{"id":243514,"date":"2016-07-14T02:00:00","date_gmt":"2016-07-13T23:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=ce110f67ed504e980a1912c261ac06a2"},"modified":"2016-07-14T02:00:00","modified_gmt":"2016-07-13T23:00:00","slug":"a-laplace-transform-approach-to-the-reflection-and-transmission-of-electrons-at-semi-infinitepotential-barriers","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=243514","title":{"rendered":"A Laplace transform approach to the reflection and transmission of electrons at semi-infinite\r\npotential barriers"},"content":{"rendered":"<p>The logic of the Schr\u00f6dinger equation may be understood most readily by a consideration of a very<br \/>\nimportant class of problems, i.e. those of the transmission and reflection of electrons through<br \/>\nsemi-infinite potential barriers. In this paper I revisit this problem by applying an alternative<br \/>\napproach via Laplace transforms, demonstrating how effective they are in the determination of the<br \/>\nsolution.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The logic of the Schr\u00f6dinger equation may be understood most readily by a consideration of a very<br \/>\nimportant class of problems, i.e. those of the transmission and reflection of electrons through<br \/>\nsemi-infinite potential barriers. In this paper I revis&#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-243514","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\/243514","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=243514"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/243514\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=243514"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=243514"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=243514"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}