{"id":6689,"date":"2026-03-09T07:36:13","date_gmt":"2026-03-09T06:36:13","guid":{"rendered":"https:\/\/www.mi.uni-koeln.de\/NumSim\/?p=6689"},"modified":"2026-03-09T07:36:13","modified_gmt":"2026-03-09T06:36:13","slug":"new-preprint-published-sbp-fdec-summation-by-parts-finite-difference-exterior-calculus","status":"publish","type":"post","link":"https:\/\/www.mi.uni-koeln.de\/NumSim\/2026\/03\/09\/new-preprint-published-sbp-fdec-summation-by-parts-finite-difference-exterior-calculus\/","title":{"rendered":"New preprint published: SBP-FDEC: Summation-by-Parts Finite Difference Exterior Calculus"},"content":{"rendered":"<p>We extend the framework of Finite Element Exterior Calculus (FEEC) to Summation-by-Parts (SBP) Finite Difference (FD) operators to derive an energy-conservative and divergence-free scheme for the homogeneous Maxwell\u2019s equations.<\/p>\n<p><a href=\"https:\/\/arxiv.org\/abs\/2511.20529v1\">https:\/\/arxiv.org\/abs\/2511.20529v1<\/a><\/p>\n<p><strong>Abstract<\/strong><br \/>\nWe demonstrate that we can carry over the strategy of Finite Element Exterior Calculus (FEEC) to Summation-by-Parts (SBP) Finite Difference (FD) methods to achieve divergence- and curl-free discretizations. This is not obvious at first sight, as for SBP-FD no basis functions are known, but only values and derivatives at points. The key is a remarkable analytic relationship that enables us to construct compatible operators using integral and nodal degrees of freedom. Pre-existing SBP-FD matrix operators can then be used to obtain nodal values from the integral degrees of freedom to derive a scheme with the desired properties.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We extend the framework of Finite Element Exterior Calculus (FEEC) to Summation-by-Parts (SBP) Finite Difference (FD) operators to derive an energy-conservative and divergence-free scheme for the homogeneous Maxwell\u2019s equations. https:\/\/arxiv.org\/abs\/2511.20529v1 Abstract We demonstrate that we can carry over the strategy &hellip; <a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/2026\/03\/09\/new-preprint-published-sbp-fdec-summation-by-parts-finite-difference-exterior-calculus\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":14,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[46],"tags":[],"post_mailing_queue_ids":[],"_links":{"self":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6689"}],"collection":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/users\/14"}],"replies":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/comments?post=6689"}],"version-history":[{"count":1,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6689\/revisions"}],"predecessor-version":[{"id":6690,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6689\/revisions\/6690"}],"wp:attachment":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/media?parent=6689"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/categories?post=6689"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/tags?post=6689"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}