158 research outputs found

    On the Q^2 Dependence of Measured Polarized Structure Funtions

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    We analyse the available data on the polarized asymmetries A1A_1 for proton, neutron and deuteron targets. We use a homogeneous and updated set of unpolarized structure functions to derive g1g_1 from A1A_1, and we accurately correct for the scaling violations in order to obtain g1(x,Q2)g_1(x,Q^2) with the same Q2Q^2 for all xx values. The contribution to the Q2Q^2 evolution of a possible large gluon polarized density is also considered. The implications for the Ellis-Jaffe and for the Bjorken sum rules are discussed.Comment: 11 pages (LaTex) + 4 figures (topdrawer, included at the end) CERN-TH 7023/9

    The strange-sea quark spin distribution in the nucleon from inclusive and semi-inclusive deep-inelastic scattering

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    We propose new method which allows determination of the strange-sea quark spin distribution in the nucleon through measurement of various inclusive and semi-inclusive polarized deep inelastic electron- or muon-proton reactions. It is shown, that using combinations of inclusive data and semi-inclusive data containing neutral pions in the final state, it is possible to extract the strange-sea quark spin distribution. Similar result can be obtained for charged pions and some other hadrons also

    Jet Production in Polarized Lepton-Hadron Scattering

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    We calculate exact analytical expressions for \oas 3-jet and \oasz \\ 4-jet cross sections in polarized deep inelastic lepton nucleon scattering. Introducing an invariant jet definition scheme, we present differential distributions of 3- and 4-jet cross sections in the basic kinematical variables xx and W2W^2 as well as total jet cross sections and show their dependence on the chosen spin-dependent (polarized) parton distributions. Noticebly differences in the predictions are found for the two extreme choices, i.e. a large negative sea-quark density or a large positive gluon density. Therefore, it may be possible to discriminate between different parametrizations of polarized parton densities, and hence between the different physical pictures of the proton spin underlying these parametrizations.Comment: 35 pages, LaTeX, 9 ps figures available upon request, MAD/PH/827, KA TTP94-

    QCD Sum Rule Calculation of Twist-4 Corrections to Bjorken and Ellis-Jaffe Sum Rules

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    We calculate the twist-4 corrections to the integral of g1(x,Q2)g_1(x,Q^2) in the framework of QCD sum rules using an interpolating nucleon field which contains explicitly a gluonic degree of freedom. This information can be used together with previous calculations of the twist-3 contribution to the second moment of g2(x)g_2(x) to estimate the higher-twist corrections to the Ellis-Jaffe and Bjorken sum rules. We get f(2)(proton)=0.037±0.006f^{(2)}(proton) = -0.037 \pm 0.006 and f(2)(neutron)=0.013±0.006f^{(2)}(neutron) = -0.013 \pm 0.006. Numerically our results roughly agree with those obtained by Balitsky, Braun and Kolesnichenko based on a sum rule for a simpler current. Our calculations are far more stable as tested within the sum rule approach but are more sensitive to less well known condensates.Comment: 18pp., 1 figure (uuencoded eps-file), Late

    Interpolating the Nucleon's Spin-Dependent Sum Rules at High and Low Energies

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    I discuss a few interpolating sum rules for spin structure functions of the nucleon. Using the concept of duality, I argue that the G1G_1 sum rule, including the elastic contribution, is useful for learning higher twist matrix elements of the nucleon.Comment: 9 pages in Plain TeX, MIT CTP #220

    Transverse Momentum in Semi-Inclusive Polarized Deep Inelastic Scattering and the Spin-Flavor Structure of the Proton

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    The non-valence spin-flavor structure of the nucleon extracted from semi-inclusive measurements of polarized deep inelastic scattering depends strongly on the transverse momentum of the detected hadrons which are used to determine the individual polarized sea distributions. This physics may explain the recent HERMES observation of a positively polarized strange sea through semi-inclusive scattering, in contrast to the negative strange sea polarization deduced from inclusive polarized deep inelastic scattering.Comment: 4 pages, revtex style, 2 figure

    Scale Dependence of Polarized DIS Asymmetries

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    We compare the Q2Q^{2} dependence of the polarized deep inelastic scattering proton asymmetry, driven by the leading order Altarelli Parisi evolution equations, to those arising from fixed order αs\alpha_{s} and αs2\alpha_{s}^{2} approximations. It is shown that the evolution effects associated with gluons, which are not properly taken into account by the leading order approximation, cannot be neglected in the analysis of the most recent experimental data.Comment: Latex file, (9 figures in postcript available from [email protected]

    Extracting the Proton ubar content from pp->Direct Photon plus Jet Cross Sections

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    An analysis procedure is proposed to measure the antiquark distributions in the proton over the region 0.01 < x < 0.1. The procedure involves the measurement of high p_t asymmetric direct photon and jet final states in pp interactions. This measurement can be made at the RHIC collider running in pp mode at an energy of sqrt(s)=500 GeV/c. This analysis identifies a region of phase space where the contribution from quark-antiquark annihilation uncharacteristically approaches the magnitude of the contribution from the leading process, quark-gluon Compton scattering. The forward-backward angular asymmetry in the parton center of mass is sensitive to the antiquark content of the proton and the ubar parton density function can be extracted.Comment: 21 pages, 7 figure

    Analytic Approaches to the Evolution of Polarised Parton Distributions at Small xx

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    The Q2Q^2 evolution of polarised parton distributions at small xx is studied. Various analytic approximations are critically discussed. We compare the full evolution with that obtained from the leading-pole approximation to the splitting functions, and show that the validity of this approximation depends critically on the x0x \to 0 behaviour of the starting distributions. A new analytic solution which is valid at small xx is obtained, and its domain of applicability is discussed.Comment: 14 pages, LATeX, 4 figures availabe as .uu-fil
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