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This paper presents optimal algorithms for preparing quantum ground states using guiding states, achieving logarithmic scaling in precision relative to the spectral gap and initial overlap. By combining amplitude amplification with error-reduction techniques, it establishes a rigorous upper bound that advances the theoretical efficiency of quantum simulation protocols.
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Optimal Ground-State Preparation with a Guiding State

arXiv2 min read

arXiv:2609.38091v1 Announce Type: new Abstract: Suppose a Hamiltonian $H$ has a unique ground state $|\psi_0\rangle$ with an eigenvalue $E_0$, and we have an estimate $\tilde{E}_0$ such that $|\tilde{E}_0-E_0|\leq\delta$, and there is a gap of at least $3\delta$ between $E_0$ and all other eigenvalues. Suppose we have a unitary $A$ available that can produce a "guiding state'" $A|0\rangle$ that has overlap at least $\gamma$ with $|\psi_0\rangle$. We show how to obtain an $\varepsilon$-approximation of $|\psi_0\rangle$ using $O(\log(1/\varepsilon)/\gamma\delta)$ applications of $U=e^{iH}$ and $A$, and their inverses. We give two different algorithms, one based on interleaving amplitude amplification and error-reduction in the style of [HMdW03], and one using the composition of transducers. This paper is the state-preparation follow-up to our two recent ground-state-energy estimation papers [JW26, SdW26]. Combined, our results show an optimal $O(\log(1/\varepsilon)/\gamma\delta)$ upper bound for ground state preparation.

Abstract:Suppose a Hamiltonian $H$ has a unique ground state $|\psi_0\rangle$ with an eigenvalue $E_0$, and we have an estimate $\tilde{E}_0$ such that $|\tilde{E}_0-E_0|\leq\delta$, and there is a gap of at least $3\delta$ between $E_0$ and all other eigenvalues. Suppose we have a unitary $A$ available that can produce a "guiding state'" $A|0\rangle$ that has overlap at least $\gamma$ with $|\psi_0\rangle$. We show how to obtain an $\varepsilon$-approximation of $|\psi_0\rangle$ using $O(\log(1/\varepsilon)/\gamma\delta)$ applications of $U=e^{iH}$ and $A$, and their inverses. We give two different algorithms, one based on interleaving amplitude amplification and error-reduction in the style of [HMdW03], and one using the composition of transducers. This paper is the state-preparation follow-up to our two recent ground-state-energy estimation papers [JW26, SdW26]. Combined, our results show an optimal $O(\log(1/\varepsilon)/\gamma\delta)$ upper bound for ground state preparation.

arXiv:2609.38091 [quant-ph]

(or arXiv:2609.38091v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.38091 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 223 words

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