There are multiple equivalent definitions of the K-function.
The direct definition:
![{\displaystyle K(z)=(2\pi )^{-{\frac {z-1}{2}}}\exp \left[{\binom {z}{2}}+\int _{0}^{z-1}\ln \Gamma (t+1)\,dt\right].}](https://wikimedia.org/api/rest_v1/media/math/render/svg/92baaaf4dc396046aef97cda91dd4f102aa06973)
Definition via
![{\displaystyle K(z)=\exp {\bigl [}\zeta '(-1,z)-\zeta '(-1){\bigr ]}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/12668025758db5c6b204ac5b1f43c1e8e05785a5)
where ζ′(z) denotes the derivative of the Riemann zeta function, ζ(a,z) denotes the Hurwitz zeta function and

Definition via polygamma function:[1]
![{\displaystyle K(z)=\exp \left[\psi ^{(-2)}(z)+{\frac {z^{2}-z}{2}}-{\frac {z}{2}}\ln 2\pi \right]}](https://wikimedia.org/api/rest_v1/media/math/render/svg/527eb0c1daf22e5bb0b92ff2ff331e64b68f597e)
Definition via balanced generalization of the polygamma function:[2]
![{\displaystyle K(z)=A\exp \left[\psi (-2,z)+{\frac {z^{2}-z}{2}}\right]}](https://wikimedia.org/api/rest_v1/media/math/render/svg/e7e5a0771140cd752c427198127287d5cc8b0466)
where A is the Glaisher constant.
It can be defined via unique characterization, similar to how the gamma function can be uniquely characterized by the Bohr-Mollerup Theorem:
Let
be a solution to the functional equation
, such that there exists some
, such that given any distinct
, the divided difference
.
Such functions are precisely
, where
is an arbitrary constant.[3]