B. Hayward , A. Hobart , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. S. Jo , K. Joo , D. Keller , A. Khanal , A. Kim , W. Kim , V. Klimenko , A. Kripko , V. Kubarovsky , M. Leali , S. Lee , P. Lenisa , K. Livingston , I. J. D. MacGregor , D. Marchand , L. Marsicano , V. Mascagna , M. Mayer , B. McKinnon , S. Migliorati , T. Mineeva , M. Mirazita , R. A. Montgomery , C. Munoz Camacho , P. Nadel-Turonski , K. Neupane , J. Newton , S. Niccolai , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , N. Pilleux , O. Pogorelko , J. W. Price , Y. Prok , B. A. Raue , T. Reed , M. Ripani , J. Ritman , A. Rizzo , P. Rossi , F. Sabatie , C. Salgado , A. Schmidt , Y. G. Sharabian , E. V. Shirokov , U. Shrestha , P. Simmerling , D. Sokhan , N. Sparveris , S. Stepanyan , I. I. Strakovsky , S. Strauch , N. Tyler , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , H. Voskanyan , E. Voutier , D. P. Watts , K. Wei , X. Wei , R. Wishart , M. H. Wood , B. Yale , N. Zachariou , J. Zhang , V. Ziegler
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