Differential Neutron Production Cross Sections for 256-MeV Protons

In this paper differential (p, xn) cross sections d{sup 2}{sigma}/d{Omega}E{sub n}, from the thin targets of beryllium, carbon, oxygen, aluminum, iron, lead, and {sup 238}U for 256-MeV protons are measured. Time-of-flight techniques are used to identify and discriminate against backgrounds and to determine the neutron energy spectrum. Comparison of the experimental data with intranuclear-cascade evaporation-model calculations using the HETC code showed discrepancies of as much as a factor of 7, notably at 7.5 and 150 deg.

[1]  G. Morgan,et al.  Neutron yields from stopping-length targets for 256-MeV protons , 1992 .

[2]  G. Morgan,et al.  Efficiency calibration of a cylindrical BC418 neutron detector at neutron energies between 135 and 800 MeV , 1992 .

[3]  Kazuo Shin,et al.  Neutron Production from Thick Targets of Carbon, Iron, Copper, and Lead by 30- and 52-MeV Protons , 1983 .

[4]  H. Bertini Intranuclear-cascade calculation of the secondary nucleon spectra from nucleon-nucleus interactions in the energy range 340 to 2900 mev and comparisons with experiment , 1969 .

[5]  Armstrong,et al.  Systematics of angular-dependent neutron production by 585 MeV protons on targets with 12 <= A <= 238: Differential cross section measurements. , 1987, Physical review. C, Nuclear physics.

[6]  M. S. Moore Rate dependence of counting losses in neutron time-of-flight measurements , 1980 .

[7]  Y. Uwamino,et al.  Neutron and photon production from thick targets bombarded by 30-MeV p, 33-MeV d, 65-MeV /sup 3/He, and 65-MeV. cap alpha. ions: Experiment and comparison with cascade Monte Carlo calculations , 1984 .

[8]  C. E. Moss,et al.  Differential Neutron Production Cross Sections and Neutron Yields from Stopping-Length Targets for 113-MeV Protons , 1989 .

[9]  G. Morgan,et al.  Neutron Yields from Stopping- and Near-Stopping-Length Targets for 256-MeV Protons , 1990 .

[10]  Richard Madey,et al.  Improved predections of neutron detection efficiency for hydrocarbon scintillators from 1 MeV to about 300 MeV , 1979 .