Distance of the boundary contour from ρ #
The geometry of the shifted contour t ↦ fdBoundary H t - ρ about the corner ρ at
parameter t = 3: the chord distance along the arc, the purely imaginary linear form
along the left vertical, the norm lower bounds on the far pieces, the slit-plane
confinement of every piece, and the exact polar forms and principal logarithms of the
shifted contour beside the corner. The corner joins the arc to the vertical at the
interior angle π/3, which is exactly the gap between the two one-sided argument limits
π/6 and π/2 — the source of the winding value -1/6 at ρ.
Main declarations #
TauCeti.ModularForm.norm_fdBoundary_sub_rho_arc(the chord distance).TauCeti.ModularForm.fdBoundary_sub_rho_of_mem_Icc_three_four(the linear form).TauCeti.ModularForm.log_fdBoundary_three_sub_sub_rho,TauCeti.ModularForm.log_fdBoundary_three_add_sub_rho(the endpoint logarithms).
References #
- AINTLIB
LeanModularForms— the valence-formula development (ForMathlib/ValenceFormula/WindingWeights/Rho.lean) this file ports onto the current Mathlib pin.
On the right vertical the contour keeps distance at least 1 from ρ: the real parts differ
by exactly 1.
On the ceiling the contour keeps distance at least |H - √3/2| from ρ: the heights
differ by exactly H - √3/2. The absolute value is what the height difference actually
gives, and it is the only form with content below the corner row, where H - √3/2 < 0
makes the signed bound vacuous.
Right of the corner column the shifted contour has real part 1: slit plane.
Before the corner the arc stays right of the corner column: the real part of the
shifted contour is cos((t+1)·π/6) + 1/2 > 0, so it lies in the slit plane.
The principal logarithm of the shifted contour just before the corner.
The contour passes through ρ only at the corner t = 3.