2021
DOI: 10.1016/j.carbon.2020.12.076
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Room-temperature negative magnetoresistance of helium-ion-irradiated defective graphene in the strong Anderson localization regime

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Cited by 7 publications
(6 citation statements)
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“…For example, Reza et al 89 found the negative MR effect with a value of −9.0% at a temperature of 5 K in carbon nanotube yarns under an external magnetic field of 5 T, which was related to the weak spin–orbit effect. Takuya et al 90 reported the room-temperature negative MR phenomenon in graphene. Recent research results denote that the semiconducting amorphous carbon could delineate a large MR effect coming from its variable band gaps and electrical properties.…”
Section: Electronic Applications Of Phthalonitrile Resinsmentioning
confidence: 99%
“…For example, Reza et al 89 found the negative MR effect with a value of −9.0% at a temperature of 5 K in carbon nanotube yarns under an external magnetic field of 5 T, which was related to the weak spin–orbit effect. Takuya et al 90 reported the room-temperature negative MR phenomenon in graphene. Recent research results denote that the semiconducting amorphous carbon could delineate a large MR effect coming from its variable band gaps and electrical properties.…”
Section: Electronic Applications Of Phthalonitrile Resinsmentioning
confidence: 99%
“…The carrier localization of helium-ion-irradiated graphene was systematically investigated by measuring the electrical resistance and its dependence on the carrier density, magnetic field, temperature and ion dose [41]. Monolayer graphene devices were fabricated using the conventional process, including the mechanical exfoliation method and electron beam lithography.…”
Section: Carrier Localization In Helium-ion-irradiated Graphenementioning
confidence: 99%
“…The VRH fitting analysis shows that the localization length decreases with an increased dose, as shown in figure 4(b). This modulation could be associated with an interval distance (d) between point defects.We derive d by considering the scattering probability of helium ions with carbon atoms in graphene [38,41].…”
Section: Carrier Localization In Helium-ion-irradiated Graphenementioning
confidence: 99%
“…In the weak B limit, as discussed in Ref. [15][16][17], Anderson localization effects due to impurity scatterings can play a role generally in graphene. Here geometric effects due to boundary scattering can be overlapped.…”
Section: 'Plain' Blg (Without Superlattice Structure/'satellites') 8)mentioning
confidence: 99%
“…An interplay of several characteristic times is crucial to fix the magnitude of such quantum interference effects. [15][16][17] For the strong B region, the magnetoresistance is non-monotonically changed with decreasing n (increasing the hole density) due to the overlap with the spectrum from the hole-side satellite, in contrast to that in the BLG device shown in Fig. 2(g).…”
Section: 'Plain' Blg (Without Superlattice Structure/'satellites') 8)mentioning
confidence: 99%