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The mapping has a simple structure and is optimal in the sense that it is impossible to construct Pauli operators in any fermion-to-qubit mapping acting nontrivially on less than<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:msub><mml:mi>log<\/mml:mi><mml:mn>3<\/mml:mn><\/mml:msub><mml:mo>\u2061<\/mml:mo><mml:mo stretchy=\"false\">(<\/mml:mo><mml:mn>2<\/mml:mn><mml:mi>n<\/mml:mi><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math>qubits on average. We apply it to the problem of learning<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>k<\/mml:mi><\/mml:math>-fermion reduced density matrix (RDM), a problem relevant in various quantum simulation applications. We show that one can determine individual elements of all<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>k<\/mml:mi><\/mml:math>-fermion RDMs in parallel, to precision<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>\u03f5<\/mml:mi><\/mml:math>, by repeating a single quantum circuit for<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mo>\u2272<\/mml:mo><mml:mo stretchy=\"false\">(<\/mml:mo><mml:mn>2<\/mml:mn><mml:mi>n<\/mml:mi><mml:mo>+<\/mml:mo><mml:mn>1<\/mml:mn><mml:msup><mml:mo stretchy=\"false\">)<\/mml:mo><mml:mi>k<\/mml:mi><\/mml:msup><mml:msup><mml:mi>\u03f5<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>\u2212<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><\/mml:math>times. This result is based on a method we develop here that allows one to determine individual elements of all<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>k<\/mml:mi><\/mml:math>-qubit RDMs in parallel, to precision<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>\u03f5<\/mml:mi><\/mml:math>, by repeating a single quantum circuit for<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mo>\u2272<\/mml:mo><mml:msup><mml:mn>3<\/mml:mn><mml:mi>k<\/mml:mi><\/mml:msup><mml:msup><mml:mi>\u03f5<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>\u2212<\/mml:mo><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><\/mml:math>times, independent of the system size. This improves over existing schemes for determining qubit RDMs.<\/jats:p>","DOI":"10.22331\/q-2020-06-04-276","type":"journal-article","created":{"date-parts":[[2020,6,4]],"date-time":"2020-06-04T11:48:29Z","timestamp":1591271309000},"page":"276","source":"Crossref","is-referenced-by-count":65,"title":["Optimal fermion-to-qubit mapping via ternary trees with applications to reduced quantum states learning"],"prefix":"10.22331","volume":"4","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-0435-655X","authenticated-orcid":false,"given":"Zhang","family":"Jiang","sequence":"first","affiliation":[{"name":"Google Research, Venice, CA 90291"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-6618-9622","authenticated-orcid":false,"given":"Amir","family":"Kalev","sequence":"additional","affiliation":[{"name":"Joint Center for Quantum Information and Computer Science, University of Maryland, College Park, MD 20742-2420, USA"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-8497-6363","authenticated-orcid":false,"given":"Wojciech","family":"Mruczkiewicz","sequence":"additional","affiliation":[{"name":"Google Research, Venice, CA 90291"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-9681-6746","authenticated-orcid":false,"given":"Hartmut","family":"Neven","sequence":"additional","affiliation":[{"name":"Google Research, Venice, CA 90291"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"9598","published-online":{"date-parts":[[2020,6,4]]},"reference":[{"key":"0","doi-asserted-by":"publisher","unstructured":"R. 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