How to prove this strange limit? Let $f:[0,\infty)\to\mathbb R$ be a function in $C^2$ such that 
$\lim_{x\to\infty} (f(x)+f'(x)+f''(x)) = a.$
Prove that $\lim_{x\to\infty} f(x)=a$
 A: Note that with $\alpha = e^{i \pi/3}$ and $\beta = e^{-i \pi/3}$ we have $\alpha \beta = 1$ and $\alpha + \beta = 1$ and , therefore,
$$\tag{1}f(x) + f'(x) + f''(x) = \alpha\beta f(x) + ( \alpha + \beta)f'(x) + f''(x) \\ =\alpha[ \, \beta f(x) + f'(x) + (\beta f(x) + f'(x))' \, ]$$
One can prove the lemma (when the real part of $\gamma$ is positive):

$$\gamma f(x)  + f'(x) \to \delta \implies f(x) \to \delta/\gamma$$

To prove the lemma use the Hardy - L'Hospital trick
$$\lim_{x \to \infty}f(x) = \lim_{x \to \infty}\frac{e^{\gamma x}f(x)}{e^{\gamma x}} = \lim_{x \to \infty}\frac{e^{\gamma x}(\gamma f(x) + f'(x))}{\gamma e^{\gamma x}} = \frac{\delta}{\gamma}.$$ 
Note that at this stage to appy L'Hospital's rule we don't need to assume anything about the  existence of the limit of $f(x)$ in the numerator, only that the limit of the denominator is $+\infty.$
Now by (1) and the lemma we have 
$$f(x) + f'(x) + f''(x) \to a \implies \beta f(x) + f'(x) \to a/\alpha,$$
and using the lemma again, 
$$f(x) \to a/(\alpha \beta) = a$$
A: Regards @merow . If $ \lim_{x \rightarrow \infty} f(x) $ exists, here is one argument : $ \lim_{x \rightarrow \infty}f(x) = \lim_{x \rightarrow \infty}f(x+h) = \lim_{x \rightarrow \infty}f(x-h) $ for any finite value $h$.
First we have 
$$ \lim_{x \rightarrow \infty}f(x)  + \lim_{x \rightarrow \infty} \left[ f'(x) + f''(x) \right] = a $$
and
$$ \lim_{x \rightarrow \infty}f(x)  + \lim_{x \rightarrow \infty} \left[ \lim_{h \rightarrow 0} \frac{(f(x+h)-f(x))}{h} + \lim_{h \rightarrow 0} \frac{(f(x+h)-2f(x)+f(x-h))}{h^{2}} \right] = a $$
$$ \lim_{x \rightarrow \infty}f(x)  + \lim_{x \rightarrow \infty} \left[ \lim_{h \rightarrow 0} \frac{(hf(x+h)-hf(x))}{h^{2}} + \frac{(f(x+h)-2f(x)+f(x-h))}{h^{2}} \right] = a $$
$$ \lim_{x \rightarrow \infty}f(x)   = \lim_{h \rightarrow 0} \left[ a -   \frac{(h \lim_{x \rightarrow \infty }f(x+h)-h\lim_{x \rightarrow \infty}f(x) )}{h^{2}} - \frac{(\lim_{x \rightarrow \infty } f(x+h)+\lim_{x \rightarrow \infty }f(x-h) - 2 \lim_{x \rightarrow \infty}f(x) )}{h^{2}} \right] $$
we may also see that $ \lim_{x \rightarrow \infty}f(x) = \lim_{x \rightarrow \infty}f(x+h) = \lim_{x \rightarrow \infty}f(x-h) $, for any finite value $h$. Using this, the numerators on the right side will be $0$, and we get
$$ \lim_{x \rightarrow \infty}f(x)   = \lim_{h \rightarrow 0} a  = a$$
Hope this will be useful, but this can be improved. Thanks.
A: Let $h(x)=f(x)+f'(x)+f''(x)-a$, so $h(x)\to0$ as $x\to\infty$. Let $\omega=e^{2\pi i/3}$ and
$$
  f_1(x)=\frac1{\omega-\bar\omega}\left(e^{\omega x}\int_0^xe^{-\omega t}h(t)\;dt-e^{\bar\omega x}\int_0^xe^{-\bar\omega t}h(t)\;dt\right).
$$
It can be verified that
$$
  f_1(x)+f_1'(x)+f_1''(x)=h(x).
$$
Thus setting $f_2(x)=f(x)-f_1(x)-a$, we have
$$
  f_2(x)+f_2'(x)+f_2''(x)=0.
$$
Then $f_2(x)$ must be a linear combination of $e^{\omega x}$ and $e^{\bar\omega x}$, implying $f_2(x)\to0$ as $x\to\infty$. It remains to show $f_1(x)\to0$ as $x\to\infty$.
Since $h(x)$ is continuous and has a limit as $x\to\infty$, it is bounded. Suppose $|h(x)|<K$ for all $x\geq0$. Consider $\epsilon>0$. Pick $L$ such that $|h(x)|<\epsilon$ for $x>L$. Pick $M$ such that $Ke^{(L-M)/2}<\epsilon$. For $x>M$ we have
$$\begin{eqnarray*}
  |f_1(x)|&\leq&\frac2{|\omega-\bar\omega|}e^{-x/2}\int_0^xe^{t/2}|h(t)|\;dt\\
    &=&\frac2{|\omega-\bar\omega|}e^{-x/2}\left(
  \int_0^Le^{t/2}|h(t)|\;dt+
  \int_L^xe^{t/2}|h(t)|\;dt\right)\\
    &\leq&\frac2{|\omega-\bar\omega|}e^{-x/2}\left(
  K\int_0^Le^{t/2}\;dt+
  \epsilon\int_L^xe^{t/2}\;dt\right)\\
    &\leq&\frac4{|\omega-\bar\omega|}\left(
  Ke^{(L-M)/2}+\epsilon\right)\\
    &\leq&\frac8{|\omega-\bar\omega|}\epsilon.
\end{eqnarray*}$$
Since $\epsilon>0$ was arbitrary, $f_1(x)\to0$ as $x\to\infty$ as required.
