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TauCeti.Analysis.Fourier.HaagerupZsido.Basic

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):

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 #

The hyperbolic weight #

noncomputable def TauCeti.HaagerupZsido.weight (y : ℝ) :

The hyperbolic weight w(y) = tanh (π y / 2) of the Haagerup–Zsidó construction.

Instances For
    @[simp]

    The weight is odd.

    theorem TauCeti.HaagerupZsido.weight_nonneg {y : ℝ} (hy : 0 ≤ y) :

    The weight is nonnegative on [0, ∞).

    The weight is less than 1.

    On [0, ∞) the weight lies below its tangent line π y / 2 at the origin.

    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.

      @[simp]

      The Laplace transform of the weight is even.

      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 #

      noncomputable def TauCeti.HaagerupZsido.realKernel (t : ℝ) :

      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
          @[simp]

          The real kernel is odd.

          @[simp]

          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.