I. Introduction
Detectors used for high-energy photon detection are often made thick in order to improve their photon-detection efficiency. Use of a thick detector, in turn, motivates depth of interaction (DOI) estimation for each gamma ray. If we estimate only the two-dimensional (2D) position of interaction in a gamma camera, ambiguity in DOI may result in a loss of detector and/or image resolution [1]. Random DOI can cause increased signal variance, which in turn can degrade the 2D resolution of a gamma camera. Additionally, DOI ambiguity for obliquely incident gamma rays causes parallax, which can subsequently limit image resolution. Random DOI can also degrade coincidence-timing resolution for a time-of-flight PET system [2]. For many clinical gamma cameras with moderately thick scintillators (< 10 mm), signal-variance and parallax issues are mitigated by choice of camera geometry and optical properties. However, to avoid these issues in general for a thicker gamma-ray detector, we must estimate the three-dimensional (3D) coordinates of interaction.