scholarly journals Possible G-Parity Nonconservation in Muon Capture Reactions: Angular Distribution of Recoils

2013 ◽  
Vol E65 (0) ◽  
pp. 96-103
Author(s):  
M. Morita ◽  
R. Morita ◽  
T. Shirafuji
Keyword(s):  
Angular Distribution ◽  
Muon Capture ◽  
Parity Nonconservation ◽  
G Parity

Possible G-Parity Nonconservation in Muon Capture Reactions

1964 ◽  
Vol 19 (10) ◽  
pp. 1759-1764 ◽  
Author(s):  
Masato Morita ◽  
Reiko Morita
Keyword(s):  
Muon Capture ◽  
Parity Nonconservation ◽  
G Parity

scholarly journals Electron-Newtrino Angular Correlation in G-Parity Nonconservation

1977 ◽  
Vol 58 (4) ◽  
pp. 1218-1230 ◽  
Author(s):  
T. Sato ◽  
J. Yamane ◽  
M. Morita
Keyword(s):  
Angular Correlation ◽  
Parity Nonconservation ◽  
G Parity

Beta-ray angular distribution in aligned 12B and 12N and G-parity irregular induced tensor current

1978 ◽  
Vol 73 (1) ◽  
pp. 17-19 ◽  
Author(s):  
Masato Morita ◽  
Michiaki Nishimura ◽  
Hisao Ohtsubo
Keyword(s):  
Angular Distribution ◽  
G Parity ◽  
Tensor Current

Neutron spectrum and asymmetry of the angular distribution in muon capture on 4He Nucleus

1972 ◽  
Vol 39 ◽  
pp. 216-226 ◽  
Author(s):  
R.A. Eramzhyan ◽  
V.N. Fetisov ◽  
Yu.A. Salganic
Keyword(s):  
Angular Distribution ◽  
Neutron Spectrum ◽  
Muon Capture

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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