Results 301 to 310 of about 188,539 (327)
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1995
In Sect. 5.5 we discussed the spectra observed in electron scattering off nuclei. As well as the elastic scattering peak some additional peaks, which we associated with nuclear excitations, were observed. Similar spectra are observed for electron-nucleon scattering.
Bogdan Povh +4 more
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In Sect. 5.5 we discussed the spectra observed in electron scattering off nuclei. As well as the elastic scattering peak some additional peaks, which we associated with nuclear excitations, were observed. Similar spectra are observed for electron-nucleon scattering.
Bogdan Povh +4 more
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AIP Conference Proceedings, 1975
Some examples of developments in the field of inelastic electron scattering are given including the physics of this study, an application of electromagnetic transition densities to beta decay, negative muon capture, and positive pion photoproduction in lithium-6 and helium-6, giant resonances, vibrational states in zinc-64, -66, and -68, shapes of ...
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Some examples of developments in the field of inelastic electron scattering are given including the physics of this study, an application of electromagnetic transition densities to beta decay, negative muon capture, and positive pion photoproduction in lithium-6 and helium-6, giant resonances, vibrational states in zinc-64, -66, and -68, shapes of ...
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Inelastic Scattering and Applications [PDF]
Reviews in Mineralogy and Geochemistry, 2006 Inelastic neutron scattering (INS) in general refers to scattering processes which involve energy and momentum exchange between the neutron and the scatterer. It is widely utilized for characterization of materials in basic and applied research across many disciplines including mineralogy.
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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
If light interacts with matter without changing its frequency, the process is called elastic scattering because the photons change only their direction and not their energy. The scattered light has the same frequency as the incident light. Rayleigh scattering is one particular elastic scattering process.
Gustav Schweiger, E. James Davis
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If light interacts with matter without changing its frequency, the process is called elastic scattering because the photons change only their direction and not their energy. The scattered light has the same frequency as the incident light. Rayleigh scattering is one particular elastic scattering process.
Gustav Schweiger, E. James Davis
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Inelastic Neutron Scattering, Applications
1999The application of both coherent and incoherent neutron scatting techniques to problems in chemistry, physics, engineering catalysis and polymers is described. The various different types of structural and dynamic molecular information that can be obtained are illustrated.
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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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Inelastic Diffraction Scattering
Physical Review, 1960The method of distorted waves Born approximation is shown to be equivalent to the first-order adiabatic method for the calculation of inelastic scattering. The flexibility of the distorted waves method was indicated and tested by numerical calculation for a simplified model.
E. Rost, N. Austern
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Inelastic Scattering Amplitudes
AIP Conference Proceedings, 1973New results from inelastic two‐body scattering reactions are reviewed. Although predictions of SU(3), factorization and simple Regge theory are found to be qualitatively in agreement with the data, direct channel or absorption effects afford the simplest interpretation of the detailed features of the scattering amplitudes.
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