scholarly journals Superscaling analysis of inclusive electron scattering and its extension to charge-changing neutrino-nucleus cross sections beyond the relativistic Fermi gas approach

2006 ◽  
Vol 74 (5) ◽  
Author(s):  
A. N. Antonov ◽  
M. V. Ivanov ◽  
M. K. Gaidarov ◽  
E. Moya de Guerra ◽  
J. A. Caballero ◽  
...  
Keyword(s):  
Electron Scattering ◽  
Cross Sections ◽  
Fermi Gas ◽  
Inclusive Electron ◽  
Relativistic Fermi

scholarly journals Parity-violating electron scattering from the pion-correlated relativistic Fermi gas

1994 ◽  
Vol 569 (4) ◽  
pp. 701-731 ◽  
Author(s):  
M.B. Barbaro ◽  
A. De Pace ◽  
T.W. Donnelly ◽  
A. Molinari
Keyword(s):  
Electron Scattering ◽  
Fermi Gas ◽  
Relativistic Fermi

scholarly journals Superscaling analyses of inclusive electron scattering and their extension to charge-changing neutrino cross sections in nuclei

2007 ◽  
Author(s):  
A. N. Antonov ◽  
M. V. Ivanov ◽  
M. K. Gaidarov ◽  
E. Moya de Guerra ◽  
J. A. Caballero ◽  
...  
Keyword(s):  
Electron Scattering ◽  
Cross Sections ◽  
Inclusive Electron

POLARIZED AND UNPOLARIZED INCLUSIVE ELECTRON SCATTERING IN NUCLEI AND THE INCLUSIVE NEUTRINO CROSS-SECTION

1995 ◽  
Vol 04 (01) ◽  
pp. 163-179
Author(s):  
S.L. MINTZ ◽  
M. POURKAVIANI
Keyword(s):  
Cross Section ◽  
Electron Scattering ◽  
Cross Sections ◽  
Inelastic Electron ◽  
Nuclear Excitation ◽  
Scattering Cross ◽  
Neutrino Cross Section ◽  
Inclusive Electron ◽  
Scattering Cross Sections ◽  
The Relationship

The unpolarized and parity violating polarized inclusive inelastic electron scattering cross-sections are calculated for incident electrons from threshold to 100 MeV, for the 12C nucleus. The relationship between these cross-sections and the inclusive neutrino cross-section on this same nucleus is discussed. The possibility of using the parity violating polarized electron scattering interaction to obtain the average nuclear excitation is also discussed.

scholarly journals Gauge and Lorentz invariant one-pion exchange currents in electron scattering from a relativistic Fermi gas

2002 ◽  
Vol 368 (4) ◽  
pp. 317-407 ◽  
Author(s):  
J.E. Amaro ◽  
M.B. Barbaro ◽  
J.A. Caballero ◽  
T.W. Donnelly ◽  
A. Molinari
Keyword(s):  
Electron Scattering ◽  
Fermi Gas ◽  
Pion Exchange ◽  
Relativistic Fermi

scholarly journals Measurement of the cross sections for inclusive electron scattering in the E12-14-012 experiment at Jefferson Lab

2019 ◽  
Vol 100 (5) ◽  
Author(s):  
M. Murphy ◽  
H. Dai ◽  
L. Gu ◽  
D. Abrams ◽  
A. M. Ankowski ◽  
...  
Keyword(s):  
Electron Scattering ◽  
Cross Sections ◽  
Jefferson Lab ◽  
The Cross ◽  
Inclusive Electron

scholarly journals Scaling in electron scattering from a relativistic Fermi gas

1988 ◽  
Vol 38 (4) ◽  
pp. 1801-1810 ◽  
Author(s):  
W. M. Alberico ◽  
A. Molinari ◽  
T. W. Donnelly ◽  
E. L. Kronenberg ◽  
J. W. Van Orden
Keyword(s):  
Electron Scattering ◽  
Fermi Gas ◽  
Relativistic Fermi

Electron Scattering in Solids

1990 ◽  
Vol 48 (2) ◽  
pp. 4-5
Author(s):  
Ryuichi Shimizu ◽  
Ze-Jun Ding
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Angular Distribution ◽  
Elastic Scattering ◽  
Electron Scattering ◽  
Cross Sections ◽  
Expansion Method ◽  
Electron Excitation ◽  
Partial Wave Expansion ◽  
Backscattered Electrons

Monte Carlo simulation has been becoming most powerful tool to describe the electron scattering in solids, leading to more comprehensive understanding of the complicated mechanism of generation of various types of signals for microbeam analysis.The present paper proposes a practical model for the Monte Carlo simulation of scattering processes of a penetrating electron and the generation of the slow secondaries in solids. The model is based on the combined use of Gryzinski’s inner-shell electron excitation function and the dielectric function for taking into account the valence electron contribution in inelastic scattering processes, while the cross-sections derived by partial wave expansion method are used for describing elastic scattering processes. An improvement of the use of this elastic scattering cross-section can be seen in the success to describe the anisotropy of angular distribution of elastically backscattered electrons from Au in low energy region, shown in Fig.l. Fig.l(a) shows the elastic cross-sections of 600 eV electron for single Au-atom, clearly indicating that the angular distribution is no more smooth as expected from Rutherford scattering formula, but has the socalled lobes appearing at the large scattering angle.

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