“…Now in system (3) the corresponding term 8 15 c g 2 r 2 , which, of course, is transformed into the first one assuming that rðxÞ ¼ 1=gðxÞ as is usually accepted in the soliton perturbation theory. The derived system (3) on the one hand generalizes the earlier results of [32] and [19,20] and on the other hand presents a general approach avoiding the restrictions of the previous approaches [29,30,24,31] for the analysis of the influence of the IRS, SS and TOD on the solutions of CCQGLE. The price to be paid, however, is the complexity of the derived system.…”