{"id":1341,"date":"2013-07-02T18:49:43","date_gmt":"2013-07-02T18:49:43","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/07\/chesin_nwleds_02.png"},"modified":"2013-07-02T18:49:43","modified_gmt":"2013-07-02T18:49:43","slug":"chesin_nwleds_02-2","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/efficiency-comparison-of-m-and-c-directional-gan-nanowire-based-leds-on-si\/chesin_nwleds_02-2\/","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\/chesin_nwleds_02.png' rel=\"lightbox[1341]\"><img width=\"300\" height=\"205\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-300x205.png\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-300x205.png 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-220x150.png 220w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02.png 498w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 2: Estimated EQE ranges for m- and c-directional axial heterostructures obtained by combining IQE modeling (via the A-B-C model) and extraction efficiency simulations from three-dimensional finite-difference time-domain photonic simulations.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/png","media_details":{"width":498,"height":341,"file":"2013\/07\/chesin_nwleds_02.png","sizes":{"thumbnail":{"file":"chesin_nwleds_02-150x150.png","width":150,"height":150,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-150x150.png"},"medium":{"file":"chesin_nwleds_02-300x205.png","width":300,"height":205,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-300x205.png"},"post-thumbnail":{"file":"chesin_nwleds_02-150x150.png","width":150,"height":150,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-150x150.png"},"abstract-thumb":{"file":"chesin_nwleds_02-220x150.png","width":220,"height":150,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02-220x150.png"},"full":{"file":"chesin_nwleds_02.png","width":498,"height":341,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02.png"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1338,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/chesin_nwleds_02.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1341"}],"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=1341"}]}}