Optimal learning of quantum Hamiltonians from high-temperature Gibbs states
We study the problem of learning a Hamiltonian H to precision \varepsilon, supposing we are given copies of its Gibbs state \rho =\exp(-\beta H)/\mathrm{Tr}(\exp(-\beta H)) at a known inverse temperature \beta. Anshu, Arunachalam, Kuwahara, and Soleimanifar [AAKS21] recently studied the sample compl...
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| Published in: | Proceedings / annual Symposium on Foundations of Computer Science pp. 135 - 146 |
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| Main Authors: | , , |
| Format: | Conference Proceeding |
| Language: | English |
| Published: |
IEEE
01.10.2022
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| Subjects: | |
| ISSN: | 2575-8454 |
| Online Access: | Get full text |
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| Summary: | We study the problem of learning a Hamiltonian H to precision \varepsilon, supposing we are given copies of its Gibbs state \rho =\exp(-\beta H)/\mathrm{Tr}(\exp(-\beta H)) at a known inverse temperature \beta. Anshu, Arunachalam, Kuwahara, and Soleimanifar [AAKS21] recently studied the sample complexity (number of copies of \rho needed) of this problem for geometrically local N-qubit Hamiltonians. In the high-temperature (low \beta) regime, their algorithm has sample complexity poly (N, 1/\beta, 1/\varepsilon) and can be implemented with polynomial, but suboptimal, time complexity. In this paper, we study the same question for a more general class of Hamiltonians. We show how to learn the coefficients of a Hamiltonian to error \varepsilon with sample complexity S=O(\log N/(\beta\varepsilon)^{2}) and time complexity linear in the sample size, O(SN). Furthermore, we prove a matching lower bound showing that our algorithm's sample complexity is optimal, and hence our time complexity is also optimal. In the appendix, we show that virtually the same algorithm can be used to learn H from a real-time evolution unitary e^{-i t H} in a small t regime with similar sample and time complexity. |
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| ISSN: | 2575-8454 |
| DOI: | 10.1109/FOCS54457.2022.00020 |