{"id":1388,"date":"2013-07-02T22:16:28","date_gmt":"2013-07-02T22:16:28","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/07\/zhou_nanorod_01.jpg"},"modified":"2013-07-02T22:16:28","modified_gmt":"2013-07-02T22:16:28","slug":"zhou_nanorod_01","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/correlation-of-doping-structure-and-carrier-dynamics-in-a-single-gan-nanorod\/zhou_nanorod_01\/","title":{"rendered":"Figure 1"},"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\/07\/zhou_nanorod_01.jpg' rel=\"lightbox[1388]\"><img width=\"300\" height=\"225\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01-300x225.jpg\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01-300x225.jpg 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01-220x165.jpg 220w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01.jpg 972w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 1: (a) Dark-field STEM, (b) panchromatic, and (c) 3.54-eV monochromatic CL images of a single GaN p-n junction nanorod taken at RT. (d) Panchromatic, (e) 3.59-eV, and (f) 3.35-eV monochromatic CL images of the same nanorod at 93 K. (d) CL spectra of taken at top and base of the nanorod. (h) CL spectrum map along the length of the nanorod indicated by the dotted line in (a).<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/jpeg","media_details":{"width":972,"height":730,"file":"2013\/07\/zhou_nanorod_01.jpg","sizes":{"thumbnail":{"file":"zhou_nanorod_01-150x150.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\/07\/zhou_nanorod_01-150x150.jpg"},"medium":{"file":"zhou_nanorod_01-300x225.jpg","width":300,"height":225,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01-300x225.jpg"},"post-thumbnail":{"file":"zhou_nanorod_01-150x150.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\/07\/zhou_nanorod_01-150x150.jpg"},"abstract-thumb":{"file":"zhou_nanorod_01-220x165.jpg","width":220,"height":165,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01-220x165.jpg"},"full":{"file":"zhou_nanorod_01.jpg","width":972,"height":730,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01.jpg"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1387,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/zhou_nanorod_01.jpg","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1388"}],"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=1388"}]}}