As an alternative to whuber's excellent answer, I will try to derive the exact limit of the probability in question. One of the properties of the gamma distribution is that sums of independent gamma random variables with the same rate/scale parameter are also gamma random variables with shape equal to the sum of the shapes of those variables. (That can be proved using the generating functions of the distribution.) In the present case we have $X_1,...X_n \sim \text{IID Gamma}(3,1)$, so we obtain the sum:
$$S_n \equiv X_1 + \cdots + X_n \sim \text{Gamma}(3n, 1).$$
We can therefore write the exact probability of interest using the CDF of the gamma distribution. Letting $a = 3n$ denote the shape parameter and $x = 3(n-\sqrt{n})$ denote the argument of interest, we have:
$$\begin{equation} \begin{aligned}
H(n)
&\equiv \mathbb{P}(S_n \geq 3(n-\sqrt{n})) \\[12pt]
&= \frac{\Gamma(a, x)}{\Gamma(a)} \\[6pt]
&= \frac{a \Gamma(a)}{a \Gamma(a) + x^a e^{-x}} \cdot \frac{\Gamma(a+1, x)}{\Gamma(a+1)}. \\[6pt]
\end{aligned} \end{equation}$$
To find the limit of this probability, we first note that we can write the second parameter in terms of the first as $x = a + \sqrt{2a} \cdot y$ where $y = -\sqrt{3/2}$. Using a result shown in Temme (1975) (Eqn 1.4, p. 1109) we have the asymptotic equivalence:
$$\begin{aligned}
\frac{\Gamma(a+1, x)}{\Gamma(a+1)}
&\sim \frac{1}{2} + \frac{1}{2} \cdot \text{erf}(-y) + \sqrt{\frac{2}{9a \pi}} (1+y^2) \exp( - y^2).
\end{aligned}$$
Using Stirling's approximation, and the limiting definition of the exponential number, it can also be shown that:
$$\begin{aligned}
\frac{a \Gamma(a)}{a \Gamma(a) + x^a e^{-x}}
&\sim \frac{\sqrt{2 \pi} \cdot a \cdot (a-1)^{a-1/2}}{\sqrt{2 \pi} \cdot a \cdot (a-1)^{a-1/2} + x^a \cdot e^{a-x-1}} \\[6pt]
&= \frac{\sqrt{2 \pi} \cdot a \cdot (1-\tfrac{1}{a})^{a-1/2}}{\sqrt{2 \pi} \cdot a \cdot (1-\tfrac{1}{a})^{a-1/2} + \sqrt{x} \cdot (\tfrac{x}{a})^{a-1/2} \cdot e^{a-x-1}} \\[6pt]
&= \frac{\sqrt{2 \pi} \cdot a \cdot e^{-1}}{\sqrt{2 \pi} \cdot a \cdot e^{-1} + \sqrt{x} \cdot e^{x-a} \cdot e^{a-x-1}} \\[6pt]
&= \frac{\sqrt{2 \pi} \cdot a}{\sqrt{2 \pi} \cdot a + \sqrt{x}} \\[6pt]
&\sim \frac{\sqrt{2 \pi a}}{\sqrt{2 \pi a} + 1}. \\[6pt]
\end{aligned}$$
Substituting the relevant values, we therefore obtain:
$$\begin{equation} \begin{aligned}
H(n)
&= \frac{a \Gamma(a)}{a \Gamma(a) + x^a e^{-x}} \cdot \frac{\Gamma(a+1, x)}{\Gamma(a+1)} \\[6pt]
&\sim \frac{\sqrt{2 \pi a}}{\sqrt{2 \pi a} + 1} \cdot \Bigg[ \frac{1}{2} + \frac{1}{2} \cdot \text{erf} \Big( \sqrt{\frac{3}{2}} \Big) + \sqrt{\frac{2}{9a \pi}} \cdot \frac{5}{2} \cdot \exp \Big( \frac{3}{2} \Big) \Bigg]. \\[6pt]
\end{aligned} \end{equation}$$
This gives us the limit:
$$\lim_{n \rightarrow \infty} H(n) = \frac{1}{2} + \frac{1}{2} \cdot \text{erf} \Big( \sqrt{\frac{3}{2}} \Big) = 0.9583677.$$
This gives us the exact limit of the probability of interest, which is larger than one-half.