MHB Can an entire function with a specific limit at infinity be non-constant?

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An entire function with the limit condition that the real part of the function divided by z approaches zero as z approaches infinity must be constant. This conclusion is supported by the properties of entire functions and Liouville's theorem, which states that a bounded entire function is constant. The problem of the week highlights the relationship between the behavior of entire functions at infinity and their constancy. Janssens provided a correct solution that confirms this result. The discussion emphasizes the significance of limits in determining the nature of entire functions.
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Here is this week's POTW:

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Show that if $f$ is an entire function with $\lim\limits_{z\to \infty} \dfrac{\operatorname{Re}f(z)}{z} = 0$, then $f$ is constant.

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Congratulations to Janssens for his correct solution, which is posted below.
Instead of the Cauchy integral formula (used for the Liouville Theorem), we invoke (a corollary of) the Poisson integral formula for harmonic functions (Bak and Newman, Complex Analysis, 2010, Theorem 16.9). Namely, writing $f = u + i v$ with $u := \Re{f}$ and $v := \Im{f}$, we have
$$
f(z) = \frac{1}{2\pi}\int_0^{2\pi} u(R e^{i\theta})\frac{R e^{i\theta} + z}{R e^{i\theta} - z}\,d\theta + i v(0),
$$
for all $z \in \mathbb{C}$ and $R > |z|$. This is useful, because it enables reconstruction of $f$ from its real part. So, for any fixed $z \in \mathbb{C}$ and arbitrary $R > |z|$,
\begin{align*}
|f(z) - f(0)| &\le \frac{1}{2\pi}\int_0^{2\pi} |u(R e^{i\theta})| \frac{2|z|}{|R e^{i\theta} - z|}\,d\theta\\
&= \frac{1}{\pi} \int_0^{2\pi} \frac{|u(R e^{i\theta})|}{|R e^{i\theta}|} \frac{|z|}{|1 - \frac{z}{R}e^{-i\theta}|}\,d\theta.
\end{align*}
By the reverse triangle inequality,
$$
\left|1 - \frac{z}{R}e^{-i\theta}\right| \ge \left|1 - \frac{|z|}{R}\right|,
$$
so
$$
|f(z) - f(0)| \le \frac{|z|}{\pi|1 - \frac{|z|}{R}|}\int_0^{2\pi} \frac{|u(R e^{i\theta})|}{|R e^{i\theta}|} \, d\theta.
$$
Now, by the definition of the complex limit, the remaining integrand tends to zero as $R \to \infty$, uniformly for $\theta \in [0,2\pi]$. Hence the integral tends to zero as well. Also, the factor in front of the integral remains bounded, so this gives the result.