The Dirichlet L-function is given by the analytic continuation of
The Dirichlet L-function at negative integers is given by
where Bn,χ is a generalized Bernoulli number defined by
for χ a Dirichlet character with conductor f.
The Kubota–Leopoldt p-adic L-function Lp(s, χ) interpolates the Dirichlet L-function with the Euler factor at p removed. More precisely, Lp(s, χ) is the unique continuous function of the p-adic number s such that
for positive integers n divisible by p − 1. The right hand side is just the usual Dirichlet L-function, except that the Euler factor at p is removed, otherwise it would not be p-adically continuous. The continuity of the right hand side is closely related to the Kummer congruences.
When n is not divisible by p − 1 this does not usually hold; instead
for positive integers n. Here χ is twisted by a power of the Teichmüller character ω.
p-adic L-functions can also be thought of as p-adic measures (or p-adic distributions) on p-profinite Galois groups. The translation between this point of view and the original point of view of Kubota–Leopoldt (as Qp-valued functions on Zp) is via the Mazur–Mellin transform (and class field theory).
Deligne & Ribet (1980), building upon previous work of Serre (1973), constructed analytic p-adic L-functions for totally real fields. Independently, Barsky (1978) and Cassou-Noguès (1979) did the same, but their approaches followed Takuro Shintani's approach to the study of the L-values.