Abstract
We consider the spin-dependent changes in the electromagnetic energy of a system when the system is inserted between infinite perfectly conducting parallel plates, separated by a distance
L
. For practicable values of the magnetic field and of
L
, the change δμ in the magnetic moment μ of an electron bound in a neutral atom is of the order δμ/μ ~ (μ/
L
)
2
, where
h
= 1 =
c
. The change A
v
in the hyperfine splitting
v
is of the order A
v/v
≈ (
a/L
)
3
, with
a
the Bohr radius; this falls many orders of magnitude short of the experimental upper limit of Guttrich & Billman. We show that, surprisingly, a non-relativistic calculation yields correct results for a bound electron, though for a free electron one needs a fully relativistic calculation, to be reported separately.
Cited by
29 articles.
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