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In sharp contrast to the dense case [1, 2], we prove that strictly <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>q<\/mml:mi><\/mml:math>-local <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mtext class=\"MJX-tex-mathit\" mathvariant=\"italic\">sparse<\/mml:mtext><\/mml:mrow><\/mml:mrow><\/mml:math> fermionic Hamiltonians have a constant Gaussian approximation ratio; the result holds for any connectivity and interaction strengths. Sparsity means that each fermion participates in a bounded number of interactions, and strictly <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>q<\/mml:mi><\/mml:math>-local means that each term involves exactly <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>q<\/mml:mi><\/mml:math> fermionic (Majorana) operators. We extend our proof to give a constant Gaussian approximation ratio for sparse fermionic Hamiltonians with both quartic and quadratic terms. With additional work, we also prove a constant Gaussian approximation ratio for the so-called sparse SYK model with strictly <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>4<\/mml:mn><\/mml:math>-local interactions (sparse SYK-<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>4<\/mml:mn><\/mml:math> model). In each setting we show that the Gaussian state can be efficiently determined. Finally, we prove that the <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>O<\/mml:mi><mml:mo stretchy=\"false\">(<\/mml:mo><mml:msup><mml:mi>n<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>&amp;#x2212;<\/mml:mo><mml:mn>1<\/mml:mn><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>\/<\/mml:mo><\/mml:mrow><mml:mn>2<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math> Gaussian approximation ratio for the normal (dense) SYK-<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>4<\/mml:mn><\/mml:math> model extends to SYK-<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>q<\/mml:mi><\/mml:math> for even <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>q<\/mml:mi><mml:mo>&amp;#x003E;<\/mml:mo><mml:mn>4<\/mml:mn><\/mml:math>, with an approximation ratio of <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>O<\/mml:mi><mml:mo stretchy=\"false\">(<\/mml:mo><mml:msup><mml:mi>n<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mn>1<\/mml:mn><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>\/<\/mml:mo><\/mml:mrow><mml:mn>2<\/mml:mn><mml:mo>&amp;#x2013;<\/mml:mo><mml:mi>q<\/mml:mi><mml:mrow class=\"MJX-TeXAtom-ORD\"><mml:mo>\/<\/mml:mo><\/mml:mrow><mml:mn>4<\/mml:mn><\/mml:mrow><\/mml:msup><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math>. Our results identify non-sparseness as the prime reason that the SYK-<mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>4<\/mml:mn><\/mml:math> model can fail to have a constant approximation ratio [1, 2].<\/jats:p>","DOI":"10.22331\/q-2023-08-10-1081","type":"journal-article","created":{"date-parts":[[2023,8,10]],"date-time":"2023-08-10T12:48:04Z","timestamp":1691671684000},"page":"1081","update-policy":"https:\/\/doi.org\/10.22331\/q-crossmark-policy-page","source":"Crossref","is-referenced-by-count":13,"title":["Optimizing sparse fermionic Hamiltonians"],"prefix":"10.22331","volume":"7","author":[{"given":"Yaroslav","family":"Herasymenko","sequence":"first","affiliation":[{"name":"QuSoft & CWI, Science Park 123 1098 XG Amsterdam, The Netherlands"},{"name":"QuTech, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, The Netherlands"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Maarten","family":"Stroeks","sequence":"additional","affiliation":[{"name":"QuTech, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, The Netherlands"},{"name":"EEMCS Faculty, Delft University of Technology, Van Mourik Broekmanweg 6, 2628 XE, Delft, The Netherlands"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Jonas","family":"Helsen","sequence":"additional","affiliation":[{"name":"QuSoft & CWI, Science Park 123 1098 XG Amsterdam, The Netherlands"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Barbara","family":"Terhal","sequence":"additional","affiliation":[{"name":"QuTech, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, The Netherlands"},{"name":"EEMCS Faculty, Delft University of Technology, Van Mourik Broekmanweg 6, 2628 XE, Delft, The Netherlands"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"9598","published-online":{"date-parts":[[2023,8,10]]},"reference":[{"key":"0","doi-asserted-by":"publisher","unstructured":"Arijit Haldar, Omid Tavakol, and Thomas Scaffidi. 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