The stretched exponential function, also called the Kohlrausch or Kohlrausch-Williams-Watts function, is the function
|
(1)
|
where ,
,
and conventionally
(Williams and Watts 1970). The case
is the ordinary exponential
function.
For ,
the function is completely
monotonic and hence is a Laplace transform.
More explicitly,
|
(2)
|
where
is the one-sided stable distribution with
stability index
(Pollard 1946). Consequently, its exact probability
density over exponential relaxation times is
|
(3)
| |||
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(4)
|
For example, when ,
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(5)
|
The improper integral of the stretched exponential, also interpreted as its mean relaxation time, is
|
(6)
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This should not be confused with using a normalized stretched exponential itself as a phenomenological probability density,
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(7)
|
which is generally different from the exact relaxation-time probability density (Ribeiro de Almeida et al. 2026).