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On a Generalized Conjecture by Alzer and Matkowski Cover

On a Generalized Conjecture by Alzer and Matkowski

Open Access
|Apr 2025

Full Article

1. Introduction

Alzer and Matkowski [1] recently studied the following functional equation:

(1.1)
fx+y=fxfyαxy,x,y,
where α ∈ ℝ is a non-zero parameter and f : ℝ → ℝ is an unknown function. They proved two theorems on equation (1.1). The first result with a short proof [1, Theorem 1] completely describes solutions of (1.1) in case f has a zero. More precisely, they showed that if f solves (1.1) and it has a zero, then α > 0 and either fx=1αx , or fx=1+αx for x ∈ ℝ. The second theorem with a longer proof [1, Theorem 2] provides the solutions to equation (1.1) under the assumption that f : ℝ → ℝ is differentiable at least at one point. In this case, there are the same two solutions (clearly, both are differentiable and have a zero). In [1] the authors formulated the following conjecture:

Conjecture (Alzer and Matkowski)

Every solution f : ℝ → ℝ of (1.1) has a zero.

This conjecture has been answered affirmatively by T. Małolepszy, see [4]. In the present note, we will determine the solutions of a more general equation, namely

(1.2)
fx+y=fxfyϕx,y,x,yX,
where X is a linear space over the field 𝕂 ∈{ℝ,ℂ}, ϕ: X × X → 𝕂 is a biadditive functional and f : X → 𝕂 is a function. The motivation for such a generalization comes from an article by K. Baron and Z. Kominek [2], in which the authors, in connection with a problem proposed by S. Rolewicz [5], studied mappings defined on a real linear space with the additive Cauchy difference bounded from below by a bilinear functional.

2. Main results

In this section, it is assumed that X is a linear space over 𝕂 ∈ {ℝ,ℂ}, ϕ: X × X → 𝕂 is a biadditive functional and f : X → 𝕂. We will consider two situations, depending on the behavior of the biadditive functional ϕ on the diagonal.

Theorem 1

Assume that ϕ and f solve (1.2) and

(2.1)
z0Xϕz0,z00.
Then there exists a unique constant a ∈ 𝕂 \ {0} such that
(2.2)
fx=aϕx,z0+1,xX,
and moreover
(2.3)
a2ϕ(x,z0)2=ϕx,x,xX.

Proof

Substituting y = z0 and then y = −z0 in (1.2) we obtain

fx+z0=fxfz0ϕx,z0,xX
and
fxz0=fxfz0+ϕx,z0,xX.
Replace x by x + z0 in the latter formula and join it with the former one to arrive at
fx=fx+z0fz0+ϕx+z0,z0=fxfz0ϕx,z0fz0+ϕx,z0+ϕz0,z0,xX.

Denote c := f(z0), d := f(−z0) and β = ϕ(z0, z0) ≠ 0. We get

1cdfx=1dϕx,z0+β,xX.
As stated in the proof of Theorem 1 in [1], it follows that f(0) = 1. The argument works in our case, as well. Indeed, substitution x = y = 0 in (1.2) gives us f(0)2 = f(0), so f(0) = 0 or f(0) = 1. But f(0) = 0 would imply β = 0, which is a contradiction with the definition of β.

Therefore, from (1.2) applied for x = z0 and y = −z0 we deduce

1=fz0z0=fz0fz0+β,
thus 1 − cd = β. Since β ≠ 0, then denoting a := (1 − d) we get (2.2). The case a = 0 is impossible, since it leads to a contradiction with (2.1).

To prove equality (2.3) apply (1.2) with substitution y = −x to obtain

fxfx=1ϕx,x,xX.
Now, use the already proven formula (2.2) to derive (2.3) after some reductions.

Remark 1

From Theorem 1, we see that under assumption (2.1) and with a fixed functional ϕ there are always either no solutions or exactly two solutions f of (1.2). Indeed, if f is a solution, then it must be of the form (2.2) with some constant a ∈ 𝕂 \ {0}. Substituting this into (1.2) leads us to the equality:

a2ϕx,z0ϕy,z0=ϕx,y,x,yX,
which is true for two different values of a ≠ 0. Therefore, in case there do exist solutions, functional ϕ is of the form
ϕx,y=a2FxFy,x,yX,
with an additive, nonzero functional F : X → 𝕂, and the two possible functions f are given by (2.2).

We have the following corollary in the real case.

Corollary 1

Assume that 𝕂 = ℝ and

(2.4)
z0Xϕz0,z0<0.
Then equation (1.2) has no solutions.

Proof

Inequality (2.4) implies that condition (2.1) holds true. Then, from Theorem 1 we obtain formula (2.3). However, in the real case formula (2.3) implies that ϕ(x, x) ≥ 0 for all xX, which leads to a contradiction with (2.1).

In the complex case, every element of the field has a complex root of second order. Therefore, we can state the next corollary.

Corollary 2

Assume that 𝕂 = ℂ, ϕ and f solve (1.2), ϕ satisfies (2.1) and w: X → ℂ is a map such that

w2x=ϕx,x,xX.
Then
fx=wx+1,xX,
or
fx=wx+1,xX.

The next theorem deals with the remaining case for ϕ and is easy to prove.

Theorem 2

Assume that ϕ and f solve (1.2) and

zXϕz,z=0.
Then ϕ = 0 on X × X and
fx+y=fxfy,x,yX.
Consequently, either f = 0 or there exists an additive functional A: X → 𝕂 such that f = exp ∘ A.

Proof

It suffices to apply a well-known result, which states that if a multiadditive function vanishes on a diagonal, then it vanishes everywhere, cf. [3, Corollary 15.9.1, p. 448]. The final part follows from the form of solutions of the exponential Cauchy equation, cf. [3, Theorem 13.1.1, p. 343].

The following corollary is immediate and offers an alternative proof of the conjecture by Alzer and Matkowski.

Corollary 3 (T. Małolepszy)

Assume that α ∈ ℝ and f : ℝ → ℝ solves (1.1). Then α ≥ 0 and moreover, in case α > 0 either fx=1αx , or fx=1+αx for x ∈ ℝ. Conversely, both mappings solve (1.1).

Proof

Firstly, substituting α = 0 in (1.1) we obtain the exponential Cauchy’s equation, for which the solutions are known. Now assume that α ≠ 0, 𝕂 = ℝ, X = ℝ and ϕ(x, y) := αxy. Let z0 = 1. Then β = ϕ(1, 1) = α ≠ 0. From (2.2) we have

fx=aϕx,1+1=aαx+1,x.
From (2.3) we obtain
a2(αx)2=ϕx,x=αx2,x.
We get a2 = 1, so α > 0 and a=±1/α . After substitution to the equation for f we arrive at fx=±αx+1 . Conversely, it is easy to check that both such mappings solve (1.1).

Our last corollary is a complex counterpart of Corollary 3.

Corollary 4

Assume that α ∈ ℂ \ {0} and f : ℂ → ℂ solves

(2.5)
fx+y=fxfyαxy,x,y.
Then either f(x) = 1 + w1x, or f(x) = 1 + w2x for x ∈ ℂ, where w1,w2 are two complex roots of the second order of α. Conversely, both mappings solve (2.5).

Proof

Assume that 𝕂 = ℂ, X = ℂ and ϕ(x, y) := αxy. By repeating steps from the previous proof (this time without assuming α > 0), we obtain demanded results.

3. Examples and final remarks

We observe that Theorem 1 generally works only in one direction, that is, the converse implications do not necessarily hold.

Example 1

Let X be an inner product space of dimension at least 2 and define ϕ := 〈·, ·〉. Then, Theorem 1 implies that the potential solutions f : X → 𝕂 of (1.2) are of the form

f(x)=x,ξ+1,xX,
with some ξX. One can check that such mapping solves (1.2) if and only if
x,ξy,ξ=x,y,x,yX,
which is impossible if dim X ≥ 2.

It may be suspected that in higher dimensions, there are no solutions to (1.2). However, the following example demonstrates that this is not the case.

Example 2

Let X be a complex linear space and A: X → ℂ an additive nonzero functional. Define ϕ(x, y) := −A(x) · A(y) for x, yX. Then, according to Theorem 1 every solution f : X → ℂ of (1.2) is of the form:

fx=γAx+1,xX
with some constant γ ∈ ℂ. A direct calculation shows that f is indeed a solution if and only if γ = ±i.

We can choose A in such a way that A(x) ≠ 0 whenever x ≠ 0, or such that A has a bigger set of zeros. Therefore, for every complex linear space X there is an abundance of nontrivial solutions (f, ϕ) to (1.2).

This example also illustrates that the assertion of Corollary 1 does not hold in the case of complex spaces, even when the values of ϕ are real (since A may only attain real values, as it does not necessarily have to be linear).

A counterpart of the above example that works in both cases, real and complex, is also possible.

Example 3

Let X be a linear space over the field 𝕂 and A: X → 𝕂 an additive nonzero functional. Define ϕ(x, y) := A(x) · A(y) for x, yX. Then, similarly every solution f : X → 𝕂 of (1.2) is of the form:

fx=δAx+1,xX
with some constant δ ∈ 𝕂. Further, f is indeed a solution if and only if δ = ±1.

DOI: https://doi.org/10.2478/amsil-2025-0007 | Journal eISSN: 2391-4238 (formerly 0860-2107) | Journal ISSN: 0860-2107
Language: English
Page range: 77 - 82
Submitted on: Feb 3, 2025
Accepted on: Mar 31, 2025
Published on: Apr 27, 2025
Published by: University of Silesia in Katowice, Institute of Mathematics
In partnership with: Paradigm Publishing Services

© 2025 Włodzimierz Fechner, Marta Pierzchałka, Gabriela Smejda, published by University of Silesia in Katowice, Institute of Mathematics
This work is licensed under the Creative Commons Attribution 4.0 License.