Touchard polynomials

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Touchard Polynomials

The Touchard polynomials, studied by Template:Harvs,[1] also called the exponential polynomials or Bell polynomials, comprise a polynomial sequence of binomial type defined by

Tn(x)=∑k=0nS(n,k)xk=∑k=0n{nk}xk,

where S(n,k)={nk} is a Stirling number of the second kind, i.e., the number of partitions of a set of size n into k disjoint non-empty subsets.[2][3][4][5]

The first few Touchard polynomials are

T1(x)=x,
T2(x)=x2+x,
T3(x)=x3+3x2+x,
T4(x)=x4+6x3+7x2+x,
T5(x)=x5+10x4+25x3+15x2+x.

Properties

Basic properties

The value at 1 of the nth Touchard polynomial is the nth Bell number, i.e., the number of partitions of a set of size n:

Tn(1)=Bn.

If X is a random variable with a Poisson distribution with expected value λ, then its nth moment is E(Xn) = Tn(λ), leading to the definition:

Tn(x)=e−x∑k=0∞xkknk!.

Using this fact one can quickly prove that this polynomial sequence is of binomial type, i.e., it satisfies the sequence of identities:

Tn(λ+μ)=∑k=0n(nk)Tk(λ)Tn−k(μ).

The Touchard polynomials constitute the only polynomial sequence of binomial type with the coefficient of x equal 1 in every polynomial.

The Touchard polynomials satisfy the Rodrigues-like formula:

Tn(ex)=e−exdndxneex.

The Touchard polynomials satisfy the recurrence relation

Tn+1(x)=x(Tn(x)+T'n(x))

and

Tn+1(x)=x∑k=0n(nk)Tk(x).

In the case x = 1, this reduces to the recurrence formula for the Bell numbers.

A generalization of both this formula and the definition, is a generalization of Spivey's formula[6]

Tn+m(x)=∑k=0n{nk}xk∑j=0m(mj)km−jTj(x)

Using the umbral notation Tn(x)=Tn(x), these formulas become:

Tn(λ+μ)=(T(λ)+T(μ))n,Template:Clarification needed
Tn+1(x)=x(1+T(x))n.

The generating function of the Touchard polynomials is

∑n=0∞Tn(x)n!tn=ex(et−1),

which corresponds to the generating function of Stirling numbers of the second kind.

Touchard polynomials have contour integral representation:

Tn(x)=n!2πi∮ex(et−1)tn+1dt.

Zeroes

All zeroes of the Touchard polynomials are real and negative. This fact was observed by L. H. Harper in 1967.[7]

The absolute value of the leftmost zero is bounded from above by[8]

1n(n2)+n−1n(n2)2−2nn−1((n3)+3(n4)),

although it is conjectured that the leftmost zero grows linearly with the index n.

The Mahler measure M(Tn) of the Touchard polynomials can be estimated as follows:[9]

{nΩn}(nΩn)≤M(Tn)≤n+1{nKn},

where Ωn and Kn are the smallest of the maximum two k indices such that {nk}/(nk) and {nk} are maximal, respectively.

Generalizations

  • Complete Bell polynomial Bn(x1,x2,…,xn) may be viewed as a multivariate generalization of Touchard polynomial Tn(x), since Tn(x)=Bn(x,x,…,x).
  • The Touchard polynomials (and thereby the Bell numbers) can be generalized, using the real part of the above integral, to non-integer order:
    Tn(x)=n!π∫0πex(ecos⁡(θ)cos⁡(sin⁡(θ))−1)cos⁡(xecos⁡(θ)sin⁡(sin⁡(θ))−nθ)dθ.

See also

References

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