I. Introduction
Optical wireless communication relies on a substantial license-free transmission bandwidth, whilst avoiding electromagnetic radiation. However, owing to its predominantly line-of-sight (LOS) propagation, the transmissions may be blocked by an obstacle between the transmitter and the receiver. Hence it is beneficial to exploit the scattered non-line-of-sight (NLOS) components [1], [2], where the transmission and the reception directions are not required to be perfectly aligned. Hence, the direct-link of NLOS optical communication has been extensively studied for example in [3]–[5]. The relevant applications span from short-range atmospheric ultraviolet communication to sensing. In case of having a weak NLOS optical path, the received signal cannot be detected by the conventional waveform detector. The photon-level energy detector, such as the photon-counting receiver or a photomultiplier tube (PMT) receiver, needs to be employed. Explicitly, the photon-counting receiver counts the number of photons received; and the PMT receiver converts the received photons to electronic signals, while applying a certain amplification factor.