“…An increase in the temperature gradient results in a supercritical Hopf bifurcation, leading to a gradual increase in oscillation amplitude, whereas a subcritical Hopf bifurcation causes an abrupt amplitude jump at the Hopf point, where the system's stable steady-state becomes unstable and a stable limit cycle emerges. Subcritical cases have been extensively documented across various thermoacoustic engine configurations, including standing wave, traveling wave, phase change, and free-piston Stirling types [3][4][5][6][7][8][9][10][11]. Furthermore, a decrease in the temperature gradient reveals hysteresis in oscillation amplitude with subcritical Hopf bifurcations, eventually ceasing through a saddle-node bifurcation at a distinct fold point [2], which signifies the minimum temperature gradient necessary for engine operation.…”