{"id":1192,"date":"2013-06-28T20:49:22","date_gmt":"2013-06-28T20:49:22","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/alobeidi_energystorage_02.jpg"},"modified":"2013-06-28T20:49:22","modified_gmt":"2013-06-28T20:49:22","slug":"alobeidi_energystorage_02-2","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/structured-silicon-for-energy-storage-in-microsystems\/alobeidi_energystorage_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\/06\/alobeidi_energystorage_02.jpg' rel=\"lightbox[1192]\"><img width=\"300\" height=\"240\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02-300x240.jpg\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02-300x240.jpg 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02-220x176.jpg 220w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02.jpg 640w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 2: After lithiation, the porous amorphous silicon film breaks into large columnar islands that remain adherent to the current  collector.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/jpeg","media_details":{"width":640,"height":512,"file":"2013\/06\/alobeidi_energystorage_02.jpg","sizes":{"thumbnail":{"file":"alobeidi_energystorage_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\/06\/alobeidi_energystorage_02-150x150.jpg"},"medium":{"file":"alobeidi_energystorage_02-300x240.jpg","width":300,"height":240,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02-300x240.jpg"},"post-thumbnail":{"file":"alobeidi_energystorage_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\/06\/alobeidi_energystorage_02-150x150.jpg"},"abstract-thumb":{"file":"alobeidi_energystorage_02-220x176.jpg","width":220,"height":176,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02-220x176.jpg"},"full":{"file":"alobeidi_energystorage_02.jpg","width":640,"height":512,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02.jpg"}},"image_meta":{"aperture":0,"credit":"","camera":"-CARL ZEISS-","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1189,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/alobeidi_energystorage_02.jpg","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1192"}],"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=1192"}]}}