Abstract
Combinatorial optimization problems over large and complex systems have many applications in social networks, image processing, artificial intelligence, computational biology and a variety of other areas. Finding the optimized solution for such problems in general are usually in non-deterministic polynomial time (NP)-hard complexity class. Some NP-hard problems can be easily mapped to minimizing an Ising energy function. Here, we present an analog all-optical implementation of a coherent Ising machine (CIM) based on a network of injection-locked multicore fiber (MCF) lasers. The Zeeman terms and the mutual couplings appearing in the Ising Hamiltonians are implemented using spatial light modulators (SLMs). As a proof-of-principle, we demonstrate the use of optics to solve several Ising Hamiltonians for up to thirteen nodes. Overall, the average accuracy of the CIM to find the ground state energy was ~90% for 120 trials. The fundamental bottlenecks for the scalability and programmability of the presented CIM are discussed as well.
Highlights
Combinatorial optimization problems over large and complex systems have many applications in social networks, image processing, artificial intelligence, computational biology and a variety of other areas
The number of slave lasers (SLs) represent the number of nodes in the Ising Hamiltonian, and they are locked by a single frequency master laser (ML) with vertical linear polarization
We begin with deriving nonlinear coupled photon rate equations describing the dynamics of a network of injectionlocked lasers for the average photon numbers in the left and Master laser Isolator
Summary
Combinatorial optimization problems over large and complex systems have many applications in social networks, image processing, artificial intelligence, computational biology and a variety of other areas. Finding the ground state spin configuration of the general Ising Hamiltonian is known to be an NP-hard problem (for three dimensions, as well as two dimensions with the Zeeman term):[55] At the same time by enabling the cross links between SLs, the mutual-coupling terms in the Ising Hamiltonian are turned on.
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