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Volume 2008, Article ID 505324,15pages doi:10.1155/2008/505324

Research Article

On the Growth of Nonoscillatory Solutions for

Difference Equations with Deviating Argument

M. Cecchi,1Z. Do ˇsl ´a,2and M. Marini1

1Department of Electronics and Telecommunications, University of Florence, Via S. Marta 3,

50139 Firenze, Italy

2Department of Mathematics and Statistics, Masaryk University, Jan´aˇckovo n´am. 2a,

60200 Brno, Czech Republic

Correspondence should be addressed to M. Cecchi,[email protected]

Received 28 March 2008; Accepted 27 May 2008

Recommended by Martin Bohner

The half-linear difference equations with the deviating argument Δan|Δxn|αsgnΔxn

bn|xnq|αsgnxnq 0 , q ∈ Z are considered. We study the role of the deviating argument q,

especially as regards the growth of the nonoscillatory solutions and the oscillation. Moreover, the problem of the existence of the intermediate solutions is completely resolved for the classical half-linear equationq 1. Some analogies or discrepancies on the growth of the nonoscillatory solutions for the delayed and advanced equations are presented; and the coexistence with different types of nonoscillatory solutions is studied.

Copyrightq2008 M. Cecchi et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

Consider the half-linear difference equations with the deviating argument

ΔanΔxnαsgnΔxnbnxnqαsgnxnq 0, 1.1 whereΔis the forward difference operatorΔxnxn1−xn,α >0,q∈Zanda{an},b{bn}

are positive real sequences forn≥0 such that

Ya

n0

1 an

1

, Yb

n0

bn<. 1.2

A large number of papers deal with the oscillatory and asymptotic properties of several particular cases of1.1, such as the classical half-linear equation

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and the equations with the advanced or delayed argumentτ∈Z,τ ≥1,

ΔanΔxnαsgnΔxnbnxn1ταsgnxn1τ 0, H

ΔanΔxnαsgnΔxnbn|xn1−τ|αsgnxn1−τ 0, H−

see, for example,1–9 , the monographs10,11 , and references therein.

By solution of1.1we mean a nontrivial sequence satisfying1.1for largen. As usual, a solutionx{xn}of1.1is said to benonoscillatoryif there exists a largenxsuch thatxnxn1>0

fornnx, otherwise it is said to beoscillatory. Equation1.1is characterized by thehomogeneity property, which means that ifxis a solution of1.1, then alsoλxis its solution for any constant λ.

It is well-known that the deviating argumentτplays an important role in the oscillation. For instance, for H the Sturm-type separation property holds and so all its solutions are either nonoscillatory or oscillatory, see, for example,11, Section 8.2 . In general, this property is no true anymore forHandH−; and the coexistence of oscillatory and nonoscillatory solutions can occur even in the linear case, that is whenα 1, as we illustrate below. Never-theless, in4 some comparison criteria, which link the nonoscillation ofHwith the existence of nonoscillatory solutions of the advanced equation H, or the delayed equation H−, are given. In particular, if a ≡ 1, the nonoscillation of H is equivalent to the existence of nonoscillatory solutions forHorH−, see4, Corollary 8 .

Nonoscillatory solutions of 1.1 can be classified as subdominant, intermediate, or dominant solutions, according to their asymptotic behavior, see below for the definition. As it is claimed in12, page 241 , the existence of the intermediate solutions is a difficult problem also in the continuous case. Moreover, another well-known problem is their possible coexistence with different types of nonoscillatory solutions, see, for example,13, page 213 . In14 , both problems have been completely resolved for the half-linear differential equation

atxαsgnxbt|x|αsgnx0, 1.3

using the extension of the Wronskian. Such approach cannot be used for H because the monotonicity of the corresponding Casoratian-type function remains an open problem.

The aim of this paper is to study intermediate solutions for 1.1 and the role of the deviating argumentq,especially as regards the growth of the nonoscillatory solutions and the oscillation. The problem of the existence of intermediate solutions is completely resolved when q 1, that is for the half-linear equationH. Whenq /1 some analogies or discrepancies on the growth of the nonoscillatory solutions, due to the presence of the deviating argument, are presented and also the coexistence with different types of nonoscillatory solutions is studied. Roughly speaking, ifan ≡ 1, the deviating argument has no effect, that is 1.1has the same types of nonoscillatory solutions for any q. On the other hand, if a is rapidly increasing, or decreasing, for largen, the delay may change the type of nonoscillatory solutions as well as the oscillation, as examples below show.

2. Main results

For any solutionxof1.1we denote byx1 {xn1}its quasidifference, where

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In view of 1.2, any nonoscillatory solution x of 1.1is eventually monotone and verifies xnxn1 > 0 for large n; we denote this property by saying that x is of class M. Let x be a solution of1.1in the classM; then for largeneitherxis positive increasing andx1 positive decreasing orxis negative decreasing andx1 negative increasing. So, we can divide the class

Minto the three subclasses:

M

∞,

x∈M: lim

n xn, limn x

1

n x, 0<x<,

M

∞,0

x∈M: lim

n xn, limn x

1

n 0 ,

M

,0

x∈M: lim

n xnx, limn x

1

n 0, 0<x<,

2.2

see also6, 9 . Following the terminology of 15 in the continuous case, solutions inM∞,, M

∞,0, M,0 are called dominant solutions, intermediate solutions, and subdominant solutions,

respectively. This terminology is justified by the fact that if x ∈ M∞,,y ∈ M∞,0, z ∈ M∞,, then|xn|>|yn|>|zn|for largen.

The series

n0

1 an

1

kn bk

1 ,

Tαq

n0

bn nq−1

k0

1 ak

1/αα ,

2.3

where the conventionn2

n1ui 0 ifn1 > n2 is used, play an important role in the classification

of nonoscillatory solutions of1.1. The possible cases for the behavior of these series are the following

C1Sα<, Tαq<∞; 2.4

C2, Tαq<∞; 2.5

C3Sα<, Tαq ∞; 2.6

C4, Tαq. 2.7

Observe that, when q 1, the caseC2is possible only when α > 1, while the case C3is

possible only whenα <12, Theorem 4 . Whenq /1, in view of the fact1≤Tαqforq >1, the caseC2is not possible whenα < 1, q > 1 and the caseC3is not possible whenα > 1,

q <1.

Ifq < 1q > 1 , it is easy to give an example of1.1satisfying the caseC2 the case C3 for anyα, seeExample 5.3below.

The main results of this paper are the following.

Theorem 2.1. ForHwe have:

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i3 ifSα<,Tα1 ∞, thenM,0/,M∞,0/,M∞,;

i4 ifSα,Tα1 ∞andHis nonoscillatory, thenM,0,M∞,0/,M∞,.

Theorem 2.2. For1.1withq /1we have:

i1 ifSα<,Tαq<, thenM,0/,M∞,0,M∞,/∅; i2 ifSα,Tαq<, thenM,0,M∞,0/,M∞,/;

i3 ifSα<,Tαqand

lim inf

n an>0, 2.8

thenM,0/,M∞, 0/,M∞,;

i4 ifSα,Tαq,the condition2.8is verified andHis nonoscillatory, thenM,0,

M

∞,0/,M∞,∅.

Theorems 2.1, 2.2 will be proved in the following sections. Observe that Theorem 2.1 is a discrete counterpart of14, Theorems 4, 6, 7 for1.3, even if the approach here used is completely different.

3. Unbounded solutions whenTαq<

In this section we study the growth of unbounded solutions of 1.1 whenTαq < ∞. The following holds.

Theorem 3.1. Assume

Sα<, Tαq<. 3.1

Then for1.1we haveM∞,0∅.

Proof. By contradiction, assume thatx∈M∞,0. Without loss of generality, letn0be large so that

n0min{q,0} ≥0 and

xn>0, xnq >0, Δxn>0, Δxnq >0 fornn0. 3.2

Setnqn0q; thenxnq> xnq forn > n0. By summation of1.1we obtain, forn > n0,

xn1 ∞

kn

bkxkq

α

3.3

and so

xnqxnq nq−1

knq

1 ak

1/αn

ik bixiq

α

in1

bixiq α

1

. 3.4

Putting

σα

1, if α≥1,

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that is, in view of3.12,

Sincex1 is decreasing, we have

γαxN1 −xn11xN1

The following result extends 3, Theorem 2 , where the existence of intermediate solutions has been proved forq≥0.

Theorem 3.2. (i1) Equation1.1has solutions in the classM∞,if and only ifTαq<. (i2) Equation1.1has solutions inM∞,0ifSαandTαq<.

Proof (outline). Ifq≥0,claimi1follows, for example, from6, Theorem 3 with minor changes

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and define the operatorT:Ω→Xgiven byTu y,where

and soTmapsΩinto itself. In virtue of the Ascoli theorem, any bounded set inXis relatively compact and so, becauseTΩ is bounded according to the topology of X, the compactness follows. Let{vk}be a sequence inΩ, converging on finite subsets ofNn

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4. Bounded solutions and proof ofTheorem 2.1

It is well-known that the existence of bounded solutions of1.1depends on the convergence of the seriesSα,and so the deviating argument does not play any role. This property follows, for example, from9, Theorem 4.2 or6, Theorem 2 , in which the caseq≥0 is considered, but the used argument can be easily modified for anyq∈Z. More precisely the following holds.

Proposition 4.1. Equation1.1has solutions in the classM,0if and only ifSα<.

Whenq 1,bounded solutions ofHare uniquely determined up to a constant factor. To prove this, we use a uniqueness result, stated in1, Theorem 1 , and the so-calledreciprocity principlesee, e.g.,11, Section 8.2.2 , which links solutions ofHwith ones of thereciprocal equationn≥1:

ΔBnΔyn1/αsgnΔynAnyn11/αsgnyn1 0, 4.1

where

Bn 1

bn−1

1/α, An 1

an1/α. 4.2

Indeed, let y be a solution of 4.1 and denote by y1 its quasidifference, that is yn1 Bnyn|1sgnΔyn.Then the sequencex, wherexny1

n , is a solution ofHand satisfies

xn1 yn, sgnynyn1 −sgnxnxn1. 4.3

Proposition 4.2. IfYaandSα <,then for any fixedc /0,Hhas a unique solutionx∈M,0

such thatlimnxnc.

Proof. First, observe thatYb<∞, becauseSα<.Consider4.1, then

n0

1 an

1

kn1

bk−1

1

n0

An

kn1

1 Bk

α1

<. 4.4

By applying1, Theorem 1 to4.1, there exists a unique solutionyof4.1such that limnyn 0, limnyn1 −c. Applying the reciprocity principle, H has a unique solutionx such that limnxncand limnxn1 0. Since1.2holds,x∈M,0.

Using the above results, we can prove our first main result.

Proof ofTheorem 2.1. The claims ik, k 1,2,4, follow from Theorems 3.1, 3.2 and Prop-osition4.1.

Claim i3. Let xbe the unique solution of H, defined for nN,satisfying x ∈ M,0 and

limnxn1. Letybe a solution ofHsuch thatyNxNandyN1 /xN1. Ify∈M,0,we have

lim

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In view of the homogeneity property, alsoz y∞−1y is a solution ofH, and limnzn 1, limnzn1 0. Then, fromProposition 4.2, we havezx,that isyyx.HenceyN yxN and soy∞ 1,which contradicts4.5. Thusy /∈M,0.Since1 ∞and all solutions ofH are nonoscillatory, fromTheorem 3.2the assertion follows.

In the proof of Theorem 2.1 we used the Sturm separation property saying that os-cillatory and nonosos-cillatory solutions cannot coexist for H. Nevertheless, when q /1, such a property can fail, as the following example shows.

Example 4.3. Consider the difference equations

Δ2xnbnxn

10, 4.6

Δ2ynbnyn

3 0, 4.7

where

bn2−6n−1224n622n31. 4.8

Since S1 < ∞, by Proposition 4.1 both equations have bounded nonoscillatory solutions.

Thus, because the Sturm separation property holds for 4.6, this equation has all solutions nonoscillatory. However4.7has the oscillatory solutiony{−1n2nn1}.Similarly,

Δ2znBnzn−

50, Bn3−10n25

3−4n−42·3−2n−11 4.9

has the oscillatory solutionz {−1n3−n2}and, again in view ofProposition 4.1, a bounded nonoscillatory solution, while the corresponding linear equation Δ2xnBnxn1 0 is

non-oscillatory, as it follows fromProposition 4.1and the Sturm separation property.

As far as we know in the literature criteria assuring that all solutions of1.1withq /1 are nonoscillatory are not available. This fact yields a strong difficulty to prove the existence of intermediate solutions of 1.1whenTαq ∞, q /1. These difficulties can be overcome by making a comparison result for intermediate solutions of1.1with q /1 andH, as it is described in the following section.

5. Comparison result and proof ofTheorem 2.2

Clearly, the convergence of the series Tαq depends on the deviating argument q. The following example illustrates this fact and shows how the presence of the deviating argument can modify the growth of nonoscillatory solutions.

Example 5.1. Let 0< α <1 and define the sequencesa, bso that

k

i0

1 ai

1

2k2, bk2−αk2 1

k1. 5.1

Hence

0 ∞

k1

bk k−1

i0

1 ai

1/αα

k1

1 k12

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while

1 ∞

k0

1 k12

−αk2

2αk2 ∞

k0

1

k1 ∞. 5.3

Moreover, if 0< X <1,we havei≥0

−ΔXi2Xi2−Xi12 Xi21−X2i−1>1−XXi2, 5.4

and so, takingX2−α, we obtain

ik

2−αi2 <β

ik

Δ2−αi2β2−αk2, 5.5

whereβ 1−2−α−1.Hence

k0

1 ak

1

ik bi

1

≤∞ k0

2k2

1 k1

1

ik 2−αi2

1

β1

k0

2k2

1 k1

1

2−k2 <.

5.6

Taking into account thatTαpTαqforpq, we have

Sα<, Tαq<∞ forq≤0, Tα1 ∞ 5.7

and so the case C3andC1occurs forHandH−forτ ≥ 1, respectively. Therefore, the

delayed argument changes the growth of unbounded solutions: all unbounded solutions of

Hare intermediate in virtue ofTheorem 2.1i3, while all unbounded solutions ofH−are

dominant for any delayτin virtue of Theorems3.1and3.2.

Now we state a comparison result for intermediate solutions of1.1.

Theorem 5.2. Assume2.8. If 1.1has solutions in the classM∞,0for a fixedq,then the same occurs for anyq.

Proof. Jointly with1.1, consider the nonlinear difference equations

ΔanΔynαsgnΔynbnxnq−1αsgnynq−10, 5.8 ΔanΔxnαsgnΔxnbnxnq1αsgnxnq10. 5.9

It is sufficient to prove that if M∞,0/∅for1.1, then the same holds for5.9and5.8. Put q min{0, q}.Letzbe a solution of1.1in the classM∞,0 and letn0 be a positive integer so

thatn0q≥1.Set

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Then

0≤n <nn0. 5.11

Without loss of generality, assumezi>0,zi1 >0 forinand

ai> h, 5.12

wherehis a positive constant. Sincez1 is positive decreasing fornn,we havez1

nzn1 for nn,that is,

zn1−zn

zn1

an 1

zn1 h

1

h1. 5.13

Summing twice1.1, we obtain, forn > n0,

znzn0

n−1

in0

1 ai

1

ki

bkzkq α

1

. 5.14

Step 1 M∞,0/∅ for 1.1 ⇒ M∞,0/∅ for 5.8. Denote by X the Fr´echet space of the real sequences defined fornn, endowed with the topology of convergence on finite subsets of Nn{n∈N, n≥n}and consider the setΩ⊂Xdefined by

Ω vvn ∈X:zn1≤vnMzn1 , 5.15

where

M1 h1 zn0

. 5.16

LetT:Ω→Xbe the map given by

Tvnzn1 if nnn0,

Tvnd n−1

in0

1 ai

1

ki

bkvkq−1

α 1

if nn01,

5.17

where

dzn0h1. 5.18

Letnnn0; clearly

zn1Tvn< Mzn1. 5.19

Now letn > n0.Sincenq−1≥n0q−1n,we have forv∈Ωandkn0

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Then, from5.14and5.20, we get

Tvnd n−1

in0

1 ai

1

ki

bkMzkq α

1

MznMzn0 d. 5.21

Since from5.16it resultsMzn0 zn0h1, from5.21we obtain

TvnMznzn0−h1dMzn< Mzn1. 5.22

Moreover, using again5.14and5.20, we obtain, forn > n0,

Tvnd n−1

in0

1 ai

1

ki

bkzkq α

1

znzn0dznh1, 5.23

that is, in view of5.13,

Tvnzn1. 5.24

Hence, from 5.19, 5.22, and 5.24 we have TΩ ⊂ Ω. Reasoning as in the proof of

Theorem 3.2, the continuity and compactness of T in Ω follows and so, by applying the

Tychonov fixed point theorem, there exists y such that y Ty. It is easy to verify that y is a solution of5.8for largenand, sincey∈Ω,we havey∈M∞,0,that is, the assertion.

Step 2 M∞,0/∅ for 1.1 ⇒ M∞,0/∅ for 5.9. Denote by X the Fr´echet space of the real sequences defined fornn, endowed with the topology of convergence on finite subsets of Nn {n∈N, n≥n}, and consider the setΩ⊂Xdefined by

Ω wwn ∈X:zn−1≤wnHzn−1 , 5.25

whereH >1 is a constant. LetT:Ω→Xbe the map given by

Twnzn−1 if nnn0,

Twnzn0

n−1

in0

1 ai

1

ki bk

wkq1

α 1

fornn01.

5.26

Letnnn0; clearly

zn−1TwnHzn−1. 5.27

Now letn > n0.Forkn01 it results thatkq1≥n0qn1nand so forw∈Ωand

kn01 :

zkqwkq1≤Hzkq. 5.28

Taking into account5.14and5.28, we have

Twnzn0

n−1

in0

1 ai

1

ki

bkzkq α

1

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Similarly, results forn > n0:

continuous and compact inΩ, by applying the Tychonov fixed point theorem, there existsx such thatxTx. It is easy to verify thatxis a solution of5.9fornlarge and, sincex∈Ω, we havex∈M∞,0,that is, the assertion.

Now we are able to proveTheorem 2.2.

Proof ofTheorem 2.2. Claimsi1,i2follow from Theorems3.1,3.2, andProposition 4.1.

We close this section by an example illustrating the role of the delayed argument, when ais rapidly varying at infinity.

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and so1 ∞and−1<.Using the inequalityin2−i22i2−n22n

,we obtain

≥ ∞

n0

1 an

1

2−n22n/α1 ∞

n1

22n/α−21. 5.35

Thus, for q ≤ −1 and any α, 1.1 satisfies the case C2 and so, by Theorem 2.2, it has

intermediate and dominant solutions. Observe that if q 1, the case C4 occurs, and,

by Theorem 2.1, the half-linear equation H is either oscillatory or all its solutions are intermediate. So, this example shows that ifqis negative, the caseC2can occur for anyα.

Moreover, whenα1 the linear equation

ΔanΔxn

bnxn10 5.36

is oscillatorysee, e.g.,10, Remark 1.11.9 , and the corresponding delayed linear equation

ΔanΔxnbnxn−τ 0, τ ∈N, 5.37

has, by Theorem 2.2, intermediate and dominant solutions. In comparison withExample 4.3, where the linear equation is nonoscillatory and the deviating argument may produce oscillatory solutions, in this case we have an opposite effect to the oscillation: the linear equation is oscillatory and the delay produces nonoscillatory solutions.

6. Conclusion and open problems

1 The role of the deviating argument. By Theorems 2.1, 2.2, the existence of subdominant solutions does not depend on the deviating argument q, the one of dominant solutions can depend onq. Especially because1−τ1≤1τ,we obtain a possible discrepancy concerning unbounded solutions of H and an equation with deviating argument. For in-stance, if the case C1 holds, H has dominant solutions and no intermediate solutions,

while it may occur thatHhas intermediate solutions and no dominant solutions. Similarly, the delayed argument may cause the opposite phenomena: if the case C3 holds, H has

intermediate solutions and no dominant solutions, while it may occur thatH−has dominant solutions and no intermediate solutions. Clearly, the deviating argument can produce also the oscillation, or nonoscillation, as Examples4.3and5.3show.

2Open problems. As we noticed inSection 4, the nonoscillation of all solutions of1.1 withq /1 is an open problem.

For this reason, whenTαqq /1, the existence of intermediate solutions has been obtained by means of a comparison result between H and 1.1, say Theorem 5.2. Such a result shows that the deviating argument does not have any influence on the existence of intermediate solutions, provided 2.8 holds. Especially, if the classical half-linear equation

H has intermediate solutions and2.8 holds, then also Hand H−have intermediate solutions for anyτ∈Z,τ ≥1.

If2.8is not satisfied,Theorem 5.2can fail, asExample 5.1illustrates. Is condition2.8 necessary for the validity of this theorem and, consequently, ofTheorem 2.2? By means of an argument similar to the one given in the proof ofTheorem 2.2i3we have that2.8yields that

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anyp, q ∈ Z. Now, the following question arises: is the statement of these theorems valid by assuming, instead of2.8, thatTαp,Tαqare both convergent or divergent?

3Future investigations. The future studies will be addressed to extend the results of this paper, especially those concerning the intermediate solutions, to Emden-Fowler-type equations of the form

ΔanΔxnαsgnΔxnbnxnqβsgnxnq0, α /β. 6.1

Acknowledgment

Supported by the Research Project 0021622409 of the Ministery of Education of the Czech Republic, and Grant no. 201/07/0145 of the Czech Grant Agency.

References

1 M. Cecchi, Z. Doˇsl´a, and M. Marini, “Nonoscillatory half-linear difference equations and recessive solutions,”Advances in Difference Equations, vol. 2005, no. 2, pp. 193–204, 2005.

2 M. Cecchi, Z. Doˇsl´a, M. Marini, and I. Vrkoˇc, “Summation inequalities and half-linear difference equations,”Journal of Mathematical Analysis and Applications, vol. 302, no. 1, pp. 1–13, 2005.

3 M. Cecchi, Z. Doˇsl´a, and M. Marini, “Intermediate solutions for nonlinear difference equations with p-Laplacian,” in Proceedings of the 11th International Conference on Difference Equations and Applications (ICDEA ’06), S. Elaydi, K. Nishimura, and M. Shishikura, Eds., Advanced Studies in Pure Mathematics, Kyoto, Japan, July 2006.

4 H. A. El-Morshedy and S. R. Grace, “Comparison theorems for second order nonlinear difference equations,”Journal of Mathematical Analysis and Applications, vol. 306, no. 1, pp. 106–121, 2005.

5 H.-F. Huo and W.-T. Li, “Oscillation of certain two-dimensional nonlinear difference systems,” Computers & Mathematics with Applications, vol. 45, no. 6–9, pp. 1221–1226, 2003.

6 W.-T. Li, “Classification schemes for nonoscillatory solutions of two-dimensional nonlinear difference systems,”Computers and Mathematics with Applications, vol. 42, no. 3–5, pp. 341–355, 2001.

7 P. ˇReh´ak, “Oscillatory properties of second order half-linear difference equations,” Czechoslovak Mathematical Journal, vol. 51, no. 2, pp. 303–321, 2001.

8 S. H. Saker, “Oscillation of second-order perturbed nonlinear difference equations,” Applied Mathematics and Computation, vol. 144, no. 2-3, pp. 305–324, 2003.

9 G. Zhang, S. S. Cheng, and Y. Gao, “Classification schemes for positive solutions of a second-order nonlinear difference equation,”Journal of Computational and Applied Mathematics, vol. 101, no. 1-2, pp. 39–51, 1999.

10 R. P. Agarwal, M. Bohner, S. R. Grace, and D. O’Regan,Discrete Oscillation Theory, Hindawi Publishing Corporation, New York, NY, USA, 2005.

11 O. Doˇsl ´y and P. ˇReh´ak,Half-Linear Differential Equations, vol. 202 ofNorth-Holland Mathematics Studies, Elsevier Science B.V., Amsterdam, The Netherlands, 2005.

12 R. P. Agarwal, S. R. Grace, and D. O’Regan, Oscillation Theory for Second Order Linear, Half-Linear, Superlinear and Sublinear Dynamic Equations, Kluwer Academic Publishers, Dordrecht, The Netherlands, 2002.

13 H. Hoshino, R. Imabayashi, T. Kusano, and T. Tanigawa, “On second-order half-linear oscillations,” Advances in Mathematical Sciences and Applications, vol. 8, no. 1, pp. 199–216, 1998.

14 M. Cecchi, Z. Doˇsl´a, and M. Marini, “On intermediate solutions and the Wronskian for half-linear differential equations,”Journal of Mathematical Analysis and Applications, vol. 336, no. 2, pp. 905–918, 2007.

References

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