“…It is expected to occur when the nucleus is heated to a moderate temperature and breaks up on a short time scale into light particles and IMFs with Z ≥ 3. Based on a statistical equilibrium assumption of the generated hot nuclear matter, different measures have been proposed to probe the liquid-gas phase transition, such as the nuclear specific heat capacity (the caloric curve) [12][13][14][15][16][17][18][19][20], the negative heat capacity [21,22], the bimodality in charge asymmetry [8,[23][24][25], the Fisher droplet model analysis [26][27][28][29][30][31][32], the Landau free energy approach [31][32][33][34][35][36][37], the moment of the charge distributions [28,[38][39][40][41], the fluctuation properties of the heaviest fragment size (charge) [28,29,[41][42][43], the Zipf's law [44,45], the multiplicity derivatives recently proposed by S. Mallik et al [46] and the derivative of cluster size [47]. With these features, considerable progress has been accomplished o...…”