Earth's thermosphere occupies the region of space between the mesopause at approximately 85-90 km altitude, and the exobase, whose altitude varies strongly with solar activity but is typically at 500 km or above. This region maintains a strongly positive temperature gradient in the vertical direction, resulting in convective stability. This stability, combined with rapid molecular diffusion and large kinematic viscosity, has long led to the presumption that neutral dynamics in the middle thermosphere would be smooth and laminar over small horizontal lengths, that is, on scales up to at least several hundred kilometers. The purpose of this work is to test the validity of these long held assumptions.Such testing requires an observational technique that is capable of resolving thermospheric flow features at length scales much smaller than previously possible. The approach presented here achieves this using several new adaptations of underlying methods that have been used since the 1960s to determine wind and temperature fields in the thermosphere, that is, using Fabry-Perot interferometers (FPI) to measure Doppler spectra of optical emissions due to airglow and aurora (Roble et al., 1968;Wark, 1960). Of particular interest are the 558 and 630 nm emissions from atomic oxygen, which are routinely measured with FPIs and widely used to infer conditions at their centroid altitudes of approximately 120 km (in aurora) and 240 km, respectively.The experimental procedure requires recording a time series of Doppler spectra of the selected emission line, for a widely separated set of look directions in the sky. Such measurements are typically taken viewing in the zenith or at zenith angles of 45°, 60°, or 70°, and with varied azimuths. Doppler shifts are derived by numerically fitting Gaussian profiles to the recorded spectra, with the component of the wind along the instrument's line-of-sight (LOS) being derived from these fitted shifts.Traditionally, the instantaneous field of view used for these measurements is only at most a few degrees in diameter, with this beam being steered across the instrument's field-of-regard between successive exposures. However,