Let $X_1,X_2,\ldots, X_{n_1}$ be IID with PDF $f(x-\theta) $, for $-\infty<x<\infty$ and $-\infty<\theta<\infty$. Denote the CDF of $X_i$ by $F(x-\theta)$. Let $Z_1,Z_2, \ldots, Z_{n_2}$ denote the censored observations. For these observations we only know that $Z_j >a $ for some $a$ that is known and that the $Z_j$s are independent of the $X_i$s.
Then the "observed" and "complete" , that is for both the observed and the censored data, likelihoods are given by:
$$L(\theta| \mathbf{x} )= [1-F(a-\theta)]^{n_2} \prod_{i=1}^{n_1} f(x_i -\theta) $$
$$ L( \theta |\mathbf{x,z})=\prod^{n_1}_{i=1}f(x_i -\theta) \prod_{i=1}^{n_2}f(z_i-\theta) $$
My question is why do the likelihoods take that form? I believe for the $Z_j$s we have a left censoring as they only take greater than $a$ values, as opposed to the $X_is$ that are not restricted in that way. We also know that they are mutually independent.
Could it be that the "observed" likelihood is obtained after using that independence? We have $n_2$ observations greater than $a$, times the joint density of the $X_i$s, right?.
A little more explanation on these two equations would go a long way.
Thank you in advance.