by U.S. Atomic Energy Commission, Division of Technical Information] in [Oak Ridge, Tenn .
Written in English
Bibliography: p. 280.
|Statement||by James F. Zigler.|
|The Physical Object|
|Pagination||vii, 280 p.|
|Number of Pages||280|
Calculation of the Inelastic Longitudinal Electron Scattering of 20Ne and 24Mg Nuclei. from the prediction of the simple shell model. The elastic electron scattering form factors of the considered nuclei were calculated using the ground state charge density b form factors of C4 transitions in even-even N = Z sd-shell nuclei (20Ne, 24Mg, 28Si and . Shell-model wave functions calculated within the complete space of 0p(,3/2)- 0p(,1/2) and 0d(,5/2)- 1s(,1/2) - 0d(,3/2) configurations are used to calculate elastic and inelastic form factors of electron scattering from p-shell and sd-shell nuclei. We analyze the magnetic elastic scattering data for p-shell and sd-shell nuclei and both the electric and magnetic inelastic electroexcitation of. It is shown that the variation with energy of the differential cross section for the scattering of high energy electrons by nuclei depends on whether the nuclear transition occurs with ΔM = 0 or with ΔM = ±1, whereM is the component of the nuclear spin in the direction of the vector change of momentum of the scattered electron. The electron excitation of ΔM = 0 transitions is then Cited by:
Shell-model wave functions obtained from a complete, unified treatment of the structure of the positive parity states in nuclei between 16O and 40Ca are used to calculate the features of inelastic. Purchase Electron Scattering From Complex Nuclei V36A - 1st Edition. Print Book & E-Book. ISBN , Book Edition: 1. Calculation of the Inelastic Longitudinal Form Factors for Some Light Nuclei used to calculate the features of inelastic electron scattering to 2+ and 4+ states in this region. Calculation. Mott Scattering Scattering of a relativistic electron by a pointlike spin 1/2 proton Similar to electron muon scattering from last Lecture Usually described in the Lab frame, where the proton is at rest: θ is the lab scattering angle of the electron pe is the incident electron beam momentum q2 is the four-momentum transfer of the virtual photon.
Abstract. The coherent density fluctuation model is applied in this chapter using the high-energy approximation to describe electron elastic scattering by nuclei (Sect. ), The problems of explaining the cross-sections and the longitudinal and transverse response functions obtained in quasielastic electron scattering by various nuclei are discussed with different theoretical methods in Sect Cited by: Inelastic electron scattering to 2+ and 4+ states for the even–even N=Zsd-shell nuclei (20Ne, 24Mg, 28Si and 32S) are discussed taking into account higher energy configurations outside the sd-shell. Inclusive Inelastic Electron Scattering from Nuclei Nadia Fomin University of Virginia, Charlottesville, VA Abstract. Inclusive electron scattering from nuclei at large x and Q2 is the result of a reaction mechanism that includes both quasi–elastic scattering from nucleons and deep inelastic scattering from the quark consitituents of the. We carry out calculations for two particular nuclei, Li' and , chosen to illustrate the general procedure and to point out some of the nuclear physics one can hope to learn from inelastic electron scattering experiments. 2. Calculation and General Discussion of Cross Sections Cited by: