ABSTRACT

This series on the International Conference on Difference Equations and Applications has established a tradition within the mathematical community. It brings together scientists from many different areas of research to highlight current interests, challenges and unsolved problems. This volume comprises selected papers presented at the Fifth Interna

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l, =

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Jt,_

iJ-a

chapter 3|11 pages

Necessary Conditions

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Selection in Population Genetics Models

Host-Pathogen Systems

chapter 1|1 pages

INTRODUCTION

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of 17

If i, j,

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if wu $ < or if 0 < < p and

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ofH ost-Pathogen Systems 19

< < K, Fe c•[o,K], > K), F(K)

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ll z:i.

_ zr + E;<• zf' + E;>• z:

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ofH ost-Pathogen Systems

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= + Jti), =

+II'+ E;<,(sfi +I/')+ E;>,<S:;

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ofH ost-Pathogen Systems

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of Host-Pathogen Systems

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On the Subtle Role oflnvertibility in Discrete Dynamics

Abstract We consider two of the most fundamental topics in

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of 35 Theorem 2.1: C

R" on an R"- of a fixed point p of f and that the derivative of f at p invertible and no eigenvalue" with modultu 1. That this theorem does not hold without the invertibility as- f of Theorem 2.1 is seen to be topologically conjugate to u(A-) of A+ and A-, respectively, > 1} and u(A-) {A E : 0 < <

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where the functions s+, and sare continuous and vanish at 0.

Example: We consider the mapping w) : the w-axis h: .N-+ := h(.N) is

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ofl nvertibility in Discrete Dynamics is a homeomorphism we get the inclusion (0, 0, 0) E int J(N). This,

:= {(0, 0)} x ( -2e, 2e) to the boundary g('P) \ int g('P) of the cylinder g('P). From (g('P)\intg('P)) =

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Theorem 2.2: Coruider a C : n n-

of the coordinate origin and that I of top. Furthermore, are tangent to the of the linearization DIP.

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(i) Hypothesis on linear part: The evolution operators and

B( k) y( k ), respectively, satisfy the estimates < K1alc-l for all k k, l I, < K2fJic-l for all k I, IE I ofF and are ... , m} have := sup (k, x, y) < oo, IGin:= sup <oo.

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assume that the number 1 lies between the growth rates a and

part of system (3.1) are only supposed to lie in £(X) (and not Theorem 3.2: We consider system (9.1} satisfying the above hy- {k E 7l : k for some E s : I x X -+ graphS:= E I,e EX}, pseudo- ..\(·; lt,e,TJ) (X x Y)}. of system of the invariance equation e)+ e)) x X, Y ·) : Y

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a+u 1 then ·) : -+ Y m-time"

Y-+ := (a+ u,{3- e, '7) E R we have (k, e, E R for of the invariance + 1, + -

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A Spectral Theory for Nonautonomous Difference Equations

ofM athematics, University ofA ugsburg,

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It follows that P,.(k,l) = •(k,l)Pt for k,l ::

If = A,z,,

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If w. w2

w. + w2 := {(t,e> e z aN : z aN : t)e 1-

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< -1 + At b for , where a, bE R , a .

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A(n) = diag(A(n), · · ·, 0,

k+ 1,· · · > 0. fl, 1 i, -Hoc

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Theorem 1 Suppose that for the system ( 10) there is an eigenvector v such

=< v > and therefore {-r,-r+1, , -1,0} andB,f: NxFr i,l!!,

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n-+ +oo.

n-+ +oo. Then

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n;o(n) = K

>no, E {E

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n. x n. Jordan matrices

k+l,···,N > 0 B, + v• l!!,.x•uf' Improvement of Theorem Band consequences

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Necessary and Sufficient Oscillation Criteria for Discrete Reaction-Diffusion Equations

ofM athematics, Tsing Hua University,

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if > it

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< -1. When u an arbitrary it

= -a, If > > > that

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u of

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fork= 0, 1, ,l-1,

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1 timu

> JA'}

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= < A

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= >A

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T:W Oul

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The generating matrix

= + EN, = N-+ VI r = {/: N-+ VI < oo}, = EN}. > 0, then this solution can be extended to the set

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, is

+ + a3y3(n), f.':, then a generating matrix of Eq. ( in S is = -2-n + f.': may consider the generating matrix

chapter 0|5 pages

(/)

rand {b(n)} satisfying (13), it possible to + 0 {r-"6 0(6')).

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References

chapter 2|1 pages

Preliminaries

+(at+ +···+(at+

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rr I

chapter I|16 pages

" :b ,et-i,

chapter 1|2 pages

/(1-

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On the Dynamics

a+Jhn+rx -1 A+Bxn of of

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INTRODUCTION AND PRELIMINARIES

+ Bzn > x /(f,x).

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of x,..143

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of 145

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B--,

a+ +

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of x,..

+ aB = a + + B'

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of .r,.., 149

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KKl:p' <

q-p-rj ....

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INVARIANT

-,-,. ) + + =q5-,.-.

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of 153

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of 155

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MR. Kulenovic

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of 157

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References

=a+ ';:•,

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Linear ODE's for Describing

Modulators, Filter Design and Error Estimations ofM athematics, Technical University ofR menau,

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References

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Introduction.

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Definitions and Background. N

If X If J :

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(The Covering Prlndple.) Suppose that X is a metric

of X, S,, ... , is of

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of X s = {s l, s,, ... s } of symbol

f : a

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fori= is I

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of and

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not be a Cantor set.

= -1 = < = = -1, sl [-1,zo] = of

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[-1,1] that are

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Fipre (z) = a- >r, for

map/,

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<-land a-ldl > LetQ=

if Q -+ R is a continuous map such that lg(:r, I of (-1,0) and (0,1], o· c

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of£, then for

= (a-by2-dz+g(z,y),z), Sis a

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ofR.f'2(W n Q) is

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Generalized Henon Maps as Difference Equations

-1, > 1, < -1. each., sl s,,

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'• is either L or R, then there is a 10lution such that x, '•·

s:,, x, E E s:l, Sic = c = .st' Si L, R. that(. ..

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If(.t,):-ao any sequence such

each"' Lor R, then there solution that z, e "•· 5. References

chapter i|1 pages

= 1,2, ... ,T, = maxiDIJ/(x,a)l, L = maxiD!f(x,a)l, =

... + 6a-r) this p = (xc + 6xt, + 6x2, ... , + 6x-r) of 6xt =

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that

(tsaLs;-l

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< 1 then it is stable. Therefore get from (9):

Xt(1-

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< a < a< Introduce

> 0. It not hard < < 1 -a),

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3 Two-dimensional map with hyperbolic attracto r

< 1, < be a square in the plane (x, y). Qare presented as a separation by the function {(x,y)EQ: y<h(x)}, {(x,y)EQ: y>h(x)}. T: (x, y) f(x, y), <ax, >ax, < The Belykh map is remarkable for the fact that it has a

chapter 0|1 pages

< < 1, 0 < 2 < 2/(1 + jal), lal < 1. Finally, for

< 1/2. Thus, for a hyperbolicity get the following inequalities:

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< 1 and the map with a> 1 have the

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Boundedness of Volterra Difference

Equations with Finite Linear Part

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satisfies the inequality where (I) the functions [0, oo) --+ (0, oo), 1 $ i $ p, are continuous

z+ --+ and : z+ --+ [d, are functions, c is a > 0, 1 $ i $ and wi-l are their Theorem A Let and assume (I) and (II) hold. Let z+ such that

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MAIN RESULTS

... n ·, satisfies the

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m) be a fundamental matrix corresponding to the

< oo. If Mu(no) < then by Theorem A it that w,-[W,(<pp-l(c))

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If the

solutions with initial conditions small enough, namely, Theorem 4. Assume that the assumptions (ii) a.nd (iii) of The- <cis

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EXTENSIONS In this section, our objetive is to extend some of the results to discrete systems of the form

z+; and I : z+ =-TN, -TN+ 1, · · · G!+lA;(s).

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On Convergence of Discrete Stochastic

Approximation Procedures ofM aths/CScience, oft he West Indies,

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of Lyness Equation

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An Elliptic Beta Integral

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< 1 and

II fi

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2 . 2)

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r(z;p, q) (2), one can check that

/r(to,

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Almost Periodicity in Difference Systems*

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It <