Components and Cycles of Random Mappings

05/11/2022
by   Steven Finch, et al.
0

Each connected component of a mapping {1,2,...,n}→{1,2,...,n} contains a unique cycle. The largest such component can be studied probabilistically via either a delay differential equation or an inverse Laplace transform. The longest such cycle likewise admits two approaches: we find an (apparently new) density formula for its length. Implications of a constraint – that exactly one component exists – are also examined. For instance, the mean length of the longest cycle is (0.7824...)√(n) in general, but for the special case, it is (0.7978...)√(n), a difference of less than 2%.

READ FULL TEXT

page 1

page 2

page 3

page 4

research
06/24/2019

On non-Hamiltonian cycle sets of satisfying Grinberg's Equation

In [1] we used a cycle basis of the cycle space to represent a simple co...
research
10/16/2017

Longer Cycles in Essentially 4-Connected Planar Graphs

A planar 3-connected graph G is called essentially 4-connected if, for e...
research
11/10/2021

Permute, Graph, Map, Derange

We study decomposable combinatorial labeled structures in the exp-log cl...
research
02/15/2022

Second Best, Third Worst, Fourth in Line

We investigate decomposable combinatorial labeled structures more fully,...
research
02/18/2019

Find Subtrees of Specified Weight and Cycles of Specified Length in Linear Time

We introduce a variant of DFS which finds subtrees of specified weight i...
research
09/04/2023

Loopless Algorithms to Generate Maximum Length Gray Cycles wrt. k-Character Substitution

Given a binary word relation τ onto A * and a finite language X ⊆ A * , ...
research
11/08/2018

On inverse product cannibalisation: a new Lotka-Volterra model for asymmetric competition in the ICTs

Product cannibalisation is a well-known phenomenon in marketing and tech...

Please sign up or login with your details

Forgot password? Click here to reset