Relationships between different measure of opacity I'm reading some papers that compare different values for a materials opacity to a particular particle.  The first is given as $\frac{dE}{dX}$, a single particles energy loss per unit column depth (X = $x\rho $) to a continuous process.  
Makes sense.  So then the author goes on to compare his value to that of other authors, who have their opacities for the process expressed in $\kappa $ given in $cm^{2}/g $.  
They're both presented as measuring the same thing, but I usually think of $ \kappa $ as being an opacity for a large group of particles that are removed discretely from a beam, so that the total energy in the beam dies of exponentially (since energy loss per distance is proportional to the number of particles left in the beam).  $\frac{dE}{dX}$ is due to a continuous process acting on all the particles, and so would have a roughly linear effect per distance.
So my question is how does one compare the two values.  What does $ \kappa $ mean in a context of continuous energy loss.
Thanks
 A: 
What does $\kappa$ mean in a context of continuous energy loss

In reference to energy $E$ (reaching "[normalized] column depth" $X$) opacity $\kappa_E$ may simply be defined as
$\kappa_E := \frac{1}{E} \frac{dE}{dX}$.
(If the so defined "opacity" is constant wrt. "[normalized] column depth $X$" this describes "exponential loss" (as a function of $X$) instead of "linear dependence on $X$".)

but I usually think of $\kappa$ as being an opacity for a large group of particles that are removed discretely from a beam

That's rather opacity $\kappa_N$, in reference to the (discrete, natural) number $N$ of particles (reaching "[normalized] column depth" $X$):
$\kappa_N := \frac{1}{N} \frac{dN}{dX}$; or perhaps rather      
$\kappa_N := \left\langle\frac{1}{N} \frac{\Delta N}{\Delta X}\right\rangle_{\text average}$.
Of course, the relation between $E$ and $N$, or correspondingly between $\kappa_E$ and $\kappa_N$ may be complicated ...
Also, instead of being defined in reference to extensive quantities $E$ or $N$, opacity may be defined in reference to the corresponding (average) intensities:    
$I := \frac{\Delta E}{\Delta t \Delta A}$ or $I := \frac{\Delta N}{\Delta t \Delta A}$, as
$\kappa_I := \frac{1}{I} \frac{dI}{dX}$.
[Note on edited version:
Consistent with the "unit of opacity $\kappa$" given as "$cm^2/g$" is the definition, in reference to "energy" $E$, as
$\kappa_E := \frac{1}{E} \frac{dE}{dX}$, and not (as stated in the initial version) $\kappa_E := \frac{dE}{dX}$.
The same consideration applies to any definition in reference to intensity.
In reference to particle number $N$ I correspondingly changed the explicit definition of "opacity $\kappa_N$" as well, even though its "unit" (or "dimension") is not affected since the number $N$ is "dimensionless".] 
