Adiabatic quantum imaginary time evolution
Abstract
We introduce an adiabatic state preparation protocol which implements quantum imaginary time evolution under the Hamiltonian of the system. Unlike the original quantum imaginary time evolution algorithm, adiabatic quantum imaginary time evolution does not require quantum state tomography during its runtime and, unlike standard adiabatic state preparation, the final Hamiltonian is not the system Hamiltonian. Instead, the algorithm obtains the adiabatic Hamiltonian by integrating a classical differential equation that ensures that one follows the imaginary time evolution state trajectory. We introduce some heuristics that allow this protocol to be implemented on quantum architectures with limited resources. We explore the performance of this algorithm via classical simulations in a one-dimensional spin model and highlight essential features that determine its cost, performance, and implementability for longer times, and compare to the original quantum imaginary time evolution for ground-state preparation. More generally, our algorithm expands the range of states accessible to adiabatic state preparation methods beyond those that are expressed as ground states of simple explicit Hamiltonians. Published by the American Physical Society 2024
Copyright and License
Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.
Acknowledgement
We thank Y. Tong, A. Dalzell, and A. Chen for helpful discussions. K.H. and G.K.C. were supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, under Grant No. DE-SC-0019374. G.K.C. acknowledges support from the Simons Foundation.
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Additional details
- Office of Basic Energy Sciences
- DE-SC-0019374
- Simons Foundation
- Accepted
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2024-06-13Accepted
- Publication Status
- Published