In this study, light elements Li ,10B for (a,n) and (n,a) reactions
as well as o-particle energy from threshold energy to 10 MeV are
used according to the available data of reaction cross sections. The
more recent cross sections data of (a,n) and (n,a) reactions are
reproduced in fine steps 42 Kev for 10B(n,o) Li in the specified
energy range, as well as cross section (o,n) Values were derived from
the published data of (n,a) as a function of a-energy in the same fine
energy steps by using the principle inverse reactions. This calculation
involves only the ground state of Li OB in the reactions 'Li(a,n) B
B (n,a) Li
Introduction
When two charged nuclei overcome their Coulomb repulsion, a
rearrangement of the constituents of the nucleus may occur. Similar
to the rearrangement of atoms in reacting molecules during a chemical
reaction this may result a
a nuclear reaction
target
Nuclear reactions are usually produced by bombarding a or
nucleus with a nuclear projectile in most cases a nucleon (neutron proton) or a light nucleus such as a deuteron or an majority of nuclear
At low excitation energies 10 MeV),the reactions involve the formation of two nuclei
one nearly equal in
charge and mass number to the target nucleus. Such reactions are
represented by an equation of the type
b
X a
the lab. System)
Where X target (at rest in bombarding particle
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