Basis modifications of a free pro-p group and the maps δ #
Let F = freeProP p X be the free pro-p group on a finite linearly ordered type X, with
canonical generators x_i = freeProP.of i, and let λ_k = λ_k(F) be its lower p-series. A
family w : X → λ_m(F) defines the basis modification θ_w : F → F, x_i ↦ x_i * w_i
(TauCeti.freeProP.basisModification). It is congruent to the identity modulo λ_m, so for a
relator r ∈ λ_1(F) it moves r inside its coset by the element r⁻¹ * θ_w r ∈ λ_{m+1}(F),
whose class in gr_{m+1}(F) is the graded deviation D_1 ρ of θ_w (TauCeti.gradedDeviation)
on the class ρ ∈ gr_1(F) of r.
For m ≥ 1 that class is given by the basis-modification map
δ = TauCeti.freeProP.basisModificationDelta: writing ρ in the standard basis
TauCeti.freeProP.degreeOneBasis as ρ = Σ_i c_i π ξ_i + Σ_{i<k} a_{ik} [ξ_i, ξ_k], where
ξ_i ∈ gr_0(F) is the class of x_i, and writing ω_i ∈ gr_m(F) for the class of w_i, the
class of r⁻¹ * θ_w r in gr_{m+1}(F) is
δ(ω) = Σ_i c_i (π ω_i + (p choose 2) • [ω_i, ξ_i]) + Σ_{i<k} a_{ik} ([ω_i, ξ_k] - [ω_k, ξ_i]),
an 𝔽_p-linear function of the classes ω_i alone, and 𝔽_p-linear in ρ as well. The bracket
part is the derivative of the commutator part of ρ in the direction ω, and for odd p the
p-power part contributes Σ_i c_i π ω_i. For p = 2 the p-power part contributes in addition
the brackets Σ_i c_i [ω_i, ξ_i]: the square of x_i * w_i is x_i ^ 2 * w_i ^ 2 * ⁅w_i, x_i⁆
up to λ_{m+2}(F), and the commutator ⁅w_i, x_i⁆ lies in λ_{m+1}(F) and may have a nonzero
class in gr_{m+1}(F). That term is the trace, in every degree, of the failure of additivity of
π on gr_0(F) at p = 2.
At level m = 0, where θ_w is an arbitrary continuous endomorphism of F, the class of
r⁻¹ * θ_w r in gr_1(F) is still a function of the classes ω_i ∈ gr_0(F) alone, but a
quadratic one; that map and its polarization identity are in
TauCeti.Topology.Algebra.Group.Profinite.Free.BasisModification.LevelZero.
The image of δ is the subspace of gr_{m+1}(F) that the successive-approximation arguments of
the classification of Demushkin groups compare with gr_{m+1}(F); there m + 1 is the modulus of
the normal-form congruence, and the classes ω_i are the level-m basis corrections.
For p = 2 those arguments compare gr_j(F) with the image of δ enlarged by one further
subspace, the span in gr_j(F) of the iterated p-powers π^j ξ_i over a set S of generators
(TauCeti.freeProP.gradedPowIterSpan). The tail T_j(ρ)
(TauCeti.freeProP.basisModificationTail) is the instance at the generators whose coefficient
c_i in ρ vanishes, which are the generators contributing no π-term to δ. For the dyadic
relator x₁² x₂^{2^f} ⁅x₂, x₃⁆ ⋯ with f ≥ 2 these are x₂, …, x_n; for the even-rank relator
x₁^{2+α} ⁅x₁, x₂⁆ x₃^{2^f} ⋯ the right index set is instead the complement of x₂, which is not
a tail.
Collecting the brackets of δ by their degree-m entry gives the partial derivatives
∂_i ρ ∈ gr_0(F) (TauCeti.freeProP.degreeOneDeriv), the i-th row of the matrix
(a_{ik}) completed skew-symmetrically with diagonal (p choose 2) c_i, and the formula
δ_ρ(ω) = π (Σ_i c_i ω_i) + Σ_i [ω_i, ∂_i ρ]. The image of δ_ρ is then computed under the
hypothesis that the derivatives ∂_i ρ span gr_0(F), which is the nondegeneracy of the form
(a_{ik}) completed with that diagonal, and holds for every Demushkin relator in normal form: the
coordinates of ∂_i ρ in the basis of generator classes form the i-th row of the matrix of the
degree-one form TauCeti.freeProP.degreeOneForm ρ in the dual basis of the generators, so the
derivatives span exactly when that form is nondegenerate.
The span statements are: if all c_i = 0, then Im δ_ρ is the span of the brackets
[gr_m(F), gr_0(F)] and gr_{m+1}(F) = Im δ_ρ + T_{m+1}(ρ) for every m ≥ 1, the tail being
spanned by all the π^{m+1} ξ_i, so that Im δ_ρ consists exactly of the classes of the
elements of λ_{m+1}(F) all of whose exponent sums are divisible by p ^ (m + 2); and if p is
odd and some c_i ≠ 0, then gr_{m+1}(F) = Im δ_ρ for every m ≥ 1. The first case is that of
the relators x₁^q (x₁, x₂) (x₃, x₄) ⋯ with q ≠ p, whose p-power part lies in λ_2(F), and
the second that of x₁^p (x₁, x₂) (x₃, x₄) ⋯ at odd p. Both rest on the spanning of
gr_{m+1}(F) by π gr_m(F) and [gr_m(F), gr_0(F)] and on the naturality π ∘ δ_ρ = δ_ρ ∘ π,
which carries the image of δ_ρ in degree m into its image in degree m + 1. For p = 2 and a
class with a p-power part the odd-p argument breaks down at the degree-zero defect of π. It
survives when some generator class ξ_{i₁} has the column B_ρ(χ_i, χ_{i₁}) of the degree-one
form at its coordinate character equal to the vector c_i of 2-power coefficients: then
gr_{m+1}(F) = Im δ_ρ + ⟨π^{m+1} ξ_i : i ≠ i₁⟩. The key membership is
ψ(y) • π v + [v, y] ∈ Im δ_ρ for ψ the coordinate at ξ_{i₁}, which makes every bracket
[v, y] available once π v is, and the degree-zero defect of π is absorbed by the brackets
[[ξ_a, y], ξ_a] with a ≠ i₁. For the dyadic relators x₁² x₂^{2^f} (x₂, x₃) ⋯ of odd rank,
x₁ carries the 2-power part, ξ₁ occurs in no bracket and i₁ is the index of x₁, so the
span is the tail T_{m+1}(ρ) and the level f is the free parameter it accounts for. For the
even-rank relators x₁^{2+α} (x₁, x₂) x₃^{2^f} ⋯, x₁ carries the 2-power part and i₁ is the
index of its bracket partner x₂, so the spanning powers include π^{m+1} ξ₁ although c₁ ≠ 0,
and exclude π^{m+1} ξ₂.
Main definitions #
TauCeti.freeProP.basisModification: the endomorphismθ_w : F → F,x_i ↦ x_i * w_i.TauCeti.freeProP.basisModificationEquiv: form ≥ 1and finiteX, the same map as a continuous automorphism ofF.TauCeti.freeProP.basisModificationDelta: form ≥ 1, the𝔽_p-bilinear mapδ : gr_1(F) → gr_m(F)^X → gr_{m+1}(F),(ρ, ω) ↦ δ_ρ(ω).TauCeti.freeProP.basisModificationTail: the tailT_j(ρ) ≤ gr_j(F), the spanTauCeti.freeProP.gradedPowIterSpanof theπ^j ξ_iwithc_i = 0.TauCeti.freeProP.degreeOneDeriv: the partial derivative∂_i : gr_1(F) →ₗ[𝔽_p] gr_0(F).
Main results #
TauCeti.freeProP.inv_mul_basisModification_mem_pLowerCentralSeries:θ_wis congruent to the identity moduloλ_m(F).TauCeti.freeProP.toAdd_exponentSum_basisModification: the exponent vector ofθ_w gisΣ_i (exponentSum g)_i • (e_i + exponentSum w_i).TauCeti.freeProP.exponentSum_basisModification:θ_wpreserves the exponent vector ofgwhenw_ilies in the closed commutator subgroup at every generator carrying a nonzero exponent ofg.TauCeti.freeProP.gradedDeviation_basisModification,TauCeti.freeProP.gradedMk_inv_mul_basisModification: the class ofr⁻¹ * θ_w ringr_{m+1}(F)isδ(ω); in particular it depends only on the classesω_i.TauCeti.freeProP.finrank_basisModificationTail:dim T_j(ρ)is the number of indicesiwithc_i = 0.TauCeti.freeProP.basisModificationTail_succ:πcarriesT_j(ρ)ontoT_{j+1}(ρ)forj ≥ 1.TauCeti.freeProP.basisModificationDelta_eq_gradedPow_add_sum,TauCeti.freeProP.gradedPow_basisModificationDelta:δ_ρ(ω) = π (Σ_i c_i ω_i) + Σ_i [ω_i, ∂_i ρ], andπ (δ_ρ(ω)) = δ_ρ(π ω).TauCeti.freeProP.exists_basisModificationDelta_smul_eq,TauCeti.freeProP.basisModificationDelta_smul_eq_gradedBracket_of_eq_zero: on a familyb • vproportional to one class,δ_ρ(b • v) = c • π v + [v, y]for any prescribedywhen the derivatives span, andδ_ρ(b • v) = [v, Σ_i b_i • ∂_i ρ]whenbvanishes at the only generator carrying ap-power coefficient.TauCeti.freeProP.degreeZeroBasis_repr_degreeOneDeriv,TauCeti.freeProP.span_range_degreeOneDeriv_eq_top_iff_nondegenerate_degreeOneForm: the coordinates of∂_i ρare thei-th row of the matrix of the degree-one form ofρ, so the derivatives spangr_0(F)exactly when that form is nondegenerate.TauCeti.freeProP.range_basisModificationDelta_eq_span_of_repr_inl_eq_zero,TauCeti.freeProP.range_basisModificationDelta_sup_basisModificationTail_eq_top: for a class withoutp-power part whose derivatives spangr_0(F),Im δ_ρ = [gr_m(F), gr_0(F)]andgr_{m+1}(F) = Im δ_ρ + T_{m+1}(ρ).TauCeti.freeProP.gradedMk_mem_range_basisModificationDelta_iff: for a class withoutp-power part whose derivatives spangr_0(F), the class ofz ∈ λ_{m+1}(F)lies inIm δ_ρif and only ifp ^ (m + 2)divides every exponent sum ofz; soIm δ_ρis the kernel of the map togr_{m+1}(F^{ab}).TauCeti.freeProP.range_basisModificationDelta_eq_top_of_odd: for oddpand a class with ap-power part whose derivatives spangr_0(F),gr_{m+1}(F) = Im δ_ρ.TauCeti.freeProP.range_basisModificationDelta_sup_gradedPowIterSpan_compl_eq_top_two: forp = 2and a class whose derivatives spangr_0(F), and a generator classξ_{i₁}whose columnB_ρ(χ_i, χ_{i₁})of the degree-one form is the vector of2-power coefficients of the class,gr_{m+1}(F) = Im δ_ρ + ⟨π^{m+1} ξ_i : i ≠ i₁⟩; for a class whose2-power part sits on a single generatorx_{i₁}not occurring in the brackets, this isgr_{m+1}(F) = Im δ_ρ + T_{m+1}(ρ).
References #
- J. Labute, Classification of Demushkin groups, Canadian J. Math. 19 (1967), §3, Proposition 5 and the proof of Theorem 3.
The basis modification x_i ↦ x_i * w_i #
The basis modification θ_w : F → F, x_i ↦ x_i * w_i, of the free pro-p group
F = freeProP p X by a family w : X → λ_m(F). It is congruent to the identity modulo λ_m(F)
(TauCeti.freeProP.inv_mul_basisModification_mem_pLowerCentralSeries).
Equations
- TauCeti.freeProP.basisModification w = TauCeti.freeProP.lift ⋯ fun (i : X) => TauCeti.freeProP.of i * ↑(w i)
Instances For
The basis modification is congruent to the identity modulo λ_m(F).
The basis modification as an automorphism #
The basis modification x_i ↦ x_i * w_i by elements of λ_m(F), m ≥ 1, as a continuous
automorphism of the free pro-p group of finite rank F: the endomorphism θ_w is congruent to
the identity modulo λ_1(F) = Φ(F), hence surjective by Burnside's criterion, hence bijective by
the Hopf property. Its underlying map is θ_w
(TauCeti.freeProP.basisModificationEquiv_apply).
Equations
Instances For
The inverse of the basis modification preserves every term of the lower p-series.
The inverse of the basis modification does not move the class of a relator in gr_1(F):
θ_w⁻¹(r) ≡ r mod λ_2(F) for r ∈ λ_1(F), since θ_w is congruent to the identity modulo
λ_1(F) and hence to the identity modulo λ_2(F) on λ_1(F).
The deviation of the basis modification on a generator class is the class of the
modification: D_0 ξ_i = ω_i in gr_m(F), where ξ_i and ω_i are the classes of x_i and
w_i.
The exponent vector of a basis modification. For u = exponentSum g, the exponent vector
of θ_w g is Σ_i u_i • (e_i + exponentSum w_i): the generator x_i contributes e_i and its
correction w_i contributes exponentSum w_i, each u_i times.
A basis modification lying in the closed commutator subgroup at every generator carrying
a nonzero exponent preserves the exponent vector: if w_i ∈ closure [F, F] for every i with
(exponentSum g)_i ≠ 0, then exponentSum (θ_w g) = exponentSum g.
A continuous endomorphism moving each generator carrying a nonzero exponent by an element of
the closed commutator subgroup preserves the exponent vector: if x_i⁻¹ * φ(x_i) ∈ closure [F, F]
for every i with (exponentSum g)_i ≠ 0, then exponentSum (φ g) = exponentSum g.
The maps δ #
The basis-modification map δ, for m ≥ 1: the 𝔽_p-bilinear map
gr_1(F) → gr_m(F)^X → gr_{m+1}(F) sending a class ρ ∈ gr_1(F) and a family v to
δ_ρ(v) = Σ_i c_i (π v_i + (p choose 2) • [v_i, ξ_i]) + Σ_{i<k} a_{ik} ([v_i, ξ_k] - [v_k, ξ_i])
where c_i and a_{ik} are the coordinates of ρ in the standard basis
TauCeti.freeProP.degreeOneBasis of gr_1(F), that is
ρ = Σ_i c_i π ξ_i + Σ_{i<k} a_{ik} [ξ_i, ξ_k] with ξ_i ∈ gr_0(F) the class of x_i. It is
defined by its values on that basis
(TauCeti.freeProP.basisModificationDelta_degreeOneBasis_inl,
TauCeti.freeProP.basisModificationDelta_degreeOneBasis_inr), and its value at a general ρ is
TauCeti.freeProP.basisModificationDelta_apply. For a relator r ∈ λ_1(F) with class ρ, and
w : X → λ_m(F) with classes v_i = ω_i, δ_ρ(v) is the class in gr_{m+1}(F) of
r⁻¹ * θ_w r, the amount by which the basis modification θ_w moves r
(TauCeti.freeProP.gradedMk_inv_mul_basisModification).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The value of δ on a p-power basis vector:
δ_{π ξ_i}(v) = π v_i + (p choose 2) • [v_i, ξ_i].
The value of δ on a bracket basis vector:
δ_{[ξ_i, ξ_k]}(v) = [v_i, ξ_k] - [v_k, ξ_i].
The value of δ: with ρ = Σ_i c_i π ξ_i + Σ_{i<k} a_{ik} [ξ_i, ξ_k],
δ_ρ(v) = Σ_i c_i (π v_i + (p choose 2) • [v_i, ξ_i]) + Σ_{i<k} a_{ik} ([v_i, ξ_k] - [v_k, ξ_i]).
The class of the moved relator is δ_ρ(ω). For m ≥ 1, w : X → λ_m(F) and
ρ ∈ gr_1(F), the graded deviation of the basis modification θ_w on ρ is δ_ρ(ω), where
ω_i ∈ gr_m(F) is the class of w_i.
The basis modification θ_w moves a relator r ∈ λ_1(F) by δ_ρ(ω): the class in
gr_{m+1}(F) of r⁻¹ * θ_w r is δ_ρ(ω), for m ≥ 1, where ρ ∈ gr_1(F) is the class of r
and ω_i ∈ gr_m(F) the class of w_i. In particular that class depends only on the classes
ω_i of the modifications.
The partial derivatives ∂_i #
The partial derivative ∂_i of a class in gr_1(F): the 𝔽_p-linear map
gr_1(F) → gr_0(F) given on the standard basis TauCeti.freeProP.degreeOneBasis by
∂_i (π ξ_i) = (p choose 2) • ξ_i, ∂_i (π ξ_j) = 0 for j ≠ i, ∂_i [ξ_i, ξ_k] = ξ_k,
∂_i [ξ_j, ξ_i] = -ξ_j and ∂_i [ξ_j, ξ_k] = 0 when i ∉ {j, k}. For
ρ = Σ_i c_i π ξ_i + Σ_{j<k} a_{jk} [ξ_j, ξ_k] this is
∂_i ρ = (p choose 2) c_i • ξ_i + Σ_{k>i} a_{ik} ξ_k - Σ_{j<i} a_{ji} ξ_j, the i-th row of the
matrix of the form (a_{jk}) completed skew-symmetrically, with diagonal (p choose 2) c_i,
read as a vector of gr_0(F). The bracket terms of the basis-modification map are
Σ_i [v_i, ∂_i ρ] (TauCeti.freeProP.basisModificationDelta_eq_gradedPow_add_sum).
Equations
- One or more equations did not get rendered due to their size.
Instances For
∂_i on the p-power basis vectors: ∂_i (π ξ_i) = (p choose 2) • ξ_i and ∂_i (π ξ_j) = 0
for j ≠ i.
∂_i on the bracket basis vectors: ∂_i [ξ_j, ξ_k] = ξ_k if j = i, -ξ_j if k = i, and
0 otherwise, for j < k.
∂_i (π ξ_i) = (p choose 2) • ξ_i.
∂_i (π ξ_j) = 0 for j ≠ i.
∂_i [ξ_i, ξ_k] = ξ_k for i < k.
∂_i [ξ_j, ξ_i] = -ξ_j for j < i.
∂_i [ξ_j, ξ_k] = 0 for j < k with i ∉ {j, k}.
A class with spanning derivatives, in rank two. In F = freeProP p (Fin 2) the
derivatives of the bracket class [ξ_0, ξ_1] are ∂_0 = ξ_1 and ∂_1 = -ξ_0, which span
gr_0(F). This is the class of the surface relation (x₁, x₂) of ℤ_p × ℤ_p.
The basis-modification map through the partial derivatives: for m ≥ 1,
δ_ρ(v) = π (Σ_i c_i • v_i) + Σ_i [v_i, ∂_i ρ], where c_i is the coefficient of π ξ_i in
ρ. The p-power part of ρ contributes the single p-power π (Σ_i c_i v_i), and all
brackets are collected in the derivatives.
δ on a family proportional to a single class: for b : X → 𝔽_p and v ∈ gr_m(F),
δ_ρ(b • v) = (Σ_i b_i c_i) • π v + [v, Σ_i b_i • ∂_i ρ].
δ on a family supported at one generator: for v ∈ gr_m(F),
δ_ρ(single i v) = c_i • π v + [v, ∂_i ρ], where c_i is the coefficient of π ξ_i in ρ.
δ_ρ realizes every bracket up to a multiple of π v when the partial derivatives of ρ
span gr_0(F): for v ∈ gr_m(F) and y ∈ gr_0(F) there are coefficients b : X → 𝔽_p and a
scalar c with δ_ρ(b • v) = c • π v + [v, y], namely b with Σ_i b_i • ∂_i ρ = y and
c = Σ_i b_i c_i.
δ_ρ on a family proportional to v and vanishing at the p-power generator: if x_{i₀}
is the only generator whose coefficient c_i of π ξ_i in ρ may be nonzero and b i₀ = 0, then
δ_ρ(b • v) = [v, Σ_i b_i • ∂_i ρ] has no p-power term.
Naturality of δ under π: for m ≥ 1, π (δ_ρ(v)) = δ_ρ(π v), where δ_ρ on the left
is the map in degree m and on the right the map in degree m + 1.
The derivatives and the degree-one form #
The coordinates of the partial derivatives are the matrix of the degree-one form: the
k-th coordinate of ∂_i ρ in the basis of generator classes of gr_0(F) is B_ρ(χ_i, χ_k), the
(i, k) entry of the matrix of the degree-one form of ρ in the dual basis of the generators.
The partial derivatives span gr_0(F) exactly when the degree-one form is nondegenerate.
The coordinates of ∂_i ρ form the i-th row of the matrix of B_ρ in the dual basis of the
generators, so the derivatives span exactly when that matrix is invertible. This is the spanning
hypothesis of the span statements below, and it holds for every Demushkin relator.
The tails T_j #
The tail T_j(ρ) of a class ρ ∈ gr_1(F): the span TauCeti.freeProP.gradedPowIterSpan
in gr_j(F) of the iterated p-powers π^j ξ_i of the generator classes ξ_i ∈ gr_0(F), over
the indices i whose coefficient c_i of π ξ_i in ρ, in the standard basis
TauCeti.freeProP.degreeOneBasis, vanishes. For the class ρ of a relator these are the
generators contributing no π-term to the basis-modification map
TauCeti.freeProP.basisModificationDelta. The vectors π^j ξ_i are linearly independent, so
T_j(ρ) has dimension the number of such indices
(TauCeti.freeProP.finrank_basisModificationTail), and above degree zero π carries T_j(ρ)
onto T_{j+1}(ρ) (TauCeti.freeProP.basisModificationTail_succ).
Equations
- TauCeti.freeProP.basisModificationTail p X ρ j = TauCeti.freeProP.gradedPowIterSpan p X {i : X | ((TauCeti.freeProP.degreeOneBasis p X).repr ρ) (Sum.inl i) = 0} j
Instances For
The defining equation of TauCeti.freeProP.basisModificationTail: the tail is the span of the
p-power classes over the indices whose coefficient in ρ vanishes.
An iterated power π^j ξ_i belongs to T_j(ρ) when its coefficient c_i in ρ
vanishes.
A submodule contains T_j(ρ) if and only if it contains every generator π^j ξ_i
whose coefficient c_i in ρ vanishes.
Membership in the tail: the elements of T_j(ρ) are the linear combinations of the
π^j ξ_i over the indices i with c_i = 0, the instance of
TauCeti.freeProP.mem_gradedPowIterSpan_iff at the index set of the tail.
π carries the tail onto the next tail above degree zero: for j ≥ 1,
T_{j+1}(ρ) = π(T_j(ρ)), since π is additive on gr_j(F) and π (π^j ξ_i) = π^{j+1} ξ_i.
The dimension of the tail: dim T_j(ρ) is the number of indices i whose coefficient
c_i of π ξ_i in ρ vanishes, because the π^j ξ_i are linearly independent
(TauCeti.freeProP.linearIndependent_gradedPowIter_gradedMkZero_of).
The image of δ #
π carries the image-plus-span sum to the next level: above degree zero it preserves
the image of δ_ρ and maps the span of the p-power classes over S in degree m + 1 onto the
span in degree m + 2.
π carries the image-plus-tail sum to the next level: above degree zero it preserves
the image of δ_ρ and maps T_{m+1}(ρ) onto T_{m+2}(ρ).
Brackets lie in the image of δ_ρ when ρ has no p-power part and its partial
derivatives span gr_0(F): for v ∈ gr_m(F) and y ∈ gr_0(F), writing y = Σ_i b_i ∂_i ρ, the
family b • v has δ_ρ(b • v) = [v, y].
The image of δ_ρ for a relator without p-power part is the span of the brackets
[v, y] with v ∈ gr_m(F) and y ∈ gr_0(F), provided the partial derivatives ∂_i ρ span
gr_0(F).
The span statement for a relator without p-power part: if ρ ∈ gr_1(F) has all
coefficients c_i of π ξ_i equal to zero and its partial derivatives ∂_i ρ span gr_0(F), then
for every m ≥ 1
gr_{m+1}(F) = Im δ_ρ + T_{m+1}(ρ),
where the tail T_{m+1}(ρ) is spanned by the p-powers π^{m+1} ξ_i of all the generator
classes. The image of δ_ρ is the span of the brackets [gr_m(F), gr_0(F)], and the tail
accounts for the p-powers: π carries Im δ_ρ in degree m into Im δ_ρ in degree m + 1 and
T_{m+1}(ρ) onto T_{m+2}(ρ). This is the case of the Demushkin relators
x₁^q (x₁, x₂) (x₃, x₄) ⋯ with q ≠ p, where the p-power part of the relator lies in λ_2(F)
and is not seen by gr_1(F).
The image of δ and the exponent sums #
For a class ρ without p-power part the image of δ_ρ is spanned by brackets, so every
continuous homomorphism to a commutative group kills it, while the tail T_{m+1}(ρ) is spanned by
the p-powers π^{m+1} ξ_i, which the exponent sums modulo p ^ (m + 2) separate
(TauCeti.freeProP.exponentSumZModPow). The decomposition gr_{m+1}(F) = Im δ_ρ + T_{m+1}(ρ)
therefore identifies Im δ_ρ with the classes killed by every exponent sum modulo p ^ (m + 2).
A continuous homomorphism to a commutative group kills the image of δ_ρ when ρ has no
p-power part: δ_ρ(v) is then a sum of brackets, and brackets vanish in a commutative group.
The image of δ_ρ through the exponent sums: if ρ ∈ gr_1(F) has no p-power part and
its partial derivatives ∂_i ρ span gr_0(F), then for m ≥ 1 the class in gr_{m+1}(F) of
z ∈ λ_{m+1}(F) lies in Im δ_ρ if and only if p ^ (m + 2) divides every exponent sum of z.
So Im δ_ρ is the kernel of the map gr_{m+1}(F) → gr_{m+1}(F^{ab}) induced by the
abelianization, the complement of the tail T_{m+1}(ρ) in
TauCeti.freeProP.range_basisModificationDelta_sup_basisModificationTail_eq_top. This is the span
statement for the relators x₁^q (x₁, x₂) (x₃, x₄) ⋯ with q ≠ p: a discrepancy between two
such relators whose exponent sums agree modulo p ^ (m + 2) is absorbed by a level-m basis
modification.
A class of the closed commutator subgroup lies in the image of δ_ρ: for ρ without
p-power part and with spanning partial derivatives, the class in gr_{m+1}(F) of an element of
λ_{m+1}(F) lying in the closure of the commutator subgroup is in Im δ_ρ. This is the form used
for the relators (x₁, x₂) (x₃, x₄) ⋯ with q = 0, whose discrepancies have trivial exponent
sums.
The span statement for odd p and a relator with a p-power part: if p is odd,
ρ ∈ gr_1(F) has some coefficient c_i of π ξ_i nonzero and its partial derivatives ∂_i ρ
span gr_0(F), then δ_ρ is onto gr_{m+1}(F) for every m ≥ 1:
gr_{m+1}(F) = Im δ_ρ.
This is the case of the Demushkin relators x₁^p (x₁, x₂) (x₃, x₄) ⋯ at odd p.
The dyadic span statements #
The dyadic span statement (Labute, Proposition 5, the cases q = 2): let ρ ∈ gr_1(F),
for F free pro-2, have its partial derivatives ∂_i ρ spanning gr_0(F), and let ξ_{i₁} be
a generator class such that the column B_ρ(χ_i, χ_{i₁}) of the degree-one form of ρ at its
coordinate character is the vector c_i of coefficients of the π ξ_i in ρ. Then for every
m ≥ 1
gr_{m+1}(F) = Im δ_ρ + ⟨π^{m+1} ξ_i : i ≠ i₁⟩.
Two cases occur among the dyadic Demushkin relators, in both of which x₁ is the only generator
with c_i ≠ 0. For x₁² x₂^{2^f} (x₂, x₃) ⋯ (x_{n-1}, x_n) of odd rank, with f ≥ 2, whose
class is π ξ₁ + [ξ₂, ξ₃] + ⋯, the generator x₁ occurs in no bracket, χ₁ is orthogonal to the
other coordinate characters with B_ρ(χ₁, χ₁) = c₁, and i₁ is the index of x₁. For
x₁^{2+α} (x₁, x₂) x₃^{2^f} (x₃, x₄) ⋯ of even rank, with 4 ∣ α and f ≥ 2, whose class is
π ξ₁ + [ξ₁, ξ₂] + [ξ₃, ξ₄] + ⋯, the character χ₂ of the bracket partner x₂ pairs only with
χ₁, with B_ρ(χ₁, χ₂) = c₁, and i₁ is the index of x₂, so the spanning powers include
π^{m+1} ξ₁ although c₁ ≠ 0, and exclude π^{m+1} ξ₂.