I want to make @Glen_b's answer more explicit, here is an extra answer just because it wouldn't fit as a comment.
The formalism etc. is well explained in Chapter 11 and 12 of Jaynes' book.
Taking the uniform distribution as the base measure, the general solution, as @Glen_b already said, is a Gaussian
$$
f(x) \propto \mathcal{N}(x | -1/2 \lambda_1/\lambda_2, -1/(2\lambda_2))
$$
For the unbounded variable, you can explicitly solve for the Lagrange multipliers $\lambda_1$ and $\lambda_2$ in terms of the constraint values ($a_1, a_2$ in the Wikipedia article). With $a_1=\mu, a_2=\mu^2 + \sigma^2$, you then get $\lambda_1=\mu/\sigma^2, \lambda_2=-0.5 \sigma^2$, so the standard Gaussian $\mathcal{N}(x|\mu, \sigma^2)$.
For the bounded variable $x>x_{min}$, I (and mathematica) cannot solve for $\lambda_{1,2}$ explicitly anymore because of the error function term that appears when computing the partition function ($1/c$ in wikipedia). This means that that the $\mu$ and $\sigma^2$ parameters of the truncated Gaussian are not the mean and variance of the continuous variable you started with. It can even happen that for $x_{min}=0$, the mode of the Gaussian is negative! Of course the numbers all agree again when you take $x_{min} \to -\infty$.
If you have concrete values for $a_1, a_2$, you can still solve for $\lambda_{1,2}$ numerically and plug in the solutions into the general equation and you are done! The values of $\lambda_{1,2}$ from the unbounded case may be a good starting point for the numerical solver.
This question is a duplicate of https://math.stackexchange.com/questions/598608/what-is-the-maximum-entropy-distribution-for-a-continuous-random-variable-on-0