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Research article

Asymptotic behavior of a generalized functional equation

  • Received: 02 December 2021 Revised: 09 January 2022 Accepted: 17 January 2022 Published: 07 February 2022
  • MSC : 39B82, 39B52, 39B62

  • In this paper, we investigate the Hyers-Ulam stability problem of the following functional equation

    f(x+y)+g(xy)=h(x)+k(y),

    on an unbounded restricted domain, which generalizes some of the results already obtained by other authors (for example [9,Theorem 2], [11,Theorem 5] and [21,Theorem 2]). Particular cases of this functional equation are Cauchy, Jensen, quadratic and Drygas functional equations. As a consequence, we obtain asymptotic behaviors of this functional equation.

    Citation: Mohammad Amin Tareeghee, Abbas Najati, Batool Noori, Choonkil Park. Asymptotic behavior of a generalized functional equation[J]. AIMS Mathematics, 2022, 7(4): 7001-7011. doi: 10.3934/math.2022389

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  • In this paper, we investigate the Hyers-Ulam stability problem of the following functional equation

    f(x+y)+g(xy)=h(x)+k(y),

    on an unbounded restricted domain, which generalizes some of the results already obtained by other authors (for example [9,Theorem 2], [11,Theorem 5] and [21,Theorem 2]). Particular cases of this functional equation are Cauchy, Jensen, quadratic and Drygas functional equations. As a consequence, we obtain asymptotic behaviors of this functional equation.



    Assume that V and W are linear spaces over the field F. Let us recall that a function f:VW satisfies the quadratic functional equation provided

    f(x+y)+f(xy)=2f(x)+2f(y),x,yV. (1.1)

    In this case f is called a quadratic function. It is well known that a function f:VW between real vector spaces V and W satisfies (1.1) if and only if there exists a unique symmetric bi-additive function B:V×VW such that f(x)=B(x,x) for all xV (see [1,7,13]). For the case V=W=R, the function f:RR defined by f(x)=ax2 satisfies (1.1). Indeed, each continuous quadratic function f:RR has this form. The functional Eq (1.1) plays an important role in the characterization of inner product spaces [8]. We notice that if . is a norm the parallelogram law is specifically true for norms derived from inner products.

    In this paper, we deal with the stability of the functional equation

    f(x+y)+g(xy)=h(x)+k(y), (1.2)

    on restricted domains, where f,g,h,k:XY are unknown functions from normed linear space X to Banach space Y. This functional equation is a generalization of the quadratic functional Eq (1.1). Special cases of this functional equation include the additive functional equation f(x+y)=f(x)+f(y), the Jensen functional equation f(x+y2)=f(x)+f(y), the Pexider Cauchy functional equation f(x+y)=g(x)+h(y), and many more. The general solutions of (1.2) were given in [4] without any regularity assumptions on functions f,g,h,k when (1.2) holds for all x,yV (see also [14]).

    The stability of the quadratic functional Eq (1.1) was first investigated by Skof [23]. Czerwik [2] generalized Skof's result. For more detailed information on the stability results of the functional Eq (1.1) and other quadratic functional equations, we refer the readers to [5,6,9,15,16,17,18,19,20,21,22,25]. We also refer the readers to the books [1,3,7,12,14].

    In this paper, stability results of the functional Eq (1.2) on an unbounded restricted domain and its applications are introduced.

    Let f be any function between two linear spaces. The symbols fe and fo denote the even and odd parts of f, respectively. Notice that fo(0)=0 and fe(0)=f(0).

    The following theorem generalizes some of the results already obtained by other authors (for example [9,Theorem 2], [11,Theorem 5] and [21,Theorem 2]).

    Theorem 2.1. Let X be a linear normed space and Y be a Banach space, and let d>0 and ε0. Suppose that f,g,h,k:XY satisfy

    f(x+y)+g(xy)h(x)k(y)ε, (2.1)

    for all x,yX with x+yd. Then there are a unique quadratic functionQ:XY and exactly two additive functions A1,A2:XY such that

    f(x)Q(x)A1(x)f(0)46ε, (2.2)
    g(x)Q(x)A2(x)g(0)46ε, (2.3)
    h(x)2Q(x)(A1+A2)(x)h(0)29ε, (2.4)
    k(x)2Q(x)(A1A2)(x)k(0)29ε, (2.5)

    for all xX.

    Proof. Replacing x by x and y by y in (2.1), and adding (subtracting) the resulting inequality to (from) (2.1), we obtain

    fe(x+y)+ge(xy)he(x)ke(y)ε, (2.6)
    fo(x+y)+go(xy)ho(x)ko(y)ε, (2.7)

    for all x,yX with x+yd. Putting x=0,y=0,y=x and y=x in (2.6), respectively, we get

    fe(y)+ge(y)h(0)ke(y)ε,yd, (2.8)
    fe(x)+ge(x)he(x)k(0)ε,xd, (2.9)
    fe(2x)+g(0)he(x)ke(x)ε,xd, (2.10)
    f(0)+ge(2x)he(x)ke(x)ε,xd. (2.11)

    It follows from (2.8)–(2.10) that

    fe(2x)2fe(x)2ge(x)+g(0)+h(0)+k(0)3ε,xd. (2.12)

    By using (2.8), (2.9) and (2.11), we have

    ge(2x)2fe(x)2ge(x)+f(0)+h(0)+k(0)3ε,xd. (2.13)

    Hence, (2.12) and (2.13) imply

    fe(2x)ge(2x)+g(0)f(0)6ε,xd.

    Then

    fe(x)ge(x)+g(0)f(0)6ε,x2d. (2.14)

    In view of (2.12) and (2.14), we obtain

    fe(2x)4fe(x)+α15ε,x2d, (2.15)

    where α:=2f(0)g(0)+h(0)+k(0). If we replace x by 2nx in (2.15), and divide the resulting inequality by 4n+1, then we obtain

    fe(2n+1x)4n+1fe(2nx)4n+α4n+115ε4n+1,x2d,n0.

    So

    fe(2n+1x)4n+1fe(2mx)4m+nk=mα4k+1nk=m15ε4k+1,x2d,nm0. (2.16)

    Therefore, {fe(2nx)4n}n is a Cauchy sequence for each fixed xX with x2d. Thus, by the completeness of Y, the sequence {fe(2nx)4n}n is convergent for each fixed xX with x2d. Then it is easy to see that the sequence {fe(2nx)4n}n is convergent for each fixed xX. We define the function Q:XY by

    Q(x)=limnfe(2nx)4n,xX.

    It follows from (2.14) that Q(x)=limnge(2nx)4n for all xX. In view of (2.8) and (2.9) we have

    2Q(x)=limnke(2nx)4nand2Q(x)=limnhe(2nx)4n,xX.

    Let x,yX{0} and choose mN such that 2nx,2nyd for all nm. Writing 2nx instead of x and 2ny instead of y in (2.6) (for nm), and dividing the resultant inequality by 4n, and then letting n approach infinity, we obtain

    Q(x+y)+Q(xy)=2Q(x)+2Q(y),x,yX{0}.

    Since Q(0)=0 and Q is even, we infer that Q is quadratic. Putting m=0 and taking the limit as n in (2.16), we get

    fe(x)Q(x)13α5ε,x2d. (2.17)

    Replacing y by y in (2.6), we have

    ge(x+y)+fe(xy)he(x)ke(y)ε,x+yd.

    This inequality is similar to inequality (2.6). By a similar argument, we have

    ge(x)Q(x)13β5ε,x2d, (2.18)

    where β:=2g(0)f(0)+h(0)+k(0). Adding (2.17) to (2.18), we get

    fe(x)+ge(x)2Q(x)13(α+β)10ε,x2d. (2.19)

    In view of (2.8), (2.9) and (2.19), we obtain

    ke(y)2Q(y)+h(0)13(α+β)11ε,y2d, (2.20)
    he(x)2Q(x)+k(0)13(α+β)11ε,x2d. (2.21)

    Now we extend inequalities (2.17), (2.18), (2.20) and (2.21) to X. Let zX, choose yX such that y2d+z and let x=zy. Then min{x,xy,y}2d. By (2.18), we have

    ge(xy)Q(xy)13β5ε. (2.22)

    It follows from (2.6) and (2.20)–(2.22) that

    fe(x+y)+Q(xy)2Q(x)2Q(y)f(0)28ε.

    Since z=x+y and Q is quadratic, we get

    fe(z)Q(z)f(0)28ε. (a)

    Similarly, for an arbitrary zX, we conclude that

    ge(z)Q(z)g(0)28ε. (b)

    Now, let xX and choose yX such that y2d+x. It is clear that x±y2d. Then by (2.17) and (2.18), we have

    fe(x+y)Q(x+y)13α5ε,ge(xy)Q(xy)13β5ε. (2.23)

    It follows from (2.6), (2.20) and (2.23) that

    Q(x+y)+Q(xy)2Q(y)he(x)+h(0)22ε.

    Since Q is quadratic, we obtain

    he(x)2Q(x)h(0)22ε. (c)

    Similarly, for an arbitrary xX, we conclude that

    ke(x)2Q(x)k(0)22ε. (d)

    Letting x=0,y=0,y=x and y=x in (2.7), respectively, we get

    fo(y)go(y)ko(y)ε,yd, (2.24)
    fo(x)+go(x)ho(x)ε,xd, (2.25)
    fo(2x)ho(x)ko(x)ε,xd, (2.26)
    go(2x)ho(x)+ko(x)ε,xd. (2.27)

    It follows from (2.24) and (2.25) that

    2fo(x)ho(x)ko(x)2ε,2go(x)ho(x)+ko(x)2ε,xd. (2.28)

    In view of (2.26)–(2.28), we obtain

    fo(2x)2fo(x)3ε,go(2x)2go(x)3ε,xd.

    It is easy to see that

    fo(2n+1x)2n+1fo(2mx)2mni=m3ε2i+1,go(2n+1x)2n+1go(2mx)2mni=m3ε2i+1, (2.29)

    for all xd. So, we can define A1,A2:XY by

    A1(x):=limnfo(2nx)2nandA2(x):=limngo(2nx)2n,xX.

    In view of (2.24) and (2.25), we conclude that

    (A1A2)(x)=limnko(2nx)2nand(A1+A2)(x)=limnho(2nx)2n,xX.

    Let xX and ,yX{0}. We can choose mN such that 2nyd for all nm. Writing 2nx instead of x and 2ny instead of y in (2.7) (for nm), and dividing the resultant inequality by 2n, and then letting n approach infinity, we obtain

    A1(x+y)+A2(xy)=(A1+A2)(x)+(A1A2)(y). (2.30)

    Since A1(0)=A2(0)=0, we get (2.30) for all x,yX. For convenience, we set A=A1+A2 and L=A1A2. Then A and L are odd because A1 and A2 are. By (2.30), we have

    A(x+y)+A(xy)2A(x)=A1(x+y)+A2(xy)A(x)L(y)+A1(xy)+A2(x+y)A(x)+L(y)=0,x,yX.

    Hence A is additive. Thus

    A1(x+y)A1(x)A1(y)=A2(x)+A2(y)A2(x+y),x,yX.

    Using (2.30), we obtain

    A2(x+y)A2(xy)=2A2(y),x,yX.

    So A2 is additive, and consequently A1 is additive.

    By (2.29), we obtain

    fo(x)A1(x)3εandgo(x)A2(x)3ε,xd. (2.31)

    In view of (2.24), (2.25) and (2.31), we get

    ho(x)(A1+A2)(x)7εandko(x)(A1A2)(x)7ε,xd. (2.32)

    Now we extend inequalities (2.31) and (2.32) to X. Let zX, choose yX with yd+z and let x=zy. Then min{x,xy,y}d. By (2.31) and (2.32), we have

    go(xy)A2(xy)3ε,ho(x)(A1+A2)(x)7ε,ko(y)(A1A2)(y)7ε.

    Since z=x+y and A1,A2 are additive, these inequalities and (2.7) yield

    fo(z)A1(z)18ε. (a')

    Similarly, one can obtain

    go(z)A2(z)18ε,zX. (b')

    To extend (2.32), let xX and choose yX such that yd+x. Then x±yd. By (2.31), we have

    fo(x+y)A1(x+y)3εandgo(xy)A2(xy)3ε.

    Using (2.7) and these inequalities, we get

    ho(x)+ko(y)A1(x+y)A2(xy)7ε. (2.33)

    Because ko is odd and A1,A2 are additive, interchanging y with y in (2.33) and adding the resulting inequality to (2.33), we get

    ho(x)(A1+A2)(x)7ε. (c')

    Similarly, one can obtain

    ko(x)(A1A2)(x)7ε,xX. (d')

    In view of (a) and (a), we get (2.2). By (b) and (b), we obtain (2.3). (2.4) follows from (c) and (c) . Finally, (d) and (d) yield (2.5).

    Corollary 2.2. Let X,Y be linear normed spaces, and f,g,h,k:XY satisfy

    limx+yf(x+y)+g(xy)h(x)k(y)=0.

    Then (f,g,h,k)) is a solution of (1.2) and they are given by

    f(x)=A1(x)+Q(x)+f(0),g(x)=A2(x)+Q(x)+g(0),h(x)=(A1+A2)(x)+2Q(x)+h(0),k(x)=(A1A2)(x)+2Q(x)+k(0),xX,

    where A1,A2:XY are additive and Q:XY is quadratic.

    Proof. Let ε>0 be an arbitrary. Then there exists d>0 such that

    f(x+y)+g(xy)h(x)k(y)<ε,x+yd.

    By Theorem 2.1 (we let Y be the completion of Y), we get

    f(x+y)+g(xy)h(x)k(y)f(0)g(0)+h(0)+k(0)150ε,x,yX.

    Since ε>0 was given arbitrarily, we get

    f(x+y)+g(xy)h(x)k(y)f(0)g(0)+h(0)+k(0)=0,x,yX.

    Hence the result follows from [10,Theorem 3.1].

    Corollary 2.3. Let X,Y be linear normed spaces, and f:XY satisfy

    limx+yf(x+y)+f(xy)2f(x)f(y)f(y)=0.

    Then f is given by

    f(x)=A(x)+Q(x)+f(0),xX,

    where A:XY is additive and Q:XY is quadratic.

    To prove the next theorem, we need the following result.

    Lemma 2.4. [24,Corollary 2.8] Let X be a linear normed space and Y be a Banach space, and let d>0 and ε0. Suppose that f:XY is a function such that

    f(x+y)+f(xy)2f(x)2f(y)ε,x+yd.

    Then there is a unique quadratic function Q:XY such that

    f(x)Q(x)76ε,xX.

    Theorem 2.5. Let X be a linear normed space and Y be a Banach space, and let d>0 and ε0. Suppose that f:XY is a function such that supxXf(x)=+ and

    f(x+y)+f(xy)af(x)bf(y)ε, (2.34)

    for all x,yX with x+yd, where a,b are real constants with b0. Then there is a unique quadratic functionQ:XY such that

    f(x)Q(x)76ε,xX. (2.35)

    Proof. By considering the proof of Theorem 2.1, there exists a unique quadratic function Q:XY such that aQ(x)=bQ(x)=2Q(x) and

    f(x)Q(x)f(0)46ε, (2.36)

    for all xX. Since f is unbounded, we get Q0 by (2.36). So a=b=2. Consequently, (2.34) implies that

    f(x+y)+f(xy)2f(x)2f(y)ε,

    for all x,yX with x+yd. By Lemma 2.4, we get (2.35).

    Corollary 2.6. Suppose that f:XY satisfies

    f(x+y)+f(xy)bf(y)ε,

    for all x,yX with x+yd, where b is a real constant. Then f is bounded.

    Theorem 2.7. Let X be a linear normed space and Y be a Banach space, and let d>0 and ε0. Suppose that f:XY is a function such that supxXf(x)=+ and

    f(x+y)+f(xy)af(x)ε, (2.37)

    for all x,yX with x+yd, where a is a real constant. Then there is a unique additive functionA:XY such that

    f(x)A(x)f(0)32ε,xX. (2.38)

    Proof. By considering the proof of Theorem 2.1, there exists a unique additive function A:XY such that aA(x)=2A(x) and

    f(x)A(x)f(0)46ε, (2.39)

    for all xX. Since f is unbounded, we get A0 by (2.39). So we get a=2 and consequently, (2.37) implies that

    f(x+y)+f(xy)2f(x)ε,x+yd. (2.40)

    Then

    A(x)f(x)+f(0)ε,xd. (2.41)

    Now we extend (2.41) to X. Let xX and choose yX such that yd+x. It is clear that x±yd. Then (2.41) yields that

    A(x+y)f(x+y)+f(0)εandA(xy)f(xy)+f(0)ε.

    These inequalities and (2.40) imply that A(x+y)+A(xy)2f(x)+2f(0)3ε. Since A is additive, we get (2.38).

    In the following corollary, we investigate the Hyers-Ulam stability of Drygas functional equation which is a special case of Theorem 2.1. In this case we get a sharp bound.

    Corollary 2.8. Suppose that f:XY satisfies

    f(x+y)+f(xy)2f(x)f(y)f(y)ε,

    for all x,yX with x+yd. Then there are a unique quadratic functionQ:XY and a unique additive function A:XY such that

    f(x)Q(x)A(x)2f(0)83ε,xX. (2.42)

    Proof. By the assumption, we obtain

    fe(x+y)+fe(xy)2fe(x)2fe(y)ε,fo(x+y)+fo(xy)2fo(x)ε,

    for all x,yX with x+yd. Then by [24,Corollary 2.8] and the argument in the proof of Theorem 2.7, there are a quadratic function Q:XY and an additive function A:XY such that

    fe(x)Q(x)76ε,fo(x)A(x)f(0)32ε,xX.

    Hence we get (2.42). The uniqueness of A and Q is clear.

    We have investigated the Hyers-Ulam stability of the Pexider functional Eq (1.2) on an unbounded restricted domain. As a consequence, we have obtained asymptotic behaviors of this functional equation.

    The authors declare that they have no competing interests.



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