Wednesday 27 March 2019

scattering - Optical theorem and conservation of particle current


The optical theorem


$$ \sigma_{tot} = \frac{4\pi}{k} \text{Im}(f(0)) $$


links the total cross section with the imaginary part of the scattering amplitude.


My lecture notes say that this is a consequence of the conservation of the particle current. How do I get to this consequence?



Answer



Conservation of particle current is nothing but the statement that a theory has to be unitary. In other words the scattering matrix $S$ has to obey


$SS^\dagger=1$



Defining $S=1+iT$ i.e. rewriting the scattering matrix as a trivial part plus interactions (encoded in $T$ which corresponds to your $f$) one finds from the unitarity condition:


$iTT^\dagger=T-T^\dagger=2Im(T)$


$TT^\dagger$ is nothing but the crosssection (I suppressed some integral signs here for brevity) the optical theorem is right there. Hence one finds $\sigma\sim Im(T)$


No comments:

Post a Comment

Understanding Stagnation point in pitot fluid

What is stagnation point in fluid mechanics. At the open end of the pitot tube the velocity of the fluid becomes zero.But that should result...