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ISSN: 2349-0632 (P), 2349-0640 (online) Published on 26 October 2014

www.researchmathsci.org

Approximation of Markov Integrated

Semigroup Induced by Dual Markov

Branching Process and its Application

to Signal Processing

Yijin Zhang and Changyou Wang

College of Science, Chongqing University of Posts and Telecommunications, Chongqing 400065, P. R. China

Email: [email protected]

Received 18 May 2014;Accepted 12 August 2014

Abstract. In this paper, some conditions and properties of approximation of Markov integrated semigroup induced by dual Markov branching process are dis-cussed ; Theorem 1 and Theorem 2 are obtained. Finally their application to signal processing is studied.

Keywords: Approximation, Markov Integrated Semigroup, Dual Markov Branch-ing Process,Signal ProcessBranch-ing,q−matrix,Transition Function.

AMS Mathematics Subject Classification (2010): 03E72, 08A72 1. Introduction

A one-dimensional Markov branching process is a continuous-time Markov chain (briefly, CTMC)[1] on a countable state space E ={0,1,2, ...}whose stochastic evo-lution is governed by the branching property.Markov branching processq-matrix is given by

(1.1) q˜ij =

ibj−i+1 j≥i−1

0 otherwise

wherebk ≥0, k6= 1, and

P

k≥0bk≤0.

Consider the Dual branching q-matrix Q which is a continuous-time Markov chains on the state spaceE =Z+ ={0,1,2,···}and theq-matrixQ= (qij, i, j ∈E): Dual Markov branching process(DMBP)[2] X(t) is a continuous-time Markov chain on the state spaceZ+={0,1,2,· · · }, where the q-matrix[3,4] Q={qij;i, j∈Z+}, is given by

(1.2) qij =

iai−j+1−(j+ 1)ai−j i≥j−1

0 otherwise

whereak=Pkj=0bj, k≥0, bj is the sequence defined by branchingq-Matrix ˜Q.a0≤

0 a1 ≥a2≥ · · · ≥ak≥ · · · ≥0. The following are from [8]:

1. The Dual branchingq-matrix Q generates a positive once integrated semigroup of contractions T(t) = (Tij(t);i, j ∈ Z+) on l∞ if and only if Q is zero-exit. And (Tij0 (t)) is exactly its Q-functionF(t) = (fij(t)).

2. The integrated semigroup T(t) generated by Dual branching q-matrix is a Markov integrated semigroup.

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Branching Process and its Application to Signal Processing

Let us consider a measured state space (X, A), where A is theσ-algebra on X.Our aim in this paper is to discuss some conditions and properties of approximation of Markov integrated semigroup induced by dual Markov branching process and its application to signal processing.

For more unmentioned notations and preliminary ,we refer to the References of this paper.

2. Theories and Proofs

Approximation problem is a very important one on Markov process and has been widely applied in many fields.It is well known that Markov integrated semigroup can be approximated by an uniformly convergence integrated semigroup.

First,we have:

Theorem 1. Let Q = (qij, i, j ∈ E)and nQ = (nqij, i, j ∈ E)are both FRR q -matrices ,let F(t) = (fij(t)) and nF(t) = (nfij(t)) are both FRR transition func-tions, Φ(λ) = (φij(λ), i, j ∈ E) and nΦ(λ) = (nφij(λ), i, j ∈ E) are both their corresponding resolvent functions respectively,then the following are equivalent:

(i) for any i, j∈E, nqij →qij as n−→ ∞;

(ii) for any i, j∈Eand t≥0,nfij(t)→fij(t)as n−→ ∞; (iii) for any i, j∈Eand λ >0,nφij(λ)→φij(λ)as n−→ ∞.

Proof. (i)⇒(ii):We known that: nΩx → Ωx, nQ and Q are both FRR q-matrices. Lettingx=ej = (0,0,· · ·,1,0,· · ·)T,for a fixed i0, we can obtain:

||nΩej −Ωej||E = ||nQej −Qej||E = ||(nqij)i−(qij)i||E = ||(nqij)i−(qij)i|| = sup

i∈E

|nqij −qij|

= |nqi0j−qi0j| →0

for anyλ >0.

0 ≤

Z +∞

0

e−2λt|nfij(t)−fij(t)|dt

Z +∞

0

e−2λt|nfi0j(t)−fij(t)|dt

≤ |nqij−qij| ≤ |nqi0j−qi0j| →0

By the squeeze theorem for limit of functions ,we must getnfij(t)→fij(t)asn−→ ∞.

(ii)⇒(iii):It can be completed easily by Lebesgue’s theorem on control and con-vergence.

(iii)⇒(i):Because nF(t) = (nfij(t))and F(t) = (fij(t)) are both FRR transition functions,nF(t)andF(t) are both positive strong continuous contraction semigroup. Letting their generators are nA and A respectively,then we know that resolvent functions Φ(λ) = (φij(λ), i, j∈E) andnΦ(λ) = (nφij(λ), i, j ∈E) are just resolvent equation of operators nA and A respectively,namely´u140 < λ ∈ ρ(nA) = ρ(A) and

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We will prove that for anyλ >0,nΦ(λ)x→Φ(λ)x asn−→ ∞. Sincenfij(t) and

fij(t) are both transition functions by [1],nφij(λ) andφij(λ) are both FRR resolvent functions,there must exist the statei0,such that

sup i∈E

|nφij(λ)−φij(λ)|=|nφi0j(λ)−φi0j(λ)|

Because span {ej, j ∈E}is dense and

||nΦ(λ)−Φ(λ)|| ≤ ||nΦ(λ)||+||Φ(λ)|| = sup

i∈E

X

j∈E

|nφij(λ)|

+ sup i∈E

X

j∈E

|φij(λ)|

≤ sup i∈E

X

j∈E

|nφi0j(λ)|

+ sup i∈E

X

j∈E

|φi0j(λ)|

≤ 4

λ

sonΦ(λ)−Φ(λ)is bounded .By the corresponding theorem in [2],we obtain :

nF(t)→F(t) t≥0 n−→ ∞

sup i∈E

|nqij−qij| = |nqi0j−qi0j|

≤ |nF(t)−F(t)| →0

The proof is completed.

Theorem 2. Suppose that T(nt)(n∈N) is a series of MIS,P(nt) is the corresponding transition function of T(nt), An is the generator of P(nt) in l1.If there exists λ0 such

that Reλ0 > 0 and the range of operator R(λ0) is dense in l1,then there exists a

unique operator A: A will generate a contraction c0 semigroup P(t).If T(t) is the

corresponding Markov integrated semigroup,then T(nt)x → T(t)x(t ≥ 0, x ∈ l∞) as

n−→ ∞.

Proof. By [3,Theorem 4.4],we know that there exists a unique operatorA:generating a contraction c0 semigroup P(t). P(nt)x→P(t)x, t≥0, x∈l1.

Letting Pij(t) =heiP(t), eji,we obtain thatP(t) = (Pij(t), i, j ∈E) is a transition function ,so we have

(2.1) h

Z ∞

0

e−λteiP(t)dt, ti=hei, λ

Z ∞

0

e−λtT(t)dti

(2.2) heiP(t), eji=

Z ∞

0

e−λtheiP(t), ejidt=

Z ∞

0

e−λtPij(t)dt=hei, T(t)eji

So Tn

(t)x→T(t)x(t≥0, x∈l∞) as n−→ ∞.

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Branching Process and its Application to Signal Processing

3. Applications

Basic morphological transformation in one-dimensional discrete signal processing is defined as: let the original signal f(n) be a discrete function ,it is defined on

E ={0,1,2,···};otherwise defining the sequence structure elementg(n) as a discrete function on G={0,1,2,· · ·M −1}.

By hypothesis the image,morphological filtering is to filter out signal structural elements through morphological transformation than the structural elements of noise.Expansion operator removes the negative pulse and signal positive pulse.Corrosion Operators remove the Positive Pulse and smooth the negative Pulse, the operator removes the positive pulse (see[9,10,11]) .Closed trading Remove the negative pulse counting and retained the Positive Pulse.Control the inverter output to Bench spin-dle speed.We now relate the local groups we have defined to the theory of approxi-mation.

Example 1. Suppose P(s) denote the probability of each digital input signals,

P(A→B)denote the integral of conditional probability density in the interval[a,b].We get:

P(A→B) =

Z B

A

P(s)ds

Because the digital signal is entered with equal probability:

0 ≤

Z +∞

0

p(t)|nfij(t)−fij(t)|dt

Z +∞

0

p(t)|nfi0j(t)−fi0j(t)|dt

≤ |nqi0j−qi0j| →0

So the digital signal is very stable and can be observed easily.It supplies a different angle to study signal processing.

Example 2. Since 1980s,HMM is successfully applied to speech recognition and text recognition.In recent years, people try to apply it to the mobile communication of multiuser detection and bioinformatics of DNA sequence comparisons.The important factor to affect the pattern recognition system recognition rate is non-standard input signal. In order to improve the robustness of the recognition system,we need to construct an adaptive signal on the input mode, anti-jamming hidden Markov model. Characteristics of HMM system are determined by its three characteristics parameter vectors completely.

We have

P(X|λ) = P(X,ΣQ|λ) = ΣP(Q)P(X|Q, λ)

= ΣP(Q) T

Y

t=1

P(xt)

= ΣP(Q)

4. Conclusion

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broadband noise, the binary PAM signal through the non-linear double-steady-state stochastic resonance receiver from the transmission can be met. Further research on non-steady state probability density of the system can better improve these results. This work was supported by the Scientific and Technological Research Program of Chongqing Municipal Education Commission (Grant No:KJ1400430).

REFERENCES

[1] W.J.Anderson, Continuous-Time Markov Chains, Springer Series in Statistics, Springer-Verlag, New York, 1991.

[2] M.F.Chen, From Markov Chains to Non-Equilibrium Particle Systems, Singapore: World Scientific, 1992.

[3] Y.R.Li, Markov integrated semigroups and their applications to continuous-time Markov chains, Integr. Equ. Oper. Theory, 60 (2008) 247-269.

[4] Li Yang-rong, Contraction integrated semigroups and their application to continuous-time markov chains, Acta Math Sinica, 19(3) (2003) 605-618.

[5] Chen Anyue, Phil Pollett, Zhang Hanjun and Li Junping, The collision branching process, Journal of Appl. Prob., 41(4) (2004) 1033-1048.

[6] R.Delaubenfels, Existence Families, Functional Calculi and Evolution

Equations,Springer-Verlag, New York, 1994.

[7] Li Yang-rong, Dual and feller-reuter-riley transition functions, J. Math. Anal. Appl., 313(2) (2006) 461-474.

[8] Zhang Yijin , Li Yangrong,Yang chunde, Markov integrated semigroups generated by dual branching q-matrix, Journal of Southwest university (Natural science edition) 32(4) (2010) 120-123.

[9] J.J.Collins, C.C.Chow, T.T.Imhoff, A period stochastic resonance in excitable systems, Physical Review E, 52(4) (1995) 1118-1231.

[10] A.Pazy, Semigroups of linear operators and applications to partial differential equations, New York, Springer-Verlag, 1983.

References

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