Math 2.0

Integral transforms, operational calculus Definition

Poisson–Mellin–Newton cycle

Builds on Mellin transformGamma functionRamanujan's master theoremHolomorphic function

Definition

Let (fn)n≥0(f_n)_{n \ge 0} be a sequence of complex numbers. The Poisson–Mellin–Newton cycle of (fn)(f_n) is the following chain of three objects.

  1. The Poisson generating function g(t)=e−t∑n≥0fntnn!g(t) = e^{-t} \sum_{n \ge 0} f_n \frac{t^n}{n!}, for t>0t > 0 where the series converges.
  2. The Newton coefficients bm=∑k=0m(mk)(−1)kfkb_m = \sum_{k=0}^{m} \binom{m}{k} (-1)^k f_k, which satisfy g(t)=∑m≥0bm(−t)mm!g(t) = \sum_{m \ge 0} b_m \frac{(-t)^m}{m!} and fn=∑k=0n(nk)(−1)kbkf_n = \sum_{k=0}^{n} \binom{n}{k} (-1)^k b_k.
  3. The Mellin transform φ(s)=∫0∞g(t) ts−1 dt\varphi(s) = \int_0^\infty g(t)\, t^{s-1}\, dt, where it converges.

Assume that bm=b(m)b_m = b(m) for a function bb that is holomorphic and of moderate growth in a half-plane. Then the cycle closes by the relations φ(s)=Γ(s) b(−s),fn=(−1)n2πi∮Cb(s) n!s(s−1)⋯(s−n) ds,\varphi(s) = \Gamma(s)\, b(-s), \qquad f_n = \frac{(-1)^n}{2\pi i} \oint_{C} b(s)\, \frac{n!}{s (s - 1) \cdots (s - n)}\, ds, where CC is a positively oriented contour that encircles the points 0,1,…,n0, 1, \dots, n and no singularity of bb.

Remarks

The two identities in clause 2 come from multiplying the power series of e−te^{-t} and ∑fntn/n!\sum f_n t^n / n! and comparing coefficients. The map (fn)↦(bm)(f_n) \mapsto (b_m) is the binomial transform, and it is its own inverse. The first closing relation is an instance of Ramanujan's master theorem, which needs growth conditions on bb. The second is the Nörlund–Rice integral: the residue of n! / (s(s−1)⋯(s−n))n!\,/\,(s (s-1) \cdots (s-n)) at s=ks = k is (−1)n−k(nk)(-1)^{n-k} \binom{n}{k}, so the residue theorem gives back fn=∑k(nk)(−1)kb(k)f_n = \sum_k \binom{n}{k} (-1)^k b(k). Here Γ\Gamma is the gamma function.

Example: fn=(1/2)nf_n = (1/2)^n. Then g(t)=e−t/2g(t) = e^{-t/2}, the Newton coefficients are bm=(1−1/2)m=2−mb_m = (1 - 1/2)^m = 2^{-m}, so b(s)=2−sb(s) = 2^{-s}. Indeed φ(s)=2s Γ(s)=Γ(s) b(−s)\varphi(s) = 2^{s}\, \Gamma(s) = \Gamma(s)\, b(-s) for Re⁡s>0\operatorname{Re} s > 0.

Non-example: for fn=(n!)2f_n = (n!)^2 the series ∑nfntn/n!\sum_n f_n t^n / n! diverges for every t>0t > 0, so there is no Poisson generating function and the cycle does not start.

Reading path

To understand this page from the ground up, read these 6 pages in order. The foundations come first.

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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.
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  1. Analytic continuation concept
  2. Gamma function concept
  3. Holomorphic function concept
  4. Mellin transform concept
  5. Ramanujan's master theorem statement
  6. Poisson–Mellin–Newton cycle definition

Further reading

  1. Web https://en.wikipedia.org/wiki/N%C3%B8rlund%E2%80%93Rice_integral
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MSC44A15, 39A70, 68W40
DefinesPoisson–Mellin–Newton cycle
UsesMellin transform, Gamma function, Ramanujan's master theorem, Holomorphic function

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