• 검색 결과가 없습니다.

In this paper, we investigate the stability of a quadratic- cubic-quartic functional equation f (x + ky

N/A
N/A
Protected

Academic year: 2022

Share "In this paper, we investigate the stability of a quadratic- cubic-quartic functional equation f (x + ky"

Copied!
10
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

Volume 33, No. 1, February 2020 http://dx.doi.org/10.14403/jcms.2020.33.1.9

STABILITY OF A QUADRATIC-CUBIC-QUARTIC FUNCTIONAL EQUATION

Yang-Hi Lee

Abstract. In this paper, we investigate the stability of a quadratic- cubic-quartic functional equation

f (x + ky) + f (x − ky) − k2f (x + y) − k2f (x − y)

− 2(1 − k2)f (x) −k2(k2− 1)

6 (f (2y) + 2f (−y) − 6f (y)) = 0 by applying the direct method in the sense of G˘avruta.

1. Introduction

In this paper, let V and W be real vector spaces, Y be a real Banach space and k ∈ R\{0, ±1}. For a given mapping f : V → W with f (0) = 0, we use the following abbreviations

fo(x) := f (x) − f (−x)

2 , fe(x) := f (x) + f (−x)

2 ,

Df (x, y) :=f (x + ky) + f (x − ky) − k2f (x + y) − k2f (x − y)

− 2(1 − k2)f (x) − k2(k2− 1)

6 (f (2y) + 2f (−y) − 6f (y)) Jnf (x) :=fo(2nx)

8n + 16fe(2nx) − fe(2n+1x) 12 · 4n

−4fe(2nx) − fe(2n+1x) 12 · 16n , Jn0f (x) :=8nfo

x 2n



+4 · 16n− 4n

3 fe

x 2n



−16n+1− 4n+2

3 fe x 2n+1



Received July 23, 2019; Accepted December 21, 2019.

2010 Mathematics Subject Classification: Primary 39B82, 39B52.

Key words and phrases: generalized Hyers-Ulam stability, quadratic-cubic-quartic functional equation, quadratic-cubic-quartic mapping.

(2)

for all x, y ∈ V and all n ∈ N∪{0}. Gordji et al. [3] proved the stability of the quadratic-cubic-quartic functional equation Df (x, y) = 0 for a fixed k ∈ Z\{0, ±1}. For the terminology “quadratic-cubic-quartic functional equation”, refer to the papers [2, 3]. This author [5] proved the stability of the functional equation Df (x, y) = 0 for the case k = 2 by using the fixed point theory, and also showed the Hyers-Ulam-Rassias stability of the quadratic-cubic-quartic functional equation

f (x + ky) + f (x − ky) − k2f (x + y) − k2f (x − y)

+ 2(k2− 1)f (x) + (k2+ k3)f (y) + (k2− k3)f (−y) − 2f (ky) = 0 [6]. In this paper, we will prove the stability of the functional equation Df (x, y) = 0 in the sense of G˘avruta [1] (See also [4, 7] ). In other words, from the given mapping f that approximately satisfies the functional equation Df (x, y) = 0, we will show that the mapping F , which is the solution of the functional equation Df (x, y) = 0, can be constructed using the formula

F (x) = lim

n→∞Jnf (x) or

F (x) = lim

n→∞Jn0f (x),

and we will prove that the mapping F is the unique solution of functional equation Df (x, y) = 0 near the mapping f .

2. Main theorems

The following lemma is needed to show the uniqueness of the solution mapping of the functional equation Df (x, y) = 0 satisfying a certain condition within the main theorem about the stability of the functional equation Df (x, y) = 0.

Lemma 2.1. If a mapping f : V → W satisfies Df (x, y) = 0 for all x, y ∈ V , then the equalities

f (x) =Jnf (x), (2.1)

f (x) =Jn0f (x) (2.2)

hold for all x ∈ V and all n ∈ N ∪ {0}.

(3)

Proof. Notice that if a mapping f : V → W satisfies Df (x, y) = 0 for all x, y ∈ V , then the equalities

fe(4x) − 20fe(2x) + 64fe(x) = 0, fo(2x) − 8fo(x) = 0

can be obtained from the equalities f (0) =2Df (0, 0)

k2(k2− 1),

fe(4x) − 20fe(2x) + 64fe(x) − 36fe(0) (2.3)

= 12k2Dfe(x, x) − 12(k2− 1)Dfe(0, x) k2(k2− 1)

− 6Dfe(0, 2x) − 12Dfe(kx, x) k2(k2− 1) , fo(2x) − 8fo(x) =−6Dfo(0, x)

k2(k2− 1) (2.4)

for all x ∈ V . Therefore, the equality (2.1) can be derived from the equality

f (x)−fo(2nx)

8n −16fe(2nx) + fe(2n+1x)

12 · 4n +4fe(2nx) − fe(2n+1x) 12 · 16n

=

n−1

X

i=0

2fo(2ix) − fo(2i+1x)

8i+1 +

n−1

X

i=0

64fe(2ix) − 20fe(2i+1x) + fe(2i+2x) 12 · 4i+1

+

n−1

X

i=0

−64fe(2ix) − 20fe(2i+1x) + fe(2i+2x) 12 · 16i+1

for all x ∈ V and n ∈ N ∪ {0}. The equality (2.2) can be easily obtained

in a similar way. 

In the following theorem, we can prove the generalized Hyers-Ulam stability of the functional equation Df (x, y) = 0 by using the direct method in the sense of G˘avruta.

Theorem 2.2. Let f : V → Y be a mapping for which there exists a function ϕ : V2 → [0, ∞) such that the inequality

(2.5) kDf (x, y)k ≤ ϕ(x, y)

(4)

holds for all x, y ∈ V and let f (0) = 0. If ϕ has the property

X

n=0

ϕ(2nx, 2ny) 4n < ∞ (2.6)

for all x, y ∈ V , then there exists a unique solution mapping F : V → Y of the functional equation Df (x, y) = 0 satisfying the inequality

kf (x) − F (x)k ≤ 1 k2|k2− 1|

X

n=0

 6ϕe(0, 2nx)

8n+1 +2k2ϕe(2nx, 2nx) 2 · 4n+1

+2|k2− 1|ϕe(0, 2nx) + ϕe(0, 2n+1x) + 2ϕe(2nkx, 2nx) 2 · 4n+1

 (2.7)

for all x ∈ V , where ϕeis the function defined by ϕe(x, y) := ϕ(x,y)+ϕ(−x,−y)

2 .

In particular, F is represented by the equality F (x) = limn→∞Jnf (x) for all x ∈ V .

Proof. From the equalities (2.3), (2.4) and (2.5), we have

kJnf (x) − Jn+1f (x)k

=

fo(2nx)

8n −fo(2n+1x) 8n+1 +

 1

12 · 4n+1 − 1 12 · 16n+1



× (64fe(2nx) − 20fe(2n+1x) + fe(2n+2x))

=

6Dfo(0, 2nx) k2(k2− 1)8n+1

+

2k2Dfe(2nx, 2nx) k2(k2− 1)2 · 4n+1

+−2(k2− 1)Dfe(0, 2nx) − Dfe(0, 2n+1x) + 2Dfe(2nkx, 2nx) k2(k2− 1)2 · 4n+1

≤ 1

k2|k2− 1|

 6ϕe(0, 2nx)

8n+1 +2k2ϕe(2nx, 2nx) + 2|k2− 1|ϕe(0, 2nx) 2 · 4n+1

e(0, 2n+1x) + 2ϕe(2nkx, 2nx) 2 · 4n+1

 (2.8)

(5)

for all x ∈ V . It follows from (2.8) that kJnf (x)−Jn+mf (x)k

n+m−1

X

i=n

kJif (x) − Ji+1f (x)k

≤ 1

k2|k2− 1|

n+m−1

X

i=n

 6ϕe(0, 2ix)

8i+1 +2k2ϕe(2ix, 2ix) 2 · 4i+1

+ 2|k2− 1|ϕe(0, 2ix) + ϕe(0, 2i+1x) + 2ϕe(2ikx, 2ix) 2 · 4i+1

 (2.9)

for all x ∈ V . In view of (2.6) and (2.9), the sequence {Jnf (x)} is a Cauchy sequence for all x ∈ V . Since Y is complete, the sequence {Jnf (x)} converges for all x ∈ V . Hence, we can define a mapping F : V → Y by

F (x) := lim

n→∞Jnf (x)

for all x ∈ V . Moreover, letting n = 0 and passing the limit m → ∞ in (2.9) we get the inequality (2.7). With the definition of F , we easily get the equality DF (x, y) = 0 from the relations

kDF (x, y)k

=

Dfo(2nx, 2ny)

8n + 16Dfe(2nx, 2ny) − fe(2n+1x, 2n+1y) 12 · 4n

−4Dfe(2nx, 2ny) − fe(2n+1x, 2n+1y) 12 · 16n

Dfo(2nx, 2ny) 8n

+

16Dfe(2nx, 2ny) 12 · 4n

+

Dfe(2n+1x, 2n+1y) 12 · 4n

≤ϕe(2nx, 2ny)

8n +16ϕe(2nx, 2ny)

12 · 4ne(2n+1x, 2n+1y) 12 · 4n

→ 0 as n → ∞.

To prove the uniqueness of F , let F0 : V → Y be another mapping satisfying the equality DF0(x, y) = 0 and the inequality (2.7). Instead of the condition (2.7), it is sufficient to show that there is a unique mapping F satisfying the simpler condition

kf (x) − F (x)k ≤

X

i=0

Φ(2ix) 2 · 4i+1

(6)

for all x ∈ V , where

Φ(2ix) :=2k2ϕe(2ix, 2ix) + 2(k2+ 4)ϕe(0, 2ix) + ϕe(0, 2i+1x) + 2ϕe(2ikx, 2ix)

k2|k2− 1| .

By (2.1), the equality F0(x) = JnF0(x) holds for all n ∈ N. Therefore, we have

kJnf (x) − F0(x)k

=kJnf (x) − JnF0(x)k

fo(2nx)

8n + 16fe(2nx) − fe(2n+1x)

12 · 4n −4fe(2nx) − fe(2n+1x) 12 · 16n

−Fo0(2nx)

8n −16Fe0(2nx) − Fe0(2n+1x)

12 · 4n +4Fe0(2nx) − Fe0(2n+1x) 12 · 16n

fo(2nx)

8n − Fo0(2nx) 8n

+

 16

12 · 4n − 4 12 · 16n



fe(2nx) − Fe0(2nx) +

 1

12 · 4n − 1 12 · 16n



fe(2n+1x) − Fe0(2n+1x)

X

i=0

Φ(2i+nx) 2 · 4i+1· 8n +4

3

X

i=0

Φ(2i+nx) 2 · 4i+1· 4n +4

3

X

i=0

Φ(2i+n+1x) 2 · 4i+1· 4n

X

i=n

Φ(2ix) 2 · 4i+1+

X

i=n

Φ(2ix) 4i+1 +

X

i=n+1

Φ(2ix) 4i+1

for all x ∈ V and all n ∈ N. Taking the limit in the above inequality as n → ∞, we conclude that F0(x) = limn→∞Jnf (x) for all x ∈ V . This means that the equality F (x) = F0(x) holds for all x ∈ V .  Corollary 2.3. Let p ∈ (0, 2) and X be a real normed space. If f : X → Y is a mapping such that

kDf (x, y)k ≤ θ(kxkp+ kykp) (2.10)

for all x, y ∈ X, then there exists a unique solution mapping F : X → Y of the functional equation Df (x, y) = 0 satisfying the inequality

kf (x) − F (x)k ≤ 6

k2|k2− 1|(8 − 2p)

+4k2+ 2|k2− 1| + 2 + 2|k|p+ 2p 2k2|k2− 1|(4 − 2p) (2.11)

for all x ∈ X.

(7)

Proof. If we put ϕ = θ(kxkp+ kykp) in Theorem 2.2, the inequality (2.11) is easily obtained from the inequality (2.7).  Theorem 2.4. Let f : V → Y be a mapping for which there exists a function ϕ : V2 → [0, ∞) such that the inequality (2.5) holds for all x, y ∈ V and let f (0) = 0. If ϕ has the property

X

n=0

16nϕ

x 2n, y

2n



< ∞ (2.12)

for all x, y ∈ V , then there exists a unique solution mapping F : V → Y of the functional equation Df (x, y) = 0 satisfying the inequality

kf (x) − F (x)k ≤

X

n=0

Ψn(x) (2.13)

for all x ∈ V , where Ψn(x) := 6 · 8n

k2|k2− 1|ϕe 0, x

2n+1



+ 8 · 16n k2|k2− 1|



2k2ϕe x 2n+2, x

2n+2



+ 2|k2− 1|ϕe 0, x

2n+2

 + ϕe

 0, x

2n+1

 + 2ϕe

 kx 2n+2, x

2n+2

  . In particular, F is represented by F (x) = limn→∞Jn0f (x) for all x ∈ V .

Proof. From the equalities (2.3), (2.4) and (2.5), we have kJn0f (x) − Jn+10 f (x)k

8n

 fox

2n

− 8fo x 2n+1



+(4 · 16n− 4n) 3

 fe

x 2n



− 20fe x 2n+1



+ 64fe

 x 2n+2



≤ 6 · 8n k2|k2− 1|

Dfo 0, x

2n+1

 + 4 · 16n

3k2|k2− 1|

− 6Dfe 0, x

2n+1



+ 12Dfe

 kx 2n+2, x

2n+2



+ 12k2Dfe

 x 2n+2, x

2n+2



− 12(k2− 1)Dfe 0, x

2n+2



≤Ψn(x) (2.14)

(8)

for all x ∈ V . It follows from (2.14) that

kJn0f (x) − Jn+m0 f (x)k ≤

n+m−1

X

i=n

Ψi(x) (2.15)

for all x ∈ V . In view of (2.12) and (2.15), the sequence {Jn0f (x)} is a Cauchy sequence for all x ∈ V . Since Y is complete, the sequence {Jn0f (x)} converges for all x ∈ V . Hence, we can define a mapping F : V → Y by F (x) := limn→∞Jn0f (x) for all x ∈ V . Moreover, letting n = 0 and passing the limit m → ∞ in (2.15) we get the inequality (2.13). From the definition of F , we easily get

kDF (x, y)k = 8nDfo

x 2n, y

2n



+4 · 16n− 4n 3 Dfe

x 2n, y

2n



−16n+1− 4n+2

3 Dfe

 x 2n+1, y

2n+1



16nDfox 2n, y

2n

 +

16nDfe x 2n, y

2n

 +

16n+1 3 Dfe

 x 2n+1, y

2n+1



≤16n+1ϕex 2n, y

2n



+ 16n+1ϕe x 2n+1, y

2n+1



→ 0 as n → ∞,

which means that DF (x, y) = 0 for all x, y ∈ V .

To prove the uniqueness of F , let F0 : V → Y be another mapping satisfying DF0(x, y) = 0 and (2.13). Instead of the condition (2.13), it is sufficient to show that there is a unique mapping satisfying the simpler condition

kf (x) − F (x)k ≤

X

i=0

16iΦ

x 2i



for all x ∈ V , where

Φx 2i



:= 16

k2|k2− 1|



2k2ϕe x 2i+2, x

2i+2



+ 2|k2− 1|ϕe 0, x

2i+2

 + 2ϕe

 0, x

2i+1

 + 2ϕe

 kx 2i+2, x

2i+2

  .

(9)

By (2.2), the equality F0(x) = Jn0F0(x) holds for all x ∈ V and all n ∈ N.

Therefore, we have kJn0f (x) − F0(x)k

=kJn0f (x) − Jn0F0(x)k

8nfo x 2n



+4 · 16n− 4n 3 fex

2n

−16n+1− 4n+2

3 fe x 2n+1



− 8nFo0

x 2n



−4 · 16n− 4n 3 Fe0

x 2n



+16n+1− 4n+2 3 Fe0

 x 2n+1



≤8n

fo x 2n

− Fo0 x 2n



+ 16n+1

fo x 2n+1

− Fo0 x 2n+1

 + 16n+1

fex 2n

− Fe0x 2n



X

i=n

16iΦx 2i

 +

X

i=n+1

16iΦx 2i

 +

X

i=n

16i+1Φx 2i



for all x ∈ V and all n ∈ N. Taking the limit in the above inequality as n → ∞, we can conclude that F0(x) = limn→∞Jn0f (x) for all x ∈ V . This means that F (x) = F0(x) for all x ∈ V .  Corollary 2.5. Let p > 4 be a real number and X be a real normed space. If f : X → Y is a mapping satisfying the inequality (2.10) for all x, y ∈ X, then there exists a unique solution mapping F : X → Y of the functional equation Df (x, y) = 0 satisfying the inequality

kf (x) − F (x)k ≤ 6

k2|k2− 1|(2p− 8) +8(4k2+ 2|k2− 1| + 2|k|p+ 2 + 2p) k2|k2− 1|2p(2p− 16) for all x ∈ X.

References

[1] P. Gˇavruta and P. G˘avruta, A generalization of the Hyers-Ulam-Rassias sta- bility of approximately additive mappings, J. Math. Anal. Appl., 184 (1994), 431–436.

[2] M. E. Gordji, S. Kaboli, and S. Zolfaghari, Stability of a mixed type quadratic, cubic and quartic functional equation, arxiv: 0812.2939v1 Math FA, 15 Dec 2008.

[3] M. E. Gordji, H. Khodaei, and R. Khodabakhsh, General quartic-cubic- quadratic functional equation in non-Archimedean normed spaces, U.P.B. Sci.

Bull. Series A, 72 (2010), no. 3, 69–84.

(10)

[4] D. H. Hyers, On the stability of the linear functional equation, Proc. Natl. Acad.

Sci. U.S.A., 27 (1941), 222–224.

[5] Y.-H. Lee, A fixed point approach to the stability of a quadratic-cubic-quartic functional equation, East Asian Math. J., 35 (2019), 559–568.

[6] Y.-H. Lee, Hyers-Ulam-Rassias stability of a quadratic-cubic-quartic functional equation, Korea J. Math., (2019), submitted.

[7] Th. M. Rassias, On the stability of the linear mapping in Banach spaces, Proc.

Amer. Math. Soc., 72 (1978), 297–300.

Department of Mathematics Education Gongju National University of Education Gongju 32553, Korea

lyhmzi@gjue.gjue.ac.kr

참조

관련 문서

We prove the existence, uniqueness, and regularity for the weak solution of the Poisson equation, through which the Hodge projection is shown to be unique and orthogonal.. Also,

• 대부분의 치료법은 환자의 이명 청력 및 소리의 편안함에 대한 보 고를 토대로

• 이명의 치료에 대한 매커니즘과 디지털 음향 기술에 대한 상업적으로의 급속한 발전으로 인해 치료 옵션은 증가했 지만, 선택 가이드 라인은 거의 없음.. •

Within the Fresnel approximation, there are two approaches to determining the complex amplitude g(x, y) in the output plane, given the complex amplitude f(x, y) in the

Modern Physics for Scientists and Engineers International Edition,

Note the point that any wave can be written as a linear combination of sinusoidal waves,.  therefore if you know how sinusoidal waves behave, you know in principle how

12) Maestu I, Gómez-Aldaraví L, Torregrosa MD, Camps C, Llorca C, Bosch C, Gómez J, Giner V, Oltra A, Albert A. Gemcitabine and low dose carboplatin in the treatment of

Levi’s ® jeans were work pants.. Male workers wore them