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Article

Distributions of runs and scans in multistate Markov exchangeable sequences

Pages 3040-3061 | Received 15 Jun 2022, Accepted 17 Nov 2022, Published online: 29 Nov 2022
 

Abstract

In this paper, we look at the distributions of runs and scans in multistate Markov exchangeable sequences. The joint distributions of runs of several lengths under four types of enumeration schemes are analyzed. We evaluate the upper tail probabilities for ratchet scan statistics exactly. By utilizing the expansion of the generating functions, we propose effective computational tools for the derivation of probability functions. The results presented here provide approaches for the evaluation of the exact distributions of runs and scans in a wide class of practical problems. Finally, we discuss several applications and numerical examples to show how our theoretical results are applied to the investigation of runs and scans, as well as a parameter estimation problem.

MATHEMATICS SUBJECT CLASSIFICATION:

Acknowledgements

The author wishes to thank the editor and referees for the careful review of our paper and helpful suggestions which led to improved results.

A. Computational technique

The derivation of the reliability of system in Section 5.2 is facilitated by the use of the expansions of the generating function, which is given by Equation(5.1). It is noteworthy that the following formula j1=0f11jm=0fm1[u1j1umjm]ϕn(01×m,u1,,um)=[u1f11umfm1]ϕn(01×m,u1,,um)i=1m(1ui) will lead to a computationally efficient tool for obtaining the reliability of the system, which can be easily carried out by using the computer algebra systems.

Algorithm

Define the initial function h0(u1,,um);

Probab (integer f1,…,fm)

 {

for (integer i = 1; im; i++) {

 Set hi(ui+1,,um)=fi1uifi1(11ui·hi1(ui,,um))|ui=0;

 }

return hm()(f11)!(f21)!(fm1)!;

 }

We can get the reliability of system Equation(5.1) by setting the initial function h0(u1,,um)=ϕn(01×m,u1,,um).

The startup demonstration test lengths in Section 5.3 are, of course, determined by the EquationEquations (5.2) and Equation(5.4) which can be performed by setting the initial functions h0(u1,,um)=ϕn(0,1,0,1,u2,1) and h0(u1,,um)=ϕn(1,1,0,u1,u2,1), respectively.

We can calculate the upper tail probability for scan statistics, using the EquationEquation (4.3). Obviously, we have j0=0r01js=0rs1[v0j0vsjs]gn(11×m,v0,,vs)=[v0r01vsrs1]gn(11×m,v0,,vs)i=0s(1vi). Accordingly, the evaluation can be performed through the above Algorithm by setting the initial function h0(v0,v1,,vs)=gn(11×m,v0,v1,,vs).

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