Planck's's radiation function is the function
| 
 
(1)
 
 | 
which is normalized so that
| 
 
(2)
 
 | 
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
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(5)
 
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and inflection points at  (OEIS A133839)
 and 
 (OEIS A133840), where
| 
 
(6)
 
 |