نتایج جستجو برای: deep inelastic scattering
تعداد نتایج: 325219 فیلتر نتایج به سال:
We point out one of the possible sources of the "NuTeV anomaly": the effect of the non-adequate application of the one-loop electroweak radiative corrections including QED hard photon emission derived by Bardin and Dokuchaeva (1986) in the NuTeV radiative corrections data analysis of deep inelastic neutrino and anti-neutrino deep inelastic scattering. c Copyright owned by the author(s) under th...
We predict the rate of deep inelastic scattering (DIS) events containing an identified forward π 0 that is expected in the experiments at the HERA electron-proton collider, in order to see if this process can be used as an indicator of the underlying small x dynamics. We determine the background due to deep inelastic events containing forward photons which are fragments of the forward jet. We c...
We derive a modified form of the BFKL equation which enables the structure of the gluon emissions to be studied in small x deep inelastic scattering. The equation incorporates the resummation of the virtual and unresolved real gluon emissions. We solve the equation to calculate the number of small x deep-inelastic events containing 0, 1, 2 . . . resolved gluon jets, that is jets with transverse...
We survey the contributions presented in the working group " Diffraction and Vector Mesons " at the XIV International Workshop on Deep Inelastic Scattering.
Analyses of event shapes and forward jet production in deep inelastic scattering at the HERA collider are described. The results are compared to QCD predictions.
A brief review on the status of unpolarized parton densities and the determination of the QCD scale ΛQCD from deep-inelastic scattering data is presented.
Recent measurements and theoretical developments on the hadronic final state in deep-inelastic scattering, p¯ p and e + e − collisions are presented.
By using the convolution formalism which consists of Fermi motion and binding effect, we investigate the deep inelastic electron scattering from A=3 mirror in the deep-valence region. The initial valence quark input is taken from the GRVs (Gluck, Reya and Vogt) fitting procedure and the next-to-leading order QCD evolution on FP2 (x,Q2) which gives very good fit to the available data in the (x,Q...
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