5.1.2. Neutrons in an External Field
For a neutron the Dirac Hamiltonian is somewhat simpler
![]() | (5.10) |
with gn = -3.82. Again for pz = 0 the states of lowest energy, the ones we shall be interested in, have energies
![]() | (5.11) |
Boosting to a finite pz we obtain
![]() | (5.12) |
The wave functions corresponding to this energy are
![]() | (5.13) |
where u(p, s = -1) is the standard spinor for a particle with momentum p, energy sqrt[p2 + Mn2] (not the energy of Eq. (5.12) and spin down.
In the non-relativistic limit
![]() | (5.14) |
and the wave functions are
![]() | (5.15) |