“…The various platforms for such optimisation include optical parametric oscillators [17,18], electronic oscillators [19,20], memristors [21], lasers [22][23][24][25], photonic simulators [26,27], cold atoms [28,29], trapped ions [30], polariton condensates [31,32], photon condensates [33], QED [34,35], and others [36][37][38]. While the demonstration of their ability to find the global minima of computationally hard problems faster than the classical von Neumann architecture remains elusive, many of these disparate physical systems can either efficiently perform matrix-vector multiplication [26,[39][40][41][42] or mimic the Hopfield neural networks [21,43,44]. For a certain choice of parameters, the time evolution of such networks can be viewed as an eigenvalue maximisation problem [45], which results in finding the energy state dictated by signs of the eigenvector corresponding to the largest eigenvalue of the interaction matrix, i.e.…”