The neutral density in the lower thermosphere, defined as an altitude range of 70-200 km in this paper, is essential to estimate the global meteoric mass input and to derive the momentum flux from tropospheric gravity waves. Also, the lower thermosphere is thought to be sensitive to the climate change due to greenhouse gases; global cooling would occur in the upper atmosphere in conjunction with global warming in the troposphere due to long-term increase of greenhouse gas concentrations, which was first pointed out by Roble and Dickinson (1989). In contrast to the troposphere, where CO 2 is optically thick and traps infrared (IR) radiation emitted by the Earth's surface, in the stratosphere and above, CO 2 is optically thin and emits IR radiation to space, causing cooling in the middle and upper atmosphere. At a given pressure, this cooling must result in a density increase. However, in the combination of the thermal shrinking, atmospheric density at a given height decreases in the middle and upper atmosphere.Measurements of neutral densities in the lower thermosphere are still scarce. Neutral densities are largely measured by means of in-situ instruments onboard sounding rockets (80-100 km) and satellites (∼400 km), and thus the 100-300 km altitude is left as the "thermospheric gap" (Oberheide et al., 2011). Although there are some early density measurements based on occultations of the Sun in ultraviolet wavelengths (e.g.,