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Gross–Stark Units in p-adic Class Field Theory

Updated 15 December 2025
  • Gross–Stark units are canonical p-units in abelian CM-extensions of totally real fields, defined using p-adic L-functions and regulators.
  • They generalize classical circular units through analytic, cohomological, and algorithmic methods, directly addressing a p-adic version of Hilbert’s 12th problem.
  • Their explicit values allow effective construction of abelian extensions and refined control of class groups, underpinning advances in p-adic Stark theory.

Gross–Stark units are canonical pp-units in abelian CM-extensions of totally real number fields, constructed as deep arithmetic avatars of pp-adic special values or derivatives of Artin LL-functions, and characterized by explicit relations to pp-adic L-functions, regulators of units, and abelian class field theory. These units generalize the classical circular units and Jacobi sums, crucially implementing “Hilbert’s 12th problem” by providing a pp-adic and arithmetic construction of abelian extensions via the values of pp-adic L-functions and modular forms.

1. Foundational Setup and Definition

Let kk be a totally real field, K/kK/k a finite abelian CM-extension with Galois group G=Gal(K/k)G=\mathrm{Gal}(K/k), and pp a rational prime unramified in kk. Denote by SS_\infty the set of archimedean places and by SpS_p the primes above pp. The “minus” SS-unit group is defined as

U={uOK[1/p]×:u1+c=1},U^- = \{u \in \mathcal{O}_K[1/p]^\times : u^{1+c}=1\},

where cGc \in G is complex conjugation. For a totally odd character χ:GQp×\chi: G \to \overline{\mathbb{Q}}_p^\times, UχU^-_\chi is the χ\chi-isotypic component of UU^-, and XχX_\chi the corresponding degree-zero subgroup of divisors of pp-places. In the rank-one case, this space is one-dimensional:

  • If χ(p)=1\chi(\mathfrak{p})=1 for exactly one prime pp\mathfrak{p}|p and χ(p)1\chi(\mathfrak{p'}) \neq 1 for other pp\mathfrak{p'}|p, then dimQpUχ=1\dim_{\overline{\mathbb{Q}}_p} U^-_\chi = 1.

A generator upχUχu_p^\chi \in U^-_\chi, well-defined up to scalars and roots of unity, is called the Gross–Stark unit (Gross et al., 2023).

2. pp-adic LL-functions and Regulators

The relevant pp-adic LL-function is the Deligne–Ribet–Cassou-Noguès function Lp(χω,s)L_p(\chi\omega, s), where ω\omega is the pp-adic cyclotomic character. Under the rank-one hypothesis, Lp(χω,0)=0L_p(\chi\omega, 0) = 0 and ords=0Lp(χω,s)=1\operatorname{ord}_{s=0} L_p(\chi\omega, s)=1, so the first derivative Lp(χω,0)Qp×L'_p(\chi\omega, 0)\in\overline{\mathbb{Q}}_p^\times is canonical.

There are two intrinsic isomorphisms UχXχU^-_\chi\to X_\chi:

  • The “valuation map” uqpfqordq(u)qu \mapsto \sum_{\mathfrak{q}|p} f_{\mathfrak{q}}\cdot \operatorname{ord}_{\mathfrak{q}}(u)\cdot \mathfrak{q}.
  • The “pp-adic logarithm” uqplogpNKq/Qp(u)qu \mapsto \sum_{\mathfrak{q}|p} \log_p N_{K_{\mathfrak{q}}/\mathbb{Q}_p}(u)\cdot \mathfrak{q}.

The Gross pp-adic regulator is

Rp(χ)=logpNKq/Qp(u)ordq(u)R_p(\chi) = \frac{ \log_p N_{K_\mathfrak{q}/\mathbb{Q}_p}(u) }{ \operatorname{ord}_\mathfrak{q}(u) }

for any generator uUχu\in U^-_\chi (Gross et al., 2023, Honnor, 2021).

3. Gross’s pp-adic Stark Conjecture and Unconditional Proofs

Gross’s conjecture (1981) in the rank-one abelian case asserts

Rp(χ)Ap(χ)=Lp(χω,0),R_p(\chi)\cdot A_p(\chi) = L'_p(\chi\omega, 0),

where Ap(χ)A_p(\chi) is the (signed) complex LL-value L(χ,0)-L(\chi, 0) (up to explicit constants). Normalizing so ordq(upχ)=1\operatorname{ord}_\mathfrak{q}(u_p^\chi)=1, one obtains

logpNKq/Qp(upχ)=Lp(χω,0)L(χ,0),\log_p N_{K_\mathfrak{q}/\mathbb{Q}_p}(u_p^\chi) = - \frac{L'_p(\chi\omega, 0)}{L(\chi,0)},

or, equivalently,

upχ=expp(Rp(χ)1Lp(χω,0)).u_p^\chi = \exp_p\left( R_p(\chi)^{-1} L'_p(\chi\omega,0) \right).

Dasgupta–Darmon–Pollack first proved this formula under Leopoldt’s conjecture and a nonvanishing hypothesis; Ventullo (2013) removed these, and Kakde–Ventullo (2018) gave a fully unconditional proof in the general rank-one abelian setting (Gross et al., 2023, Ventullo, 2013, Dasgupta et al., 2016).

In higher-rank, for r>1r > 1 places above pp with χ(p)=1\chi(\mathfrak{p}) = 1, the derivative ords=0Lp(χω,s)r\operatorname{ord}_{s=0}L_p(\chi\omega,s)\ge r, and the rr-th order term is conjecturally and provenly governed by the determinant of the r×rr\times r Gross regulator matrix (Gross et al., 2023, Dasgupta et al., 2016).

4. Explicit Analytic and Cohomological Constructions

The explicit formula for Gross–Stark units involves pp-adic integration over Shintani domains. Dasgupta provided an analytic construction using pp-adic multiplicative integrals and measures μ(b,D)\mu(\mathfrak{b}, D) on local units, which, up to compensators and canonical powers of uniformizers, gives units in Fp×F_\mathfrak{p}^\times matching the conjectural Gross–Stark units. This construction is formulated as:

up,T(b,D)=ϵ(b,D,π)πζR,T(H/F,b,0)O×xdμ(b,D,x)u_{\mathfrak{p}, T}(\mathfrak{b}, D) = \epsilon(\mathfrak{b}, D, \pi)\cdot\pi^{\zeta_{R,T}(H/F, \mathfrak{b}, 0)}\cdot \prod_\mathcal{O}^\times x\, d\mu(\mathfrak{b}, D, x)

(Honnor, 2021).

Concurrently, the cohomological formula of Dasgupta–Spieß realizes the regulator as a cup-cap pairing in the group cohomology of units, relating Eisenstein cocycles (arising from Shintani zeta values) with local cocycles of pp-adic logarithms and valuations. The regulator matrix

Lalg(χ)p,q=q(up,χ)oq(up,χ)\mathcal{L}_{\mathrm{alg}}(\chi)_{\mathfrak{p},\mathfrak{q}} = - \frac{ \ell_\mathfrak{q}(u_{\mathfrak{p}, \chi}) }{ o_\mathfrak{q}(u_{\mathfrak{p}, \chi}) }

is shown to coincide (diagonally, and for [F:Q]=3[F:\mathbb{Q}]=3 in totality) with the analytic regulator (Honnor, 2021). This establishes a bridge between arithmetic and cohomological constructions.

5. Applications in Explicit Class Field Theory

Gross–Stark units realize abelian extensions of totally real fields “p-adically,” paralleling the role of special values of modular functions in complex multiplication for imaginary quadratic fields. The explicit values of the units at Frobenius elements allow for explicit Galois actions, furnishing class field theory extensions—addressing a pp-adic version of Hilbert’s 12th problem.

The proof of the Brumer–Stark and “integral Gross–Stark” conjectures over Z[1/2]\mathbb{Z}[1/2] exploits Gross–Stark units as pp-adic analogues of the canonical generators of abelian extensions. Furthermore, explicit generation results demonstrate that the maximal abelian extension of any totally real field is achieved by adjoining Gross–Stark units (across conductors) together with suitably chosen totally positive square roots (Gross et al., 2023, Dasgupta et al., 2021).

6. Algorithmic Computation and Examples

Recent advances include effective algorithms for computing pp-adic logarithms and recovering explicit Gross–Stark units in concrete number fields, using overconvergent modular forms and reduction theory. Explicit tables for narrow Hilbert class fields of real quadratic fields and various primes pp showcase the computational tractability for fields of moderate discriminant and class number, relying on q-expansions, Newton polygons, and lattice reductions for unit identification (Damm-Johnsen, 2023).

A classical example is the case k=Qk=\mathbb{Q} and K=Q(D)K=\mathbb{Q}(\sqrt{-D}) with quadratic Dirichlet character χ\chi; then

upχa(modD),χ(a)=1J(a,p)a,χ(a)=1J(a,p)u_p^\chi \sim \frac{\prod_{a\,(\mathrm{mod}\, D), \chi(a)=1} J(a,p)}{ \prod_{a, \chi(a)=-1} J(a,p)}

and pp-adic logarithms of uu recover the LL-derivative Lp(χω,0)L'_p(\chi\omega, 0) up to explicit constants (Gross et al., 2023).

7. Conceptual and Theoretical Significance

Gross–Stark units unify and refine the theory of Stark units, pp-adic and complex LL-functions, Shintani zeta values, and the Eisenstein cocycle framework. The proof of Gross’s conjecture in both rank-one and higher-rank cases by Dasgupta, Kakde, and Ventullo provides a cornerstone for pp-adic Stark theory. Consequences include refined control of Fitting ideals of class groups (in the minus part) and advances toward the Equivariant Tamagawa Number Conjecture.

Moreover, extensions and refinements—such as period-ring-valued enhancements via pp-adic Hodge theory and generalizations to Beilinson–Flach classes and adjoint Artin representations—indicate ongoing developments forming the “axiomatic exceptional zero theory” landscape in modern Iwasawa theory (Gross et al., 2023, Kashio, 2017, Rivero, 2021).


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