47 research outputs found

    Lessons from Hadron Phenomenology

    Get PDF
    Meson spectra can be well approximated by a specific form of a nonlinear Regge trajectory which is consistent with a finite number of bound states. This may have important consequencies for experiment, and may be a hint for the theory.Comment: talk presented by MB at the Light-Cone Meeting in Heidelberg, June 2000. To appear in the proceedings, requires elsart.cls. 4 page

    The Spin and Flavour Dependence of High-Energy Photoabsorption

    Full text link
    We review the present data on high-energy, spin-dependent photoabsorption. We find a strong isotriplet term in (σA−σP)(\sigma_A - \sigma_P) which persists from Q2∼0.25Q^2 \sim 0.25GeV2^2 to high Q2Q^2 polarised deep inelastic scattering. For Q2∼4Q^2 \sim 4GeV2^2 and xx between 0.01 and 0.12 the isotriplet part of g1g_1 behaves as g1(p−n)∼x−12g_1^{(p-n)} \sim x^{-{1 \over 2}}, in contrast to soft Regge theory which predicts that g1(p−n)g_1^{(p-n)} should converge as x→0x \to 0. The isotriplet, polarised structure function 2xg1(p−n)2x g_1^{(p-n)} is significantly greater than the isotriplet, unpolarised structure function F2(p−n)F_2^{(p-n)} in this kinematic region. We analyse the low Q2Q^2 photoabsorption data from E-143 and SMC and use this data to estimate the high-energy Regge contribution to the Drell-Hearn-Gerasimov sum-rule.Comment: 19 pages, LaTeX, 3 figures generated as g1,g1F2 and A1.te

    The Drell-Hearn-Gerasimov Sum-Rule at Polarized HERA

    Get PDF
    We discuss the potential of polarized HERA to measure the spin dependent part of the total photoproduction cross-section at large sγp\sqrt{s_{\gamma p}}.Comment: 7 pages, LaTeX, 1 figure generated as fig1.tex. To appear in Proc. Workshop on ``Physics with Polarized Protons at HERA'

    Quarkonia in Hamiltonian Light-Front QCD

    Full text link
    A constituent parton picture of hadrons with logarithmic confinement naturally arises in weak coupling light-front QCD. Confinement provides a mass gap that allows the constituent picture to emerge. The effective renormalized Hamiltonian is computed to O(g2){\cal O}(g^2), and used to study charmonium and bottomonium. Radial and angular excitations can be used to fix the coupling α\alpha, the quark mass MM, and the cutoff Λ\Lambda. The resultant hyperfine structure is very close to experiment.Comment: 9 pages, 1 latex figure included in the text. Published version (much more reader-friendly); corrected error in self-energ
    corecore