Generally, the initial conditions determine m and k∥. Then k⊥ is calculated from the dispersion relation. We need to express kρ and n as a function of m, k∥ and k⊥. We have
| (116) |
and
| (117) |
We get an expression for n
| (118) |
which is inserted back in (??) to get
| (119) |
and kρ is solution of the equation
| (120) |
Defining
| (121) |
and
we have
| (124) |
such that
| (125) |
which gives
| (126) |
To sum up
| (127) |
where σρ = ±1. We can also express kρ as
| (128) |
The correct solution for kρ can be determined from (??).