Estimating ground state energies of many-body Hamiltonians is a central task in many areas of quantum physics. In this work, we give quantum algorithms which, given any k-body Hamiltonian H, compute an estimate for the ground state energy and prepare a quantum state achieving said energy, respectively. Specifically, for any ε>0, our algorithms return, with high probability, an estimate of the ground state energy of H within additive error ε M, or a quantum state with the corresponding energy. Here, M is the total strength of all interaction terms, which in general is extensive in the system size. Our approach makes no assumptions about the geometry or spatial locality of interaction terms of the input Hamiltonian and thus handles even long-range or all-to-all interactions, such as in quantum chemistry, where lattice-based techniques break down. In this fully general setting, the runtime of our algorithms scales as 2cn/2 for $c<1$, yielding the first quantum algorithms for low-energy estimation breaking the natural bound based on Grover search. The core of our approach is remarkably simple, and relies on showing that any k-body Hamiltonian has a low-energy subspace of exponential dimension.
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Buhrman et al. (2024) studied this question.
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