Mott polynomials

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In mathematics the Mott polynomials sn(x) are polynomials given by the exponential generating function:

ex(1t21)/t=nsn(x)tn/n!.

They were introduced by Nevill Francis Mott who applied them to a problem in the theory of electrons.[1]

Because the factor in the exponential has the power series

1t21t=k0Ck(t2)2k+1

in terms of Catalan numbers Ck, the coefficient in front of xk of the polynomial can be written as

[xk]sn(x)=(1)kn!k!2nn=l1+l2++lkC(l11)/2C(l21)/2C(lk1)/2, according to the general formula for generalized Appell polynomials, where the sum is over all compositions n=l1+l2++lk of n into k positive odd integers. The empty product appearing for k=n=0 equals 1. Special values, where all contributing Catalan numbers equal 1, are
[xn]sn(x)=(1)n2n.
[xn2]sn(x)=(1)nn(n1)(n2)2n.

By differentiation the recurrence for the first derivative becomes

s(x)=k=0(n1)/2n!(n12k)!22k+1Cksn12k(x).

The first few of them are Template:OEIS

s0(x)=1;
s1(x)=12x;
s2(x)=14x2;
s3(x)=34x18x3;
s4(x)=32x2+116x4;
s5(x)=152x158x3132x5;
s6(x)=2258x2+158x4+164x6;

The polynomials sn(x) form the associated Sheffer sequence for –2t/(1–t2)[2]

An explicit expression for them in terms of the generalized hypergeometric function 3F0:[3]

sn(x)=(x/2)n3F0(n,1n2,1n2;;4x2)

References

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