{"id":813,"date":"2013-06-26T13:39:19","date_gmt":"2013-06-26T13:39:19","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/rakheja_vsmodelgraphene_01a.png"},"modified":"2013-06-26T13:39:19","modified_gmt":"2013-06-26T13:39:19","slug":"rakheja_vsmodelgraphene_01a","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/a-unified-charge-current-vs-compact-model-for-graphene-transistors-applicable-in-analog-circuit-simulations\/rakheja_vsmodelgraphene_01a\/","title":{"rendered":"Figure 2"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"

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

Figure 1a: ID versus VGS of the top gate in graphene for a VDS of 1V. Experimental data from [5] for a channel length is 240 nm and channel width of 1 \u00b5m. The extracted mobility is 1480 cm2\/Vs and vxo = 2.5e7 cm\/s.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/png","media_details":{"width":422,"height":338,"file":"2013\/06\/rakheja_vsmodelgraphene_01a.png","sizes":{"thumbnail":{"file":"rakheja_vsmodelgraphene_01a-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\/rakheja_vsmodelgraphene_01a-150x150.png"},"medium":{"file":"rakheja_vsmodelgraphene_01a-300x240.png","width":300,"height":240,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_01a-300x240.png"},"post-thumbnail":{"file":"rakheja_vsmodelgraphene_01a-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\/rakheja_vsmodelgraphene_01a-150x150.png"},"abstract-thumb":{"file":"rakheja_vsmodelgraphene_01a-220x176.png","width":220,"height":176,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_01a-220x176.png"},"full":{"file":"rakheja_vsmodelgraphene_01a.png","width":422,"height":338,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_01a.png"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":809,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_01a.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/813"}],"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=813"}]}}