“…[11] Upon irradiation, the process parameters, except beam power, were fixed to the optimum conditions established in the institute, as shown in Table I. [10,14] Beam power, which is decisive to heat input subjected to the sam- ple, was varied in the range from 6580 to 9940 W. The process parameters, such as beam power (P), beam travel speed (v), and transverse scanning width of electron beam (l), can be assembled into a normalized parameter, viz., input energy density, W 0 , via the following equation:…”