ABSTRACT
In this appendix, singularity theory is applied to the simplified master equation of form II:
˜G (
˜I , A, p˜ ) = 0, (D.1)
where
˜G = ˜θ A3 + (
(K2 − 1) ˜θ + ˜I − 1 )
A2
+ (
K1 + 1 + (K2 − 1)˜I − K2 ˜θ )
A − K2 ˜I ,
and
p˜ = ( ˜θ, K1, K2), ˜θ = αβ, ˜I = βγ I.
