“…In the particular case of Ga, the undercooling is large enough (θ ≈ 0.50) using the dispersion technique (30) to occur very near to the nose of the θ − C n curve. Since the maximum value for C n (i.e., for θ = 2/3) diminishes with K * V , the scaling supports the possibility for extremely small Ga droplets, through favorable characteristic times, to stay liquid (i.e., to bypass the nose) at the temperature of liquid nitrogen as realized by Koverda et al (31). As a last remark, undercooling experiments are quite systematically performed by continuous cooling of the melt until nucleation.…”