{"id":961,"date":"2025-12-04T14:24:53","date_gmt":"2025-12-04T14:24:53","guid":{"rendered":"https:\/\/faculty.uccs.edu\/iacocca\/?p=961"},"modified":"2025-12-04T14:27:53","modified_gmt":"2025-12-04T14:27:53","slug":"magnetostatic-waves-via-ps-ll","status":"publish","type":"post","link":"https:\/\/faculty.uccs.edu\/iacocca\/2025\/12\/04\/magnetostatic-waves-via-ps-ll\/","title":{"rendered":"Magnetostatic waves via PS-LL"},"content":{"rendered":"\n<div class=\"wp-block-media-text is-stacked-on-mobile\" style=\"grid-template-columns:40% auto\"><figure class=\"wp-block-media-text__media\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"809\" src=\"https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic-1024x809.png\" alt=\"\" class=\"wp-image-960 size-full\" srcset=\"https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic-1024x809.png 1024w, https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic-300x237.png 300w, https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic-768x607.png 768w, https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic-1536x1213.png 1536w, https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2025\/11\/Caustic.png 1560w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure><div class=\"wp-block-media-text__content\">\n<p class=\"wp-block-paragraph\">Our work to numerically solve for magnetostatic waves within the pseudospectral Landau-Lifshitz (PS-LL) model was just published in <a href=\"https:\/\/www.nature.com\/articles\/s41524-025-01848-3\">npj Computational Materials<\/a>.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">While the PS-LL model was initially developed to resolve the transition from atomic to continuum dynamics, its general formulation allows for the use of any kernel. Here, we use a magnetodipolar kernel that can represent in-plane magnetostatic waves, both backward volume and surface. We demonstrate that the use of this kernel can speed up simulations by a factor of two at the expense of losing the particularities of the magnetization distribution at physical edges.<\/p>\n<\/div><\/div>\n\n\n\n\n<style class=\"advgb-styles-renderer\">\n.post-thumbnail, .entry-meta {\ndisplay: none;\n}\nfooter.entry-footer {\n  display: none;\n}\n<\/style>","protected":false},"excerpt":{"rendered":"<p>Our work to numerically solve for magnetostatic waves within the pseudospectral Landau-Lifshitz (PS-LL) model was just published in npj Computational Materials. While the PS-LL model was initially developed to resolve the transition from atomic to continuum dynamics, its general formulation allows for the use of any kernel. Here, we use a magnetodipolar kernel that can [&hellip;]<\/p>\n","protected":false},"author":33,"featured_media":272,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_uag_custom_page_level_css":"","advgb_blocks_editor_width":"","advgb_blocks_columns_visual_guide":"","footnotes":""},"categories":[5],"tags":[],"class_list":["post-961","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-papers"],"author_meta":{"display_name":"eiacocca","author_link":"https:\/\/faculty.uccs.edu\/iacocca\/author\/eiacocca\/"},"featured_img":"https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801-300x270.png","uagb_featured_image_src":{"full":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801.png",663,596,false],"thumbnail":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801-150x150.png",150,150,true],"medium":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801-300x270.png",300,270,true],"medium_large":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-768x637.png",640,531,true],"large":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801.png",640,575,false],"1536x1536":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801.png",663,596,false],"2048x2048":["https:\/\/faculty.uccs.edu\/iacocca\/wp-content\/uploads\/sites\/36\/2022\/02\/Papers-e1779477855801.png",663,596,false]},"uagb_author_info":{"display_name":"eiacocca","author_link":"https:\/\/faculty.uccs.edu\/iacocca\/author\/eiacocca\/"},"uagb_comment_info":0,"uagb_excerpt":"Our work to numerically solve for magnetostatic waves within the pseudospectral Landau-Lifshitz (PS-LL) model was just published in npj Computational Materials. While the PS-LL model was initially developed to resolve the transition from atomic to continuum dynamics, its general formulation allows for the use of any kernel. Here, we use a magnetodipolar kernel that can&hellip;","coauthors":[],"tax_additional":{"categories":{"linked":["<a href=\"https:\/\/faculty.uccs.edu\/iacocca\/category\/papers\/\" class=\"advgb-post-tax-term\">Papers<\/a>"],"unlinked":["<span class=\"advgb-post-tax-term\">Papers<\/span>"]}},"comment_count":"0","relative_dates":{"created":"Posted 8 months ago","modified":"Updated 8 months ago"},"absolute_dates":{"created":"Posted on December 4, 2025","modified":"Updated on December 4, 2025"},"absolute_dates_time":{"created":"Posted on December 4, 2025 2:24 pm","modified":"Updated on December 4, 2025 2:27 pm"},"featured_img_caption":"","series_order":"","_links":{"self":[{"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/posts\/961","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/users\/33"}],"replies":[{"embeddable":true,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/comments?post=961"}],"version-history":[{"count":4,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/posts\/961\/revisions"}],"predecessor-version":[{"id":971,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/posts\/961\/revisions\/971"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/media\/272"}],"wp:attachment":[{"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/media?parent=961"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/categories?post=961"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/faculty.uccs.edu\/iacocca\/wp-json\/wp\/v2\/tags?post=961"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}