We investigate the kinematics of ionized gas within the nuclear starburst of NGC 253 with observations of the Brackett α recombination line at 4.05 µm. The goal is to distinguish motions driven by star-formation feedback from gravitational motions induced by the central mass structure. Using NIRSPEC on Keck II, we obtained 30 spectra through a 0. 5 slit stepped across the central ∼5 ×25 (85 × 425 pc) region to produce a spectral cube. The Brα emission resolves into four nuclear sources: S1 at the infrared core (IRC), N1 at the radio core near nonthermal source TH2, and the fainter sources N2 and N3 in the northeast. The line profile is characterized by a primary component with ∆v primary ∼90-130 km s −1 (FWHM) on top of a broad blue wing with ∆v broad ∼300-350 km s −1 , and an additional redshifted narrow component in the west. The velocity field generated from our cube reveals several distinct patterns. A mean NE-SW velocity gradient of +10 km s −1 arcsec −1 along the major axis traces the solidbody rotation curve of the nuclear disk. At the radio core, isovelocity contours become S-shaped, indicating the presence of secondary nuclear bar of total extent ∼5 (90 pc). The symmetry of the bar places the galactic center near the radio peak TH2 of the galaxy rather than the IRC, and makes this the most likely location of a SMBH. A third kinematic substructure is formed by blueshifted gas on the southeast side of the IRC. This feature likely traces a ∼100-250 km s −1 starburst-driven outflow, linking the IRC to the galactic wind observed on kpc scales.