Residues along square-zero directions #
Certificates for the residue / trace-direction mechanism in the three-axes problem.
Conventions: Y_j = 1 + x_j evaluated; H0(Y) = [[Yx²+Yy², Yx²],[Yx², Yx²+Yz²]].
Main results #
polar:2×2Cayley–Hamilton polarizationAB + BA = tr A • B + tr B • A + (tr(AB) − tr A tr B) • 1;polar_traceless.det_add_smul:det(A + εB) = det A + ε (tr A tr B − tr(AB)) + ε² det B;adjugate_add_smul.residue_sqzero:tr N = 0,det N = 0⇒det(N + εΔ) = ε (ε det Δ − tr(NΔ))andadj(N + εΔ) = −N + ε • adj Δ(the residue does not seetr Δ);inv_sub_one_sqzero.h4_general: the determinant ofH0atA_j = τ_j • 1 + σ_j • N_jin closed form.arc_det: an exact example along a square-zero arc.witness: an integer witness on the zero set ofdet H0, withY_j ∈ SL₂(ℤ).
polar and det_add_smul are restatements of the 2 × 2 identities of
Formalizations.LinearAlgebra.Matrix.FinTwo; blk, det4, Nsq and the witness matrices are in
Formalizations.RingTheory.FreeField.ThreeAxes.Basic.
theorem
ThreeAxes.TraceResidue.h4_general
{R : Type u_1}
[CommRing R]
(a0 b0 a1 b1 a2 b2 tx ty tz sx sy sz : R)
:
(H) first coefficient of H0 along a trace-direction arc, general square-zero triple.
Equations
- ThreeAxes.TraceResidue.Nx = !![0, -1; 0, 0]
Instances For
Equations
- ThreeAxes.TraceResidue.Ny = !![1, -1; 1, -1]
Instances For
Equations
- ThreeAxes.TraceResidue.Nz = !![2, -1; 4, -2]
Instances For
(E) the arc Y_j = N_j + εΔ_j with Δx = !![σ, 0; −1, 0], Δy = !![0,0;−1,0], Δz = !![0,0;−3,1].
Equations
- ThreeAxes.TraceResidue.Yx e s = ThreeAxes.TraceResidue.Nx + e • !![s, 0; -1, 0]
Instances For
Equations
- ThreeAxes.TraceResidue.Yy e = ThreeAxes.TraceResidue.Ny + e • !![0, 0; -1, 0]
Instances For
Equations
- ThreeAxes.TraceResidue.Yz e = ThreeAxes.TraceResidue.Nz + e • !![0, 0; -3, 1]