S. V. Vostokov's 2013 Mat. Sb. paper on Shafarevich's 'A general reciprocity law' develops a method based on Witt's identification of the Brauer group of a field with its group of primary elements and proves explicit formulas for the Hilbert symbol in a classical local field (Theorem 1) and for the Hilbert pairing on a complete nn-dimensional field with perfect residue field (Theorems 2-4) — in every case only for odd pp; the value is expressed as a power of a root of unity with exponent aφ=Aφ−Aa_\varphi=A^\varphi-A, where AΔ−A=aA^\Delta-A=a, but aφa_\varphi is determined only modulo (pm,℘)(p^m,\wp). The open problem addressed here is the residue-characteristic-2 case in the higher-dimensional setting: construct, with complete proof, an explicit and effectively computable formula for the Hilbert pairing on complete higher-dimensional fields containing the 2m2^m-th roots of unity. The one-dimensional case is known by other methods (Henniart; Vostokov-Fesenko; Kölcze; Belyaeva-Vostokov); for higher fields only an announced, incompletely published p=2p=2 construction exists (Beliaeva-Vostokov 1998/2001), and all subsequent approaches work with pp odd.

Background

Explicit reciprocity laws are closed-form expressions for the norm-residue (Hilbert) symbol, the pairing that encodes local class field theory. For a field KK that is a finite extension of Qp\mathbb{Q}_p and contains the group μpn\mu_{p^n} of pnp^n-th roots of unity, the Hilbert symbol is defined by (α,β)=ΨK(α)(βpn)/βpn(\alpha,\beta)=\Psi_K(\alpha)(\sqrt[p^n]{\beta})/\sqrt[p^n]{\beta}, where ΨK:K∗→Gal⁡(Kab/K)\Psi_K:K^*\to\operatorname{Gal}(K^{ab}/K) is the local reciprocity map of class field theory; computing it explicitly is regarded as the final step of Hilbert's ninth problem on the most general reciprocity law. I. R. Shafarevich's 1950 paper 'A general reciprocity law' introduced the technique of primary elements — an element ω∈K∗\omega\in K^* is pnp^n-primary if the extension K(ωpn)/KK(\sqrt[p^n]{\omega})/K is unramified — together with explicit generating systems of K∗K^* now called Shafarevich bases, and these ideas underlie most explicit formulas, notably S. V. Vostokov's 1978 formula expressing (α,β)(\alpha,\beta) through the residue of a power series built from the Artin-Hasse function E(X)=exp⁡(X+Xp/p+Xp2/p2+⋯ )E(X)=\exp(X+X^p/p+X^{p^2}/p^2+\cdots) and the logarithms of the arguments.

The higher-dimensional setting is as follows. A complete nn-dimensional field is a field complete with respect to a discrete valuation whose residue field is a complete (n−1)(n-1)-dimensional field, the chain ending in a perfect field kk of characteristic p>0p>0; when kk is finite this is a higher local field in the usual sense. For such fields A. N. Parshin and K. Kato constructed local class field theory on the topological Milnor KK-groups Kntop(K)K_n^{top}(K) (Milnor KK-theory endowed with the topology in which valuation-open unit subgroups generate the topological group), and I. B. Fesenko extended the theory to complete fields with an arbitrary perfect residue field. Writing W(k)W(k) for the ring of Witt vectors (infinite sequences of residue-field elements with carry-wise addition, on which the Frobenius Δ\Delta acts coordinate-wise) and ℘(x)=xΔ−x\wp(x)=x^\Delta-x, the theory requires κ=dim⁡Fpk/℘(k)>0\kappa=\dim_{\mathbb{F}_p}k/\wp(k)>0, i.e. the residue field admits a nontrivial Artin-Schreier extension. For KK containing μpm\mu_{p^m} one then has the Hilbert pairing

(⋅,⋅): Kntop(K)×K∗/K∗pm⟶μpm,(\cdot,\cdot):\ K_n^{top}(K)\times K^*/K^{*p^m}\longrightarrow\mu_{p^m},

defined through Fesenko's reciprocity map ΨK:VKntop(K)→Hom⁡Zp(Gal⁡(Kab,p/Knr,p),μpm)\Psi_K:VK_n^{top}(K)\to\operatorname{Hom}_{\mathbb{Z}_p}(\operatorname{Gal}(K^{ab,p}/K^{nr,p}),\mu_{p^m}), where Knr,p=K⋅W(kab,p)K^{nr,p}=K\cdot W(k^{ab,p}) is the maximal abelian unramified pp-extension of KK and VKntop(K)VK_n^{top}(K) is the subgroup generated by principal units (units congruent to 1 modulo the maximal ideal); evaluating at each φ∈Gal⁡(Knr,p/K)\varphi\in\operatorname{Gal}(K^{nr,p}/K) yields the μpm\mu_{p^m}-valued pairing written informally in the source and used in the Problem Statement below.

Vostokov's 2013 paper, dedicated to Shafarevich's memory, returns to this circle of ideas with a new method based on Witt's observation that the Brauer group of a field containing μpm\mu_{p^m} identifies with the group of pmp^m-primary elements. It proves the classical local-field formula (Theorem 1) and the higher-dimensional formula (Theorems 2-4): for local parameters t1,…,tnt_1,\dots,t_n and arguments α1,…,αn+1∈K∗\alpha_1,\dots,\alpha_{n+1}\in K^*,

({α1,…,αn},αn+1)(φ)=ζaφ,φ∈Gal⁡(Knr,p/K),(\{\alpha_1,\dots,\alpha_n\},\alpha_{n+1})(\varphi)=\zeta^{a_\varphi},\qquad\varphi\in\operatorname{Gal}(K^{nr,p}/K),

where ζ\zeta is a primitive pmp^m-th root of unity, aa is a multidimensional residue of an explicitly written differential expression Φ(α1,…,αn+1)/(ζpm−1)\Phi(\alpha_1,\dots,\alpha_{n+1})/(\zeta^{p^m}-1) built from logarithms and logarithmic derivatives of the power-series expansions of the αi\alpha_i in t1,…,tnt_1,\dots,t_n, and aφ=Aφ−Aa_\varphi=A^\varphi-A for a solution AA of the Artin-Schreier-type equation AΔ−A=aA^\Delta-A=a. Every theorem is proved under the hypothesis p≠2p\neq 2: the two congruence lemmas carrying the computation (Lemma 3 and the main Lemma 9, comparing the truncated logarithm l(ε)l(\varepsilon) with (1−Δ)log⁡ε(1-\Delta)\log\varepsilon modulo pnp^n) are stated and proved only for p>3p>3, and Remark 5 notes that aφa_\varphi is determined only modulo (pm,℘)(p^m,\wp) — the element AA exists and aφa_\varphi is independent of its choice, but AA is not described explicitly.

For one-dimensional local fields the p=2p=2 explicit formulas are classical: G. Henniart (1981) and Vostokov-Fesenko (1984-85, Lubin-Tate setting) obtained them, P. Kölcze (1995) proved the Brückner-Vostokov series formula is valid for p=2p=2, and Belyaeva-Vostokov worked out the detailed one-dimensional theory for arbitrary pp, odd and even, including the correction terms (adding 1/21/2 to the term 1/(ζpn−1)1/(\zeta^{p^n}-1)) that the 2013 paper itself cites. For higher fields, however, every complete published formula assumes pp odd: Vostokov's 1985 multidimensional construction, the Lubin-Tate generalizations of Afanas'eva-Bekker-Vostokov and Afanas'eva (2013-14, residue characteristic p>2p>2), Zinov'ev's Artin-Hasse and Iwasawa type formulas (2002-06), Abrashkin-Jenni's field-of-norms derivation (2012, from the characteristic-pp Witt-symbol formula for p>2p>2), and Flórez's norm-residue symbol (2017, p>2p>2). The only p=2p=2 higher-dimensional line is an announced construction of Beliaeva-Vostokov (1998; 2001 Part I) whose published proof of the crucial symbol property is incomplete, the complete proof being promised in a continuation that never appeared. This is the open problem addressed here: the effectively computable, completely proved residue-characteristic-2 formula in the higher-dimensional setting.

Problem Statement

Let p=2p=2. Let KK be a complete nn-dimensional field with n≥2n\ge 2, of characteristic 0, whose last residue field kk is perfect of characteristic 2 with κ=dim⁡F2k/℘(k)>0\kappa=\dim_{\mathbb{F}_2}k/\wp(k)>0, and assume μ2m⊂K\mu_{2^m}\subset K, so that the Hilbert pairing

(⋅,⋅): Kntop(K)×K∗/K∗2m⟶μ2m(\cdot,\cdot):\ K_n^{top}(K)\times K^*/K^{*2^m}\longrightarrow\mu_{2^m}

of Fesenko's higher local class field theory is defined, evaluated at each φ∈Gal⁡(Knr,2/K)\varphi\in\operatorname{Gal}(K^{nr,2}/K). Construct, with complete proof, an explicit formula for this pairing of the Shafarevich-Vostokov type — an effectively computable value ζaφ\zeta^{a_\varphi}, where aφa_\varphi is obtained from the arguments α1,…,αn+1∈K∗\alpha_1,\dots,\alpha_{n+1}\in K^* through residues of explicitly constructed power series in their expansions in local parameters t1,…,tnt_1,\dots,t_n — in the spirit of Theorems 2-4 of Vostokov (2013), which cover only p≠2p\neq 2. The formula must be well defined — independent of the choices of series expansions, local parameters, prime element, and of the solution AA of AΔ−A=aA^\Delta-A=a entering aφ=Aφ−Aa_\varphi=A^\varphi-A — and must coincide with the Hilbert pairing via the 2-primary reciprocity map. The formula is sought in the generality of the source's Theorems 3-4: complete higher-dimensional fields with an arbitrary perfect residue field of characteristic 2 satisfying κ>0\kappa>0, in the mixed-characteristic case; standard higher local fields (finite last residue field) form the particular case corresponding to the source's Corollary 4. The one-dimensional case is excluded because it is already known by other methods (Henniart; Vostokov-Fesenko; Kölcze).

References

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