Definitions/Def_Deformation_SplitCoordinates.lean
Connected–étale splitting data for Honda system lifting
Throughout, \mathcal{O} is a commutative ring with a fixed algebra map to \mathbb{F}_p (p prime), r a natural number, H_1 a Honda system for the element p on \mathcal{O}^r (i.e. commuting \mathcal{O}-linear F,V with FV=VF=p, together with a submodule L satisfying the three Honda axioms), and (G_v)_{v\ge 0} a tower of commutative Hopf \mathbb{F}_p-algebras with bialgebra transition maps s_v\colon G_{v+1}\to G_v and additive maps \pi_v\colon\mathcal{O}^r\to M(G_v) into the Dieudonné module of G_v, the latter being the colimit over n of the groups of truncated Witt-vector covectors u with \Delta u=u\otimes1+1\otimes u.
SplitCoordinates is pure data: integers d,h^c,h^e; towers (G^c_v,s^c_v) and (G^e_v,s^e_v) of commutative Hopf \mathbb{F}_p-algebras; bialgebra maps q^c_v\colon G_v\to G^c_v, \pi^e_v\colon G_v\to G^e_v, a section \sigma_v\colon G^e_v\to G_v, and \Theta_v\colon G_v\to G^c_v\otimes_{\mathbb{F}_p}G^e_v; a d-dimensional formal group law \Phi_0 over \mathbb{F}_p with presentations \kappa_v\colon\mathbb{F}_p[[X_1,\dots,X_d]]\to G^c_v; a tower (E_v,s^t_v) of Hopf \mathcal{O}-algebras with maps \theta^e_v\colon\mathbb{F}_p\otimes_{\mathcal{O}}E_v\to G^e_v and elements \hat c_{i,k,v}\in E_v; submodules M^c,M^{et}\subseteq\mathcal{O}^r, an \mathcal{O}-basis \alpha of L indexed by \mathrm{Fin}\,d, and power series \bar a_{i,k} over \mathbb{F}_p with lifts a_{i,k} over \mathcal{O}.
The predicate Lawful collects, as fields, the identities that make such a datum a connected–étale splitting with coordinates; its hypotheses are grouped as follows, and the groups are summarised. (i) h^c+h^e=r, the p-divisible tower axioms for G^c and G^e (local resp. reduced and formally unramified levels, cocommutative, finite, surjective transitions with kernels the p^v-torsion ideals, ranks p^{vh^c}, p^{vh^e}). (ii) q^c_v,\pi^e_v surjective, \ker\pi^e_v the nilradical, \pi^e_v\circ\sigma_v=\mathrm{id}, \ker q^c_v the ideal generated by \sigma_v of the augmentation ideal, \Theta_v bijective and equal to comultiplication followed by q^c_v\otimes\pi^e_v, and compatibility of q^c,\pi^e,\sigma,\Theta with all transitions. (iii) \Phi_0 commutative, \kappa_v surjective with kernel the ideal generated by the p^v-series of \Phi_0, compatible with s^c_v, given by adic evaluation, with comultiplication of \kappa_v(X_i) computed by the group law, rank p^{h^c} for the quotient by the p-series, d the cotangent rank of the augmentation ideal of G^c_1, kernels of \kappa_v eventually inside arbitrary powers of (X), and joint injectivity and surjectivity onto the inverse limit. (iv) E_v cocommutative, finite free and formally étale over \mathcal{O}, s^t_v surjective with p^v-torsion kernel, \theta^e_v bijective and transition-compatible, and the lifting property that for every p-adically complete \mathcal{O}-algebra reduction mod p is a bijection on \mathcal{O}-algebra maps out of E_v. (v) Witt-coordinate realisations: for each v,i the image of \pi_v(\alpha_i) under \pi^e_v (resp. q^c_v) is represented by a covector of some length n whose (n-1-k)-th coefficient is \theta^e_v(1\otimes\hat c_{i,k,v}) (resp. \kappa_v(\bar a_{i,k})), these terms vanishing for k\ge n. (vi) The Fitting splitting: M^c and M^{et} are complementary, F- and V-stable, free of ranks h^c,h^e, with F^N M^c\subseteq pM^c for some N, F bijective-type behaviour on M^{et}, the divisibility characterisations of membership in M^c and M^{et}, L\cap M^{et}=0, the Honda axioms for the projection of L into M^c along M^{et}, and vanishing of \pi_v composed with \pi^e_v on M^c and with q^c_v on M^{et}. (vii) Normalisations of the coefficient series: a_{i,k} reduces to \bar a_{i,k}, has zero constant term, and \bar a_{i,k}\to0 adically.
The second predicate, NormalForm, constrains the lifted series: the linear part of (a_{i,0})_i reduces mod p to the identity, and the (i,j) entries of the linear part of (a_{i,1})_i with j\le i lie in (p).
Relation to Mathlib
Mathlib has no notion of Honda systems, of Dieudonné modules of towers of Hopf algebras, or of connected–étale splittings; these are the project's own, built on Mathlib's bialgebra and Hopf algebra API, truncated Witt vectors and multivariate power series. The p^v-torsion ideals occurring in the transition-kernel conditions are those of the project's PDivisibleGroup.Hopf development, defined as the image of the augmentation ideal under the p^v-fold convolution power of the identity.
Where it is used
These data package Fontaine's connected–étale splitting with coordinates, used in formalising the classification of p-divisible groups and finite flat group schemes in characteristic p by Honda systems. That classification underlies the analysis of the local-at-p deformation conditions in the Galois deformation theory of the Frey curve.
References
- J.-M. Fontaine, Groupes p-divisibles sur les corps locaux, Astérisque 47–48, Société Mathématique de France, 1977, Ch. IV §1
- J. T. Tate, p-divisible groups, in: Proceedings of a Conference on Local Fields (Driebergen, 1966), Springer, 1967, 158–183
- B. Conrad, Finite group schemes over bases with low ramification, Compositio Mathematica 119 (1999), 239–320
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 196 lines
- 70 declarations
- used in the statements of 9 theorems and imported by 10 proofs
- imports 6 definition modules
Source file: Definitions/Def_Deformation_SplitCoordinates.lean
Imports
Imported by
- no other definition module
Declarations
- structure
Deformation.HondaSystem.SplitCoordinates - field
Deformation.HondaSystem.SplitCoordinates.d - field
Deformation.HondaSystem.SplitCoordinates.hc - field
Deformation.HondaSystem.SplitCoordinates.he - field
Deformation.HondaSystem.SplitCoordinates.Gc - field
Deformation.HondaSystem.SplitCoordinates.Ge - field
Deformation.HondaSystem.SplitCoordinates.sc - field
Deformation.HondaSystem.SplitCoordinates.se - field
Deformation.HondaSystem.SplitCoordinates.qc - field
Deformation.HondaSystem.SplitCoordinates.Et - field
Deformation.HondaSystem.SplitCoordinates.st - field
Deformation.HondaSystem.SplitCoordinates.Mc - field
Deformation.HondaSystem.SplitCoordinates.Met - field
Deformation.HondaSystem.SplitCoordinates.abar - field
Deformation.HondaSystem.SplitCoordinates.a - structure
Deformation.HondaSystem.SplitCoordinates.Lawful - field
Deformation.HondaSystem.SplitCoordinates.Lawful.hc_add_he - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isLocalRing_Gc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isReduced_Ge - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isCocomm_Gc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isCocomm_Ge - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finite_Gc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finite_Ge - field
Deformation.HondaSystem.SplitCoordinates.Lawful.sc_surjective - field
Deformation.HondaSystem.SplitCoordinates.Lawful.se_surjective - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finrank_Gc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finrank_Ge - field
Deformation.HondaSystem.SplitCoordinates.Lawful.ker_sc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.ker_se - field
Deformation.HondaSystem.SplitCoordinates.Lawful.qc_surjective - field
Deformation.HondaSystem.SplitCoordinates.Lawful.ker_qc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.qc_comp_s - field
Deformation.HondaSystem.SplitCoordinates.Lawful.formallyUnramified_Ge - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finrank_quot_nthSeries - field
Deformation.HondaSystem.SplitCoordinates.Lawful.MvPowerSeries - field
Deformation.HondaSystem.SplitCoordinates.Lawful.d_eq_finrank_cotangent - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isCocomm_Et - field
Deformation.HondaSystem.SplitCoordinates.Lawful.free_Et - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finite_Et - field
Deformation.HondaSystem.SplitCoordinates.Lawful.formallyEtale_Et - field
Deformation.HondaSystem.SplitCoordinates.Lawful.st_surjective - field
Deformation.HondaSystem.SplitCoordinates.Lawful.ker_st - field
Deformation.HondaSystem.SplitCoordinates.Lawful.bijective_comp_mk - field
Deformation.HondaSystem.SplitCoordinates.Lawful.realisation_etale - field
Deformation.HondaSystem.SplitCoordinates.Lawful.isCompl - field
Deformation.HondaSystem.SplitCoordinates.Lawful.F_mem_Mc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.V_mem_Mc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.F_mem_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.V_mem_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.pow_F_Mc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.F_surjOn_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.Met_le_range_F - field
Deformation.HondaSystem.SplitCoordinates.Lawful.mem_Met_iff - field
Deformation.HondaSystem.SplitCoordinates.Lawful.mem_Mc_iff - field
Deformation.HondaSystem.SplitCoordinates.Lawful.free_Mc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.free_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finrank_Mc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.finrank_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.L_inf_Met - field
Deformation.HondaSystem.SplitCoordinates.Lawful.sh1_le_Lc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.sh1_ge_Lc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.p - field
Deformation.HondaSystem.SplitCoordinates.Lawful.sh2_Lc - field
Deformation.HondaSystem.SplitCoordinates.Lawful.a_map - field
Deformation.HondaSystem.SplitCoordinates.Lawful.constantCoeff_a - field
Deformation.HondaSystem.SplitCoordinates.Lawful.abar_tendsto - field
Deformation.HondaSystem.SplitCoordinates.Lawful.realisation_conn - structure
Deformation.HondaSystem.SplitCoordinates.NormalForm - field
Deformation.HondaSystem.SplitCoordinates.NormalForm.linearPart_zero - field
Deformation.HondaSystem.SplitCoordinates.NormalForm.linearPart_one
Source
import Mathlib import Definitions.Def_Dieudonne_DatumAndHonda import Definitions.Def_Dieudonne_WittVectorHom import Definitions.Def_Dieudonne_WittHomColimit import Definitions.Def_PDivisibleGroup_Basic import Definitions.Def_MvFormalGroup_BasicV2 import Definitions.Def_MvFormalGroup_PointsV2 set_option autoImplicit false open scoped TensorProduct open MvPowerSeries universe u v namespace Deformation.HondaSystem variable {𝓞 : Type u} [CommRing 𝓞] (p : ℕ) [Fact p.Prime] [Algebra 𝓞 (ZMod p)] variable (r : ℕ) (H₁ : Deformation.HondaSystem (p : 𝓞) (Fin r → 𝓞)) variable (G : ℕ → Type v) [∀ v, CommRing (G v)] [∀ v, HopfAlgebra (ZMod p) (G v)] structure SplitCoordinates (s : ∀ v, G (v + 1) →ₐc[ZMod p] G v) (π : ∀ v, (Fin r → 𝓞) →+ Deformation.DieudonneModule (ZMod p) p (G v)) where d : ℕ hc : ℕ he : ℕ Gc : ℕ → Type v Ge : ℕ → Type v [instCommRingGc : ∀ v, CommRing (Gc v)] [instHopfGc : ∀ v, HopfAlgebra (ZMod p) (Gc v)] [instCommRingGe : ∀ v, CommRing (Ge v)] [instHopfGe : ∀ v, HopfAlgebra (ZMod p) (Ge v)] sc : ∀ v, Gc (v + 1) →ₐc[ZMod p] Gc v se : ∀ v, Ge (v + 1) →ₐc[ZMod p] Ge v qc : ∀ v, G v →ₐc[ZMod p] Gc v πe : ∀ v, G v →ₐc[ZMod p] Ge v σ : ∀ v, Ge v →ₐc[ZMod p] G v Θ : ∀ v, G v →ₐc[ZMod p] Gc v ⊗[ZMod p] Ge v Φ₀ : MvFormalGroup d (ZMod p) κ : ∀ v, MvPowerSeries (Fin d) (ZMod p) →ₐ[ZMod p] Gc v Et : ℕ → Type u [instCommRingEt : ∀ v, CommRing (Et v)] [instHopfEt : ∀ v, HopfAlgebra 𝓞 (Et v)] st : ∀ v, Et (v + 1) →ₐc[𝓞] Et v θe : ∀ v, ZMod p ⊗[𝓞] Et v →ₐc[ZMod p] Ge v ĉ : Fin d → ℕ → ∀ v, Et v Mc : Submodule 𝓞 (Fin r → 𝓞) Met : Submodule 𝓞 (Fin r → 𝓞) α : Module.Basis (Fin d) 𝓞 H₁.L abar : Fin d → ℕ → MvPowerSeries (Fin d) (ZMod p) a : Fin d → ℕ → MvPowerSeries (Fin d) 𝓞 attribute [instance] SplitCoordinates.instCommRingGc SplitCoordinates.instHopfGc SplitCoordinates.instCommRingGe SplitCoordinates.instHopfGe SplitCoordinates.instCommRingEt SplitCoordinates.instHopfEt namespace SplitCoordinates variable {p r H₁ G s π} variable (𝒮 : SplitCoordinates p r H₁ G s π) structure Lawful : Prop where hc_add_he : 𝒮.hc + 𝒮.he = r isLocalRing_Gc : ∀ v, IsLocalRing (𝒮.Gc v) isReduced_Ge : ∀ v, IsReduced (𝒮.Ge v) isCocomm_Gc : ∀ v, Coalgebra.IsCocomm (ZMod p) (𝒮.Gc v) isCocomm_Ge : ∀ v, Coalgebra.IsCocomm (ZMod p) (𝒮.Ge v) finite_Gc : ∀ v, Module.Finite (ZMod p) (𝒮.Gc v) finite_Ge : ∀ v, Module.Finite (ZMod p) (𝒮.Ge v) sc_surjective : ∀ v, Function.Surjective (𝒮.sc v) se_surjective : ∀ v, Function.Surjective (𝒮.se v) finrank_Gc : ∀ v, Module.finrank (ZMod p) (𝒮.Gc v) = p ^ (v * 𝒮.hc) finrank_Ge : ∀ v, Module.finrank (ZMod p) (𝒮.Ge v) = p ^ (v * 𝒮.he) ker_sc : ∀ v, RingHom.ker (𝒮.sc v) = PDivisibleGroup.Hopf.torsionIdeal (ZMod p) (𝒮.Gc (v + 1)) (p ^ v) ker_se : ∀ v, RingHom.ker (𝒮.se v) = PDivisibleGroup.Hopf.torsionIdeal (ZMod p) (𝒮.Ge (v + 1)) (p ^ v) qc_surjective : ∀ v, Function.Surjective (𝒮.qc v) πe_surjective : ∀ v, Function.Surjective (𝒮.πe v) ker_πe : ∀ v, RingHom.ker (𝒮.πe v : G v →ₐ[ZMod p] 𝒮.Ge v) = nilradical (G v) πe_comp_σ : ∀ v, (𝒮.πe v).comp (𝒮.σ v) = BialgHom.id (ZMod p) (𝒮.Ge v) ker_qc : ∀ v, RingHom.ker (𝒮.qc v : G v →ₐ[ZMod p] 𝒮.Gc v) = Ideal.map (𝒮.σ v : 𝒮.Ge v →ₐ[ZMod p] G v) (RingHom.ker (Bialgebra.counitAlgHom (ZMod p) (𝒮.Ge v))) Θ_bijective : ∀ v, Function.Bijective (𝒮.Θ v) Θ_apply : ∀ v b, 𝒮.Θ v b = Algebra.TensorProduct.map (𝒮.qc v : G v →ₐ[ZMod p] 𝒮.Gc v) (𝒮.πe v : G v →ₐ[ZMod p] 𝒮.Ge v) (Coalgebra.comul (R := ZMod p) b) qc_comp_s : ∀ v, (𝒮.qc v).comp (s v) = (𝒮.sc v).comp (𝒮.qc (v + 1)) πe_comp_s : ∀ v, (𝒮.πe v).comp (s v) = (𝒮.se v).comp (𝒮.πe (v + 1)) s_comp_σ : ∀ v, (s v).comp (𝒮.σ (v + 1)) = (𝒮.σ v).comp (𝒮.se v) Θ_comp_s : ∀ v, (𝒮.Θ v).comp (s v) = (Bialgebra.TensorProduct.map (𝒮.sc v) (𝒮.se v)).comp (𝒮.Θ (v + 1)) formallyUnramified_Ge : ∀ v, Algebra.FormallyUnramified (ZMod p) (𝒮.Ge v) isComm_Φ₀ : 𝒮.Φ₀.IsComm κ_surjective : ∀ v, Function.Surjective (𝒮.κ v) ker_κ : ∀ v, RingHom.ker (𝒮.κ v) = Ideal.span (Set.range (𝒮.Φ₀.nthSeries (p ^ v))) sc_comp_κ : ∀ v, (𝒮.sc v : 𝒮.Gc (v + 1) →ₐ[ZMod p] 𝒮.Gc v).comp (𝒮.κ (v + 1)) = 𝒮.κ v counit_κ_X : ∀ v i, Coalgebra.counit (R := ZMod p) (𝒮.κ v (X i)) = 0 κ_X_mem_radical : ∀ v i, 𝒮.κ v (X i) ∈ (Ideal.span {(p : 𝒮.Gc v)}).radical κ_eval : ∀ v F, 𝒮.κ v F = MvFormalGroup.adicEval (Ideal.span {(p : 𝒮.Gc v)}) (fun i => 𝒮.κ v (X i)) F comul_κ_X : ∀ v i, Coalgebra.comul (R := ZMod p) (𝒮.κ v (X i)) = MvFormalGroup.adicEval (Ideal.span {(p : 𝒮.Gc v ⊗[ZMod p] 𝒮.Gc v)}) (Sum.elim (fun j => 𝒮.κ v (X j) ⊗ₜ[ZMod p] (1 : 𝒮.Gc v)) (fun j => (1 : 𝒮.Gc v) ⊗ₜ[ZMod p] 𝒮.κ v (X j))) (𝒮.Φ₀.toPowerSeries i) finrank_quot_nthSeries : Module.finrank (ZMod p) (MvPowerSeries (Fin 𝒮.d) (ZMod p) ⧸ Ideal.span (Set.range (𝒮.Φ₀.nthSeries p))) = p ^ 𝒮.hc d_eq_finrank_cotangent : 𝒮.d = Module.finrank (ZMod p) (PDivisibleGroup.Hopf.augIdeal (ZMod p) (𝒮.Gc 1)).Cotangent ker_κ_le_pow : ∀ N : ℕ, ∃ v, RingHom.ker (𝒮.κ v) ≤ (Ideal.span (Set.range (X : Fin 𝒮.d → MvPowerSeries (Fin 𝒮.d) (ZMod p)))) ^ N κ_injective_joint : ∀ F, (∀ v, 𝒮.κ v F = 0) → F = 0 κ_surjective_joint : ∀ z : ∀ v, 𝒮.Gc v, (∀ v, 𝒮.sc v (z (v + 1)) = z v) → ∃ F, ∀ v, 𝒮.κ v F = z v isCocomm_Et : ∀ v, Coalgebra.IsCocomm 𝓞 (𝒮.Et v) free_Et : ∀ v, Module.Free 𝓞 (𝒮.Et v) finite_Et : ∀ v, Module.Finite 𝓞 (𝒮.Et v) formallyEtale_Et : ∀ v, Algebra.FormallyEtale 𝓞 (𝒮.Et v) st_surjective : ∀ v, Function.Surjective (𝒮.st v) ker_st : ∀ v, RingHom.ker (𝒮.st v) = PDivisibleGroup.Hopf.torsionIdeal 𝓞 (𝒮.Et (v + 1)) (p ^ v) θe_bijective : ∀ v, Function.Bijective (𝒮.θe v) θe_comp : ∀ v, (𝒮.θe v).comp (Bialgebra.TensorProduct.map (BialgHom.id (ZMod p) (ZMod p)) (𝒮.st v)) = (𝒮.se v).comp (𝒮.θe (v + 1)) bijective_comp_mk : ∀ (g : Type u) [CommRing g] [Algebra 𝓞 g] [IsAdicComplete (Ideal.span {(p : g)}) g] (v : ℕ), Function.Bijective fun f : 𝒮.Et v →ₐ[𝓞] g => (Ideal.Quotient.mkₐ 𝓞 (Ideal.span {(p : g)})).comp f st_ĉ : ∀ i k v, 𝒮.st v (𝒮.ĉ i k (v + 1)) = 𝒮.ĉ i k v counit_ĉ : ∀ i k v, Coalgebra.counit (R := 𝓞) (𝒮.ĉ i k v) = 0 realisation_etale : ∀ v i, ∃ (n : ℕ) (u : Deformation.wittHom (ZMod p) p n (𝒮.Ge v)), Deformation.DieudonneModule.of (ZMod p) p (𝒮.Ge v) n u = Deformation.DieudonneModule.map (ZMod p) p (𝒮.πe v) (π v ((𝒮.α i : H₁.L) : Fin r → 𝓞)) ∧ (∀ (k : ℕ) (hk : k < n), (u : TruncatedWittVector p n (𝒮.Ge v)).coeff ⟨n - 1 - k, by omega⟩ = 𝒮.θe v ((1 : ZMod p) ⊗ₜ[𝓞] 𝒮.ĉ i k v)) ∧ (∀ k, n ≤ k → 𝒮.θe v ((1 : ZMod p) ⊗ₜ[𝓞] 𝒮.ĉ i k v) = 0) isCompl : IsCompl 𝒮.Mc 𝒮.Met F_mem_Mc : ∀ m ∈ 𝒮.Mc, H₁.F m ∈ 𝒮.Mc V_mem_Mc : ∀ m ∈ 𝒮.Mc, H₁.V m ∈ 𝒮.Mc F_mem_Met : ∀ m ∈ 𝒮.Met, H₁.F m ∈ 𝒮.Met V_mem_Met : ∀ m ∈ 𝒮.Met, H₁.V m ∈ 𝒮.Met pow_F_Mc : ∃ N : ℕ, ∀ m ∈ 𝒮.Mc, ∃ y ∈ 𝒮.Mc, (H₁.F ^ N) m = (p : 𝓞) • y F_surjOn_Met : ∀ m ∈ 𝒮.Met, ∃ m' ∈ 𝒮.Met, H₁.F m' = m Met_le_range_F : 𝒮.Met ≤ LinearMap.range H₁.F mem_Met_iff : ∀ m, m ∈ 𝒮.Met ↔ ∀ N : ℕ, ∃ y, (H₁.F ^ N) y = m mem_Mc_iff : ∀ m, m ∈ 𝒮.Mc ↔ ∀ k : ℕ, ∃ N : ℕ, ∃ y, (H₁.F ^ N) m = (p : 𝓞) ^ k • y free_Mc : Module.Free 𝓞 𝒮.Mc free_Met : Module.Free 𝓞 𝒮.Met finrank_Mc : Module.finrank 𝓞 𝒮.Mc = 𝒮.hc finrank_Met : Module.finrank 𝓞 𝒮.Met = 𝒮.he L_inf_Met : H₁.L ⊓ 𝒮.Met = ⊥ sh1_le_Lc : ∀ x ∈ (H₁.L).map (𝒮.Mc.subtype ∘ₗ Submodule.projectionOnto 𝒮.Mc 𝒮.Met isCompl), x ∈ LinearMap.range H₁.F → ∃ y ∈ (H₁.L).map (𝒮.Mc.subtype ∘ₗ Submodule.projectionOnto 𝒮.Mc 𝒮.Met isCompl), x = (p : 𝓞) • y sh1_ge_Lc : ∀ y ∈ (H₁.L).map (𝒮.Mc.subtype ∘ₗ Submodule.projectionOnto 𝒮.Mc 𝒮.Met isCompl), (p : 𝓞) • y ∈ LinearMap.range H₁.F sh2_Lc : LinearMap.range H₁.F ⊔ (H₁.L).map (𝒮.Mc.subtype ∘ₗ Submodule.projectionOnto 𝒮.Mc 𝒮.Met isCompl) = ⊤ map_πe_π_eq_zero : ∀ v, ∀ m ∈ 𝒮.Mc, Deformation.DieudonneModule.map (ZMod p) p (𝒮.πe v) (π v m) = 0 map_qc_π_eq_zero : ∀ v, ∀ m ∈ 𝒮.Met, Deformation.DieudonneModule.map (ZMod p) p (𝒮.qc v) (π v m) = 0 a_map : ∀ i k, (𝒮.a i k).map (algebraMap 𝓞 (ZMod p)) = 𝒮.abar i k constantCoeff_a : ∀ i k, MvPowerSeries.constantCoeff (𝒮.a i k) = 0 abar_tendsto : ∀ i N, ∃ k₀, ∀ k, k₀ ≤ k → 𝒮.abar i k ∈ (Ideal.span (Set.range (X : Fin 𝒮.d → MvPowerSeries (Fin 𝒮.d) (ZMod p)))) ^ N realisation_conn : ∀ v i, ∃ (n : ℕ) (u : Deformation.wittHom (ZMod p) p n (𝒮.Gc v)), Deformation.DieudonneModule.of (ZMod p) p (𝒮.Gc v) n u = Deformation.DieudonneModule.map (ZMod p) p (𝒮.qc v) (π v ((𝒮.α i : H₁.L) : Fin r → 𝓞)) ∧ (∀ (k : ℕ) (hk : k < n), (u : TruncatedWittVector p n (𝒮.Gc v)).coeff ⟨n - 1 - k, by omega⟩ = 𝒮.κ v (𝒮.abar i k)) ∧ (∀ k, n ≤ k → 𝒮.κ v (𝒮.abar i k) = 0) structure NormalForm : Prop where linearPart_zero : (MvFormalGroup.linearPart fun i => 𝒮.a i 0).map (Ideal.Quotient.mk (Ideal.span {(p : 𝓞)})) = 1 linearPart_one : ∀ i j : Fin 𝒮.d, j ≤ i → MvFormalGroup.linearPart (fun i => 𝒮.a i 1) i j ∈ Ideal.span {(p : 𝓞)} end SplitCoordinates end Deformation.HondaSystem
Statements phrased using this module (9)
- Unique split coordinates of a continuous point of Fontaine's functor
Deformation.HondaSystem.existsUnique_coords_of_mem_fontaineFunctor_of_splitCoordinates70 below · depth 25 - Existence in Fontaine's functor with prescribed split coordinates
Deformation.HondaSystem.exists_mem_fontaineFunctor_of_coords_of_splitCoordinates61 below · depth 25 - Lifted formal group law and its extension cocycle
Deformation.HondaSystem.exists_mvFormalGroup_cocycle_of_splitCoordinates66 below · depth 25 - Fontaine's lifting theorem from split coordinates and a cocycle
Deformation.HondaSystem.exists_pDivisibleTower_bijective_map_mem_fontaineHodge_of_splitCoordinates_of_cocycle35 below · depth 25 - Existence of lawful split coordinates in normal form
Deformation.HondaSystem.exists_splitCoordinates_lawful_normalForm111 below · depth 25 - Reduction of Φ modulo p equals Φ₀
Deformation.HondaSystem.SplitCoordinates.map_eq_phi0_of_forall_exists_convMul_apply_kappa_X0 below · depth 26 - Naturality of the Fontaine functor in the test algebra
Deformation.HondaSystem.SplitCoordinates.map_mem_fontaineFunctor_and_described2 below · depth 26 - Special fibre of the twisted tower: Gᶜᵥ⊗ G^eᵥ≅𝔽ₚ⊗ Lᵥ
Deformation.HondaSystem.exists_bijective_tensorProduct_specialFibre_of_cocycle2 below · depth 26 - Fontaine–Hodge membership at a twisted Tate level
Deformation.HondaSystem.map_apply_basis_mem_fontaineHodge_of_cocycle3 below · depth 26