Math 2.0

Integral transforms, operational calculus Transforms with special function kernels Theorem

Hankel inversion theorem

Builds on Hankel transformBessel function of the first kind

Statement

Let ν≥−12\nu \ge -\frac12, and let JνJ_\nu be the Bessel function of the first kind of order ν\nu. Let f ⁣:(0,∞)→ℂf \colon (0, \infty) \to \C satisfy ∫0∞∣f(r)∣ r1/2 dr<∞\int_0^\infty \abs{f(r)}\, r^{1/2}\, dr < \infty, and let Fν(k)=∫0∞f(r)Jν(kr) r drF_\nu(k) = \int_0^\infty f(r) J_\nu(kr)\, r\, dr be its Hankel transform of order ν\nu. Let r>0r > 0, and assume that ff is of bounded variation on a neighbourhood of rr. Then lim⁡K→∞∫0KFν(k) Jν(kr) k dk=f(r+)+f(r−)2.\lim_{K \to \infty} \int_0^K F_\nu(k)\, J_\nu(kr)\, k\, dk = \frac{f(r^+) + f(r^-)}{2}. In particular, the limit is f(r)f(r) at every point rr where ff is continuous.

Remarks

The proof follows the pattern of the Fourier inversion theorem for Fourier integrals. After exchanging the integrals, the inner integral ∫0KJν(kr)Jν(kt) k dk\int_0^K J_\nu(kr) J_\nu(kt)\, k\, dk is computed in closed form from Bessel's equation, and it acts as an approximate identity concentrated at t=rt = r as K→∞K \to \infty. A Riemann–Lebesgue argument disposes of the parts away from rr, and the bounded variation near rr controls the part near rr, exactly as in Dirichlet's theorem for Fourier series. There is also an L2L^2 version: the Hankel transform of order ν\nu extends to a unitary operator of L2((0,∞),r dr)L^2((0, \infty), r\, dr) that is its own inverse.

Example: for ν=0\nu = 0 and f(r)=e−r2/2f(r) = e^{-r^2/2} one has F0(k)=e−k2/2F_0(k) = e^{-k^2/2}, and transforming again gives back e−r2/2e^{-r^2/2}. For the indicator function of [0,1][0, 1] and ν=0\nu = 0, F0(k)=J1(k)/kF_0(k) = J_1(k)/k, and at r=1r = 1 the inversion integral converges to the mean value 12\frac12 of the jump.

Going deeper

For a student

The theorem is the radial form of the Fourier inversion theorem, and for ν=n2−1\nu = \frac{n}{2} - 1 it can be derived from it for radial functions on ℝn\R^n. It justifies the solution of boundary value problems in cylindrical coordinates: transform in rr, solve an ordinary differential equation in the remaining variable, and transform back. The hypotheses parallel those of Dirichlet's pointwise convergence theorem for Fourier series.

Reading path

To understand this page from the ground up, read these 3 pages in order. The foundations come first.

Show the path as a graph
Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
  • no evidence level
  1. Bessel function of the first kind concept
  2. Hankel transform concept
  3. Hankel inversion theorem statement

Further reading

  1. Web https://en.wikipedia.org/wiki/Hankel_transform
About this page
TagBMXZSXETDW
URIm2://BMXZSXETDW
Kindstatement, theorem
WritingW0 stub
MSC44A20, 33C10
StatusThis copy of the site has no build data. Run m2 status BMXZSXETDW.
AboutHankel transform
UsesHankel transform, Bessel function of the first kind

Markdown · JSON · Edit on GitHub

What this page needs for W1

  • an inventory row: the row of the inventory that the node accounts for (0 of 1)
  • a source with a locator (0 of 1)

The writing levels say how complete the text of a page is. They do not measure its truth.

What links here

No page links to this page yet.