We investigate the dynamics of dark optical solitons of the defocusing nonlinear Schrödinger (NLS) equation under the influence of small perturbations. Building on the integrable structure of the unperturbed NLS equation, we present two complementary analytical frameworks: a perturbed conservation-law approach and a linearization-based eigenfunction expansion rooted in inverse scattering theory. Both yield consistent evolution equations for the key soliton parameters—velocity, depth, center and phase—but the eigenfunction approach additionally provides an explicit expression for the firstorder correction, from which the structure of the shelf, a plateau-like radiation field that inevitably develops around the soliton due to the nonvanishing boundary conditions, can be extracted. It is found that the existence of the shelf is characterized by a single parameter α, which depends on the form of the perturbation. A central result of this work is an exact algebraic relation between the shelf parameter α and the renormalized soliton energy: the rate of energy change is directly and exclusively coupled to α, while all other macroscopic conserved quantities—momentum, Hamiltonian, and center of energy—are shown to decouple from the shelf at leading order. This energy–shelf relation provides a unified and physically transparent accounting of how perturbation energy is partitioned between the soliton core and the radiation it emits. Our analytical results—which are illustrated through several examples of physically relevant perturbations—are consistent with established results in limiting cases. To our knowledge, the energy–shelf relation and the systematic comparison of the two perturbative frameworks within a single, unified treatment are presented here for the first time.



