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Anisotropic spin stripe domains in bilayer La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub>. [PDF]
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1978
Deep inelastic electron and muon scattering experiments, first performed at the Stanford Linear Accelerator, have given a tantalizing glimpse of the inner structure of the proton and the neutron. The results of these experiments agree well with the hypothesis that the nucleon consists of more elementary constituents, called partons.
P. V. Landshoff, H. Osborn
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Deep inelastic electron and muon scattering experiments, first performed at the Stanford Linear Accelerator, have given a tantalizing glimpse of the inner structure of the proton and the neutron. The results of these experiments agree well with the hypothesis that the nucleon consists of more elementary constituents, called partons.
P. V. Landshoff, H. Osborn
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Physics Education, 1998
Feynman diagrams can be used to explain deep inelastic scattering, but it must be remembered that the emission and absorption of a photon are not independent events - the underlying field is important.
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Feynman diagrams can be used to explain deep inelastic scattering, but it must be remembered that the emission and absorption of a photon are not independent events - the underlying field is important.
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2002
Deep inelastic scattering (DIS) is the prototype of hard hadronic processes. As such, it provides an important — and very successful — test of perturbative QCD. It represents also the most direct way to explore the internal structure of hadrons.
Enrico Predazzi, Vincenzo Barone
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Deep inelastic scattering (DIS) is the prototype of hard hadronic processes. As such, it provides an important — and very successful — test of perturbative QCD. It represents also the most direct way to explore the internal structure of hadrons.
Enrico Predazzi, Vincenzo Barone
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Deep Inelastic Electron Scattering [PDF]
Annual Review of Nuclear Science, 1972 CONTENTS I. INfRODUcnON. . . .. .. . . . . . . . . . . . .. .. . .. .. . . . .. .. .. .. . . . . . . . . . . . . . .. 204 II. EXPERIMENTAL METHOD.... . . . . . . . . . . . . . . • . . . • • • . . . . . • • • . . . . . . . . . . .. 205 Equipment .. . Radiative corrections . III. PROTON AND DEUTERIUM CROSS SECfIONS . IV. KINEMATICS AND VARIABLES .
Jerome I. Friedman, H. W. Kendall
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Structure functions in deep inelastic scattering and in deep inelastic annihilation
Il Nuovo Cimento A, 1976Structure functions in ep → e + X are directly obtained by using Wilson’s short-distance expansion and the conformal covariant light-cone expansion. It is shown that Bjorken scaling is broken in general due to the existence of anomalous dimensions in the expansions.
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Neutrino Deep Inelastic Scattering
AIP Conference Proceedings, 2007This paper presents neutrino cross section and structure function measurements. The recent results from NuTeV and Chorus experiments are discussed. The status of the MINOS measurements of the cross section energy dependence and of the structure functions are summarized.
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Applications in deep inelastic scattering
1997The preceding chapters have established the theoretical framework which ought to describe the perturbative scattering of strongly interacting particles at high centre-of-mass energies (in the Regge region). In this chapter (and the next), we shall attempt to place this framework under the experimental spotlight.
J. R. Forshaw, D. A. Ross
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