English

Generating Function for Pinsky's Combinatorial Second Moment Formula for the Generalized Ulam Problem

Combinatorics 2023-05-04 v3

Abstract

Given a uniform random permutation πSn\pi \in S_n, let Zn,kZ_{n,k} be equal to the number of increasing subsequences of length kk: so Zn,k={(i1,,ik)Zk:1i1<<ikn, πi1<<πik}Z_{n,k}=|\{(i_1,\dots,i_k) \in \mathbb{Z}^k\, :\, 1\leq i_1<\dots<i_k\leq n\, ,\ \pi_{i_1}<\dots<\pi_{i_k}\}|. In an important paper, Ross Pinsky proved E[Zn,k2]\mathbf{E}\big[Z_{n,k}^2\big] is equal to iA(ki,i)B(n,2ki)\sum_{i} A(k-i,i)B(n,2k-i), where for any nonnegative integers NN and jj, we have B(N,j)=(Nj)/j!B(N,j) = \binom{N}{j}/j! and A(N,j)A(N,j) is a particular nonnegative integer, which Pinsky characterized in two different ways. One characterization of A(N,j)A(N,j) involves the occupation time of the xx-axis prior to a first return to the origin. Using this, he proved a law of large numbers for the sequence Zn,knZ_{n,k_n} when kn=o(n2/5)k_n=o(n^{2/5}) as nn \to \infty. In a follow-up paper, he also proved the sequence Zn,knZ_{n,k_n} fails to obey a law of large numbers when 1/kn=o(1/n4/9)1/k_n = o(1/n^{4/9}) as nn \to \infty. Here, we return to his combinatorial formula for the the second moment of Zn,kZ_{n,k}, and we obtain a generating function for the A(N,j)A(N,j) triangular array. We are motivated by the hope of applying spin glass techniques to the well-known Ulam's problem to see if this gives a new perspective.

Keywords

Cite

@article{arxiv.2301.00125,
  title  = {Generating Function for Pinsky's Combinatorial Second Moment Formula for the Generalized Ulam Problem},
  author = {Samen Hossein and Shannon Starr},
  journal= {arXiv preprint arXiv:2301.00125},
  year   = {2023}
}

Comments

35 pages, 6 figures: added complete Elliptic integrals

R2 v1 2026-06-28T07:58:00.285Z