Numerically solving the likelihood equation remains possible when some or all of the observations are censored.
For instance, suppose we have observations of failure times $\boldsymbol x = (x_1, \ldots, x_n)$, and observations of censoring times $\boldsymbol y = (c_1, \ldots, c_m)$, for a total sample of $m+n$ bulbs, where observations are IID gamma with shape $a$ and rate $b$. Then the likelihood is simply $$\mathcal L(a, b \mid \boldsymbol x, \boldsymbol c) = \prod_{i=1}^n \frac{b^a x_i^{a-1} e^{-b x_i}}{\Gamma(a)} \prod_{j=1}^m S_X(c_j),$$ where $S$ is the survival function of the lifetime; i.e. $$S_X(c_j) = \Pr[X > c_j] = \int_{x = c_j}^\infty \frac{b^a x^{a-1} e^{-b x}}{\Gamma(a)} \, dx = \Gamma(a;c_j).$$ A closed-form solution in the general case is not possible. Software exists to calculate the solution when the data are provided.