Page 49 - Tunable Lasers Handbook

30 F. J. Duarte

Notice that = (tan $l,JnnJ, S2.nl (tan $2,n,/nnJ and that Eq. (41) can be easily
=
obtained from the generalized single-pass dispersion equation [Eq. (1 3)] and by
using the identity

For a generalized multiple-prism array [47]

A,.=M, M, ,

c,.=o,

D,. = (MI M,)-I ,

F,. =( %)( $) (50j
,