Planck's's radiation function is the function
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(1)
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which is normalized so that
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(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
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(3)
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(4)
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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
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(5)
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and inflection points at (OEIS A133839)
and
(OEIS A133840), where
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(6)
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