The p-adic gamma function is the unique continuous function of a p-adic integer x (with values in Z p {\displaystyle \mathbb {Z} _{p}} ) such that
for positive integers x, where the product is restricted to integers i not divisible by p. As the positive integers are dense with respect to the p-adic topology in Z p {\displaystyle \mathbb {Z} _{p}} , Γ p ( x ) {\displaystyle \Gamma _{p}(x)} can be extended uniquely to the whole of Z p {\displaystyle \mathbb {Z} _{p}} . Here Z p {\displaystyle \mathbb {Z} _{p}} is the ring of p-adic integers. It follows from the definition that the values of Γ p ( Z ) {\displaystyle \Gamma _{p}(\mathbb {Z} )} are invertible in Z p {\displaystyle \mathbb {Z} _{p}} ; this is because these values are products of integers not divisible by p, and this property holds after the continuous extension to Z p {\displaystyle \mathbb {Z} _{p}} . Thus Γ p : Z p → Z p × {\displaystyle \Gamma _{p}:\mathbb {Z} _{p}\to \mathbb {Z} _{p}^{\times }} . Here Z p × {\displaystyle \mathbb {Z} _{p}^{\times }} is the set of invertible p-adic integers.
The classical gamma function satisfies the functional equation Γ ( x + 1 ) = x Γ ( x ) {\displaystyle \Gamma (x+1)=x\Gamma (x)} for any x ∈ C ∖ Z ≤ 0 {\displaystyle x\in \mathbb {C} \setminus \mathbb {Z} _{\leq 0}} . This has an analogue with respect to the Morita gamma function:
The Euler's reflection formula Γ ( x ) Γ ( 1 − x ) = π sin ( π x ) {\displaystyle \Gamma (x)\Gamma (1-x)={\frac {\pi }{\sin {(\pi x)}}}} has its following simple counterpart in the p-adic case:
where x 0 {\displaystyle x_{0}} is the first digit in the p-adic expansion of x, unless x ∈ p Z p {\displaystyle x\in p\mathbb {Z} _{p}} , in which case x 0 = p {\displaystyle x_{0}=p} rather than 0.
and, in general,
At x = 1 2 {\displaystyle x={\frac {1}{2}}} the Morita gamma function is related to the Legendre symbol ( a p ) {\displaystyle \left({\frac {a}{p}}\right)} :
It can also be seen, that Γ p ( p n ) ≡ 1 ( mod p n ) , {\displaystyle \Gamma _{p}(p^{n})\equiv 1{\pmod {p^{n}}},} hence Γ p ( p n ) → 1 {\displaystyle \Gamma _{p}(p^{n})\to 1} as n → ∞ {\displaystyle n\to \infty } .1: 369
Other interesting special values come from the Gross–Koblitz formula, which was first proved by cohomological tools, and later was proved using more elementary methods.2 For example,
where − 1 ∈ Z 5 {\displaystyle {\sqrt {-1}}\in \mathbb {Z} _{5}} denotes the square root with first digit 3, and − 3 ∈ Z 7 {\displaystyle {\sqrt {-3}}\in \mathbb {Z} _{7}} denotes the square root with first digit 2. (Such specifications must always be done if we talk about roots.)
Another example is
where − 2 {\displaystyle {\sqrt {-2}}} is the square root of − 2 {\displaystyle -2} in Q 3 {\displaystyle \mathbb {Q} _{3}} congruent to 1 modulo 3.3
The Raabe-formula for the classical Gamma function says that
This has an analogue for the Iwasawa logarithm of the Morita gamma function:4
The ceiling function to be understood as the p-adic limit lim n → ∞ ⌈ x n p ⌉ {\displaystyle \lim _{n\to \infty }\left\lceil {\frac {x_{n}}{p}}\right\rceil } such that x n → x {\displaystyle x_{n}\to x} through rational integers.
The Mahler expansion is similarly important for p-adic functions as the Taylor expansion in classical analysis. The Mahler expansion of the p-adic gamma function is the following:5: 374
where the sequence a k {\displaystyle a_{k}} is defined by the following identity:
Robert, Alain M. (2000). A course in p-adic analysis. New York: Springer-Verlag. /wiki/Springer-Verlag ↩
Robert, Alain M. (2001). "The Gross-Koblitz formula revisited". Rendiconti del Seminario Matematico della Università di Padova. The Mathematical Journal of the University of Padova. 105: 157–170. doi:10.1016/j.jnt.2009.08.005. hdl:2437/90539. ISSN 0041-8994. MR 1834987. http://www.numdam.org/item?id=RSMUP_2001__105__157_0 ↩
Cohen, H. (2007). Number Theory. Vol. 2. New York: Springer Science+Business Media. p. 406. /wiki/Springer_Science%2BBusiness_Media ↩
Cohen, Henri; Eduardo, Friedman (2008). "Raabe's formula for p-adic gamma and zeta functions". Annales de l'Institut Fourier. 88 (1): 363–376. doi:10.5802/aif.2353. hdl:10533/139530. MR 2401225. http://www.numdam.org/item/AIF_2008__58_1_363_0/ ↩