“…It is a function of various parameters [27,28] such as the entrance-channel mass asymmetry, beam energy, the target thickness, the exit channels of interest, the angular acceptance of the separator, the magnetic field and gas pressure settings, and the size of the focal plane detector. Entrance channel mass asymmetry, target thickness, angular acceptance of the HYRA, and size of the focal plane detector remain unchanged throughout the experiment, while the rest of the parameters change.…”