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Numerically simulating such dynamics is generically challenging, which motivates the consideration of quantum computing strategies. However, the relatively high gate errors and limited coherence times of today's quantum computers pose their own challenge, highlighting the need to be frugal with quantum resources. In this work we report simulations on quantum hardware of infinite-temperature energy transport in the mixed-field Ising chain, a paradigmatic many-body system that can exhibit a range of transport behaviors at intermediate times. We consider a chain with <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>L<\/mml:mi><mml:mo>=<\/mml:mo><mml:mn>12<\/mml:mn><\/mml:math> sites and find results broadly consistent with those from ideal circuit simulators over 90 Trotter steps, containing up to 990 entangling gates. To obtain these results, we use two key problem-tailored insights. First, we identify a convenient basis<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mtext>&amp;#x2013;<\/mml:mtext><\/mml:math>the Pauli <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>Y<\/mml:mi><\/mml:math> basis<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mtext>&amp;#x2013;<\/mml:mtext><\/mml:math>in which to sample the infinite-temperature trace and provide theoretical and numerical justifications for its efficiency relative to, e.g., the computational basis. Second, in addition to a variety of problem-agnostic error mitigation strategies, we employ a renormalization strategy that compensates for global nonconservation of energy due to device noise. We discuss the applicability of the proposed sampling approach beyond the mixed-field Ising chain and formulate a variational method to search for a sampling basis with small sample-to-sample fluctuations for an arbitrary Hamiltonian. This opens the door to applying these techniques in more general models.<\/jats:p>","DOI":"10.22331\/q-2024-12-03-1545","type":"journal-article","created":{"date-parts":[[2024,12,3]],"date-time":"2024-12-03T11:49:52Z","timestamp":1733226592000},"page":"1545","update-policy":"https:\/\/doi.org\/10.22331\/q-crossmark-policy-page","source":"Crossref","is-referenced-by-count":4,"title":["Problem-tailored Simulation of Energy Transport on Noisy Quantum Computers"],"prefix":"10.22331","volume":"8","author":[{"given":"I-Chi","family":"Chen","sequence":"first","affiliation":[{"name":"Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA"},{"name":"Ames National Laboratory, Ames, Iowa 50011, USA"}]},{"given":"Kl\u00e9e","family":"Pollock","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA"}]},{"given":"Yong-Xin","family":"Yao","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA"},{"name":"Ames National Laboratory, Ames, Iowa 50011, USA"}]},{"given":"Peter P.","family":"Orth","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA"},{"name":"Ames National Laboratory, Ames, Iowa 50011, USA"},{"name":"Department of Physics, Saarland University, 66123 Saarbr\u00fccken, Germany"}]},{"given":"Thomas","family":"Iadecola","sequence":"additional","affiliation":[{"name":"Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA"},{"name":"Ames National Laboratory, Ames, Iowa 50011, USA"}]}],"member":"9598","published-online":{"date-parts":[[2024,12,3]]},"reference":[{"key":"0","doi-asserted-by":"publisher","unstructured":"Benjamin Doyon. ``Lecture notes on Generalised Hydrodynamics&apos;&apos;. 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