“…In this method the linear and nonlinear structures are handled in a similar manner without any need to restrictive assumptions. This approach is successfully and effectively applied to various equations such as autonomous ordinary differential equations [32], delay differential equations [33], Fokker-Planck equation [34], nonlinear fractional differential equation with Riemann-Liouville's fractional derivatives [35], quadratic Riccati differential equation [36], one-phase direct and inverse Stefan problems [37], one-dimensional elastic half-space model subjected initially to a prescribed harmonic displacement [38], the linear and the nonlinear Goursat problems [39], Klein-Gordon equation [40], shock-peakon and shockcompacton solutions for K ( p, q) equation [41], generalized Burgers-Huxley equation [42], wave equation [43], some problems in calculus of variations [44], nonlinear PDEs arising in the process of understanding the role of nonlinear dispersion and in the forming of structures like liquid drops and exhibiting compactons [45], generalized Zakharov equation [46], Jaulent-Miodek equation [47], characteristic and non-characteristic Cauchy reaction-diffusion problems [48], two-point boundary value problems [49], cubic nonlinear Schrödinger equation [50], parabolic integro-differential equations arising in heat conduction in materials with memory [51], nonlinear integro-differential equations which arise in biology [52], generalized pantograph equation [53], Kawahara PDE arising in the modelling of water waves [54], systems of differential equations [55], differential equation arising in astrophysics [56], the telegraph and fractional telegraph equations [57], identifying an unknown function in a parabolic equation with overspecified data [58], etc.…”