Criterion for Boundedness of Power Series
Table of Contents
Introduction & Problem Statement #
Power series constitute one of the most ubiquitous objects in analysis. A power series $\sum_{n=0}^{\infty}a_n x^n$ with infinite radius of convergence defines a real-entire function $f:\mathbb{R}\to\mathbb{R}$. Whereas the question of convergence is completely settled by Cauchy–Hadamard theory, the question of boundedness of the sum function is far subtler and, as of this writing, remains open.
Let $(a_n) _{n\ge 0}$ be a sequence of real numbers such that the power series $\sum _{n=0}^{\infty}a_n x^n$ converges for every $x\in\mathbb{R}$, thereby defining a smooth function $f:\mathbb{R}\to\mathbb{R}$. Give a necessary and sufficient criterion on $(a_n)$ for $f$ to be bounded on $\mathbb{R}$.
The problem is rated low importance on the Open Problem Garden and is recommended as accessible to undergraduates; nevertheless, a complete answer appears to be unknown.
Motivating examples.
| Function | Power series | Bounded? |
|---|---|---|
| $\cos x$ | $\displaystyle\sum_{k=0}^{\infty}\frac{(-1)^k}{(2k)!}x^{2k}$ | $|\cos x|\le 1$ |
| $\sin x$ | $\displaystyle\sum_{k=0}^{\infty}\frac{(-1)^k}{(2k+1)!}x^{2k+1}$ | $|\sin x|\le 1$ |
| $e^x$ | $\displaystyle\sum_{n=0}^{\infty}\frac{x^n}{n!}$ | $e^x\to+\infty$ |
| $p(x)=a_0+\cdots+a_Nx^N,\ N\ge 1$ | (polynomial) | unbounded |
Background & Prerequisites #
This section collects the core mathematical tools needed to engage seriously with Question 1.
Power Series and Entire Functions #
A power series centred at the origin is a formal series $\sum_{n=0}^{\infty}a_n x^n$ with $a_n\in\mathbb{R}$. Its radius of convergence is $$ R = \frac{1}{\limsup_{n\to\infty}|a_n|^{1/n}} \in [0,+\infty]. $$
Throughout this note we always assume $R=+\infty$, i.e., $\limsup_{n\to\infty}|a_n|^{1/n}=0$.
A function $f:\mathbb{C}\to\mathbb{C}$ is called entire if it is holomorphic on all of $\mathbb{C}$. Every power series with $R=+\infty$ defines a real-entire function, and by the identity theorem its complex extension is entire.
The radius of convergence of $\sum a_n z^n$ equals $$ R = \Bigl(\limsup_{n\to\infty}|a_n|^{1/n}\Bigr)^{-1}. $$
The condition $R=+\infty$ is equivalent to $a_n = O(r^n/n!)$ for every $r>0$, i.e., the coefficients decay faster than any geometric sequence. This is the Paley–Wiener type condition for entire functions of order $1$.
Order and Type of Entire Functions #
The order of an entire function $f$ is $$ \rho = \limsup_{r\to\infty}\frac{\log\log M(r)}{\log r}, \qquad M(r)=\max_{|z|=r}|f(z)|. $$ The type $\sigma$ (for $0<\rho<\infty$) is $$ \sigma = \limsup_{r\to\infty}\frac{\log M(r)}{r^{\rho}}. $$
A bounded complex entire function has order $\rho=0$ (by Liouville’s theorem it must be constant), while a bounded real-valued entire function can be non-constant. Boundedness is therefore a genuinely real-variable phenomenon.
Liouville’s Theorem and Its Limitations #
Every bounded entire function $f:\mathbb{C}\to\mathbb{C}$ is constant.
Question 1 concerns real-valued functions $f:\mathbb{R}\to\mathbb{R}$. A function may be bounded on $\mathbb{R}$ while its complex extension is unbounded. For instance, $\cos z$ satisfies $|\cos z|\to\infty$ along the imaginary axis (since $\cos(iy)=\cosh y\to+\infty$). Liouville’s theorem therefore does not apply, and the problem is genuinely non-trivial.
Algebraic Structure of the Relevant Function Space #
Let $\mathcal{B}$ denote the set of all functions $f:\mathbb{R}\to\mathbb{R}$ that can be represented as a convergent power series $\sum_{n\ge 0}a_n x^n$ (with $R=+\infty$) and that are bounded on $\mathbb{R}$.
- $\mathcal{B}$ is a linear subspace of $C^\infty(\mathbb{R})$: if $f,g\in\mathcal{B}$ and $\lambda\in\mathbb{R}$ then $f+\lambda g\in\mathcal{B}$.
- $\mathcal{B}$ is closed under pointwise multiplication: if $f,g\in\mathcal{B}$ then $fg\in\mathcal{B}$.
- $\mathcal{B}$ contains all functions of the form $c\cos(h(x))$, where $c\in\mathbb{R}$ and $h:\mathbb{R}\to\mathbb{R}$ is any entire function.
Part (3) follows from $\cos(h(x)) = \operatorname{Re}(e^{ih(x)})$ together with $|\cos(h(x))|\le 1$. The class is strictly larger than ${c\cos(bx):c,b\in\mathbb{R}}$; for example, $\cos(x^3-x)\in\mathcal{B}$.
Known Partial Results #
Necessary Conditions #
Suppose $f(x)=\sum_{n=0}^{\infty}a_n x^n$ is bounded on $\mathbb{R}$. Then either:
- $a_0$ is the only non-zero coefficient (i.e., $f$ is the constant function $f\equiv a_0$), or
- there are infinitely many indices $n$ with $a_n\neq 0$, and the signs of the non-zero $a_n$ change infinitely often.
The sign-change condition is necessary: if the non-zero coefficients are eventually of one sign, the dominant-term comparison shows $f(x)\to\pm\infty$ as $x\to+\infty$ or $x\to-\infty$.
Every non-constant polynomial is unbounded on $\mathbb{R}$.
Proof.
A polynomial has only finitely many non-zero coefficients. By Proposition 2 (1), the only bounded polynomial is the constant function. Any non-constant polynomial satisfies $|p(x)|\to\infty$ as $|x|\to\infty$.The Sign-Change Condition Is Not Sufficient #
The condition of Proposition 2 is not sufficient, as the following examples show.
Consider the geometric series $$ f(x) = \sum_{n=0}^{\infty}(-1)^n x^{2n} = \frac{1}{1+x^2}, \qquad |x|<1. $$ The coefficients alternate in sign, yet $R=1\neq+\infty$. One must first require $R=+\infty$ before the sign-change condition becomes meaningful.
For a subtler case with $R=+\infty$: take $a_n=(-1)^n/n!$, so $$ f(x) = \sum_{n=0}^{\infty}\frac{(-1)^n}{n!}x^n = e^{-x}. $$ The signs alternate, yet $e^{-x}\to+\infty$ as $x\to-\infty$.
The $e^{-x}$ example reveals the key gap: sign alternation of the coefficients does not prevent the function from growing in one direction, because the series for $e^{-x}$ reconstructs exponential growth in the negative half-line. A complete criterion must capture cancellation in both directions.
Connections to Entire Function Theory #
Let $f$ be holomorphic in $|z|\le R$. Then for $0<r<R$, $$ M(r) \le \frac{2r}{R-r}\sup_{|z|=R}\operatorname{Re}f(z) + \frac{R+r}{R-r},|f(0)|. $$
Borel–Carathéodory shows that the real part of a complex-valued entire function controls its modulus. For a real-valued function on $\mathbb{R}$ the analogous control is more delicate, since we only observe the function on a line, not on a disk.
Every entire function of finite order $\rho$ can be written as $$ f(z) = z^m e^{g(z)}\prod_{n=1}^{\infty} E_p!\left(\frac{z}{z_n}\right), $$ where $m\ge 0$, $p=\lfloor\rho\rfloor$, $g$ is a polynomial of degree $\le\rho$, and the $E_p$ are Weierstrass elementary factors.
A bounded real entire function of infinite order (if one exists) would not be directly covered by the Hadamard factorisation. Understanding the zero set and the exponential factor in $e^{g(z)}$ may be key to classifying all $f\in\mathcal{B}$.
The Open Sub-Question on the Generators of $\mathcal{B}$ #
Does $\mathcal{B}$ consist precisely of functions of the form $c\cos(h(x))$ and their linear combinations and products, where $h:\mathbb{R}\to\mathbb{R}$ is entire and $c\in\mathbb{R}$?
A positive answer would give an implicit characterisation via algebraic generators. A negative answer would require producing a bounded entire function on $\mathbb{R}$ that does not lie in the $\mathbb{R}$-algebra generated by ${\cos\circ, h : h\text{ entire}}$.
By Proposition 1 (3), every $c\cos(h(x))$ belongs to $\mathcal{B}$, and $\mathcal{B}$ is an algebra, so all products and sums remain in $\mathcal{B}$. What is unknown is whether every element of $\mathcal{B}$ arises this way. Note that $\sin x = \cos(x-\pi/2) \in \mathcal{B}$, so sine is already covered.
Research Directions and Conjectures #
Direction 1: Coefficient Growth Rate #
A promising approach is to examine the rate of decay of $|a_n|$, not just the sign pattern.
Is there a decay condition on $|a_n|$, combined with the sign-change condition, that gives a sufficient criterion for $f\in\mathcal{B}$?
Approach. The Cauchy estimates give $|a_n| = |f^{(n)}(0)|/n!\le M(r)/r^n$ for all $r>0$. If $f\in\mathcal{B}$ with $|f|\le B$, the bound $|a_n|\le B/r^n$ holds for every $r>0$, but this recovers only the $R=+\infty$ condition. Is there a sharper constraint?
Direction 2: Fourier-Analytic Approach #
Every $f\in L^\infty(\mathbb{R})\cap L^2(\mathbb{R})$ possesses a square-integrable Fourier transform. If $f$ is also entire, Paley–Wiener forces the transform to be compactly supported. However, a generic $f\in\mathcal{B}$ may not lie in $L^2$ (e.g., $\cos x\notin L^2(\mathbb{R})$).
Can the Fourier theory for tempered distributions give a necessary and sufficient condition for $f\in\mathcal{B}$ in terms of the spectral support of $f$?
Direction 3: Differential Equation Characterisation #
Bounded entire functions often arise as solutions to ODEs. For instance $y’’+y=0$ has bounded solutions $A\cos x + B\sin x$. More generally, $y’’+\omega(x)y=0$ with $\omega$ entire and bounded can produce bounded solutions.
Characterise those linear differential operators $L$ with entire coefficients whose full solution space lies within $\mathcal{B}$.
Direction 4: Even/Odd Decomposition and Reduction #
Every $f\in\mathcal{B}$ splits as $f=f_e+f_o$ where $$ f_e(x)=\tfrac{1}{2}(f(x)+f(-x))=\sum_{k\ge 0}a_{2k}x^{2k} \quad\text{and}\quad f_o(x)=\tfrac{1}{2}(f(x)-f(-x))=\sum_{k\ge 0}a_{2k+1}x^{2k+1}. $$ Since $f_e(x)=g(x^2)$ for the entire function $g(t)=\sum_{k\ge 0}a_{2k}t^k$, boundedness of $f_e$ reduces to: is $g$ bounded on $[0,+\infty)$? This reduction may make the even and odd parts easier to study separately.
Direction 5: Polynomial Approximation and Numerics #
If the partial sums $S_N(x)=\sum_{n=0}^{N}a_n x^n$ are uniformly bounded on growing intervals $[-R_N,R_N]$ (with $R_N\to\infty$), does it follow that $f\in\mathcal{B}$? Conversely, if $f\in\mathcal{B}$, how fast must $R_N$ grow relative to $N$ for the bound to hold?
Summary of Open Problems #
| # | Statement |
|---|---|
| Q1 | Give a necessary and sufficient condition on $(a_n)$ for $f=\sum a_n x^n$ to be bounded on $\mathbb{R}$. |
| Q2 | Is $\mathcal{B}$ generated (as an algebra) precisely by ${c\cos(h(x)):h\text{ entire}}$? |
| Q3 | Does a sharper decay condition on $ |
| Q4 | Can spectral-support (Paley–Wiener / distribution) theory characterise $\mathcal{B}$? |
| Q5 | Which linear ODEs with entire coefficients have solution space $\subseteq\mathcal{B}$? |
| Q6 | What is the precise relationship between truncation bounds on $[-R_N,R_N]$ and $f\in\mathcal{B}$? |
References #
- Ahlfors, L. V. (1979). Complex Analysis, 3rd ed. McGraw-Hill.
- Boas, R. P. (1954). Entire Functions. Academic Press.
- Conway, J. B. (1978). Functions of One Complex Variable, 2nd ed. Springer.
- Levin, B. Ya. (1996). Lectures on Entire Functions. AMS Translations of Mathematical Monographs, vol. 150.
- Rudin, W. (1976). Principles of Mathematical Analysis, 3rd ed. McGraw-Hill.
- Rudin, W. (1987). Real and Complex Analysis, 3rd ed. McGraw-Hill.
- Rüdinger, A. (2009). Criterion for boundedness of power series. Open Problem Garden. http://www.openproblemgarden.org/op/criterion_for_boundedness_of_power_series
- Stein, E. M. and Shakarchi, R. (2003). Fourier Analysis: An Introduction. Princeton University Press.
- Stein, E. M. and Shakarchi, R. (2010). Complex Analysis. Princeton University Press.
- Titchmarsh, E. C. (1939). The Theory of Functions, 2nd ed. Oxford University Press.