TY - JOUR
T1 - Cross sections for the Li7(p,n)Be7 reaction between 4.2 and 26 MeV
AU - Poppe, C. H.
AU - Anderson, J. D.
AU - Davis, J. C.
AU - Grimes, S. M.
AU - Wong, C.
PY - 1976
Y1 - 1976
N2 - Using pulsed-beam neutron time-of-flight spectrometry relative differential cross sections for Li7(p,n0)Be7(g.s.) and Li7(p,n1)Be*7 (0.431 MeV) have been measured over the laboratory angular range 3.5°to 159°and from an incident bombarding energy of 4.2 to 26 MeV. These cross sections have been integrated over angle and at 5 MeV the resulting integral was normalized to the absolute measurement of Macklin and Gibbons in order to obtain absolute differential and total cross sections for each neutron group. At energies above 6 MeV the 3.5°cross section for each group decreases monotonically, reaching a minimum at about 12 MeV. Both cross sections then increase, the ground-state cross section approaching a center-of-mass value of 15 mb/sr at 26 MeV. The forward-angle ratio of n1 to n0 neutrons remains around 30% from 8 to 26 MeV, obtaining a maximum of about 35% at 26 MeV. The integrated cross sections, on the other hand, both decrease from 6 MeV to the maximum energy. Neutrons from states in Be7 at 4.55, 6.51, 7.19, and possibly 10.79 MeV as well as those from three-body breakup were also observed in this experiment. NUCLEAR REACTIONS Li7(p,n)E=4.2-26 MeV; measured σ(E,θ) to Be7 ground state and first excited state; θ=3.5°-159°.
AB - Using pulsed-beam neutron time-of-flight spectrometry relative differential cross sections for Li7(p,n0)Be7(g.s.) and Li7(p,n1)Be*7 (0.431 MeV) have been measured over the laboratory angular range 3.5°to 159°and from an incident bombarding energy of 4.2 to 26 MeV. These cross sections have been integrated over angle and at 5 MeV the resulting integral was normalized to the absolute measurement of Macklin and Gibbons in order to obtain absolute differential and total cross sections for each neutron group. At energies above 6 MeV the 3.5°cross section for each group decreases monotonically, reaching a minimum at about 12 MeV. Both cross sections then increase, the ground-state cross section approaching a center-of-mass value of 15 mb/sr at 26 MeV. The forward-angle ratio of n1 to n0 neutrons remains around 30% from 8 to 26 MeV, obtaining a maximum of about 35% at 26 MeV. The integrated cross sections, on the other hand, both decrease from 6 MeV to the maximum energy. Neutrons from states in Be7 at 4.55, 6.51, 7.19, and possibly 10.79 MeV as well as those from three-body breakup were also observed in this experiment. NUCLEAR REACTIONS Li7(p,n)E=4.2-26 MeV; measured σ(E,θ) to Be7 ground state and first excited state; θ=3.5°-159°.
UR - https://www.scopus.com/pages/publications/0242286332
U2 - 10.1103/PhysRevC.14.438
DO - 10.1103/PhysRevC.14.438
M3 - Article
AN - SCOPUS:0242286332
SN - 0556-2813
VL - 14
SP - 438
EP - 445
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 2
ER -