{"id":283119,"date":"2016-09-22T02:00:00","date_gmt":"2016-09-21T23:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=624b091d8404bc67ac424124ffbf9f9c"},"modified":"2016-09-22T02:00:00","modified_gmt":"2016-09-21T23:00:00","slug":"on-the-changes-in-optical-interferometry-induced-by-the-relativistic-motion-of-an-optical-medium","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=283119","title":{"rendered":"On the changes in optical interferometry induced by the relativistic motion of an optical medium"},"content":{"rendered":"<p>We investigate the effects of the relativistic movement of an optical medium on the conditions of<br \/>\nconstructive and destructive interference, reflection and transmission pattern, and performance of<br \/>\nspectroscopes. First, we consider the case of two beams reflected from a relativistically moving<br \/>\nthin film and derive the conditions of constructive and destructive interference. Then we broaden<br \/>\nthe idea to multiple beam interference and formulate a new modified equation of reflection and<br \/>\ntransmission pattern of light from a relativistically moving plane parallel dielectric film.<br \/>\nFinally, we determine the new effective resolving power of a Fabry\u2013Perot spectroscope, which has a<br \/>\nmoving dielectric medium in its etalon. Here, we consider the case where the optical media move<br \/>\nparallel to the plane of incidence of light. Throughout this paper, we use the basic Lorentz<br \/>\ntransformation of space and time co-ordinates and electromagnetic fields to conduct these<br \/>\ninvestigations. This paper can stro&#8230;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We investigate the effects of the relativistic movement of an optical medium on the conditions of<br \/>\nconstructive and destructive interference, reflection and transmission pattern, and performance of<br \/>\nspectroscopes. First, we consider the case of two bea&#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-283119","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\/283119","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=283119"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/283119\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=283119"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=283119"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=283119"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}