{"id":1694,"date":"2013-07-09T20:41:21","date_gmt":"2013-07-09T20:41:21","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/07\/yaacobi_chirpedrods_02.jpg"},"modified":"2013-07-09T20:41:21","modified_gmt":"2013-07-09T20:41:21","slug":"yaacobi_chirpedrods_02","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/frequency-chirped-sub-wavelength-nanoantennas\/yaacobi_chirpedrods_02\/","title":{"rendered":"Figure 2"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"<p class=\"attachment\"><a href='https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02.jpg' rel=\"lightbox[1694]\"><img width=\"257\" height=\"300\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-257x300.jpg\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-257x300.jpg 257w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-188x220.jpg 188w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02.jpg 600w\" sizes=\"(max-width: 257px) 100vw, 257px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 2. (a) Simulated vertical emission for different structures, (b) Final structure with time integrated field box showing radiated field, (c) Free space far field pattern of same structure at \u03bb=1550 nm.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/jpeg","media_details":{"width":600,"height":700,"file":"2013\/07\/yaacobi_chirpedrods_02.jpg","sizes":{"thumbnail":{"file":"yaacobi_chirpedrods_02-150x150.jpg","width":150,"height":150,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-150x150.jpg"},"medium":{"file":"yaacobi_chirpedrods_02-257x300.jpg","width":257,"height":300,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-257x300.jpg"},"post-thumbnail":{"file":"yaacobi_chirpedrods_02-150x150.jpg","width":150,"height":150,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-150x150.jpg"},"abstract-thumb":{"file":"yaacobi_chirpedrods_02-188x220.jpg","width":188,"height":220,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02-188x220.jpg"},"full":{"file":"yaacobi_chirpedrods_02.jpg","width":600,"height":700,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02.jpg"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1691,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/yaacobi_chirpedrods_02.jpg","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1694"}],"collection":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media"}],"about":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/types\/attachment"}],"author":[{"embeddable":true,"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/users\/370"}],"replies":[{"embeddable":true,"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/comments?post=1694"}]}}