We study the energy propagation in subwavelength waveguides and demonstrate that the mechanism of material gain, previously suggested for loss compensation, is also a powerful tool to manipulate dispersion and propagation characteristics of electromagnetic pulses at the nanoscale. We show theoretically that the group velocity in lossy nano-waveguides can be controlled from slow to superluminal values by the material gain and waveguide geometry and develop an analytical description of the relevant physics. We utilize the developed formalism to show that gain-assisted dispersion management can be used to control the transition between "photonic-funnel" and "photonic-compressor" regimes in tapered nano-waveguides. The phenomenon of strong modulation of group velocity in subwavelength structures can be realized in waveguides with different geometries, and is present for both volume and surface-modes.Conventional optical fibers support propagating modes only when waveguide radius is sufficiently large [1]. In contrast to this behavior, plasmonic systems, anisotropybased waveguides, nanoparticle chains, and optical coaxial cables [2,3,4,5] support energy propagation even when the typical waveguide cross-section is much smaller than the wavelength. Unfortunately, since the majority of these nano-waveguides rely on plasmonic materials to confine the radiation beyond the diffraction limit, the propagation of nano-constrained radiation is often limited by material losses. While the emerging field of active plasmonics [6] promises to overcome absorption limitations in nano-waveguides, full compensation of losses appears to be experimentally challenging [7].In this Letter we focus on gain-assisted phenomena beyond absorption compensation and study the perspectives of controlling the dispersive properties of active nanoscale waveguides. We show that even relatively weak material gain, which is unable to compensate losses, is capable of producing large variations of the group velocity, bringing such exotic phenomena as slow (0 < v g ≪ c) and ultra-fast (v g < 0) light [8,9,10] to the nanoscale domain. However, in contrast to diffractionlimited systems, where the group velocity is controlled solely by material dispersion, the energy propagation in nano-waveguides is also strongly affected by the waveguide geometry. We demonstrate that interplay between geometry-and material-controlled modal dispersion in tapered waveguides leads to the transition between photonic compressor regime, where the reduction of phase velocity is accompanied by the simultaneous reduction of group velocity [11,12] and photonic funnel [13] regime where the product of phase and group velocities remains constant [1]. The developed formalism is illustrated on the examples of two fundamentally different nanowaveguides: a surface-mode-based plasmonic nanorod, and a volume-mode fiber with anisotropic core. Applications include nanosized tunable delay lines, all-optical buffers and data synchronizers.The geometry of a typical waveguide structure is schematical...