{"id":1241,"date":"2013-07-01T14:42:47","date_gmt":"2013-07-01T14:42:47","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/07\/flores_nanoimprint_01.png"},"modified":"2013-07-01T14:42:47","modified_gmt":"2013-07-01T14:42:47","slug":"flores_nanoimprint_01-2","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/applications-of-nanoimprinted-structures-in-organic-photovoltaics\/flores_nanoimprint_01-2\/","title":{"rendered":"Figure 1"},"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\/flores_nanoimprint_01.png' rel=\"lightbox[1241]\"><img width=\"300\" height=\"224\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01-300x224.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\/flores_nanoimprint_01-300x224.png 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01-220x164.png 220w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01.png 912w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 1: Model of power flow and absorption of single nanowedge unit cell. Arrows designate the Poynting vector of time-averaged power flow. Absorbing active layer is sandwiched between layers of glass. Incident light is TE polarized and varied from 300 to 900 nm.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/png","media_details":{"width":912,"height":682,"file":"2013\/07\/flores_nanoimprint_01.png","sizes":{"thumbnail":{"file":"flores_nanoimprint_01-150x150.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\/flores_nanoimprint_01-150x150.png"},"medium":{"file":"flores_nanoimprint_01-300x224.png","width":300,"height":224,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01-300x224.png"},"post-thumbnail":{"file":"flores_nanoimprint_01-150x150.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\/flores_nanoimprint_01-150x150.png"},"abstract-thumb":{"file":"flores_nanoimprint_01-220x164.png","width":220,"height":164,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01-220x164.png"},"full":{"file":"flores_nanoimprint_01.png","width":912,"height":682,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01.png"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1238,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/flores_nanoimprint_01.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1241"}],"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=1241"}]}}