1.1. Part I — The Kubota–Leopoldt p-adic L-function
The goal of Part I is a single analytic object \zeta_p and a single
interpolation theorem.
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What a
p-adicL-function should be (§2). The Riemann zeta function\zeta(s)has rational special values\zeta(1-n) = -B_n/n. After removing the Euler factor atp, the values(1 - p^{n-1})\zeta(1-n)satisfy Kummer's congruences modulo powers ofp, which is exactly the statement that they extend to a continuous (indeed analytic) function on\Zp— thep-adicL-function. This chapter fixes the interpolation property we are aiming for. -
Measures and the Iwasawa algebra (§3). A
p-adic measure on\Zpis a bounded\Cp-linear functional on continuous functions; the Mahler transform identifies measures with power series, giving the ring isomorphism\Lam := \Zp[[\Zpx]] \cong \Zp[[T]](the Iwasawa algebra). This is the foundational chapter: measures, the Iwasawa algebra, Mahler transforms, the measure-theoretic toolbox, pseudo-measures, and locally analytic distributions. -
Construction of
\zeta_p(§4). Following Kubota–Leopoldt, one writes down, foracoprime top, an explicit measure\mu_aon\Zp, restricts it to\Zpx, and rescales away the dependence onato obtain the pseudo-measure whose Mellin transform is the Kubota–Leopoldtp-adicL-function. -
Interpolation at Dirichlet characters (§5). Integrating
\zeta_pagainst a Dirichlet character\chiofp-power conductor — and then against tame conductors — recovers, up to explicit Euler and Gauss-sum factors, the special valuesL(\chi, 1-n)of the complex DirichletL-function. The Mellin transform turns measures on\Zpxinto analytic functions on\Zp. -
The value at
s=1(§6) and the residue ats=1(§7). Thep-adic analytic class number formula:\zeta_phas a simple pole ats=1whose residue is thep-adic analogue of1 - 1/p, mirroring the complex residue of\zeta. -
The
p-adic family of Eisenstein series (§8). The constant terms of ap-adic family of Eisenstein series are values of\zeta_p, foreshadowing the modular-forms picture of Part II.