This is clearly not the case, soncider e.g. the density that is proportional to $\exp(-x^4)$.
The important part is that the two-dimensional Gaussian distribution has the property that it has independent coordinates and the distribution is rotationally invariant. This does in fact characterise the Gaussian distribution uniquely (if we say that a constant random variable has distribution $\mathcal{N}(\mu, 0)$).
I couldn't find a simple proof for this general characterisation, but under the further assumption of finite variance it is relatively easily proven.
If $X$ has a finite variance and for every independent copy $Y$ of $X$, the distribution of $\frac{X + Y}{\sqrt{2}}$ is the same distibution as the distribution of $X$, then $X$ is normally distributed.
From our assumption we can conclude $E[X] = \frac{E[X] + E[Y]}{\sqrt{2}} = \sqrt{2} E[X]$, which means that $E[X] = 0$.
Let $X_1, X_2, \ldots$ be i.i.d. copies of $X$. Then by assumption we know that $\frac{X_1 + X_2}{\sqrt{2}}$ and $\frac{X_3 + X_4}{\sqrt{2}}$ have the same distribution as $X$. Since they are also independent, we can conclude that $X$ has the same distribution as
$$\frac{\frac{X_1 + X_2}{\sqrt{2}} + \frac{X_3 + X_4}{\sqrt{2}}}{\sqrt{2}} = \frac{X_1 + X_2 + X_3 + X_4}{2}.$$
Now an inductive argument shows that $X$ has the same distribution as $2^{-n/2} \sum \limits_{i = 1}^{2^n} X_i$. But by the central limit theorem, this sequence converges in distribution to a normal distribution, which means that $X$ has a normal distribution.
Remark: $\frac{X + Y}{\sqrt{2}}$ is the first coordinate of the rotation of $(X, Y)$ by $45^\circ$, which connects this theorem to the above mentioned characterisation.