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A Kannappan-Cosine Functional Equation on Semigroups

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Apr 27, 2024

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Introduction

The addition law for cosine is cosx+y=cosx cosysinx siny,x,y. \cos \left( {x + y} \right) = \cos \left( x \right)\cos \left( y \right) - \sin \left( x \right)\sin \left( y \right),\;\;\;\;x,\;y \in {\mathbb {R}}. This gives the origin of the following functional equation on any semigroup S: gxy=gxgyfxfy,x,yS, g\left( {xy} \right) = g\left( x \right)g\left( y \right) - f\left( x \right)f\left( y \right),\;\;\;\;x,\;y \in S, for the unknown functions f, g : S → ℂ, which is called the cosine addition law. In Aczél’s monograph [1, Section 3.2.3] we find continuous real valued solutions of (1.1) in case S = ℝ.

The functional equation (1.1) has been solved on groups by Poulsen and Stetkær [10], on semigroups generated by their squares by Ajebbar and Elqorachi [3], and recently by Ebanks [5] on semigroups.

In [12, Theorem 3.1], Stetkær solved the following functional equation gxy=gxgyfyfx+αfxy,x,yS, g\left( {xy} \right) = g\left( x \right)g\left( y \right) - f\left( y \right)f\left( x \right) + \alpha f\left( {xy} \right),\;\;\;\;x,\;y \in S, where α is a fixed constant in ℂ. He expressed the solutions in terms of multiplicative functions and the solution of the special case of the sine addition law. In [13, Proposition 16], he solved the functional equation fxyz0=fxfy,x,yS, f\left( {xy{z_0}} \right) = f\left( x \right)f\left( y \right),\;\;\;\;x,\;y \in S, on semigroups, and where z0 is a fixed element in S. We shall use these results in our computations.

In this paper, we deal with the following Kannappan-cosine addition law gxyz0=gxgyfxfy,x,yS, g\left( {xy{z_0}} \right) = g\left( x \right)g\left( y \right) - f\left( x \right)f\left( y \right),\;\;\;\;x,\;y \in S, on a semigroup S. The functional equation (1.4) is called Kannappan functional equation because it brings up a fixed element z0 in S as in the paper of Kannappan [9].

In the special case, where {f, g} is linearly dependent and g ≠ 0, we get that there exists a constant λ ∈ ℂ such that the function (1 − λ2)g satisfies the functional equation (1.3).

If S is a monoid with an identity element e, and f (e) = 0 and g(e) ≠ 0, or g(e) = 0 and f (e) ≠ 0, the last functional equation is the cosine addition law which was solved recently on general semigroups by Ebanks [5].

Now, if α := f (e) ≠ 0 and β := g(e) ≠ 0 we get that the pair gβ,fβ \left( {{g \over \beta },\;{f \over \beta }} \right) satisfies the following functional equation gβxy=gβxgβyfβxfβy+αβfβxy, {g \over \beta }\left( {xy} \right) = {g \over \beta }\left( x \right){g \over \beta }\left( y \right) - {f \over \beta }\left( x \right){f \over \beta }\left( y \right) + {\alpha \over \beta }{f \over \beta }\left( {xy} \right), which is of the form (1.2), and then explicit formulas for f and g on groups exist in the literature (see for example [8, Corollary 3.2.]).

The natural general setting of the functional equation (1.4) is for S being a semigroup, because the formulation of (1.4) requires only an associative composition in S, not an identity element and inverses. Thus we study in the present paper Kannappan-cosine functional equation (1.4) on semigroups S, generalizing previous works in which S is a group. So, the result of the present paper is a natural continuation of results contained in the literature.

The purpose of the present paper is to show how the relations between (1.4) and (1.2)–(1.3) on monoids extend to much wider framework, in which S is a semigroup. We find explicit formulas for the solutions, expressing them in terms of homomorphisms and additive maps from a semigroup into ℂ (Theorem 4.1). The continuous solutions on topological semigroups are also found.

Set up, notations and terminology

Throughout this paper, S is a semigroup (a set with an associative composition) and z0 is a fixed element in S. If S is topological, we denote by 𝒞(S) the algebra of continuous functions from S to the field of complex numbers ℂ.

Let f : S → ℂ be a function. We say that f is central if f (xy) = f (yx) for all x, yS, and that f is abelian if f (x1x2, . . . , xn) = f (xσ(1)xσ(2), . . . , xσ(n)) for all x1, x2, . . . , xnS, all permutations σ of n elements and all n ∈ ℕ. A map A : S → ℂ is said to be additive if A(xy) = A(x) + A(y), for all x, yS and a map χ : S → ℂ is multiplicative if χ(xy) = χ(x)χ(y), for all x, yS. If χ ≠ 0, then the nullspace Iχ := {xS | χ(x) = 0} is either empty or a proper subset of S and Iχ is a two sided ideal in S if not empty and S \ Iχ is a subsemigroup of S. Note that additive and multiplicative functions are abelian.

For any subset TS let T2 := {xy | x, yT } and for any fixed element z0 in S we let T2z0 := {xyz0 | x, yT}.

To express solutions of our functional equations studied in this paper we will use the set Pχ:=pIχ\Iχ2|up,pv,upvIχ\Iχ2forallu,vS\Iχ {P_\chi }: = \left\{ {p \in {I_\chi }\backslash I_\chi ^2|up,pv,upv \in {I_\chi }\backslash I_\chi ^2\;{\rm{for}}\;{\rm{all}}\;u,v \in S\backslash I\chi } \right\} . For more details about Pχ we refer the reader to [4], [5] and [6].

Preliminaries

In this section, we give useful results to solve the functional equation (1.4).

Lemma 3.1.

Let S be a semigroup, n ∈ ℕ, and χ, χ1, χ2, . . . , χn : S → ℂ be different non-zero multiplicative functions. Then

{χ1, χ2, · · ·, χn} is linearly independent.

If A : S \ Iχ → ℂ is a non-zero additive function, then the set {χA, χ} is linearly independent on S \ Iχ.

Proof

(a) See [11, Theorem 3.18]. (b) See [2, Lemma 4.4].

The proposition below gives the solutions of the functional equation fxyz0=χz0fxχy+χz0fyχx,x,yS. f\left( {xy{z_0}} \right) = \chi \left( {{z_0}} \right)f\left( x \right)\chi \left( y \right) + \chi \left( {{z_0}} \right)f\left( y \right)\chi \left( x \right),\;\;\;\;x,\;y \in S.

Proposition 3.2.

Let S be a semigroup, and χ : S → ℂ be a multiplicative function such that χ(z0) ≠ 0. If f : S → ℂ is a solution of (3.1), then fx=χxAx+Az0for xS\Iχ,ρxfor xPχ,0for xIχ\Pχ, f\left( x \right) = \left\{ {\matrix{ {\chi \left( x \right)\left( {A\left( x \right) + A\left( {{z_0}} \right)} \right)} \hfill & {for\;x \in S\backslash {I_\chi },} \hfill \cr {\rho \left( x \right)} \hfill & {for\;x \in {P_\chi },} \hfill \cr 0 \hfill & {for\;x \in {I_\chi }\backslash {P_\chi },} \hfill \cr } } \right. where A : S\ Iχ → ℂ is additive and ρ : Pχ → ℂ is the restriction of f to Pχ. In addition, f is abelian and satisfies the following conditions:

f (xy) = f (yx) = 0 for all xIχ \ Pχ and yS \ Iχ.

If x ∈ {up, pv, upv} with pPχ and u, vS \ Iχ, then xPχ and we have respectively ρ(x) = ρ(p)χ(u), ρ(x) = ρ(p)χ(v) or ρ(x) = ρ(p)χ(uv).

Conversely, the function f of the form (3.2) define a solution of (3.1). Moreover, if S is a topological semigroup and f𝒞(S), then χ𝒞(S), A𝒞(S \ Iχ) and ρ𝒞(Pχ).

Proof

See [7, Proposition 4.3].

To shorten the way to finding the solutions of functional equation (1.4), we prove the following lemma that contains some key properties.

Lemma 3.3.

Let S be a semigroup and let f, g : S → ℂ be the solutions of the functional equation (1.4) with g ≠ 0. Then

If f (z0) = 0 then

for all x, yS, gz02gxy=gz0gxgyfxfy+fz02fxy, g\left( {z_0^2} \right)g\left( {xy} \right) = g\left( {{z_0}} \right)\left[ {g\left( x \right)g\left( y \right) - f\left( x \right)f\left( y \right)} \right] + f\left( {z_0^2} \right)f\left( {xy} \right),

g(z02)2=g(z0)3+f(z02)2 g{(z_0^2)^2} = g{({z_0})^3} + f{(z_0^2)^2} .

If f and g are linearly independent then g(z0) ≠ 0.

If f (z0) ≠ 0, then there exists µ ∈ ℂ such that fxyz0=fxgy+fygx+μfxfy,x,yS. f\left( {xy{z_0}} \right) = f\left( x \right)g\left( y \right) + f\left( y \right)g\left( x \right) + \mu f\left( x \right)f\left( y \right),\;\;\;\;x,\;y \in S.

Proof

Suppose that f (z0) = 0.

Making the substitutions xy,z02 \left( {xy,z_0^2} \right) and (xyz0, z0) in (1.4) we get gxyz03=gxygz02fxyfz02 g\left( {xyz_0^3} \right) = g\left( {xy} \right)g\left( {z_0^2} \right) - f\left( {xy} \right)f\left( {z_0^2} \right) and gxyz03 g\left( {xyz_0^3} \right) = g(xyz0)g(z0)−f (xyz0)f (z0) = g(z0)g(x)g(y) − g(z0)f (x)f (y), respectively. Comparing these expressions, we deduce that gxygz02fz02fxy g\left( {xy} \right)g\left( {z_0^2} \right) - f\left( {z_0^2} \right)f\left( {xy} \right) = g(z0)g(x)g(y)−g(z0)f (y)f (x). This proves the desired identity.

It follows directly by putting x = y = z0 in the equation (3.3).

For a contradiction we suppose that g(z0) = 0. Then using (1.4), we get gxyz02 g\left( {xyz_0^2} \right) = g(x)g(yz0) − f (x)f (yz0) = g(xy)g(z0) − f (xy)f (z0) = 0 since f (z0) = g(z0) = 0. Then we deduce that gxgyz0=fxfyz0,x,yS. g\left( x \right)g\left( {y{z_0}} \right) = f\left( x \right)f\left( {y{z_0}} \right),\;\;\;\;x,\;y \in S.

If g(yz0) = 0 for all yS then 0 = g(xyz0) = g(x)g(y) − f (x)f (y), x, yS. So, g(x)g(y) = f (x)f (y), x, yS. Hence, f = g or f = − g, which contradicts the fact that f and g are linearly independent. So g ≠ 0 on Sz0, and from (3.5) we get that g = c1f with c1 := f (az0)/g(az0) for some aS such that g(az0) ≠ 0. This is also a contradiction, since f and g are linearly independent. So we conclude that g(z0) ≠ 0.

Suppose that f (z0) ≠ 0. By the substitutions x,yz02 \left( {x,yz_0^2} \right) and (xyz0, z0) in (1.4) we get gxyz03 g\left( {xyz_0^3} \right) = gxgyz02 g\left( x \right)g\left( {yz_0^2} \right) fxfyz02 f\left( x \right)f\left( {yz_0^2} \right) = g(z0)g(x)g(y) − g(x)f(z0)f(y) − fxfyz02 f\left( x \right)f\left( {yz_0^2} \right) and gxyz03 g\left( {xyz_0^3} \right) = g(xyz0)g(z0) − f (xyz0)f (z0) = g(z0)g(x)g(y) − g(z0)f (x)f (y) − f (xyz0)f (z0), respectively. Then, by the associativity of the operation in S we obtain fz0fxyz0fxgyfygx=fxfyz02fygz0fz0gy. \matrix{ {f\left( {{z_0}} \right)\left[ {f\left( {xy{z_0}} \right) - f\left( x \right)g\left( y \right) - f\left( y \right)g\left( x \right)} \right]} \hfill \cr {\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; = f\left( x \right)\left[ {f\left( {yz_0^2} \right) - f\left( y \right)g\left( {{z_0}} \right) - f\left( {{z_0}} \right)g\left( y \right)} \right].} \hfill \cr } Since f (z0) ≠ 0, dividing (3.6) by f (z0) we get fxyz0=fxgy+fygx+fxψy, f\left( {xy{z_0}} \right) = f\left( x \right)g\left( y \right) + f\left( y \right)g\left( x \right) + f\left( x \right)\psi \left( y \right), where ψy:=f(z0)1fyz02fygz0fz0gy \psi \left( y \right): = f{({z_0})^{ - 1}}\left[ {f\left( {yz_0^2} \right) - f\left( y \right)g\left( {{z_0}} \right) - f\left( {{z_0}} \right)g\left( y \right)} \right] . Substituting (3.7) back into (3.6), we find out that f (z0)f (x)ψ(y) = f (x)f (y)ψ(z0), which implies that ψ(y) = µf (y) with µ := ψ(z0)/f (z0). Therefore, (3.7) becomes f (xyz0) = f (x)g(y) + f (y)g(x) + µf (x)f (y). This completes the proof of Lemma 3.3.

Main results

Now, we are ready to describe the solutions of the functional equation (1.4).

Let ΨAχ,ρ : S → ℂ denote the function of the form in [6, Theorem 3.1 (B)], i.e., ΨAχ,ρx=χxAxfor xS\Iχ,ρxfor xPχ,0for xIχ\Pχ, {\Psi _{A\chi ,\rho }}\left( x \right) = \left\{ {\matrix{ {\chi \left( x \right)A\left( x \right)} \hfill & {{\rm{for}}\;x \in S\backslash {I_\chi },} \hfill \cr {\rho \left( x \right)} \hfill & {{\rm{for}}\;x \in {P_\chi },} \hfill \cr 0 \hfill & {{\rm{for}}\;x \in {I_\chi }\backslash {P_\chi },} \hfill \cr } } \right. where χ : S → ℂ is a non-zero multiplicative function, A : S \ Iχ → ℂ is additive, ρ : Pχ → ℂ is the restriction of ΨAχ,ρ, and the following conditions hold.

ΨAχ,ρ(qt) = ΨAχ,ρ(tq) = 0 for all qIχ and tS \ Iχ.

If x ∈ {up, pv, upv} for pPχ and u, vS\Iχ, then xPχ and we have ρ(x) = ρ(p)χ(u), ρ(x) = ρ(p)χ(v), or ρ(x) = ρ(p)χ(uv), respectively.

Theorem 4.1.

The solutions f, g : S → ℂ of the functional equation (1.4) are the following pairs of functions.

f = g = 0.

SS2z0 and we have f=±gandgx=gz0xfor xS\S2z0,0forxS2z0, f = \pm g\;\;\;and\;\;\;g\left( x \right) = \left\{ {\matrix{ {{g_{{z_0}}}\left( x \right)} \hfill & {for\;x \in S\backslash {S^2}{z_0},} \hfill \cr 0 \hfill & {forx \in {S^2}{z_0},} \hfill \cr } } \right. where gz0 : S \ S2z0 → ℂ is an arbitrary non-zero function.

There exist a constant d ∈ ℂ \ {±1} and a multiplicative function χ on S with χ(z0) ≠ 0, such that f=dχz01d2χandg=χz01d2χ. f = {{d\chi \left( {{z_0}} \right)} \over {1 - {d^2}}}\chi \;\;\;and\;\;\;g = {{\chi \left( {{z_0}} \right)} \over {1 - {d^2}}}\chi .

There exist a constant c ∈ ℂ* \ {±i} and two different multiplicative functions χ1 and χ2 on S, with χ1(z0) ≠ 0 and χ2(z0) ≠ 0 such that f=χ1z0χ1χ2z0χ2ic1+candg=c1χ1z0χ1+cχ2z0χ2c1+c. f = - {{{\chi _1}\left( {{z_0}} \right){\chi _1} - {\chi _2}\left( {{z_0}} \right){\chi _2}} \over {i\left( {{c^{ - 1}} + c} \right)}}\;\;\;and\;\;\;g = {{{c^{ - 1}}{\chi _1}\left( {{z_0}} \right){\chi _1} + c{\chi _2}\left( {{z_0}} \right){\chi _2}} \over {{c^{ - 1}} + c}}.

There exist constants q, γ ∈ ℂ* and two different non-zero multiplicative functions χ1 and χ2 on S, with χ1z0=q2(1+ξ)22γq,χ2z0=q2(1ξ)22γq, {\chi _1}\left( {{z_0}} \right) = {{{q^2} - {{(1 + \xi )}^2}} \over {2\gamma q}},\;\;\;{\chi _2}\left( {{z_0}} \right) = - {{{q^2} - {{(1 - \xi )}^2}} \over {2\gamma q}}, and ξ:=±1+q2 \xi : = \pm \sqrt {1 + {q^2}} such that f=χ1+χ22γ+ξχ1χ22γandg=qχ1χ22γ. f = {{{\chi _1} + {\chi _2}} \over {2\gamma }} + \xi {{{\chi _1} - {\chi _2}} \over {2\gamma }}\;\;\;and\;\;\;g = q{{{\chi _1} - {\chi _2}} \over {2\gamma }}.

There exist constants q ∈ ℂ \ {±α}, γ ∈ ℂ* \ {±α} and δ ∈ ℂ \ {±1}, and two different non-zero multiplicative functions χ1 and χ2 on S, with χ1z0=(1+δ)2(α+q)22γ1+δ,χ2z0=(1δ)2(αq)22γ1δ, {\chi _1}\left( {{z_0}} \right) = {{{{(1 + \delta )}^2} - {{(\alpha + q)}^2}} \over {2\gamma \left( {1 + \delta } \right)}},\;\;\;\;{\chi _2}\left( {{z_0}} \right) = {{{{(1 - \delta )}^2} - {{(\alpha - q)}^2}} \over {2\gamma \left( {1 - \delta } \right)}}, and δ:=±1+q2α2 \delta : = \pm \sqrt {1 + {q^2} - {\alpha ^2}} such that f=αχ1+χ22γ+qχ1χ22γandg=χ1+χ22γ+δχ1χ22γ. f = \alpha {{{\chi _1} + {\chi _2}} \over {2\gamma }} + q{{{\chi _1} - {\chi _2}} \over {2\gamma }}\;\;\;and\;\;\;g = {{{\chi _1} + {\chi _2}} \over {2\gamma }} + \delta {{{\chi _1} - {\chi _2}} \over {2\gamma }}.

There exist a constant β ∈ ℂ*, a non-zero multiplicative function χ on S, an additive function A : S \ Iχ → ℂ and a function ρ : Pχ → ℂ with χ(z0) = 1/β and A(z0) = 0 such that f=1βΨAχ,ρandg=1βχ±ΨAχ,ρ. f = {1 \over \beta }{\Psi _{A\chi ,\rho }}\;\;\;and\;\;\;g = {1 \over \beta }\left( {\chi \pm {\Psi _{A\chi ,\rho }}} \right).

There exist a multiplicative function χ on S with χ(z0) ≠ 0, an additive function A : S \ Iχ → ℂ and a function ρ : Pχ → ℂ such that f=Az0χ+ΨAχ,ρandg=χz0±Az0χ+ΨAχ,ρ. f = A\left( {{z_0}} \right)\chi + {\Psi _{A\chi ,\rho }}\;\;\;and\;\;\;g = \left( {\chi \left( {{z_0}} \right) \pm A\left( {{z_0}} \right)} \right)\chi + {\Psi _{A\chi ,\rho }}.

Moreover, if S is a topological semigroup and f𝒞(S) then g𝒞(S) in cases (1), (2), (4)(8), and if d ≠ 0 then also in (3).

Proof

If g = 0, then (1.4) reduces to f (x)f (y) = 0 for all x, yS. This implies that f = 0, so we get the first part of solutions. From now we may assume that g ≠ 0.

If f and g are linearly dependent, then there exists d ∈ ℂ such that f = dg. Substituting this into (1.4) we get the following functional equation gxyz0=1d2gxgy,x,yS. g\left( {xy{z_0}} \right) = \left( {1 - {d^2}} \right)g\left( x \right)g\left( y \right),\;\;\;\;x,\;y \in S.

If d2 = 1, then g(xyz0) = 0 for all x, yS. Therefore, SS2z0 because g ≠ 0. So, we are in solution family (2) with gz0 an arbitrary non-zero function.

If d2 ≠ 1, then by [13, Proposition 16] there exists a multiplicative function χ on S such that χ(z0)χ := (1 − d2)g and χ(z0) ≠ 0. Then we deduce that g=χz01d2χ g = {{\chi \left( {{z_0}} \right)} \over {1 - {d^2}}}\chi and f=dg=dχz01d2χ f = dg = {{d\chi \left( {{z_0}} \right)} \over {1 - {d^2}}}\chi , so we have the solution family (3).

For the rest of the proof, we assume that f and g are linearly independent. We split the proof into two cases according to whether f (z0) = 0 or f (z0) ≠ 0.

Case I. Suppose f (z0) = 0. Then by Lemma 3.3 (i)-(3) and (i)-(1), we have g(z0) ≠ 0 and gz02gxy=gz0gxgygz0fxfy+fz02fxy,x,yS, g\left( {z_0^2} \right)g\left( {xy} \right) = g\left( {{z_0}} \right)g\left( x \right)g\left( y \right) - g\left( {{z_0}} \right)f\left( x \right)f\left( y \right) + f\left( {z_0^2} \right)f\left( {xy} \right),\;\;\;x,y \in S, respectively.

Subcase I.1. Assume that gz02=0 g\left( {z_0^2} \right) = 0 . Then by Lemma 3.3 (i)-(2) and (i)-(3), we get fz020 f\left( {z_0^2} \right) \ne 0 since f and g are linearly independent and then (4.1) can be rewritten as f (xy) = γf (x)f (y) − γg(x)g(y), x, yS, where γ:=gz0fz020 \gamma : = {{g\left( {{z_0}} \right)} \over {f\left( {z_0^2} \right)}} \ne 0 . Consequently, the pair (γf, γg) satisfies the cosine addition formula (1.1). So, according to [12, Theorem 6.1] and taking into account that f and g are linearly independent, we know that there are only the following possibilities.

(I.1.i) There exist a constant q ∈ ℂ* and two different non-zero multiplicative functions χ1 and χ2 on S such that γg=qχ1χ22 \gamma g = q{{{\chi _1} - {\chi _2}} \over 2} and γf=χ1+χ22±1+q2χ1χ22 \gamma f = {{{\chi _1} + {\chi _2}} \over 2} \pm \left( {\sqrt {1 + {q^2}} } \right){{{\chi _1} - {\chi _2}} \over 2} , which gives f=χ1+χ22γ±1+q2χ1χ22γ f = {{{\chi _1} + {\chi _2}} \over {2\gamma }} \pm \left( {\sqrt {1 + {q^2}} } \right){{{\chi _1} - {\chi _2}} \over {2\gamma }} and g=qχ1χ22γ g = q{{{\chi _1} - {\chi _2}} \over {2\gamma }} . By putting ξ:=±1+q2 \xi : = \pm \sqrt {1 + {q^2}} and using (1.4) we get 14γ2(q21+ξ)2χ1xy+14γ2(q21ξ)2χ2xy=q2γχ1z0χ1xyq2γχ2z0χ2xy, \matrix{ {{1 \over {4{\gamma ^2}}}({q^2} - \left( {1 + \xi {)^2}} \right){\chi _1}\left( {xy} \right) + {1 \over {4{\gamma ^2}}}({q^2} - \left( {1 - \xi {)^2}} \right){\chi _2}\left( {xy} \right)} \hfill \cr {\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; = {q \over {2\gamma }}{\chi _1}\left( {{z_0}} \right){\chi _1}\left( {xy} \right) - {q \over {2\gamma }}{\chi _2}\left( {{z_0}} \right){\chi _2}\left( {xy} \right),} \hfill \cr } which implies by Lemma 3.1 (i) that q2γχ1z0=14γ2(q21+ξ)2 {q \over {2\gamma }}{\chi _1}\left( {{z_0}} \right) = {1 \over {4{\gamma ^2}}}({q^2} - \left( {1 + \xi {)^2}} \right) and q2γχ2z0=14γ2(q21ξ)2 {q \over {2\gamma }}{\chi _2}\left( {{z_0}} \right) = - {1 \over {4{\gamma ^2}}}({q^2} - \left( {1 - \xi {)^2}} \right) , since χ1 and χ2 are different and non-zero. Then we deduce that χ1z0=12γq(q21+ξ)2andχ2z0=12γq(q21ξ)2. {\chi _1}\left( {{z_0}} \right) = {1 \over {2\gamma q}}({q^2} - \left( {1 + \xi {)^2}} \right)\;\;\;{\rm{and}}\;\;\;{\chi _2}\left( {{z_0}} \right) = - {1 \over {2\gamma q}}({q^2} - \left( {1 - \xi {)^2}} \right). So, we are in part (5).

(I.1.ii) There exist a non-zero multiplicative function χ on S, an additive function A on S \ Iχ and a function ρ on Pχ such that γg = ΨAχ,ρ and γf = χ ± ΨAχ,ρ.

If z0Iχ \ Pχ we have γg(z0) = ΨAχ,ρ(z0) = 0 by definition of ΨAχ,ρ. If z0Pχ we have χ(z0) = 0 and |γg(z0)|=(z0)|=(z0) ± ρ(z0)|=|γf (z0)|= 0. So, if z0Iχ we get that γg(z0) = 0, which is a contradiction because g(z0) ≠ 0 and γ=gz0fz02 \gamma = {{g\left( {{z_0}} \right)} \over {f\left( {z_0^2} \right)}} .

Hence, z0S \ Iχ and we have χ(z0) ≠ 0. Since f (z0) = 0, by the assumption, we get fz0=1γχz0±Az0χz0=0 f\left( {{z_0}} \right) = {1 \over \gamma }\left[ {\chi \left( {{z_0}} \right) \pm A\left( {{z_0}} \right)\chi \left( {{z_0}} \right)} \right] = 0 , which implies that A(z0) = −1. Now for all x, yS \ Iχ, we have xyz0S \ Iχ, then by using (1.4) we get 1γχz0χxy+1γ+χz0χxyAxy=0 \left( {{1 \over \gamma } - \chi \left( {{z_0}} \right)} \right)\chi \left( {xy} \right) + \left( {{1 \over \gamma } + \chi \left( {{z_0}} \right)} \right)\chi \left( {xy} \right)A\left( {xy} \right) = 0 , which implies according to Lemma 3.1(i), that 1γχz0=0 {1 \over \gamma } - \chi \left( {{z_0}} \right) = 0 and 1γ+χz0=0 {1 \over \gamma } + \chi \left( {{z_0}} \right) = 0 , since A ≠ 0. Therefore, χz0=1γ=1γ \chi \left( {{z_0}} \right) = {1 \over \gamma } = - {1 \over \gamma } , which is a contradiction because 1γ0 {1 \over \gamma } \ne 0 by the assumption. So we do not have a solution corresponding to this possibility.

Subcase I.2. Suppose that gz020 g\left( {z_0^2} \right) \ne 0 , then (4.1) can be rewritten as follows βg(xy) = β2g(x)g(y) − β2f (x)f (y) + αβf (xy), x, yS with β:=gz0gz020 \beta : = {{g\left( {{z_0}} \right)} \over {g\left( {z_0^2} \right)}} \ne 0 and α:=fz02gz02 \alpha : = {{f\left( {z_0^2} \right)} \over {g\left( {z_0^2} \right)}} . This shows that the pair (βg, βf) satisfies the functional equation (1.2). So, according to [12, Theorem 3.1], and taking into account that f and g are linearly independent, there are only the following possibilities.

(I.2.i) There exist a constant q ∈ ℂ\{±α} and two different non-zero multiplicative functions χ1 and χ2 on S such that βf=αχ1+χ22+qχ1χ22 \beta f = \alpha {{{\chi _1} + {\chi _2}} \over 2} + q{{{\chi _1} - {\chi _2}} \over 2} and βg=χ1+χ22±1+q2α2χ1χ22 \beta g = {{{\chi _1} + {\chi _2}} \over 2} \pm \sqrt {1 + {q^2} - {\alpha ^2}} {{{\chi _1} - {\chi _2}} \over 2} . Introducing δ:=±1+q2α2 \delta : = \pm \sqrt {1 + {q^2} - {\alpha ^2}} we find that f=αχ1+χ22β+qχ1χ22β f = \alpha {{{\chi _1} + {\chi _2}} \over {2\beta }} + q{{{\chi _1} - {\chi _2}} \over {2\beta }} and g=χ1+χ22β+δχ1χ22β g = {{{\chi _1} + {\chi _2}} \over {2\beta }} + \delta {{{\chi _1} - {\chi _2}} \over {2\beta }} . By using (1.4), we get 14β2((1+δ)2α+q)2χ1xy+14β2((1δ)2αq)2χ2xy=12β1+δχ1z0χ1xy+12β1δχ2z0χ2xy. \matrix{ {{1 \over {4{\beta ^2}}}({{(1 + \delta )}^2} - \left( {\alpha + q{)^2}} \right){\chi _1}\left( {xy} \right) + {1 \over {4{\beta ^2}}}({{(1 - \delta )}^2} - \left( {\alpha - q{)^2}} \right){\chi _2}\left( {xy} \right)} \hfill \cr {\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\; = {1 \over {2\beta }}\left( {1 + \delta } \right){\chi _1}\left( {{z_0}} \right){\chi _1}\left( {xy} \right) + {1 \over {2\beta }}\left( {1 - \delta } \right){\chi _2}\left( {{z_0}} \right){\chi _2}\left( {xy} \right).} \hfill \cr } So, by Lemma 3.1(i) we obtain 12β1+δχ1z0=14β2((1+δ)2α+q)2 {1 \over {2\beta }}\left( {1 + \delta } \right){\chi _1}\left( {{z_0}} \right) = {1 \over {4{\beta ^2}}}({(1 + \delta )^2} - \left( {\alpha + q{)^2}} \right) and 12β1δχ2z0=14β2((1δ)2αq)2 {1 \over {2\beta }}\left( {1 - \delta } \right){\chi _2}\left( {{z_0}} \right) = {1 \over {4{\beta ^2}}}({(1 - \delta )^2} - \left( {\alpha - q{)^2}} \right) , since χ1 and χ2 are different non-zero multiplicative functions. Notice that δ ≠ ±1 because q ≠ ±α. Therefore we deduce that χ1z0=(1+δ)2(α+q)22β1+δ {\chi _1}\left( {{z_0}} \right) = {{{{(1 + \delta )}^2} - {{(\alpha + q)}^2}} \over {2\beta \left( {1 + \delta } \right)}} and χ2z0=(1δ)2(αq)22β1δ {\chi _2}\left( {{z_0}} \right) = {{{{(1 - \delta )}^2} - {{(\alpha - q)}^2}} \over {2\beta \left( {1 - \delta } \right)}} . Hence, by writing γ instead of β we get part (6).

(I.2.ii) α ≠ 0 and there exist two different non-zero multiplicative functions χ1 and χ2 on S such that βf = αχ1 and βg = χ2. By using (1.4) again we get 1βχ2z01βχ2xy+α2β2χ1xy=0 {1 \over \beta }\left( {{\chi _2}\left( {{z_0}} \right) - {1 \over \beta }} \right){\chi _2}\left( {xy} \right) + {{{\alpha ^2}} \over {{\beta ^2}}}{\chi _1}\left( {xy} \right) = 0 , which gives χ2z0=1β {\chi _2}\left( {{z_0}} \right) = {1 \over \beta } and α = 0, since χ1 and χ2 are different. This possibility is excluded because α ≠ 0.

(I.2.iii) There exist a non-zero multiplicative function χ on S, an additive function A on S \ Iχ and a function ρ on Pχ such that βf = αχ + ΨAχ,ρ and βg = χ ± ΨAχ,ρ, which gives f=1βαχ+ΨAχ,ρ f = {1 \over \beta }\left( {\alpha \chi + {\Psi _{A\chi ,\rho }}} \right) and g=1βχ±ΨAχ,ρ g = {1 \over \beta }\left( {\chi \pm {\Psi _{A\chi ,\rho }}} \right) .

If g=1βχ+ΨAχ,ρ g = {1 \over \beta }\left( {\chi + {\Psi _{A\chi ,\rho }}} \right) then z0Iχ \ Pχ. Indeed, otherwise we have χ(z0) = 0 and ΨAχ,ρ(z0) = 0. Then βg(z0) = χ(z0) + ΨAχ,ρ(z0) = 0. This contradicts the fact that g(z0) ≠ 0.

On the other hand z0Pχ. Indeed, otherwise we have χ(z0) = 0. Then βg(z0) = ΨAχ,ρ(z0) = βf (z0) = 0, which is a contradiction because g(z0) ≠ 0. So, z0S \ Iχ and then χ(z0) ≠ 0. Since f (z0) = 0 we get that fz0=χz0βα+Az0=0 f\left( {{z_0}} \right) = {{\chi \left( {{z_0}} \right)} \over \beta }\left[ {\alpha + A\left( {{z_0}} \right)} \right] = 0 , which implies that A(z) = − α. Now, let x, yS \ Iχ be arbitrary. We have xyz0S \ Iχ. By using (1.4), we get 1α2β2+α1βχz0χxy+1αβ21βχz0χxyAxy=0. \left( {{{1 - {\alpha ^2}} \over {{\beta ^2}}} + {{\alpha - 1} \over \beta }\chi \left( {{z_0}} \right)} \right)\chi \left( {xy} \right) + \left( {{{1 - \alpha } \over {{\beta ^2}}} - {1 \over \beta }\chi \left( {{z_0}} \right)} \right)\chi \left( {xy} \right)A\left( {xy} \right) = 0.

If A = 0 then ρ ≠ 0 because ΨAχ,ρ ≠ 0, α = 0, and χz0=1β \chi \left( {{z_0}} \right) = {1 \over \beta } by (4.2). This is a special case of solution part (7).

If A ≠ 0 then by Lemma 3.1 (ii) we get from (4.2) that 1α2β2+α1βχz0=0and1αβ21βχz0=0. {{1 - {\alpha ^2}} \over {{\beta ^2}}} + {{\alpha - 1} \over \beta }\chi \left( {{z_0}} \right) = 0\;\;\;{\rm{and}}\;\;\;{{1 - \alpha } \over {{\beta ^2}}} - {1 \over \beta }\chi \left( {{z_0}} \right) = 0. As α ≠ 1, because χ(z0) ≠ 0, we deduce that χz0=1αβ \chi \left( {{z_0}} \right) = {{1 - \alpha } \over \beta } and χz0=1+αβ \chi \left( {{z_0}} \right) = {{1 + \alpha } \over \beta } . So, we obtain that α = 0 and χz0=1β \chi \left( {{z_0}} \right) = {1 \over \beta } , and the form of f reduces to f=1βΨAχ,ρ f = {1 \over \beta }{\Psi _{A\chi ,\rho }} . So we are in part (7).

If g=1βχΨAχ,ρ g = {1 \over \beta }\left( {\chi - {\Psi _{A\chi ,\rho }}} \right) , by using a similar computation as above, we show that we are also in part (7).

Case II. Suppose f (z0) ≠ 0. By using system (1.4) and (3.4), we deduce by an elementary computation that for any λ ∈ ℂ gλfxyz0=gλfxgλfyλ2+μλ+1fxfy,x,yS. \matrix{ {\left( {g - \lambda f} \right)\left( {xy{z_0}} \right)} \hfill \cr {\;\;\;\;\;\;\;\;\; = \left( {g - \lambda f} \right)\left( x \right)\left( {g - \lambda f} \right)\left( y \right) - \left( {{\lambda ^2} + \mu \lambda + 1} \right)f\left( x \right)f\left( y \right),\;\;\;\;x,\;y \in S.} \hfill \cr } Let λ1 and λ2 be the two roots of the equation λ2 +µλ+1 = 0. Then λ1λ2 = 1 which gives λ1 ≠ 0 and λ2 ≠ 0. According to [13, Proposition 16] we deduce from (4.3) that gλ1f := χ1(z0)χ1 and gλ2f := χ2(z0)χ2, where χ1 and χ2 are two multiplicative functions such that χ1(z0) ≠ 0 and χ2(z0) ≠ 0, because f and g are linearly independent.

If λ1λ2, then χ1χ2 and we get g=λ2χ1z0χ1λ1χ2z0χ2λ2λ1 g = {{{\lambda _2}{\chi _1}\left( {{z_0}} \right){\chi _1} - {\lambda _1}{\chi _2}\left( {{z_0}} \right){\chi _2}} \over {{\lambda _2} - {\lambda _1}}} and f=χ1z0χ1χ2z0χ2λ2λ1 f = {{{\chi _1}\left( {{z_0}} \right){\chi _1} - {\chi _2}\left( {{z_0}} \right){\chi _2}} \over {{\lambda _2} - {\lambda _1}}} . By putting λ1 = ic, we get the solution of category (4).

If λ1 = λ2 =: λ, then gλf =: χ(z0)χ where χ is a multiplicative function on S such that χ(z0) ≠ 0, because f and g are linearly independent. Hence, g=χz0χ+λf. g = \chi \left( {{z_0}} \right)\chi + \lambda f. Substituting this in (3.4), an elementary computation shows that fxyz0=χz0fxχy+χz0fyχx+2λ+μfxfy, f\left( {xy{z_0}} \right) = \chi \left( {{z_0}} \right)f\left( x \right)\chi \left( y \right) + \chi \left( {{z_0}} \right)f\left( y \right)\chi \left( x \right) + \left( {2\lambda + \mu } \right)f\left( x \right)f\left( y \right), for all x, yS.

Moreover λ = 1 or λ = −1 because λ1λ2 = 1. Hence, (λ, µ) = (1, −2) or (λ, µ) = (−1, 2) since λ2 + µλ + 1 = 0 and λ ∈ {−1, 1}. So, the functional equation above reduces to fxyz0=χz0fxχy+χz0fyχx, f\left( {xy{z_0}} \right) = \chi \left( {{z_0}} \right)f\left( x \right)\chi \left( y \right) + \chi \left( {{z_0}} \right)f\left( y \right)\chi \left( x \right), for all x, yS. Thus, the function f satisfies (3.1). Hence, in view of Proposition 3.2, we get f = A(z0)χ + ΨAχ,ρ. Then, by (4.4), we derive that g = χ(z0)χ + λ f = (χ(z0) + λ A(z0))χ + λ2ΨAχ,ρ = (χ(z0) ± A(z0))χ + ΨAχ,ρ. This is part (8).

Conversely, it is easy to check that the formulas for f and g listed in Theorem 4.1 define solutions of (1.4).

Finally, suppose that S is a topological semigroup. The continuity of the solutions of the forms (1)–(6) follows directly from [11, Theorem 3.18], and for the ones of the forms (7) and (8) it is parallel to the proof used in [5, Theorem 2.1] for categories (7) and (8). This completes the proof of Theorem 4.1.

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