The optical absorption properties of free-standing InAs nanomembranes of thicknesses ranging from 3 nm to 19 nm are investigated by Fourier transform infrared spectroscopy. Stepwise absorption at room temperature is observed, arising from the interband transitions between the subbands of 2D InAs nanomembranes. Interestingly, the absorptance associated with each step is measured to be ∼1.6%, independent of thickness of the membranes. The experimental results are consistent with the theoretically predicted absorptance quantum, A Q = πα/n c for each set of interband transitions in a 2D semiconductor, where α is the fine structure constant and n c is an optical local field correction factor. Absorptance quantization appears to be universal in 2D systems including III-V quantum wells and graphene.T he optical properties of heterostructure quantum wells (QWs) have been extensively studied since the 1970s, in GaAs/ AlGaAs (1), GaInAs/AlInAs (2, 3), InGaAs/InP (4), and HgCdTe/ CdTe (5). Here we do a careful quantitative examination of the intrinsic absorption properties of free-standing 2D semiconductor thin films, which has previously been done only for layered structures, such as MoS 2 (6). (The criterion of real two-dimensionality is that the material thickness be smaller than the electron Bohr radius.)Previous work has shown that graphene, a 2D semimetal, has a universal value of light absorption, namely πα, where α is the fine structure constant (7). Here, we use free-standing InAs membranes with exceptionally small thickness as a model material system to accurately probe the absorption properties of 2D semiconductors as a function of thickness. We demonstrate that the magnitude of the light absorption is an integer product of a quantum of absorptance. Specifically, each set of interband transitions between the 2D subbands results in a quantum unit of absorptance of A Q ∼ πα/n c , where n c is the optical local field correction factor. The total absorptance for the first several sets of interband transitions is simply given as A = MA Q , where M is the integer number of allowed transitions for a given photon energy. The result here appears to be universal, except for small correction factors associated with higher bands.Recently, there has been a high level of interest in exploring the fundamental science (6-10) and associated devices (11-20) of free-standing (i.e., attached to a substrate by van der Waals or other weak forces) 2D semiconductors. In one example system, InAs quantum membranes (QMs) with adjustable thicknesses down to a few atomic layers have been realized by a layer transfer process onto a user-defined substrate (12). The approach enables the direct optical absorption studies of fully relaxed (i.e., unstrained) (21) 2D III-V semiconductors by using transparent substrates, without the constraints of the original growth substrate (10). Here, we use InAs membranes of thickness L z ∼ 3-19nm on CaF 2 support substrates as a model material system for examining the absorption properties of 2D semiconduc...