{"id":935,"date":"2013-06-27T19:21:30","date_gmt":"2013-06-27T19:21:30","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/jean_nanowiresolar_02.png"},"modified":"2013-06-27T19:21:30","modified_gmt":"2013-06-27T19:21:30","slug":"jean_nanowiresolar_02-2","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/zno-nanowire-arrays-for-enhanced-photocurrent-in-pbs-quantum-dot-solar-cells\/jean_nanowiresolar_02-2\/","title":{"rendered":"Figure 2"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"

\"\"<\/a><\/p>\n"},"caption":{"rendered":"

Figure 2: J-V characteristics under AM1.5G illumination for representative planar (black) and nanowire-based (red) QDPV devices. Incorporating ZnO nanowires boosts the short-circuit current density (JSC) and the power conversion efficiency (PCE) by 50% and 35%, respectively. Black crosses indicate the maximum power point.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/png","media_details":{"width":3598,"height":2418,"file":"2013\/06\/jean_nanowiresolar_02.png","sizes":{"thumbnail":{"file":"jean_nanowiresolar_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\/06\/jean_nanowiresolar_02-150x150.png"},"medium":{"file":"jean_nanowiresolar_02-300x201.png","width":300,"height":201,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/jean_nanowiresolar_02-300x201.png"},"large":{"file":"jean_nanowiresolar_02-1024x688.png","width":1024,"height":688,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/jean_nanowiresolar_02-1024x688.png"},"post-thumbnail":{"file":"jean_nanowiresolar_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\/06\/jean_nanowiresolar_02-150x150.png"},"abstract-thumb":{"file":"jean_nanowiresolar_02-220x147.png","width":220,"height":147,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/jean_nanowiresolar_02-220x147.png"},"full":{"file":"jean_nanowiresolar_02.png","width":3598,"height":2418,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/jean_nanowiresolar_02.png"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":933,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/jean_nanowiresolar_02.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/935"}],"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=935"}]}}