The Haagerup–Zsidó kernel #
The Haagerup–Zsidó kernel is an integrable function k : ℝ → ℂ whose Fourier integral
∫ k(t) e^{itx} dt equals 1 / x for every |x| ≥ 1, and whose L¹ norm is exactly π / 2.
Integrating a bounded operator-valued function against it is what gives the sharp constant π / 2
in the norm bound for the solution of the Sylvester equation AX - XB = C when the spectra of the
self-adjoint operators A and B are separated pairwise, and hence in the corresponding
Davis–Kahan sin Θ theorem. Those two identities are not proved in this file, which sets up the
kernel and its elementary properties.
The kernel is built in four steps from the hyperbolic weight w(y) = tanh (π y / 2):
TauCeti.HaagerupZsido.weight: the weightw(y) = tanh (π y / 2);TauCeti.HaagerupZsido.weightLaplaceTransform: its Laplace transform at|t|,L(t) = ∫_{y > 0} w(y) e^{-|t| y} dy;TauCeti.HaagerupZsido.realKernel: the real kernelr(t) = (sin t / 2) L(t);TauCeti.HaagerupZsido.reciprocalKernel: the kernelk(t) = -i r(t).
This file proves the elementary properties of these objects: the weight is continuous, odd,
nonnegative on [0, ∞) and bounded there by min 1 (π y / 2); the Laplace transform is a
genuine (absolutely convergent) integral for t ≠ 0, is even, nonnegative, measurable, and
satisfies L(t) ≤ 1 / |t| and L(t) ≤ π / (2 t²); the two kernels are measurable and odd, with
‖k(t)‖ = |r(t)|. The two bounds on L give |r(t)| ≤ π / (2 (1 + t²))
(TauCeti.HaagerupZsido.abs_realKernel_le): near the origin |sin t| ≤ |t| cancels the
1 / |t| growth of L, and at infinity L decays like 1 / t² because w(y) ≤ π y / 2
near y = 0. Hence both kernels are integrable on ℝ.
References #
- U. Haagerup, L. Zsidó, the extremal kernel attaining the constant
π / 2; see the account in S. Albeverio, K. A. Makarov, A. K. Motovilov, Graph subspaces and the spectral shift function, Canad. J. Math. 55 (2003), 449–503. - R. Bhatia, C. Davis, A. McIntosh, Perturbation of spectral subspaces and solution of linear operator equations, Linear Algebra Appl. 52/53 (1983), 45–67.
The hyperbolic weight #
The hyperbolic weight w(y) = tanh (π y / 2) of the Haagerup–Zsidó construction.
Instances For
The Laplace transform of the weight #
The Laplace transform of the weight at |t|,
L(t) = ∫_{y > 0} tanh (π y / 2) e^{-|t| y} dy. The integral converges absolutely for t ≠ 0
(integrableOn_weight_mul_exp); at t = 0 it diverges and the Bochner integral is 0.
Instances For
For t ≠ 0 the integrand of the Laplace transform is integrable on (0, ∞): it is
dominated by e^{-|t| y}.
The Laplace transform of the weight is nonnegative.
The Laplace transform of the weight is even.
The Laplace transform of the weight is measurable.
Since the weight is less than 1, L(t) ≤ ∫_{y > 0} e^{-|t| y} dy = 1 / |t|.
Since the weight lies below π y / 2,
L(t) ≤ (π / 2) ∫_{y > 0} y e^{-|t| y} dy = π / (2 t²).
The real and reciprocal kernels #
The real Haagerup–Zsidó kernel r(t) = (sin t / 2) L(t).
Instances For
The Haagerup–Zsidó kernel k(t) = -i r(t). For |x| ≥ 1, the rotation by -i turns the
Fourier integral ∫ r(t) e^{itx} dt = i / x of the odd real kernel into
∫ k(t) e^{itx} dt = 1 / x.
Instances For
The real kernel is odd.
The kernel has the same modulus as the real kernel.
The decay bound for the real kernel. For every t, |r(t)| ≤ π / (2 (1 + t²)). For
|t| ≤ 1 this combines |sin t| ≤ |t| with L(t) ≤ 1 / |t|; for |t| ≥ 1 it combines
|sin t| ≤ 1 with L(t) ≤ π / (2 t²).
The real kernel is integrable on ℝ: it is dominated by π / (2 (1 + t²)).
The real Haagerup–Zsidó kernel times a sine is integrable.
The Haagerup–Zsidó kernel is integrable on ℝ.