{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,5,13]],"date-time":"2025-05-13T21:58:53Z","timestamp":1747173533221,"version":"3.40.5"},"reference-count":33,"publisher":"Cambridge University Press (CUP)","issue":"1","license":[{"start":{"date-parts":[[2023,8,11]],"date-time":"2023-08-11T00:00:00Z","timestamp":1691712000000},"content-version":"unspecified","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"content-domain":{"domain":["cambridge.org"],"crossmark-restriction":true},"short-container-title":["Combinator. Probab. Comp."],"published-print":{"date-parts":[[2024,1]]},"abstract":"<jats:title>Abstract<\/jats:title><jats:p>We demonstrate a quasipolynomial-time deterministic approximation algorithm for the partition function of a Gibbs point process interacting via a stable potential. This result holds for all activities <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline1.png\"\/><jats:tex-math>\n$\\lambda$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> for which the partition function satisfies a zero-free assumption in a neighbourhood of the interval <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline2.png\"\/><jats:tex-math>\n$[0,\\lambda ]$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula>. As a corollary, for all finiterange stable potentials, we obtain a quasipolynomial-time deterministic algorithm for all <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline3.png\"\/><jats:tex-math>\n$\\lambda \\lt 1\/(e^{B + 1} \\hat C_\\phi )$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> where <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline4.png\"\/><jats:tex-math>\n$\\hat C_\\phi$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> is a temperedness parameter and <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline5.png\"\/><jats:tex-math>\n$B$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> is the stability constant of <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline6.png\"\/><jats:tex-math>\n$\\phi$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula>. In the special case of a repulsive potential such as the hard-sphere gas we improve the range of activity by a factor of at least <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline7.png\"\/><jats:tex-math>\n$e^2$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> and obtain a quasipolynomial-time deterministic approximation algorithm for all <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline8.png\"\/><jats:tex-math>\n$\\lambda \\lt e\/\\Delta _\\phi$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula>, where <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline9.png\"\/><jats:tex-math>\n$\\Delta _\\phi$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula> is the potential-weighted connective constant of the potential <jats:inline-formula><jats:alternatives><jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" mime-subtype=\"png\" xlink:href=\"S0963548323000251_inline10.png\"\/><jats:tex-math>\n$\\phi$\n<\/jats:tex-math><\/jats:alternatives><\/jats:inline-formula>. Our algorithm approximates coefficients of the cluster expansion of the partition function and uses the interpolation method of Barvinok to extend this approximation throughout the zero-free region.<\/jats:p>","DOI":"10.1017\/s0963548323000251","type":"journal-article","created":{"date-parts":[[2023,8,11]],"date-time":"2023-08-11T09:42:44Z","timestamp":1691746964000},"page":"1-15","update-policy":"https:\/\/doi.org\/10.1017\/policypage","source":"Crossref","is-referenced-by-count":2,"title":["Quasipolynomial-time algorithms for Gibbs point processes"],"prefix":"10.1017","volume":"33","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-0026-8501","authenticated-orcid":false,"given":"Matthew","family":"Jenssen","sequence":"first","affiliation":[]},{"given":"Marcus","family":"Michelen","sequence":"additional","affiliation":[]},{"given":"Mohan","family":"Ravichandran","sequence":"additional","affiliation":[]}],"member":"56","published-online":{"date-parts":[[2023,8,11]]},"reference":[{"key":"S0963548323000251_ref9","doi-asserted-by":"publisher","DOI":"10.1016\/0031-9163(62)90198-1"},{"key":"S0963548323000251_ref4","doi-asserted-by":"publisher","DOI":"10.1007\/978-1-4899-6653-7_21"},{"key":"S0963548323000251_ref14","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRev.126.883"},{"key":"S0963548323000251_ref31","doi-asserted-by":"publisher","DOI":"10.1142\/4090"},{"volume-title":"An Introduction to the Theory of Point Processes: Volume II: General Theory and Structure","year":"2007","author":"Daley","key":"S0963548323000251_ref5"},{"key":"S0963548323000251_ref29","doi-asserted-by":"publisher","DOI":"10.1016\/0003-4916(63)90336-1"},{"key":"S0963548323000251_ref25","doi-asserted-by":"publisher","DOI":"10.1137\/16M1101003"},{"key":"S0963548323000251_ref16","doi-asserted-by":"publisher","DOI":"10.1007\/BF00050669"},{"volume-title":"International Computing and Combinatorics Conference (COCOON)","year":"2022","author":"Friedrich","key":"S0963548323000251_ref6"},{"key":"S0963548323000251_ref19","unstructured":"[19] Michelen, M. and Perkins, W. 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