{"id":520171,"date":"2017-09-27T02:00:00","date_gmt":"2017-09-26T23:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=c924a3d3fd2a9b8e8b977be9ea0f6b80"},"modified":"2017-09-27T02:00:00","modified_gmt":"2017-09-26T23:00:00","slug":"an-effective-introduction-to-structural-crystallography-using-1d-gaussian-atoms","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=520171","title":{"rendered":"An effective introduction to structural crystallography using 1D Gaussian atoms"},"content":{"rendered":"<p>The most important quantitative aspects of computational structural crystallography can be<br \/>\nintroduced in a satisfactory way using 1D truncated and periodic Gaussian functions to represent the<br \/>\natoms in a crystal lattice. This paper describes in detail and demonstrates 1D structural<br \/>\ncrystallography starting with the definition of such truncated Gaussians. The availability of the<br \/>\ncomputer programme CRONE makes possible the repetition of the examples provided in the paper as well<br \/>\nas the creation of new ones.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The most important quantitative aspects of computational structural crystallography can be<br \/>\nintroduced in a satisfactory way using 1D truncated and periodic Gaussian functions to represent the<br \/>\natoms in a crystal lattice. This paper describes in detail&#8230;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[178],"tags":[],"class_list":{"0":"post-520171","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-fuusikaharidus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/520171","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=520171"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/520171\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=520171"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=520171"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=520171"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}