Subatomic Physics Flashcards
Differential Cross Section
d sigma / d Omega =
N/jA
j is flux
A is area
for elastic scattering in a 1/r potential
use conservation of angular momentum and the change in linear momentum (in one direction)
Condition for a localised potential
V(r) = 0 for r>r0
or
rV(r) -> 0 as r->infinity
probability current
j=
-i hbar/m [phi* nabla phi - phi nabla phi*]
Lippmann-Schwinger Equation
|psi> =
|phi> - V/(H0 - E ± ie) |psi>
e is a small number
What is the Born approximation?
If the perturbation due to the scattering is not too big, we can approximate
|psi> -> |phi>
= (the solution to the free particle)
in the Born approximation, how are the scattering amplitude and the scattering potential related
scattering amplitude is the fourier transform of the scattering potential (with some constants)
What pairs are not/allowed in the strong nuclear force?
What does this imply?
p-n allowed
n-n, p-p not allowed
this is because we can spin align n-p but not the others due to the pauli eclusion principal.
Hence the nuclear force must be very spin dependant.