{"id":814,"date":"2013-06-26T13:39:21","date_gmt":"2013-06-26T13:39:21","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/rakheja_vsmodelgraphene_3a.png"},"modified":"2013-06-26T13:39:21","modified_gmt":"2013-06-26T13:39:21","slug":"rakheja_vsmodelgraphene_3a","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_3a\/","title":{"rendered":"Figure 3a"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"

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

Figure 3a: Experimental data (symbols) for the device of length and width = 5 \u00b5m from ((H. Wang, A. Hsu, J. Kong, D. A. Antoniadis, and T. Palacios, \u201cCompact virtual-source current-voltage model for top- and back-gated graphene field-effect transistors,\u201d IEEE Transactions on Electron Devices, vol. 58, no. 5, May 2011.)). The drift-diffusion model is fitted as shown in solid lines. <\/p>\n"},"alt_text":"Figure 3a","media_type":"image","mime_type":"image\/png","media_details":{"width":430,"height":338,"file":"2013\/06\/rakheja_vsmodelgraphene_3a.png","sizes":{"thumbnail":{"file":"rakheja_vsmodelgraphene_3a-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_3a-150x150.png"},"medium":{"file":"rakheja_vsmodelgraphene_3a-300x235.png","width":300,"height":235,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_3a-300x235.png"},"post-thumbnail":{"file":"rakheja_vsmodelgraphene_3a-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_3a-150x150.png"},"abstract-thumb":{"file":"rakheja_vsmodelgraphene_3a-220x172.png","width":220,"height":172,"mime_type":"image\/png","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/rakheja_vsmodelgraphene_3a-220x172.png"},"full":{"file":"rakheja_vsmodelgraphene_3a.png","width":430,"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_3a.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_3a.png","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/814"}],"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=814"}]}}