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 excel on tasks using functional data%2C such as those originating from partial differential equations. Such characteristics render them an effective approach for simulating the time evolution of quantum wavefunctions%2C which is a computationally challenging%2C yet coveted task for understanding quantum systems. In this manuscript%2C we use FNOs to model the evolution of random quantum spin systems%2C so chosen due to their representative quantum dynamics and minimal symmetry. We explore two distinct FNO architectures and examine their performance for learning and predicting time evolution using both random and low-energy input states. Additionally%2C we apply FNOs to a compact set of Hamiltonian observables (%24simtext{poly}(n)%24) instead of the entire %242^n%24 quantum wavefunction%2C which greatly reduces the size of our inputs and outputs and%2C consequently%2C the requisite dimensions of the resulting FNOs. Moreover%2C this Hamiltonian observable-based method demonstrates that FNOs can effectively distill information from high-dimensional spaces into lower-dimensional spaces. The extrapolation of Hamiltonian observables to times later than those used in training is of particular interest%2C as this stands to fundamentally increase the simulatability of quantum systems past both the coherence times of contemporary quantum architectures and the circuit-depths of tractable tensor networks.?quality=80&w=800)
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