Abstract

In recent years there has been a growing interest in the physical implementation of classical spin models through networks of optical oscillators. However, a key missing step in this mapping is to formally prove that the dynamics of such a nonlinear dynamical system is toward minimizing a global cost function which is equivalent with the spin model Hamiltonian. Here, we introduce a minimal dynamical model for a network of dissipatively coupled optical oscillators and prove that the dynamics of such a system is governed by a Lyapunov function that serves as a cost function for the system. This cost function is in general a function of both phases and intensities of the oscillators and depends strongly on the pump parameter. In case of bipartite network topologies, the amplitudes of the oscillators become identical in the steady state and the cost function reduces to the XY Hamiltonian. In the general case for non-trivial network topologies, however, the cost function approaches the XY Hamiltonian only in the strong pump limit. We show that by adiabatically tuning the pump parameter, the network can largely avoid trapping into the local minima of the governing cost function and stabilize into the ground state of the associated XY Hamiltonian. These results show the great potential of laser networks for unconventional computing.

Highlights

  • Classical spin models are widely utilized in statistical mechanics and condensed matter physics for exploring critical phenomena and phase transitions in magnetic materials [1,2]

  • Networks of coherently coupled degenerate optical parametric oscillators were used for implementing a binary spin system in analogy with the Ising model and utilized for solving NP-hard problems [8,9]

  • The results suggest that the nonbipartite network involves a more complex cost function with a larger number of local minima states

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Summary

INTRODUCTION

Classical spin models are widely utilized in statistical mechanics and condensed matter physics for exploring critical phenomena and phase transitions in magnetic materials [1,2]. In the case of coupled lasers, assuming that the intensities of all lasers are equal, the phases are shown to be governed by an energy landscape function which turns out to be identical to an antiferromagnetic XY Hamiltonian [10]. Assuming that the two oscillators reach the same steady-state intensity |a1,2| = |a|, the dissipated power simplifies to Pdiss ∝ κ12|a|[1 + cos(φ1 − φ2)], which is identical to the classical XY Hamiltonian for a lattice with two spins. When assuming globally uniform intensities, the phases are governed by a sinusoidal coupling In this case, one can define an energy landscape that is identical to the XY Hamiltonian for an antiferromagnetic spin system.

MAPPING THE XY MODEL
LOCAL MINIMA
Findings
CONCLUSION
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