The retained coefficients are nonzero (Proposition 12.8, a_i ∈ k^*) #
deformation-refinements.tex: "Specializing t_j = ε, all other parameters zero and
ε² = 0, identifies a_j[p_j] with Ψ[μ_j]. This is nonzero because Ψ is injective
(Proposition 7.6). Hence a_j ≠ 0."
At t = 1 the lifts have relative weights in the cone C of the χ_i, and χ_j is an atom of
C. The components of relative weight χ_j (and internal degree q_j) of the lifted actions
and arrows are therefore the square-zero lifts of Lemma 6.6 for μ_j (ν1, y1), i.e. the
specialization t = ε e_j; their mesh errors are λ_j R_j (zE_psi). So Ψ[μ_j] = λ_j [R_j],
and λ_j ≠ 0 because μ_j is not a coboundary.
The cocycle condition #
Each μ_j is a Hochschild cocycle: the linear term of associativity in t_j.
The atoms of the cone #
χ_j is an atom of the cone.
The χ_j-parts of the lifted actions #
The first-order action ν = (ν_{q_j})_{χ_j}, the t_j-linear part of the lifted action.
Instances For
The atom component of ν_l(ν_{j'}(m, a), b).
The atom component of ν_{j'}(m, μ_l(a, b)).
The first-order action satisfies the square-zero equation for μ_j.
The first-order lifted action as a square-zero lift for μ_j.
Instances For
Joint homogeneity #
Linear maps agreeing on jointly homogeneous vectors agree.
Bilinear maps agreeing on jointly homogeneous pairs agree.
A map raising the degree by exactly s commutes with the degree projections.
The total lifted action: bottom part and degree components #
The first-order parts of the lifted arrows #
The first-order arrow g_a: the part of relative weight χ_j and internal degree
1 + q_j of the lifted arrow.
Instances For
The first-order arrows satisfy the square-zero linearity of Lemma 6.6.
The lift data for μ_j and its mesh errors #
The first-order lift data for μ_j: the specialization t = ε e_j of the lifts.
Instances For
The mesh errors of the first-order lift data are λ_j R_j.
Ψ[μ_j] = λ_j [R_j].
The retained coefficients are nonzero (a_j ∈ k^*), when μ_j is not a coboundary.