• 検索結果がありません。

VALUE PROBLEMS VIA FIXED POINT INDEX FOR WEAKLY INWARD A-PROPER MAPS

N/A
N/A
Protected

Academic year: 2022

シェア "VALUE PROBLEMS VIA FIXED POINT INDEX FOR WEAKLY INWARD A-PROPER MAPS"

Copied!
9
0
0

読み込み中.... (全文を見る)

全文

(1)

VALUE PROBLEMS VIA FIXED POINT INDEX FOR WEAKLY INWARD A-PROPER MAPS

GENNARO INFANTE

Received 23 November 2003 and in revised form 2 November 2004

We use the theory of fixed point index for weakly inwardA-proper maps to establish the existence of positive solutions of some second-order three-point boundary value prob- lems in which the highest-order derivative occurs nonlinearly.

1. Introduction

In the present paper, we discuss the existence of positive solutions of the nonlinear three- point boundary value problem (BVP)

u(t)=f(t,u,u,u), t(0, 1), (1.1) with the nonlocal boundary conditions (BCs)

u(0)=0, αu(η)=u(1), 0< η <1,αη <1, (1.2) in which the second derivative may occur nonlinearly.

Positive solutions for the case f(t,u,u,u)=g(t)h(u) have been studied by Ma [15]

and Webb [20,21], when f(t,u,u,u)=h(t,u) by He and Ge [5] and also by Lan [11].

The case f(t,u,u,u)=g(t)h(u,u) has been studied by Feng [4]. The results in [4,15]

are obtained by means of Krasnosel’ski˘ı’s theorem [8], the ones in [5] use Leggett and Williams’ theorem [14] and the results in [11,20,21] are achieved via the classical fixed point index for compact maps, see for example [1].

Lafferriere and Petryshyn [9] and Cremins [2] studied existence of positive solutions of the so-called Picard boundary value problem

u(t)=f(t,u,u,u), (1.3)

with BCs

u(0)=u(1)=0, (1.4)

Copyright©2005 Hindawi Publishing Corporation Fixed Point Theory and Applications 2005:2 (2005) 177–184 DOI:10.1155/FPTA.2005.177

(2)

by means of fixed point index theory forA-proper maps. A key restriction in [2,9] is that f must take positive values. Lan and Webb [13] improved the results of [2,9] by allowing f to possibly take some negative values.

Here we will exploit Lan and Webb’s theory [12] of fixed point index for weakly inward A-proper maps, to prove new results on the existence of positive solutions of the BVP (1.1)-(1.2).

We mention that with very little change, this technique may be applied to a variety of BCs, (e.g., other three-point BCs [6,7], orm-point BCs [16]), but for brevity, we refrain from discussing other cases.

2. Preliminaries

Let X denote an infinite-dimensional Banach space endowed with a fixed projection schemeΓ= {Xn,Pn}, where{Xn}is a sequence of finite-dimensional subspaces ofXand Pn:XXn is a linear projection withPnxx for every xX. We recall below the concept ofA-proper mapping, introduced by Petryshyn, and we refer to his book [18]

for further information on projection schemes, properties, and applications ofA-proper maps.

Definition 2.1. Given a mapT:DXX,T is said to beA-proper at a point yX relative toΓif

Tn:=PnT:DXn−→Xn (2.1)

is continuous for eachnNand if{xnj|xnjXnj}is a bounded sequence such that PnTxnj

y−→0 asj−→ ∞, (2.2)

there exists a subsequence{xnj(k)}of{xnj}andxXsuch thatxnj(k)xandT(x)=y.T isA-proper on a setKif it isA-proper at all points ofK.A-proper alone meansA-proper onX.

In a similar way, for a fixedγ0,T is said to bePγ-compactat a pointyXwith respect toΓifλIT is A-proper at yfor each λdominatingγ (i.e.,λγ ifγ >0 and λ >0 ifγ=0).Tis said to bePγ-compact on a setKif it isPγ-compact at all points ofK.

We recall the definitions of weakly inward set and map, see for example [3].

Definition 2.2. LetKbe a closed convex set inX. ForxKthe set IK(x)=

x+c(zx) :zK,c0 (2.3)

is called theinwardset ofx relative toK. The closure ofIK(x),IK(x) is said to be the weakly inwardset ofxrelative toK.

(3)

Geometrically, the inward setIK(x) is the union of all rays beginning atxand passing through some other point ofK.

Recall thatK is called awedgeifλxK forxK andλ0. If, furthermore,K (K)= {0}, we say thatKis acone.

Definition 2.3. Given a mapT:ΩKK,Tis said to beinwardonΩrelative toKif TxIK(x) forxΩ. IfTxIK(x) forxΩ,Tis said to beweakly inward.

We recall the definition ofk-semicontractive map.

Definition 2.4. Let D be a nonempty subset of X. A map A:DX is said to be k- semicontractivemap with constantk0 if there exists a mapV:D×DX such that the following conditions hold.

(S1) For each fixedxD,V(x,·) :DXis compact.

(S2) For eachyD, the mapV(·,y) :DXis a Lipschitz map with Lipschitz con- stantk.

(S3)A(x)=V(x,x) forxD.

Lan and Webb [12] defined a fixed point index for weakly inwardA-proper maps, which has the usual properties of the classical fixed point index, that is, existence, nor- malization, additivity, and homotopy invariance.

In this paper, we focus on some applications of this theory. Throughout the following, Kis a cone. We setKr= {xK:x< r}andKr= {xK:xr}.

First we state a lemma which implies that the fixed point index,iK(T,Kr), is 1. This uses the well-known Leray-Schauder condition.

Lemma2.5 (see [12]). Assume thatT:KrX is weakly inward,P1-compact onK, and satisfies

(LS)x=tT(x)forx =randt[0, 1).

ThenThas a fixed point inKr. Furthermore, ifx=T(x)forx =r, theniK(T,Kr)= {1}. Now we give a condition which ensures that the fixed point index is 0.

Lemma2.6 (see [12]). Assume thatT:KrX is weakly inward,P1-compact onK, and T(Kr)is bounded. Suppose thatx=Txforx =r, and

(E)there existseK\ {0}such thatx=Tx+λeforx =randλ >0.

TheniK(T,Kr)= {0}.

These conditions imply the following theorem.

Theorem2.7 (see [12]). LetT:KrXbe weakly inward,P1-compact onK, withT(Kr) bounded. Suppose the following conditions are satisfied:

(LS)there existsρ(0,r)such thatx=tTxforx =ρand0t <1, (E)there existseK\ {0}such thatx=Tx+λeforx =randλ >0.

ThenT has a fixed point inKr\Kρ. The same conclusion remains valid if (LS)holds for x =rand(E)holds forx =ρ.

One benefit of such type or result, as compared with the well-known Krasnosel’ski˘ı theorem, is that we do not require the cone to be sent into itself, but into a larger set.

(4)

3. Applications to three-point BVPs

In this section, we consider the existence of positive solutions of BVP

u(t)=f(t,u,u,u), t(0, 1), (3.1) with boundary conditions

u(0)=0, αu(η)=u(1), 0< η <1,αη <1. (3.2) We restrict our attention to the case 1 +αη22αη.

In order to apply the results ofSection 2, we set c1=1

8

1αη2 1αη

2

, c2=1 2

12αη+αη2 1αη

, c3=1 2

1αη2 1αη

, (3.3)

see (3.9) and (3.10) for the interpretation of these constants.

We make the following assumptions onf:

(C1) there existsr >0 such that f : [0, 1]×[0,c1r]×[c2r,c3r]×[r, 0]Ris a con- tinuous function,

(C2) there existsk(0, 1) such that|f(t,u,v,s1)f(t,u,v,s2)| ≤k|s1s2|fort [0, 1],u[0,c1r],v[c2r,c3r], ands1,s2[0,r],

(C3) f(t,u,v, 0)0 fort[0, 1],u[0,c1r], andv[c2r,c3r], (C4) f(t,u,v,r)rfort[0, 1],u[0,c1r], andv[c2r,c3r],

(C5) there exists ρ(0,r) such that f(t,u,v,ρ)ρ fort[0, 1], u[0,c1r] and v[c2r,c3r].

Remark 3.1. As in [13], we point out that condition (C3) is weaker than the usual posi- tivity requirement for f(t,u,v,s). If f is not positive, the standard theory of fixed point index cannot be applied since it needs the cone to be sent back into itself (see, e.g., [18]).

Furthermore, we stress that weakly inward fixed point index only exists in nonreflexive spaces usingA-proper theory, even for compact maps.

With respect to the alternative method of “solving” (1.1) for the highest-order de- rivative by means of the contractive hypothesis (C2), the reader might find interesting comments in [19,22].

For these reasons, we employ Lan and Webb’s theory for weakly inwardA-proper maps [12].

We work inX=C[0, 1], the space of continuous functions on [0, 1] with the usual maximum norm and use the projection schemeΓ= {Xn,Pn}associated with the standard Schauder basis [17]. We use the cone of positive functions

K=

uC[0, 1] :u(t)0 fort[0, 1]. (3.4) It is known thatPnKK.

We recall the following result which is a consequence of [3, Lemma 18.2].

(5)

Lemma3.2 (see [10]). LetX=C[0, 1]andKas above. TakeuKand define E(u)=

t[0, 1] :u(t)=0. (3.5)

Then,

(1)ifE(u)= ∅, that is,u(t)>0for everyt[0, 1], or equivalently,uis an interior point ofK, thenIK(u)=X,

(2)ifE(u)= ∅, that is,u∂K, then the set{vX:v(t)0fortE(u)}is a subset of IK(u), that is, if the values ofvare nonnegative at all points at which the values ofu are zero, thenvbelongs to the weakly inward setIK(u)ofu.

We can now state a theorem for the positive solutions of (3.1)-(3.2).

Theorem3.3. Assume that the conditions (C1)–(C5) hold. Then (3.1)-(3.2) has a positive solutionvwithρvr.

Proof. LetU= {uC2[0, 1] :u(0)=0, αu(η)=u(1)}. Define a mapL:UXbyLu=

u. ThenLis a linear isomorphism and L1v(t)=

1

0k(t,s)v(s)ds, (3.6)

where

k(t,s)= 1

1αηt(1s)

αt

1αηs), sη 0, s > η

ts, st,

0, s > t. (3.7) We define a continuous mapT:KrXby

Tv(t)=f

t,L1v, d

dtL1v,v

, (3.8)

whereKr= {uK:u< r}. By direct calculation, it may be shown that

tmax[0,1]

1

0k(t,s)ds=c1. (3.9)

So ifvKr, then 0L1v(t)c1r. Also by routine calculations, it may be shown that if vKr, then

c2r d

dtL1v(t)c3r. (3.10)

Therefore,Tis well defined and (C1) implies thatTis continuous.

To show thatTisP1-compact, one studies the mapV:Kr×KrXdefined by V(u,v)= f

t,L1v, d

dtL1v,u

. (3.11)

(6)

Then by (C2),V(u,·) is Lipschitz with constantkand, sinceL1and (d/dt)L1are com- pact,V(·,v) is compact. These conditions imply thatVis ak-semicontraction withk <1, and henceTu=V(u,u) isPγ-compact for everyγ(k, 1). For the proof of this assertion, we refer to [18], see also [13].

To prove thatTis weakly inward relative toK, letv∂K, that is, E(v)=

t[0, 1] :v(t)=0= ∅. (3.12) Then (Tv)(t)= f(t,L1v, (d/dt)L1v, 0) for everytE(v). It follows from (C3) that

(Tv)(t)0 for everytE(v). (3.13)

UsingLemma 3.2, we see thatTvIK(v) and soTis weakly inward.

We show thatTsatisfies the condition (LS) inTheorem 2.7, that is,v=λTvforv∂Kr

andλ(0, 1). In fact, if not, there existv0∂Krandλ0(0, 1) such thatv0=λTv0. Let t0[0, 1] be such thatv0(t0)=r. Then by (C4), we have

r=v0

t0

=λ0f

t0,L1vt0

, d dtL1vt0

,r

λ0r < r, (3.14) a contradiction.

Finally, we prove thatT satisfies the condition (E) inTheorem 2.7withe(t)1 for t[0, 1], that is,v=T y+βeforv∂Kρandβ >0. In fact, if not, there existv0∂Kρ

andβ0>0 such thatv0=Tv0+β0e. Lett0[0, 1] be such thatv0(s)= v0 =ρ. Then we have

ρ=f

t0,L1vt0

, d dtL1vt0

+β0eρ+β0e > ρ, (3.15) a contradiction.

It follows fromTheorem 2.7thatThas a fixed pointvKsatisfyingρvr.

Takeu=L1v, thenuis a positive solution of (3.1)-(3.2).

Example 3.4. The functionf(t,u,u,u)3/4 cos(u) withr=πandρ=π/6 shows that the class of maps that satisfies the conditions (C1)–(C5) is nonempty.

Remark 3.5. In order to show the existence of two solutions viaTheorem 2.7, one would be tempted to require the following (this is a standard argument in fixed point index theory):

(C6) there exists ˜ρ(0,ρ) such that f(t,u,v,ρ)˜ ρ˜fort[0, 1],u[0,c1r] andv [0,r].

This would provide the existence of ˜vK satisfying ˜ρv˜ρ. However, as noted in [13, Remark 4.3], it is impossible to simultaneously satisfy (C2), (C5), and (C6).

This error occurred in [2,9], when the authors discussed the existence of one positive solution of the Picard BVP.

(7)

Remark 3.6. For the case 1 +αη2<2αη, which occurs only whenα >1, the value of the constantc1given in (3.9) has to be replaced by

tmax[0,1]

1

0k(t,s)ds=1 2

αη(1η) 1αη

. (3.16)

This is because the constantmon [21, page 914] should read

m=

8(1αη)2

1αη22 if 1 +αη22αη, 2(1αη)

αη(1η) if 1 +αη2<2αη.

(3.17)

A similar result toTheorem 3.3holds in this case for (the new)c1. Acknowledgments

The author thanks Professor J. R. L. Webb for valuable discussions and suggestions, in particular, for pointing out the misprint in [21]. The author would also like to thank both referees for their helpful and constructive comments.

References

[1] H. Amann,Fixed point equations and nonlinear eigenvalue problems in ordered Banach spaces, SIAM Rev.18(1976), no. 4, 620–709.

[2] C. T. Cremins,Existence theorems for semilinear equations in cones, J. Math. Anal. Appl.265 (2002), no. 2, 447–457.

[3] K. Deimling,Nonlinear Functional Analysis, Springer, Berlin, 1985.

[4] W. Feng,Solutions and positive solutions for some three-point boundary value problems, Discrete Contin. Dyn. Syst.2003(2003), suppl., 263–272.

[5] X. He and W. Ge,Triple solutions for second-order three-point boundary value problems, J. Math.

Anal. Appl.268(2002), no. 1, 256–265.

[6] G. Infante,Eigenvalues of some non-local boundary-value problems, Proc. Edinburgh Math. Soc.

(2)46(2003), no. 1, 75–86.

[7] G. Infante and J. R. L. Webb,Loss of positivity in a nonlinear scalar heat equation, to appear in Nonlinear Differential Equations Appl.

[8] M. A. Krasnosel’ski˘ı,Positive Solutions of Operator Equations, P. Noordhoff, Groningen, 1964.

[9] B. Lafferriere and W. V. Petryshyn,New positive fixed point and eigenvalue results forPγ-compact maps and some applications, Nonlinear Anal.13(1989), no. 12, 1427–1440.

[10] K. Q. Lan,Theories of fixed point index and applications, Ph.D. thesis, Unversity of Glasgow, Glasgow, 1998.

[11] ,Multiple positive solutions of three point boundary value problems with singularities, to appear in J. Dynam. Differential Equations.

[12] K. Q. Lan and J. R. L. Webb,A fixed point index for weakly inwardA-proper maps, Nonlinear Anal.28(1997), no. 2, 315–325.

[13] , A-properness of contractive and condensing maps, Nonlinear Anal. Ser. A: Theory Methods49(2002), no. 7, 885–895.

[14] R. W. Leggett and L. R. Williams,Multiple positive fixed points of nonlinear operators on ordered Banach spaces, Indiana Univ. Math. J.28(1979), no. 4, 673–688.

(8)

[15] R. Ma,Positive solutions of a nonlinear three-point boundary-value problem, Electron. J. Differ- ential Equations1999(1999), no. 34, 1–8.

[16] ,Positive solutions of a nonlinearm-point boundary value problem, Comput. Math. Appl.

42(2001), no. 6-7, 755–765.

[17] J. T. Marti,Introduction to the Theory of Bases, Springer Tracts in Natural Philosophy, vol. 18, Springer, New York, 1969.

[18] W. V. Petryshyn,Approximation-Solvability of Nonlinear Functional and Differential Equations, Monographs and Textbooks in Pure and Applied Mathematics, vol. 171, Marcel Dekker, New York, 1993.

[19] J. R. L. Webb,Topological degree andA-proper operators, Linear Algebra Appl.84(1986), 227–

242.

[20] ,Positive solutions of some three point boundary value problems via fixed point index theory, Nonlinear Anal.47(2001), no. 7, 4319–4332.

[21] ,Remarks on positive solutions of some three point boundary value problems, Discrete Contin. Dyn. Syst.2003(2003), suppl., 905–915.

[22] J. R. L. Webb and S. C. Welsh,Existence and uniqueness of initial value problems for a class of second-order differential equations, J. Differential Equations82(1989), no. 2, 314–321.

Gennaro Infante: Dipartimento di Matematica, Universit`a della Calabria, 87036 Arcavacata di Rende, Cosenza, Italy

E-mail address:[email protected]

(9)

Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

mts.hindawi.com/according to the following timetable:

Manuscript Due March 1, 2009 First Round of Reviews June 1, 2009 Publication Date September 1, 2009

Guest Editors

Edson Denis Leonel,Department of Statistics, Applied Mathematics and Computing, Institute of Geosciences and Exact Sciences, State University of São Paulo at Rio Claro, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil; [email protected]

Alexander Loskutov,Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

Hindawi Publishing Corporation http://www.hindawi.com

参照

関連したドキュメント

We establish generic well-posedness of certain null and fixed point problems for ordered Banach space-valued continuous mappings.. The notion of well-posedness is of great importance

O’Regan, “A Lefschetz fixed point theorem for admissible maps in Fr´echet spaces,” Dynamic Systems and Applications, vol.. G ´orniewicz, Topological Fixed Point Theory of

Some common fixed point theorems for weakly commuting, compatible, δ-compatible and weakly compatible mappings under different contractive conditions in metric spaces have appeared

Using the theory of coincidence degree, we establish existence results of positive solutions for higher-order multi-point boundary value problems at resonance for ordinary

We establish generic well-posedness of certain null and fixed point problems for ordered Banach space-valued continuous mappings.. The notion of well-posedness is of great importance

In section 2, fixed point methods, in particular a nonlinear alternative of Leray-Schauder typc, will be used to establish existence principles for (1.1) with the various

Motivated and inspired by results of papers [5, 6, 14], we established some new common fixed point theorems for weakly compatible mappings in fuzzy metric spaces by using the

The intent of this paper is to define the concept of R-weakly commuting maps of the type (P) in this newly defined space and prove a common fixed theorem for R-weakly commuting