Precise 3D Track Reconstruction Algorithm for the ICARUS T600 Liquid Argon Time Projection Chamber Detector
Figure 4
Simulation: the absolute difference between the reconstructed hit energy deposit () and the simulated hit energy deposit () as a function of . The hits shown are originating from muon tracks simulated with isotropic initial direction. The tail of the distribution with MeV corresponds to the hits at track end points, only partially crossing the distance between consecutive wires. The peak of the distribution corresponds to the hits of minimum ionizing particles; the points at high values of come from low energy, highly ionizing parts of tracks.
