780 research outputs found

    Deeply pseudoscalar meson electroproduction with CLAS and Generalized Parton Distributions

    Full text link
    We discuss the recent data of exclusive π0\pi^0 (and π+\pi^+) electroproduction on the proton obtained by the CLAS collaboration at Jefferson Lab. It is observed that the cross sections, which have been decomposed in σT+ϵσL\sigma_T +\epsilon\sigma_L, σTT\sigma_{TT} and σLT\sigma_{LT} structure functions, are dominated by transverse amplitude contributions. The data can be interpreted in the Generalized Parton Distribution formalism provided that one includes helicity-flip transversity GPDs.Comment: 4 pages, 2 figures PANIC14 conference proceedin

    Study of narrow baryon resonance decaying into Ks0pK^0_s p in pApA-interactions at 70GeV/c70 GeV/c with SVD-2

    Get PDF
    The inclusive reaction pApKs0+Xp A \to pK^0_s + X was studied at IHEP accelerator with 70GeV70 GeV proton beam using SVD-2 detector. Two different samples of Ks0K^0_s, statistically independent and belonging to different phase space regions were used in the analyses and a narrow baryon resonance with the mass M=1523±2(stat.)±3(syst.)MeV/c2M=1523\pm 2(stat.)\pm 3(syst.) MeV/c^2 was observed in both samples of the dataComment: 3 pages, 6 figures, to be published in the Proceedings of the XXXIII International Conference of High Energy Physics (ICHEP'06), Moscow, 200

    Deeply Virtual Pseudoscalar Meson Production with CLAS

    Full text link
    Deeply virtual meson scattering cross sections and asymmetries for the pi^0 and eta exclusive electroproduction in a very wide kinematic range of Q^2, t and x_B have been measured with CLAS (JLab). Initial analysis is already showing remarkable results. These data will help us to better understand the transition from soft to hard mechanisms.Comment: Prepared for XII Workshop on High Energy Spin Physics DSPIN-07, Dubna, September 3-7, 200

    Status of Pentaquark Search at Jlab

    Full text link
    We review the current experimental situation of pentaquark searches, and second generation experiments, with emphasis on the Jefferson Lab program.Comment: Invited talk at the 6th International Conference on Hyperons, Charm and Beauty Hadrons (BEACH2004), Chicago, USA, June 28 - July 3, 2004. 10 pages, 14 figures. One reference adde

    Absence of evidence for pentaquarks on the lattice

    Full text link
    We study the question of whether or not QCD predicts a pentaquark state. We use the improved, fixed point lattice QCD action which has very little sensitivity to the lattice spacing and also allows us to reach light quark masses. The analysis was performed on a single volume of size (1.8fm)3×3.6fm(1.8 {\rm fm})^3\times 3.6 {\rm fm} with lattice spacing of a=0.102a=0.102 fm. We use the correlation matrix method to identify the ground and excited states in the isospin 0, negative parity channel. In the quenched approximation where dynamical quark effects are omitted, we do not find any evidence for a pentaquark resonance in QCD.Comment: 17 pages, 5 figures replaced with revised versio

    Two-Hadron-Irreducible QCD Sum Rule for Pentaquark Baryon

    Full text link
    We point out that naive pentaquark correlations function include two-hadron-reducible contributions, which are given by convolution of baryon and meson correlation functions and have nothing to do with pentaquark. We show that the two-hadron-reducible contributions are large in the operator product expansion of the correlation functions of three existing works on the pentaquark. Therefore, it is dangerous to draw a conclusion from the sum rules using naive pentaquark correlation functions with naive ansatz for the spectral function under the dispersion integral. Instead, we propose to use the two-hadron-irreducible correlation function, which is obtained by subtracting the two-hadron-reducible contribution from the naive correlation function. Taking one of the works as an example we demonstrate how drastically the results can change if we remove the two-hadron-reducible part from the naive correlation function. We obtain the result opposite to the original work for the parity of the pentaquark.Comment: 12 pages, 3 figure
    corecore