Systematics of angular-dependent neutron production by 585 MeV protons on targets with12 ≤ A ≤ 238: Differential cross section measurements

1987 ◽  
Vol 36 (5) ◽  
pp. 1976-1987 ◽  
Author(s):  
S. Cierjacks ◽  
Y. Hino ◽  
F. Raupp ◽  
L. Buth ◽  
D. Filges ◽  
...  
Keyword(s):  
Differential Cross Section ◽  
Cross Section ◽  
Differential Cross ◽  
Neutron Production ◽  
Mev Protons

Polarization and Differential Cross Section for Elastic Scattering of 40-MeV Protons. II

1967 ◽  
Vol 156 (4) ◽  
pp. 1207-1218 ◽  
Author(s):  
M. P. Fricke ◽  
E. E. Gross ◽  
B. J. Morton ◽  
A. Zucker
Keyword(s):  
Elastic Scattering ◽  
Differential Cross Section ◽  
Cross Section ◽  
Differential Cross ◽  
Mev Protons

scholarly journals Experimental Neutron-Production Double-Differential Cross Section for the Nuclear Reaction by 1.5-GeV π+Mesons Incident on Iron

1997 ◽  
Vol 34 (8) ◽  
pp. 860-862 ◽  
Author(s):  
Tatsushi NAKAMOTO ◽  
Kenji ISHIBASHI ◽  
Naruhiro MATSUFUJI ◽  
Nobuhiro SHIGYO ◽  
Keisuke MAEHATA ◽  
...  
Keyword(s):  
Differential Cross Section ◽  
Nuclear Reaction ◽  
Cross Section ◽  
Differential Cross ◽  
Neutron Production ◽  
Double Differential Cross Section

scholarly journals Double-differential cross section measurement with low threshold detector for proton production induced by several tens of MeV protons

2020 ◽  
Vol 239 ◽  
pp. 01038
Author(s):  
Yuji Yamaguchi ◽  
Toshiya Sanami ◽  
Yusuke Koba ◽  
Yusuke Uozumi
Keyword(s):  
Differential Cross Section ◽  
Cross Section ◽  
Differential Cross ◽  
Particle Identification ◽  
Double Differential Cross Section ◽  
Threshold Detector ◽  
Proton Production ◽  
Nuclear Data Library ◽  
Low Threshold ◽  
Mev Protons

We have developed a low threshold detector consisting of Bragg curve counter (BCC), two siliconsurface barrier detectors (SSDs) and BGO scintillator to obtain experimental double-differential cross section (DDX) data for low energy proton production. Since the BCC offers advantage of self particle identification capability and a few μm-thick entrance window, protons produced by nuclear reactions down to 1 MeV have been identified. The capability of the detector is demonstrated in measurements using 70-MeV protons. Measured spectra are compared with calculation results of intra-nuclear cascade (INC) plus evaporation models and nuclear data library.

scholarly journals Excitation of the 9·50 MeV (9/2+) State of 13C in Intermediate Energy Scattering Experiments

1982 ◽  
Vol 35 (1) ◽  
pp. 9
Author(s):  
L Rickus ◽  
SF Collins ◽  
KA Amos ◽  
BM Spicer ◽  
GG Shute ◽  
...  
Keyword(s):  
Angular Momentum ◽  
Angular Distribution ◽  
Differential Cross Section ◽  
Inelastic Scattering ◽  
Cross Section ◽  
Differential Cross ◽  
Total Angular Momentum ◽  
Intermediate Energy ◽  
Large Asymmetry ◽  
Mev Protons

The differential cross section for the inelastic scattering of 135 MeV protons leading to the9/2+ (9·5 MeV) state in 13C has been measured. Microscopic DWBA analyses show that the angular distribution is well described by a pure (or nearly pure) 1p3/2 to 1d5/2 neutron transition with a total angular momentum transfer of 4, a description which is consistent with the previously observed large asymmetry in inelastic π+ and π- scattering to this state.

scholarly journals An Analysis of Inelastic Scattering to the 2+ State in 54Fe at 1·409 MeV

1973 ◽  
Vol 26 (5) ◽  
pp. 575 ◽  
Author(s):  
R Smith ◽  
K Amos
Keyword(s):  
Differential Cross Section ◽  
Inelastic Scattering ◽  
Cross Section ◽  
Differential Cross ◽  
Distorted Wave ◽  
Polarization Model ◽  
Core Polarization ◽  
Spin Flip ◽  
Asymmetry Data ◽  
Mev Protons

The differential cross section, spin-flip probability amplitude, and asymmetry for the inelastic scattering of19�6 MeV protons to the 2+ state in 54Feat 1�409 MeV are analysed. The antisymmetrized distorted wave approximation is used to evaluate the scattering amplitudes in which the reaction mechanism is represented by a generalized core polarization model. Good fits are obtained to the differential cross section and spin-flip probability data. The exchange core polarization contributions are shown to be essential to obtain such fits. However, the asymmetry data cannot be fitted simultaneously, and this failure demonstrates the limitations of the current collective model representation of the core polarization process

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