now, we impose 1 more things, the Reduced Planck constant, h_bar also set to 1. that simplify all equations with angular momentum or spin.
the Angular momentum:
L^2 | l, m > = h_bar l ( l+1) |l, m >
Lz |l, m > = h_bar m |l, m >
now becomes :
L^2 | l, m > = l ( l+1) |l, m >
Lz |l, m > = m |l, m >
this is same for the spin.
by doing so, the magnetic moment will be
mu = g x muB x S or g x muB x L
since there is no h_bar in S or L anymore.
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