Parameterized quantum circuit defined by a vector θ = (θ 1, …, θ m ) of m parameters, here for m = 19. (a) For a number p of circuit layers the block of gates inside the dashed rectangle is repeated p times. Here we show the circuit for p = 1. The F-VQE algorithm samples the entire circuit to evaluate a global observable indicated by the blue rectangle. (b) and (c) Highlighted qubits and gates constitute the causal cone that HE-ITE uses to evaluate two-local observables on two neighboring qubits and two non-neighboring qubits, respectively.

Parameterized quantum circuit defined by a vector θ = (θ 1, …, θ m ) of m parameters, here for m = 19. (a) For a number p of circuit layers the block of gates inside the dashed rectangle is repeated p times. Here we show the circuit for p = 1. The F-VQE algorithm samples the entire circuit to evaluate a global observable indicated by the blue rectangle. (b) and (c) Highlighted qubits and gates constitute the causal cone that HE-ITE uses to evaluate two-local observables on two neighboring qubits and two non-neighboring qubits, respectively.

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Current gate-based quantum computers have the potential to provide a computational advantage if algorithms use quantum hardware efficiently. To make combinatorial optimization more efficient, we introduce the Filtering Variational Quantum Eigensolver (F-VQE) which utilizes filtering operators to achieve faster and more reliable convergence to the o...

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