{"id":1160,"date":"2013-06-28T19:26:55","date_gmt":"2013-06-28T19:26:55","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/warnock_ballisticmodel_02.png"},"modified":"2013-06-28T19:26:55","modified_gmt":"2013-06-28T19:26:55","slug":"warnock_ballisticmodel_02-2","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/a-ballistic-transport-model-for-iii-v-hemts-and-mosfets\/warnock_ballisticmodel_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\/warnock_ballisticmodel_02.png' rel=\"lightbox[1160]\"><img width=\"300\" height=\"202\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02-300x202.png\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02-300x202.png 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02-220x148.png 220w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02.png 723w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 2. Dit distribution for III-V MOSFET in [2], extracted from C-V characteristics in Figure 1. The Dit distribution is inside the band gap of the InP barrier layer. <\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/png","media_details":{"width":723,"height":487,"file":"2013\/06\/warnock_ballisticmodel_02.png","sizes":{"thumbnail":{"file":"warnock_ballisticmodel_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\/warnock_ballisticmodel_02-150x150.png"},"medium":{"file":"warnock_ballisticmodel_02-300x202.png","width":300,"height":202,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02-300x202.png"},"post-thumbnail":{"file":"warnock_ballisticmodel_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\/warnock_ballisticmodel_02-150x150.png"},"abstract-thumb":{"file":"warnock_ballisticmodel_02-220x148.png","width":220,"height":148,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02-220x148.png"},"full":{"file":"warnock_ballisticmodel_02.png","width":723,"height":487,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02.png"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1157,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/warnock_ballisticmodel_02.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1160"}],"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=1160"}]}}