๐’๐ก๐จ๐ญ-๐ง๐จ๐ข๐ฌ๐ž ๐ซ๐ž๐๐ฎ๐œ๐ญ๐ข๐จ๐ง ๐Ÿ๐จ๐ซ ๐ฅ๐š๐ญ๐ญ๐ข๐œ๐ž ๐‡๐š๐ฆ๐ข๐ฅ๐ญ๐จ๐ง๐ข๐š๐ง๐ฌ published in ๐๐‘๐—๐๐ฎ๐š๐ง๐ญ๐ฎ๐ฆ.

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Our work ๐’๐ก๐จ๐ญ-๐ง๐จ๐ข๐ฌ๐ž ๐ซ๐ž๐๐ฎ๐œ๐ญ๐ข๐จ๐ง ๐Ÿ๐จ๐ซ ๐ฅ๐š๐ญ๐ญ๐ข๐œ๐ž ๐‡๐š๐ฆ๐ข๐ฅ๐ญ๐จ๐ง๐ข๐š๐ง๐ฌ has just been published in ๐๐‘๐—๐๐ฎ๐š๐ง๐ญ๐ฎ๐ฆ. Directly go to the paper here: https://doi.org/10.1103/xy36-drb3

By: Timo Eckstein, Refik Mansuroglu, Stefan Wolf, Ludwig Nรผtzel, Stephan Tasler, Martin Kliesch, and Hartmann Michael

In quantum computing, in contrast to its classical counterpart, the result of our computation is typically not a single deterministic bitstring but a probability distribution encoded into a quantum state. Hence, a central task after state preparation is to efficiently extract information from this probability distribution, which, on a real-world quantum device, corresponds to measuring the generated quantum state. Particularly relevant near-term measurement tasks are those for energy estimation of low-energy stats, as they are considered an enabler for material science research via quantum computing.

Here, we present a measurement scheme for estimating the energy of quantum lattice models from measurements of a prepared quantum state. We prove that it always requires fewer measurements for the same precision as โ€œnaiveโ€ sampling in mutually commuting groups. Our method is based on partitioning the lattice into local patches and then measuring those in the eigenbases of their local Hamiltonians via a transformation of local eigenstates into the measurement basis, typically reducing the required number of measurements by several orders of magnitude.

We expect our results to have a noticeable impact on near-term eigenstate preparation algorithms, as those typically need to estimate the stateโ€™s energy numerous times. Importantly, the patch size can be freely chosen to fit the available gate budget, starting from as little as ๐‘›/2 additional 2-qubit gates, which are simply appended to the end of the existing quantum circuit.


We acknowledge support from FAU Erlangen-Nรผrnberg, FAU Profile Center Light.Matter.QuantumTechnologies, Max Planck Institute for the Science of Light, University of Vienna, Hamburg University of Technology, Erlangen National High Performance Computing Center (NHR@FAU), Deutsche Forschungsgemeinschaft (DFG) – German Research Foundation (QuCoLiMa), Bundesministerium fรผr Bildung und Forschung (EQUAHUMO), IMPRS Physics of Light, Fujitsu Germany GmbH and Bavarian State Ministry of Science and the Arts and Bayerisches Staatsministerium fรผr Wirtschaft, Landesentwicklung und Energie via Munich Quantum Valley, Elite Network of Bavaria, Hightech Agenda Bavaria