{"id":327657,"date":"2016-11-30T03:00:00","date_gmt":"2016-11-30T00:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=1970c9c02ee9a7f82074a21d35b10387"},"modified":"2016-11-30T03:00:00","modified_gmt":"2016-11-30T00:00:00","slug":"a-general-theorem-on-indeterminism-in-classical-particle-dynamics-inflationary-scenarios","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=327657","title":{"rendered":"A general theorem on indeterminism in classical particle dynamics: inflationary scenarios"},"content":{"rendered":"<p>In the study of systems with an infinite number of particles, the results of indeterminism through<br \/>\ndeterministic collisions have until now usually made use of the temporal symmetry of mechanics. In<br \/>\nthis paper we take a more general path. This path furnishes proof that (in such systems)<br \/>\nindeterminism based on deterministic collisions is rather more common than is suggested in studies<br \/>\npublished to date. A detailed analysis is made of what are known as inflationary scenarios, an<br \/>\ninteresting type of very general situations that display indeterminism.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In the study of systems with an infinite number of particles, the results of indeterminism through<br \/>\ndeterministic collisions have until now usually made use of the temporal symmetry of mechanics. In<br \/>\nthis paper we take a more general path. This path fu&#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-327657","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\/327657","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=327657"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/327657\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=327657"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=327657"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=327657"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}