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Volume 2008, Article ID 749392,15pages doi:10.1155/2008/749392

Research Article

Fixed Point Methods for the Generalized Stability

of Functional Equations in a Single Variable

Liviu C ˘adariu1 and Viorel Radu2

1Departamentul de Matematic˘a, Universitatea Politehnica din Timis¸oara, Piat¸a Victoriei no. 2, 300006 Timis¸oara, Romania

2Facultatea de Matematic˘a S¸i Informatic˘a, Universitatea de Vest din Timis¸oara, Bv. Vasile Pˆarvan 4, 300223 Timis¸oara, Romania

Correspondence should be addressed to Liviu C˘adariu,[email protected]

Received 4 October 2007; Accepted 14 December 2007

Recommended by Andrzej Szulkin

We discuss on the generalized Ulam-Hyers stability for functional equations in a single variable, including the nonlinear functional equations, the linear functional equations, and a generalization of functional equation for the square root spiral. The stability results have been obtained by a fixed point method. This method introduces a metrical context and shows thatthe stability is related to some fixed pointof a suitable operator.

Copyrightq2008 L. C˘adariu and V. Radu. 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 and preliminaries

The study of functional equations stability originated from a question of Ulam1940 concern-ing the stability of group homomorphisms is as follows.

LetG be a group endowed with a metric d.Givenε > 0,does there exist ak > 0such that for every functionf :GGsatisfying the inequality

dfx·y, fx·fy< ε, ∀x, y∈G, 1.1 there exists an automorphismaofG with

dfx, ax< kε, ∀x∈G? 1.2 In 1941, Hyers1gave an affirmative answer to the question of Ulam for Cauchy equa-tion in Banach spaces.

LetE1andE2be Banach spaces and let f:E1→E2be such a mapping that

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for allx, yE1and aδ >0, that is,fisδ-additive. Then there exists a unique additiveT :E1→E2,

which satisfies

fxTxδ, ∀xE1. 1.4

In fact, according to Hyers,

Tx lim

n→∞

f2nx

2n , ∀x∈E1. 1.5

For this reason, one says that the Cauchy equation isstable in the sense of Ulam-Hyers.

In2,3as well as in4–7, the stability problem with unbounded Cauchy differences is consideredsee also8,9. Their results include the following two theorems.

Theorem 1.1see1,2,4,7. Suppose thatEis a real-normed space,F is a real Banach space, and

f :EFis a given function, such that the following condition holds:

fxyfxfy

Fθ

xpEypE, ∀x, y∈E, 1p

for somep∈0,∞\ {1}andθ >0. Then there exists a unique additive functiona:EFsuch that

fxax

F

2θ 22px

p

E, ∀x∈E. 2p

Also, if for eachxEthe functiontftxfromRtoFis continuous for each fixedxE, thenais linear mapping.

It is worth mentioning that the proofs used the idea conceived by Hyers. Namely, the additive functiona:EFis constructed, starting from the given functionf, by the following formula:

ax lim

n→∞ 1 2nf

2nx, ifp <1, 2p<1

ax lim

n→∞2 nf

x

2n

, ifp >1. 2p>1

This method is calledthe direct method or Hyers’ method.

We also mention a result concerning the stability properties with unbounded control conditions invoking products of different powers of normssee5,6,10.

Theorem 1.2. Suppose thatE is a real-normed space,F is a real Banach space, and f : EF is a given function, such that the following condition holds

fxyfxfy

Fθx

p

E· y

q

E, ∀x, y∈E, 1p

for some fixedθ >0andp, q ∈Rsuch thatr pq / 1. Then there exists a unique additive function

L:EFsuch that

fxLx

F

θ 2r2x

r

E, ∀x∈E. 2p

If in additionf : EF is a mapping such that the transformationtftxis continuous int∈R,

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Generally, whenever the constant δ in 1.3is replaced by a control function x, yδx, ywith appropriate properties, as in3, one uses the generic termgeneralized Ulam-Hyers stabilityorstability in Ulam-Hyers-Bourgin sense.

In the general case, one uses control conditions of the form

Dfx, yδx, y 1.6

and thestability estimationsare of the form

fxSxεx, 1.7

whereSis a solution, that is, itverifies the functional equationDSx, y 0, and forεx, explicit

formulae are given, which depend on the controlδas well as on the equationDfx, y.

We refer the reader to the expository papers11,12or to the books13–15 see also the recent articles of Forti16,17, for supplementary details.

On the other hand, in18–25,a fixed point method was proposed, by showing that many theorems concerning the stability of Cauchy, Jensen, quadratic, cubic, quartic, and monomial functional equations are consequences of the fixed point alternative. Subsequently, the method has been successfully used, for example, in26–30. This method introduces a metrical context and shows thatthe stability is related to some fixed pointof a suitable operator.

The control conditions are responsible for three fundamental facts:

1thecontraction propertyof a Schr ¨oder-type operatorJ,

2the first two approximations,f andJf, to be at afinite distance,

3they force the fixed point ofJto be asolution of the initial equation.

Our main purpose here is to study the generalized stability for some functional equa-tions in a single variable. We prove the generalized Ulam-Hyers stability of the single variable equation

wfηfh. 1.8

As an application of our result for1.8, the stability for the following generalized functional equation of the square root spiral

fp−1px kfx hx 1.9

is obtained.

Thereafter, we present the generalized Ulam-Hyers stability of the nonlinear equation

fx Fx, fηx. 1.10

The main result is seen to slightly extend the Ulam-Hyers stability previously given in 31, Theorem 2. As a direct consequence of this result, the generalized Ulam-Hyers stability of the linear equationfx gx·fηx hxis highlighted. Notice that in all these equations,f

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Proposition 1.3cf.32or33. Suppose that a complete generalized metric spaceX, d(i.e., one for which d may assume infinite values) and a strictly contractive mapping A : XX with the Lipschitz constant L < 1 are given. Then, for a given element xX,exactly one of the following assertions is true:

A1dAnx, An1x ∞, for all n≥0;

A2there existsksuch thatdAnx, An1x<∞, for all nk.

Actually, ifA2holds, then

A21the sequenceAnxis convergent to a fixed pointyofA;

A22yis the unique fixed point ofAinY :{y∈X, dAkx, y<∞};

A23dy, y∗≤1/1−Ldy, Ay, for all yY.

2. A general fixed point method

Firstly we prove, by the fixed point alternative, a stability result for the single variable equation

wgηgh,where

i wis a Lipschitz self-mappingwith constantwof the Banach spaceY;

ii ηis a self-mapping of the nonempty setG;

iii h:GY is a given function;

ivthe unknown is a mappingg :GY, that leads to the following. Theorem 2.1. Suppose thatf:GY satisfies

wfηxfxhx

Yψx, ∀x∈G, Cψ

with some given mappingψ:G→0,. If there existsL <1such that

w·ψηxLψx, ∀x∈G, Hψ

then there exists a unique mappingc:GY which satisfies both the equation

wcηx cx hx, ∀x∈G, Eω,η

and the estimation

fxcx

Y

ψx

1−L, ∀x∈G. Estψ

Proof. Let us consider the setE:{g :GY}and introduce acomplete generalized metriconE

as usual, inf∅∞:

dg1, g2

g1, g2

infK∈R,g1xg2xYKψx, ∀x∈G . GMψ

Now, define thenonlinearmapping

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Step 1. Using the hypothesisHψit follows thatJ is strictly contractiveonE. Indeed, for any

g1, g2∈ Ewe have

dg1, g2

< Kg1xg2xYKψx, ∀x∈G, Jg1xJg2x

Y wg1◦η

xhxwg2◦η

xhxYw·g1

ηxg2

ηxY.

2.1

Therefore

Jg1xJg2x

Yw·K·ψ

ηxK·L·ψx, ∀x∈G, 2.2 so thatdJg1, Jg2≤LK,which implies

dJg1, Jg2

Ldg1, g2

, ∀g1, g2∈ E. CCL This says thatJis astrictly contractiveself-mapping ofE,with the constantL <1.

Step 2. df, Jf<∞. In fact, using the relationCψit results thatdf, Jf≤1.

Step 3. We can apply the fixed point alternative and we obtain the existence of a mapping

c:GY such that the following hold.

icis a fixed point ofJ, that is,

wcηx cx hx, ∀x∈G. Ew,η

The mappingcis the unique fixed point ofJin the set

F{g∈ E, df, g<∞}. 2.3

This says thatcis the unique mapping verifyingbothEw,ηand2.4, where

∃K <∞ such thatcxfxYKψx, ∀x∈G. 2.4

iidJnf, c −→

n→∞0,which implies

cx lim

n→∞J

nfx, ∀xG, 2.5

where

Jnfx wJn−1fηxhx

wwJn−2fη2xhηxhx, ∀x∈G, 2.6

whence

Jnf ωωωω· · ·ωωfηnhηn−1−hηn−2− · · ·−hη3−hη2−hηh.

2.7

iiiFinally,df, c≤1/1−Ldf, Jf,which implies the inequality

df, c≤ 1

1−L, 2.8

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Theorem 2.1extends our recent result in34, where the generalized stability in Ulam-Hyers sense was obtained for the equation

wgηg. 2.9

3. Applications to the generalized equation of the square root spiral

As a consequence ofTheorem 2.1, we obtain a generalized stability result for the equation

fp−1px kfx hx, ∀x∈G. 3.1

The “unknowns” are functions f : GY between two vector spaces while p, h are given functions, p−1 is the inverse of p, and k /0 is a fixed constant. The solution of 3.1 and a generalized stability result in Ulam-Hyers sense for the above equation are given in35, by the direct method.

A vector spaceGand a Banach spaceY will be considered.

Theorem 3.1. Let kG\ {0}and suppose thatp : GG is bijective andh : GY is a given mapping. Iff :GY satisfies

f

p−1px kfxhxYψx, ∀x∈G, Sψ

with a mapping:ψ :G→0,for which there existsL <1such that

ψp−1px kxLψx, ∀x∈G, Hψ,p

then there exists a unique mappingc:GY which satisfies both the equation

cp−1px kcx hx, ∀x∈G, Ep,h

and the estimation

fxcx

Y

ψx

1−L, ∀x∈G. Estψ

Moreover,

cx lim

n→∞

fp−1px nk

n−1

i0

hp−1px ik

, ∀x∈G. 3.2

Proof. We applyTheorem 2.1, withw:YY, η:GG, ψ :G→0,∞,

wx:x, ηx:p−1px k. 3.3

Clearly,lw1 andJgx:gp−1px khx.

By usingSψand the hypothesisHψ,p, we immediately see thatCψandHψhold.

Since

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then

Jnfx

fp−1px nk

n−1

i0

hp−1px ik

, 3.5

whence there exists a unique mappingc:GY,

cx: lim

n→∞

Jnfx, ∀x∈G, 3.6

which satisfies the equationJcx cx,that is,

cp−1px kcx hx, ∀x∈G, 3.7

and the inequality

fxcx

Y

ψx

1−L, ∀x∈G. 3.8

A special caseof3.1is obtained for k1, px xn, n≥2,andhx arctan1/x. It is the so-called “nth root spiral equation”

fnxn1fx arctan1

x. 3.9

As a consequence ofTheorem 3.1, we obtain the following generalized stability result for the above equation.

Theorem 3.2. Iff :R→Rsatisfies

fnxn1fxarctan 1

x

ψx, ∀x∈R, 3.10

with some fixed mappingψ:R→0,and there existsL <1such that

ψnxn1x, ∀xR, 3.11

then there exists a unique mappingc:R→R,

cx lim

m→∞

n

xnmm−1

i0

arctan√n 1

xni

, ∀x∈R, 3.12

which satisfies both3.9and the estimation

fxcx ψx

1−L, ∀x∈R. 3.13

Notice that forn 2, Jung and Sahoo36 proved in 2002 a generalized Ulam-Hyers stability result for the functional equation3.9, by using the direct method.

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Corollary 3.3. Iff :R→ Rsatisfies

fnxn1fxarctan1

x

axn, ∀x∈R, 3.14

with some fixed0< a <1, then there exists a unique mappingc:R→R,

cx lim

m→∞

n

xnmm−1

i0

arctan√n 1

xni

, ∀x∈R, 3.15

which satisfies both3.9and the estimation

fxcx axn

1−a, ∀x∈R. 3.16

Proof. We apply Theorem 3.2, by choosing ψx axn

0 < a < 1, n ∈ N. It is clear that the relation3.11holds, withLa <1.

Remark 3.4. A similar result of stability as inCorollary 3.3can be obtained for a control map-pingψ:R→0,, ψx 1/axn a >1, n∈N. The estimation relation3.16becomes

fxcx a1−xn

a−1, ∀x∈R. 3.17

4. The generalized Ulam-Hyers stability of a nonlinear equation

The Ulam-Hyers stability for the nonlinear equation

fx Fx, fηx 4.1

was discussed by Baker31. The “unknowns” are functionsf : GY,between two vector spaces. In this section, we will extend the Baker’s result and we will obtain the generalized stability in Ulam-Hyers sense for4.1, by using the fixed point alternative.

Let us consider a nonempty setGand a complete metric spaceY, d. Theorem 4.1. Letη:GG, g:G→R(orC) andF :G×YY. Suppose that

dFx, u, Fx, vgx·du, v, ∀x∈G, ∀u, v∈Y. 4.2

Iff :GY satisfies

dfx, Fx, fηxψx, ∀x∈G, 4.3

with a mappingψ :G→0,for which there existsL <1such that

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then there exists a unique mappingc:GY which satisfies both the equation

cx Fx, cηx, ∀x∈G, 4.5

and the estimation

dfx, cxψx

1−L, ∀x∈G. 4.6

Moreover,

cx lim

n→∞F

x, FFηx, . . . , Fηx,fηnηx, ∀x∈G. 4.7

Proof. We use the same method as in the proof ofTheorem 2.1, namely,the fixed point alternative. Let us consider the setE: {h:GY}and introduce acomplete generalized metriconE

as usual, inf∅∞:

ρh1, h2

infK∈R, dh1x, h2xKψx, ∀x∈G . 4.8

Now, define the mapping

J :E −→ E, Jhx:Fx, hηx. 4.9

Step 1. Using the hypothesis in4.2and4.4it follows thatJis strictly contractiveonE. Indeed, for anyh1, h2∈ Ewe have

ρh1, h2

< Kdh1x, h2xKψx, ∀x∈G, dJh1x, Jh2xdFx, h1

ηx, Fx, h2

ηxgx·dh1

ηx, h2

ηxK·gx·ψηx.

4.10

Therefore

dJh1x, Jh2xK·gx·ψηxK·L·ψx, ∀x∈G, 4.11

so thatρJh1, Jh2≤LK,which implies

ρJh1, Jh2

Lρh1, h2

, ∀h1, h2∈ E. 4.12

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Step 3. We can apply the fixed point alternativeseeProposition 1.3, and we obtain the exis-tence of a mappingc:GY such that the following hold.

icis a fixed point ofJ, that is,

cx Fx, cηx, ∀x∈G. 4.13 The mappingcis the unique fixed point ofJin the set

Fh∈ E, ρf, h<. 4.14

This says thatcis the unique mapping verifyingboth4.13and4.15where

∃K <∞ such thatdcx, fxKψx, ∀x∈G. 4.15

iiρJnf, c −→

n→∞0,which implies

cx lim

n→∞J

nfx, ∀xG, 4.16

where

Jnfx Fx,Jn−1fηx

Fx, Fηx,Jn−2fηx, ∀x∈G, 4.17

hence

Jnfx Fx, FFηx, . . . Fηx,fηnηx. 4.18

iiiρf, c≤1/1−Lρf, Jf,which implies the inequality

ρf, c≤ 1

1−L, 4.19

that is,4.6holds.

As a direct consequence of Theorem 4.1, the following Ulam-Hyers stability resultcf.

31, Theorem 2or37, Theorem 13for the nonlinear equation4.1is obtained.

Corollary 4.2. LetG be a nonempty set and let Y, dbe a complete metric space. Let η : GG,

F :G×YY, and0≤L <1. Suppose that

dFx, u, Fx, vL·du, v, ∀x∈G, ∀u, v∈Y. 4.20 Iff :GY satisfies

dfx, Fx, fηxδ, ∀x∈G, 4.21 with a fixed constantδ > 0, then there exists a unique mappingc : GY which satisfies both the equation

cx Fx, cηx, ∀x∈G, 4.22 and the estimation

dfx, cxδ

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Moreover,

cx lim

n→∞F

x, FFηx, . . . , Fηx,fηnηx, ∀x∈G. 4.24

Proof. It follows byTheorem 4.1, by choosingψx δ >0. Example 4.3. If in4.1we considerF :R×1,∞→1,,

Fx, u ⎧ ⎨ ⎩

u1/p, ifp >1,

up, if 0< p <1, 4.25

we obtain the equation of B ¨ottcher:

fηx1/pfx, p >1, or fηxpfx, 0< p <1. 4.26

Agarwal et al. proved in37, Theorem 14that the above equations are stable in Ulam-Hyers sense, by using the result of Baker31, with

L ⎧ ⎪ ⎨ ⎪ ⎩ 1

p, ifp >1, p, if 0< p <1.

4.27

It is worth noticing that our formula4.24gives the solutions c of4.26:

cx ⎧ ⎪ ⎨ ⎪ ⎩

lim

n→∞

fηnx1/pn, ifp >1,∀xR,

lim

n→∞

fηnxpn, if 0< p <1, ∀xR. 4.28

5. The generalized Ulam-Hyers stability of a linear functional equation

In this section, we emphasize the importance ofTheorem 4.1. In fact, if

Fx, fηxgx·fηxhx, 5.1

equation4.1becomes

fx gx·fηxhx, 5.2

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Theorem 5.1. Consider Ga nonempty set and Y a real (or complex) Banach space. Suppose thatη :

GG, g:G→R(orC). Iff:GY satisfies

fxgxf

ηxhxYψx, ∀x∈G, 5.3

with some fixed mappingψ:G→0,and there existsL <1such that

|gx|ψηxLψx, ∀x∈G, 5.4

then there exists a unique mappingc:GY,

cx hx lim

n→∞

fηnx·

n−1

i0

gηix

n−2

j0

hηj1x·

j

i0

gηix

, 5.5

for allxG,which satisfies both the equation

cx gx·cηxhx, ∀x∈G, 5.6

and the estimation

fxcxYψx

1−L, ∀x∈G. 5.7

Proof. We consider in Theorem 4.1 the metric d on Y, given by du, v ||u−v||Y and the function

Fx, fηx:gxfηxhx, ∀x∈G, 5.8

withg, η, has in hypothesis ofTheorem 5.1. The relation4.2holds with equality. Applying

Theorem 4.1, there exists a unique mapping c which satisfies 5.2and the estimation 5.7. Moreover,

cx lim

n→∞J

nfx, ∀xG, 5.9

where

Jnfx gx·Jn−1fηxhx

gx·gηx·Jn−22xgx·hηxhx, ∀x∈G, 5.10

whence, for allxG,

Jnfx:hx fηnx·

n−1

i0

gηix

n−2

j0

hηj1x·

j

i0

gηix

. 5.11

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Corollary 5.2. Consider a nonempty set G and a real (or complex) Banach space Y. Suppose that

η:GG, g :G→R(orC), andh:GY are given. Iff :GY satisfies

fxgxf

ηxhxYδ, ∀x∈G, 5.12

with a fixed constantδ >0and there existsL <1such that

|gx| ≤L, ∀x∈G, 5.13

then there exists a unique mappingc:GY,

cx hx lim

n→∞

fηnx·

n−1

i0

gηix

n−2

j0

hηj1x·

j

i0

gηix

, 5.14

for allxG,which satisfies both the equation

cx gx·cηxhx, ∀x∈G, 5.15

and the estimation

fxcx

Y

δ

1−L, ∀x∈G. 5.16

Remark 5.3. It is easy to see that3.1is a particular case of5.2. To prove this, it is sufficient to consider in5.2g ≡1,h:−h1,ηx:p−1px k, ∀x∈G, withpbijective onGandk /0

a fixed constant. By using the above notations,Theorem 3.1can be obtained as a consequence ofTheorem 5.1, with

cx hx lim

n→∞

fηnx·

n−1

i0

gηix

n−2

j0

hηj1x·

j

i0

gηix

−h1x lim

n→∞

fpp−1x nk

n−1

i1

h1

pp−1x ik

lim

n→∞

fp−1px nk

n−1

i0

h1

p−1px ik

, ∀x∈G.

5.17

Acknowledgment

The authors would like to thank the referees and the editors for their help and suggestions in improving this paper.

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