Planck's's radiation function is the function
(1)
|
which is normalized so that
(2)
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However, the function is sometimes also defined without the numerical normalization factor of
(e.g., Abramowitz and Stegun 1972, p. 999).
The first and second raw moments are
(3)
| |||
(4)
|
where
is Apéry's constant, but higher order raw
moments do not exist since the corresponding integrals do not converge.
It has a maximum at (OEIS A133838),
where
(5)
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and inflection points at (OEIS A133839)
and
(OEIS A133840), where
(6)
|