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dc.contributor.authorWang, X
dc.contributor.authorCelebi, G
dc.contributor.authorHarris, HR
dc.contributor.authorTemkin, H
dc.contributor.authorGangopadhyay, S
dc.contributor.authorBiswas, N
dc.date.accessioned2021-03-05T18:26:17Z
dc.date.available2021-03-05T18:26:17Z
dc.date.issued2001
dc.identifier.citationBiswas N., Harris H., Wang X., Celebi G., Temkin H., Gangopadhyay S., "Electrical properties of fluorinated amorphous carbon films", JOURNAL OF APPLIED PHYSICS, cilt.89, ss.4417-4421, 2001
dc.identifier.issn0021-8979
dc.identifier.otherav_ca561cb3-1cfa-4019-83a1-23d1298da1c9
dc.identifier.othervv_1032021
dc.identifier.urihttp://hdl.handle.net/20.500.12627/134034
dc.identifier.urihttps://doi.org/10.1063/1.1353804
dc.description.abstractWe have studied the capacitance–voltage (C–V), conductance–voltage (G–V), and current–voltage characteristics of fluorinated amorphous carbon (a-C:Fx) films using metal/a-C:Fx/Si and metal/a-C:Fx/metal structures, respectively. Samples annealed in a vacuum were also studied. The C–V curves of the as-deposited sample are stretched about the voltage axis. Interface state density of 4.1×1011?cm-2?eV-1 at the midgap was calculated. Annealing the sample deposited on Si in a vacuum caused more frequency dispersion in the C–V and G–V curves, probably due to the diffusion of carbon into silicon. The bulk density of states for samples deposited on metal, measured by space-charge-limited current technique, decreased from 4×1018?eV-1?cm-3 for the as-deposited sample, to 7×1017?eV-1?cm-3 for the annealed sample.
dc.language.isoeng
dc.subjectTemel Bilimler (SCI)
dc.subjectFİZİK, UYGULAMALI
dc.subjectFizik
dc.subjectTemel Bilimler
dc.titleElectrical properties of fluorinated amorphous carbon films
dc.typeMakale
dc.relation.journalJOURNAL OF APPLIED PHYSICS
dc.contributor.department, ,
dc.identifier.volume89
dc.identifier.issue8
dc.identifier.startpage4417
dc.identifier.endpage4421
dc.contributor.firstauthorID444167


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