Update event_processing.md

docs/user/event_processing.md

@@ -17,10 +17,12 @@ the following for the paralyzing case:
 $$
 C_{par} = -{\cal Re}W_0(-R\tau/\Delta_{TOF}) \Delta_{TOF}/R
 $$
+
 where $R$ is the number of triggers per accelerator pulse within a time-of-flight bin $\Delta_{TOF}$.
 The dead time for the current BL4B detector is $\tau=4.2$ $\mu s$. In the equation avove, ${\cal Re}W_0$ referes to the principal branch of the Lambert W function.
 
 The following is used for the non-paralyzing case:
+
 $$
 C_{non-par} = 1/(1-R\tau/\Delta_{TOF})
 $$
@@ -157,4 +159,4 @@ With this new weigth, we can compute reflectivity directly from the $S(q_z)$ equ
 
 $$
 R(q_z) = \frac{1}{Q} \sum_{i \in q_z \pm \Delta{q_z}/2}  w_i / \phi(\lambda_i) q_{z,i} / \lambda_i
-$$
+$$