The real part of a principal-value winding number #
Hungerbühler--Wasem Proposition 2.3 replaces the singular complex index integrand along a curve
through w by the real integrand
((γ - w)⁻¹ * γ').im = (x y' - y x') / (x² + y²).
The complex integral generally exists only as a Cauchy principal value. By contrast, once the
real integrand is interval-integrable, deleting the part of the curve inside an ε-ball about
w does not change its limiting integral. This file identifies the imaginary part of the
complex principal value with that ordinary real integral. After the normalization by
(2πi)⁻¹, this is exactly the real part of the generalized winding number.
The result is the analytic bridge needed by the on-curve form of HW Proposition 2.3: the geometric part of that proposition supplies integrability (from boundedness at the finitely many crossings), while the remaining assertion that the principal value is purely imaginary upgrades the real-part identity here to the full real winding formula.
Main results #
HasCauchyPVAt.im_eq_integral_realWindingIntegrandidentifies the imaginary part of the Cauchy-kernel principal value with the ordinary integral ofrealWindingIntegrand.windingNumber_re_eq_real_integralgives the corresponding formula for the real part of the generalized winding number.
References #
- N. Hungerbühler, M. Wasem, Non-integer valued winding numbers and a generalized Residue Theorem, arXiv:1808.00997 (2018), Proposition 2.3.
The imaginary part of a Cauchy principal value of the index integral is the ordinary integral
of the real winding integrand, provided that real integrand is interval-integrable. This remains
valid when the curve passes through w: both truncations delete the same ε-ball, and dominated
convergence restores the point values at crossings, where realWindingIntegrand 0 v = 0.
The on-curve real-integral identity for the real part of the winding number. If the
Cauchy principal value defining windingNumber γ a b w exists and its real winding integrand is
interval-integrable, then
(windingNumber γ a b w).re = (1 / 2π) ∫ realWindingIntegrand (γ - w) γ'.
No avoidance hypothesis is imposed, so the curve may pass through w.