{"schema":"pith.reference-change-event.v1","doi":"10.1038/srep01228","canonical_url":"https://pith.science/event/10.1038/srep01228","json_url":"https://pith.science/event/10.1038/srep01228.json","not_a_judgment":"This page records that a citing paper's bibliography includes a work with a published notice. It is not a judgment on the citing paper.","primary":{"event_id":482810,"doi":"10.1038/srep01228","event_type":"correction","event_type_label":"Correction","source":"crossref","source_label":"Crossref","event_date":"2013-03-04","title":"Erratum: A bottom-up route to enhance thermoelectric figures of merit in graphene nanoribbons","work_title":"Sevinçli, C","work_doi":"10.1038/srep01228","work_arxiv_id":null,"notice_doi":"10.1038/srep01355","flag_count":0,"flags_open":0,"flags_disputed":0,"latest_flag_at":null,"human_href":"/event/10.1038/srep01228","json_href":"/event/10.1038/srep01228.json"},"events":[{"event_id":482810,"doi":"10.1038/srep01228","event_type":"correction","event_type_label":"Correction","source":"crossref","source_label":"Crossref","event_date":"2013-03-04","title":"Erratum: A bottom-up route to enhance thermoelectric figures of merit in graphene nanoribbons","work_title":"Sevinçli, C","work_doi":"10.1038/srep01228","work_arxiv_id":null,"notice_doi":"10.1038/srep01355","flag_count":0,"flags_open":0,"flags_disputed":0,"latest_flag_at":null,"human_href":"/event/10.1038/srep01228","json_href":"/event/10.1038/srep01228.json"}],"flags":[{"id":8232,"status":"open","status_label":"Open","citing_arxiv_id":"2602.17453","citing_title":"Charge and energy transport in graphene with smooth finite-range disorder","ref_index":60,"evidence_raw":"H. Sevinçli, C. Sevik, T. Ça ˘gın, G. Cuniberti, A bottom-up route to enhance thermoelectric figures of merit in graphene nanoribbons, Sci- entific Reports 3 (1) (2013) 1228.doi:10.1038/srep01228. URLhttps://doi.org/10.1038/srep01228 :Preprint submitted to Elsevier Page 10 of 10 0.0 0.2 0.4 0.6 0.8 1.0 0 10 20 30 40 50 60 (a) 0.0 0.2 0.4 0.6 0.8 1.0 0 10 20 30 40 50 60 (b) Figure 2:Transport relaxation time (in picoseconds) as a function of the Fermi energy, calculated using Eq.(18)for a random distribution of 3 nm-radius soft spheres with a concentration of𝑛 imp =1×10 12 cm−2, and for various poten- tials. The subfigure (a) corresponds to positive soft sphere potentials, whereas (b) corresponds to negative ones. -40 -20 0 20 40 0 100 200 300 400 500 600 (a) 2.5 3.0 3.5 4.0 4.5 5.00 100 200 300 400 500 600 700 (b) Figure 3:DC conductivity at zero temperature versus (a) the radii of the spheres and (b) the soft-sphere potential. In both cases, the Fermi energy isℰ 𝐹 =200meV. :Preprint submitted to Elsevier Page 11 of 10 0.0 0.2 0.4 0.6 0.8 1.00 2 4 6 8 10 12 14 (a) 0.0 0.2 0.4 0.6 0.8 1.00 1 2 3 4 5 (b) 0.0 0.2 0.4 0.6 0.8 1.00.0 0.5 1.0 1.5 (c) Figure 4:DC conductivity versus the F","evidence_cleaned":null,"evidence_source_label":"bibliography line","event_type":"correction","event_type_label":"Correction","source_label":"Crossref","event_date":"2013-03-04","work_title":"Sevinçli, C","work_doi":"10.1038/srep01228","event_doi":"10.1038/srep01228","flag_href":"/flags/8232","event_href":"/event/10.1038/srep01228","paper_href":"/paper/2602.17453","created_at":"2026-08-03T00:20:06.777703Z","dispute_note":null,"disputed_at":null,"disputed_by":null}],"flag_count":1,"flags_open":1,"flags_disputed":0,"desk_url":"https://pith.science/flags"}