2012
DOI: 10.1109/tns.2012.2221479
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Total Ionizing Dose Induced Charge Carrier Scattering in Graphene Devices

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Cited by 36 publications
(31 citation statements)
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“…For large values of effective vertical field (E eff ) the extractions merge at the pre-irradiation curve as mechanisms other than charged impurity scattering become dominant for large carrier densities ( ). Similar results were observed recently for Cu-CVD back-gated GFETs irradiated with Co-60 gamma rays [24]. Additionally, an increase in μ eff is observed for E eff < 1 MV/cm that is consistent with the observations made in [19] and attributed to scatterer transparency that occurs as carrier wavelengths becomes larger than scatterer spacing.…”
Section: Discussionsupporting
confidence: 91%
“…For large values of effective vertical field (E eff ) the extractions merge at the pre-irradiation curve as mechanisms other than charged impurity scattering become dominant for large carrier densities ( ). Similar results were observed recently for Cu-CVD back-gated GFETs irradiated with Co-60 gamma rays [24]. Additionally, an increase in μ eff is observed for E eff < 1 MV/cm that is consistent with the observations made in [19] and attributed to scatterer transparency that occurs as carrier wavelengths becomes larger than scatterer spacing.…”
Section: Discussionsupporting
confidence: 91%
“…Similar turn-around behavior was found in all four devices under test. These results contrast significantly with the responses of exposed graphene structures in contact with SiO or high-K insulators, where larger shifts and no turnaround effects are typically observed with 10-keV x-ray irradiation [17]- [19]. Fig.…”
Section: Methodsmentioning
confidence: 57%
“…The Dirac point of the device shifts slightly negatively at low radiation doses (evidence of hole trapping), and then shifts positively (evidence of negatively charged interface defects) for higher dose exposures to 1 Mrad(SiO ). The changes in Dirac point and decreases in mobility are relatively small in these devices, compared with devices having graphene layers in contact with SiO or high-K dielectric materials [17]- [19]. The potential nature of the charge trapping in the boron nitride is discussed, and a potential, additional role for interface defects is investigated via first principles calculations.…”
Section: Introductionmentioning
confidence: 97%
“…On the contrary, when irradiated in vacuum, ambipolar graphene devices on 100-nm SiO 2 exhibited negative V th [76]. These devices, however, also included a trimethylsiloxy (TMS) monolayer between graphene and SiO 2 in order to stabilize the polarity of the electric field at the TMS/graphene interface and subsequently reduce gate hysteresis.…”
Section: Thin Film 2-d Material and Nanotube Transistorsmentioning
confidence: 99%