“…Remarkably, these different forms of dissipative solitons coexist to each other when the equation coefficients belong to certain regions [14,[17][18][19]27]. Moreover, the basic CGLE can easily be extended to more general models accounting for the impact of such high-order effects as third-order dispersion, fourth-order spectral filtering, self-stepping, and stimulated Raman scattering [28][29][30][31][32] as well as an external control [33,34]. In fact, more specific models have been used to study the turbulent-like intensity * tvr@jlu.edu.cn; tvr@rian.kharkov.ua and polarization rogue waves in a Raman fiber laser [35], stationary solitary pulses in a dual-core fiber laser [36], the interaction of stationary, oscillatory and exploding counter-propagating dissipative solitons [37,38], the existence of stable three-dimensional dissipative localized structures in the output of a laser coupled to a distant saturable absorber [39], the emergence and the stability of temporally localized structures in the output of a semiconductor laser passively mode locked by a saturable absorber in the long-cavity regime [40], and dissipative solitons in Bose-Einstein condensates [41][42][43][44][45][46].…”