Sector Curve PV Lemmas #
Higher-order PV computations and the generalized winding number for the
model sector-curve defined in SectorCurve.lean.
Main Results #
pv_sector_higher_power-- for n >= 1,PV int z^{n-1} dz = 0(angle condition)cauchyPV_sectorCurve_simplePole-- Lemma 3.1 for simple poles: PV =I * alpha * residuecauchyPV_sectorCurve_eq_mul_residueSimplePole-- variant for arbitraryf = c/z + gpv_sector_negative_power-- Equation (3.4): PV ofz^{-n}is 0 under angle conditiongeneralizedWindingNumber_sectorCurve-- winding number equalsalpha / (2 * pi)
Lemma 3.1 (Simple pole version):
For f(z) = c/z + g(z) where g is analytic on a ball containing the sector,
the principal value along the sector curve equals I * α * c.
The hypotheses require g analytic on a ball strictly containing the sector image
(to guarantee a primitive exists) and f = c/z + g at all nonzero points.
Variant of Lemma 3.1: for an arbitrary f equal to c/z + g at nonzero points,
with g analytic on a ball containing the sector, the PV equals I * α * c.
Equation (3.4): The PV of z^{-n} along the sector curve is 0 when
(n-1) * α is a multiple of 2π. The cutoff integral equals
ε^{1-n} * (exp(i(1-n)α) - 1) / (1-n), which vanishes identically under
the angle condition. By FTC with primitive F(t) = γ(t)^{1-n}/(1-n).
The generalized winding number of the sector curve around 0
equals alpha / (2 * pi).