Usually
luminosity is a flux density, with dimension L
-2 T
-1, instead of dimension L
-2. Thus, what we get as a result proportional to luminosity is not # of events, but, instead, an event rate (# events per unit time) with a dimension T
-2.
The proportionality constant must have a dimension L
2. However, the proportionality constant should be proportional to the number of scatterers, which is dimensionless. The proportionality constant corresponding to ONE scatterer is a characteristic of the dynamics of the scattering event, and is customarily referred to as a cross-section.
What I tried to say could be summarized as:
<br />
\frac{d N_{\mathrm{reactons}}}{d t} = K \, \mathcal{L}<br />
where \mathcal{L} is the luminosity of the incident beam, and:
<br />
K = N_{\mathrm{scatters}} \, \sigma<br />
where N_{\mathrm{scatters}} is the total number of scatterers in the target, and \sigma is the total scattering cross-section for a single scattering event.