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Let $a_n$ be a sequence of strictly positive real numbers such that $\lim_{n \to \infty}a_n=0$. Find all functions $f: \mathbb{R} \to \mathbb{R}$ that admit primitives (i.e. there exists a function $F:\mathbb{R} \to \mathbb{R}$ such that $\frac{dF(x)}{dx}=f(x), \forall x \in \mathbb{R}$) and satisfy the following equality $$2f(x)=f(x+a_n)+f(x-a_n), \forall x \in \mathbb{R}, \forall n \in \mathbb{N}$$ I have already posted this question here but I got no answer.

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$\newcommand{\De}{\Delta}$This problem can be solved by using the Fourier transform -- cf. this previous answer.

Let us present here an elementary solution:

Letting $G_n(x):=F(x+a_n)+F(x-a_n)-2F(x)$, we get $G'_n(x)=f(x+a_n)+f(x-a_n)-2f(x)=0$ for all $x$. So, \begin{equation*} c_n:=G_n(x) \tag{1}\label{1} \end{equation*} does not depend on $x$.

Take any real $A$ and $B$ such that $A<B$. Let $k_n:=\lfloor\frac{B-A}{a_n}\rfloor$, so that \begin{equation*} k_n\sim \frac{B-A}{a_n}, \end{equation*} $A+k_n a_n\to B$, and, by \eqref{1}, $\De_x(a_n):=F(x+a_n)-F(x)=\De_{x-a_n}(a_n)+c_n$ for all $x$, so that \begin{equation*} F(A+k_n a_n)-F(A)=k_n \De_A(a_n)+\frac{k_n(k_n-1)}2\,c_n \\ =(1+o(1))(B-A)\frac{\De_A(a_n)}{a_n}+\frac{1+o(1)}2\,(B-A)^2\frac{c_n}{a_n^2}, \end{equation*} whence \begin{equation*} \frac{\De_A(a_n)}{a_n} =(1+o(1))\frac{F(A+k_n a_n)-F(A)}{B-A}-\frac{1+o(1)}2\,(B-A)\frac{c_n}{a_n^2}. \tag{2}\label{2} \end{equation*} Similarly, for any real $C>B$, \begin{equation*} \frac{\De_A(a_n)}{a_n} =(1+o(1))\frac{F(A+m_n a_n)-F(A)}{C-A}-\frac{1+o(1)}2\,(C-A)\frac{c_n}{a_n^2}, \tag{3}\label{3} \end{equation*} where $m_n:=\lfloor\frac{C-A}{a_n}\rfloor$.

The function $F$ is differentiable and hence continuous. So, $F(A+k_n a_n)\to F(B)$ and $F(A+m_n a_n)\to F(C)$. Subtracting now \eqref{2} from \eqref{3}, we get \begin{equation} \frac12\,\frac{c_n}{a_n^2}\to\frac{\De_A(C-A)-\De_A(B-A)}{C-B}. \end{equation} It follows now by \eqref{2} that $\frac{\De_A(a_n)}{a_n}$ converges to a finite limit as well, and thus \begin{equation} F(B)-F(A)=K_1(B-A)+\frac{K_2}2\,(B-A)^2 \end{equation} for some real $K_1,K_2$ and all real $A$ and $B$ such that $A<B$.

We conclude that $F$ is a quadratic polynomial and hence $f=F'$ is an affine function. (Vice versa, any affine function $f$ satisfies your system of functional equations.)


The above proof can be simplified a bit by noting that the limit of $\frac{\De_A(a_n)}{a_n}$ exists (and equals $F'(0)$). However, the advantage of the above proof is that it shows that the conclusion that the only solutions to the system \eqref{1} of functional equations are quadratic polynomials can be reached assuming a priori only the continuity of $F$.

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$\newcommand\de\delta$Let us also present the Fourier transform argument, assuming that $|F|$ is bounded by a polynomial, so that $F$ may be considered a (tempered) distribution (in the generalized-function sense). Let then $\hat F$ denote the Fourier transform of $F$.

Equation (1) in the other answer yields $$c_n\de(t)=\hat G_n(t)=e^{ita_n}\hat F(t)+e^{-ita_n}\hat F(t)-2\hat F(t) =2\hat F(t)(\cos ta_n-1),$$ where $\de$ is the delta function.

If the equality $\cos ta_n-1=0$ takes place for some real $t$ and all $n$, then $t=0$ (since the $a_n$'s are nonzero and go to $0$). So, the support of $\hat F$ is $\{0\}$. So (see e.g. "For every compact subset $K\subseteq U$ there exist constants $C_{K}>0$ and $N_{K}\in \mathbb {N}$ such that for all $f\in C_{c}^{\infty }(U)$ with support contained in $K$ [...]" here), we have $\hat F=\sum_{j=0}^n a_j\de^{(j)}$ for some $n\in\{0,1,\dots\}$ and some complex $a_j$'s, where $\de^{(j)}$ is the $j$th derivative of the delta function $\de$. So, $F$ is a polynomial. Since the second difference $G_n$ of $F$ is (the) constant ($c_n$), it follows that the polynomial $F$ is quadratic. Thus, $f=F'$ is an affine function. (Vice versa, any affine function $f$ satisfies your system of functional equations.)

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  • $\begingroup$ @AlexandreEremenko : Thank you for your comment. This is now fixed. $\endgroup$ Commented Feb 10, 2023 at 17:04
  • $\begingroup$ @AlexandreEremenko : You seem to be referring to Theorem 16.4.1 in Hormander's The analysis of linear partial differential operators. However, (i) that theorem seems to describe only smooth solutions and (ii) it describes them as limits in $C^\infty$ of linear combinations of exponential solutions. So, I don't see ready-to-use more general conditions there. On the other hand, the simple and elementary solution at mathoverflow.net/a/440497/36721 is indeed more general, as it is applicable to any continuous $F$. $\endgroup$ Commented Feb 12, 2023 at 17:35
  • $\begingroup$ @AlexandreEremenko : I cannot understand your latter comment. It does not seem to contain a sentence. $\endgroup$ Commented Feb 12, 2023 at 17:49
  • $\begingroup$ @AlexandreEremenko : Again, I do not understand your latter comment. In my first answer, the Fourier transform is not used at all. In my second answer, the polynomial growth condition is imposed, under which the Fourier transform does exist. However, the issue now is with your "more general" claim, discussed in my long comment, to which I have not seen an adequate response. $\endgroup$ Commented Feb 12, 2023 at 18:27
  • $\begingroup$ @AlexandreEremenko : How do you propose to do that (of course without requiring the $C^\infty$ condition)? My first answer here does exactly do that, in a simple and elementary way, only assuming the continuity of $F$. On the other hand, you seemed to claim to have more general conditions in your answer at mathoverflow.net/questions/438494/… -- but, after all this discussion, I still do not see more general conditions there. ?? $\endgroup$ Commented Feb 12, 2023 at 22:03

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