Math 2.0

Integral transforms, operational calculus Definition

Abel transform

Builds on Lebesgue integral

Definition

Let f ⁣:[0,∞)→ℂf \colon [0, \infty) \to \C be measurable, and let y≥0y \ge 0 be such that ∫y∞∣f(r)∣ rr2−y2 dr<∞\int_y^\infty \frac{\abs{f(r)}\, r}{\sqrt{r^2 - y^2}}\, dr < \infty. The Abel transform of ff at yy is the Lebesgue integral F(y)=2∫y∞f(r) rr2−y2 dr.F(y) = 2 \int_y^\infty \frac{f(r)\, r}{\sqrt{r^2 - y^2}}\, dr.

Remarks

The integrand has an integrable singularity at r=yr = y, of order (r−y)−1/2(r - y)^{-1/2}, when ff is bounded near yy and y>0y > 0. If ff is continuously differentiable and decays fast enough at infinity, the transform can be inverted by f(r)=−1π∫r∞F′(y)y2−r2 dy.f(r) = -\frac{1}{\pi} \int_r^\infty \frac{F'(y)}{\sqrt{y^2 - r^2}}\, dy.

Example: f(r)=e−r2f(r) = e^{-r^2}. The substitution s=r2−y2s = r^2 - y^2, ds=2r drds = 2r\, dr, gives F(y)=∫0∞e−y2−ss ds=e−y2 Γ(1/2)=π e−y2F(y) = \int_0^\infty \frac{e^{-y^2 - s}}{\sqrt s}\, ds = e^{-y^2}\, \Gamma(1/2) = \sqrt{\pi}\, e^{-y^2}.

Non-example: f(r)=1f(r) = 1 for all rr. Then rr2−y2≥1\frac{r}{\sqrt{r^2 - y^2}} \ge 1 for r>yr > y, so the integral diverges for every yy and ff has no Abel transform.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Abel_transform
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