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Introduction
The addition law for cosine is
\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:
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
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
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
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
\left( {{g \over \beta },\;{f \over \beta }} \right)
satisfies the following functional equation
{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, y ∈ S, and that f is abelian if f (x1x2, . . . , xn) = f (xσ(1)xσ(2), . . . , xσ(n)) for all x1, x2, . . . , xn ∈ S, 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, y ∈ S and a map χ : S → ℂ is multiplicative if χ(xy) = χ(x)χ(y), for all x, y ∈ S. If χ ≠ 0, then the nullspace Iχ := {x ∈ S | 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 T ⊆ S let T2 := {xy | x, y ∈ T } and for any fixed element z0 in S we let T2z0 := {xyz0 | x, y ∈ T}.
To express solutions of our functional equations studied in this paper we will use the set
{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
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), thenf\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 x ∈ Iχ \ Pχ and y ∈ S \ Iχ.
If x ∈ {up, pv, upv} with p ∈ Pχ and u, v ∈ S \ Iχ, then x ∈ Pχ 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 f ∈ 𝒞(S), then χ ∈ 𝒞(S), A ∈ 𝒞(S \ Iχ) and ρ ∈ 𝒞(Pχ).
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, y ∈ S,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{(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 thatf\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
\left( {xy,z_0^2} \right)
and (xyz0, z0) in (1.4) we get
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
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
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
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
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 y ∈ S then 0 = g(xyz0) = g(x)g(y) − f (x)f (y), x, y ∈ S. So, g(x)g(y) = f (x)f (y), x, y ∈ S. 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 a ∈ S 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
\left( {x,yz_0^2} \right)
and (xyz0, z0) in (1.4) we get
g\left( {xyz_0^3} \right)
=
g\left( x \right)g\left( {yz_0^2} \right)
−
f\left( x \right)f\left( {yz_0^2} \right)
= g(z0)g(x)g(y) − g(x)f(z0)f(y) −
f\left( x \right)f\left( {yz_0^2} \right)
and
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
\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
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
\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.,
{\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 q ∈ Iχ and t ∈ S \ Iχ.
If x ∈ {up, pv, upv} for p ∈ Pχ and u, v ∈ S\Iχ, then x ∈ Pχ 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.
S ≠ S2z0and we havef = \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 thatf = {{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 χ1and χ2on S, with χ1(z0) ≠ 0 and χ2(z0) ≠ 0 such thatf = - {{{\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 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 thatf = {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 thatf = 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 f ∈ 𝒞(S) then g ∈ 𝒞(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, y ∈ S. 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
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, y ∈ S. Therefore, S ≠ S2z0 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 = {{\chi \left( {{z_0}} \right)} \over {1 - {d^2}}}\chi
and
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
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
g\left( {z_0^2} \right) = 0
. Then by Lemma 3.3 (i)-(2) and (i)-(3), we get
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, y ∈ S, where
\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
\gamma g = q{{{\chi _1} - {\chi _2}} \over 2}
and
\gamma f = {{{\chi _1} + {\chi _2}} \over 2} \pm \left( {\sqrt {1 + {q^2}} } \right){{{\chi _1} - {\chi _2}} \over 2}
, which gives
f = {{{\chi _1} + {\chi _2}} \over {2\gamma }} \pm \left( {\sqrt {1 + {q^2}} } \right){{{\chi _1} - {\chi _2}} \over {2\gamma }}
and
g = q{{{\chi _1} - {\chi _2}} \over {2\gamma }}
. By putting
\xi : = \pm \sqrt {1 + {q^2}}
and using (1.4) we get
\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
{q \over {2\gamma }}{\chi _1}\left( {{z_0}} \right) = {1 \over {4{\gamma ^2}}}({q^2} - \left( {1 + \xi {)^2}} \right)
and
{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
{\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 z0 ∈ Iχ \ Pχ we have γg(z0) = ΨAχ,ρ(z0) = 0 by definition of ΨAχ,ρ. If z0 ∈ Pχ we have χ(z0) = 0 and |γg(z0)|=|ρ(z0)|=|χ(z0) ± ρ(z0)|=|γf (z0)|= 0. So, if z0 ∈ Iχ we get that γg(z0) = 0, which is a contradiction because g(z0) ≠ 0 and
\gamma = {{g\left( {{z_0}} \right)} \over {f\left( {z_0^2} \right)}}
.
Hence, z0 ∈ S \ Iχ and we have χ(z0) ≠ 0. Since f (z0) = 0, by the assumption, we get
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, y ∈ S \ Iχ, we have xyz0 ∈ S \ Iχ, then by using (1.4) we get
\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
{1 \over \gamma } - \chi \left( {{z_0}} \right) = 0
and
{1 \over \gamma } + \chi \left( {{z_0}} \right) = 0
, since A ≠ 0. Therefore,
\chi \left( {{z_0}} \right) = {1 \over \gamma } = - {1 \over \gamma }
, which is a contradiction because
{1 \over \gamma } \ne 0
by the assumption. So we do not have a solution corresponding to this possibility.
Subcase I.2. Suppose that
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, y ∈ S with
\beta : = {{g\left( {{z_0}} \right)} \over {g\left( {z_0^2} \right)}} \ne 0
and
\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
\beta f = \alpha {{{\chi _1} + {\chi _2}} \over 2} + q{{{\chi _1} - {\chi _2}} \over 2}
and
\beta g = {{{\chi _1} + {\chi _2}} \over 2} \pm \sqrt {1 + {q^2} - {\alpha ^2}} {{{\chi _1} - {\chi _2}} \over 2}
. Introducing
\delta : = \pm \sqrt {1 + {q^2} - {\alpha ^2}}
we find that
f = \alpha {{{\chi _1} + {\chi _2}} \over {2\beta }} + q{{{\chi _1} - {\chi _2}} \over {2\beta }}
and
g = {{{\chi _1} + {\chi _2}} \over {2\beta }} + \delta {{{\chi _1} - {\chi _2}} \over {2\beta }}
. By using (1.4), we get
\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
{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
{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
{\chi _1}\left( {{z_0}} \right) = {{{{(1 + \delta )}^2} - {{(\alpha + q)}^2}} \over {2\beta \left( {1 + \delta } \right)}}
and
{\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
{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
{\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 = {1 \over \beta }\left( {\alpha \chi + {\Psi _{A\chi ,\rho }}} \right)
and
g = {1 \over \beta }\left( {\chi \pm {\Psi _{A\chi ,\rho }}} \right)
.
If
g = {1 \over \beta }\left( {\chi + {\Psi _{A\chi ,\rho }}} \right)
then z0 ∉ Iχ \ 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 z0 ∉ Pχ. 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, z0 ∈ S \ Iχ and then χ(z0) ≠ 0. Since f (z0) = 0 we get that
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, y ∈ S \ Iχ be arbitrary. We have xyz0 ∈ S \ Iχ. By using (1.4), we get
\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
\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
{{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
\chi \left( {{z_0}} \right) = {{1 - \alpha } \over \beta }
and
\chi \left( {{z_0}} \right) = {{1 + \alpha } \over \beta }
. So, we obtain that α = 0 and
\chi \left( {{z_0}} \right) = {1 \over \beta }
, and the form of f reduces to
f = {1 \over \beta }{\Psi _{A\chi ,\rho }}
. So we are in part (7).
If
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
\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 g−λ1f := χ1(z0)χ1 and g−λ2f := 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 λ1 ≠ λ2, then χ1 ≠ χ2 and we get
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 = {{{\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 g − λf =: 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 = \chi \left( {{z_0}} \right)\chi + \lambda f.
Substituting this in (3.4), an elementary computation shows that
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, y ∈ S.
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
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, y ∈ S. 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.