2009
DOI: 10.1103/physrevb.80.075406
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Electronic doping and scattering by transition metals on graphene

Abstract: We investigate the effects of transition metals ͑TM͒ on the electronic doping and scattering in graphene using molecular-beam epitaxy combined with in situ transport measurements. The room-temperature deposition of TM onto graphene produces clusters that dope n type for all TM investigated ͑Ti, Fe, and Pt͒. We also find that the scattering by TM clusters exhibits different behavior compared to 1 / r Coulomb scattering. At high coverage, Pt films are able to produce doping that is either n type or weakly p type… Show more

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Cited by 257 publications
(241 citation statements)
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“…This nearly 3.3 times reduction in contact resistance may possibly be attributed to the gate-induced electron injection from graphene layer to MoS 2 . At the hetero-contact structure, the positive back-gate bias not only electro-statically dopes MoS 2 , but also could move the Fermi-level in Ti doped n-type graphene [18][19][20][21] further up beyond the Ti/MoS 2 pinning level, thus enhance the electron injection from metal into the conduction band of MoS 2 leading to a lower contact resistance. The key difference from previous devices is that the back-gate can modulate not only the Fermi-level of the channel but also the contact (graphene) as shown in the inset of Figure 3(b) [19].…”
Section: Resultsmentioning
confidence: 99%
“…This nearly 3.3 times reduction in contact resistance may possibly be attributed to the gate-induced electron injection from graphene layer to MoS 2 . At the hetero-contact structure, the positive back-gate bias not only electro-statically dopes MoS 2 , but also could move the Fermi-level in Ti doped n-type graphene [18][19][20][21] further up beyond the Ti/MoS 2 pinning level, thus enhance the electron injection from metal into the conduction band of MoS 2 leading to a lower contact resistance. The key difference from previous devices is that the back-gate can modulate not only the Fermi-level of the channel but also the contact (graphene) as shown in the inset of Figure 3(b) [19].…”
Section: Resultsmentioning
confidence: 99%
“…368,369 Finally, as the electron beams can now be focused onto the areas with diameters of less than 1 Å, displacement of individual carbon atoms 333 followed by "plugging" of the vacancies with noncarbon atoms may give rise to novel nanostructures with very interesting electronic and magnetic properties. 370 Indeed, recent simulations 371,372 indicate that bonding of transition metal atoms to defects in graphenic structures is strong, while metal adatoms on graphene surface are mobile at room and elevated temperature, so that it should be possible to produce such structures by depositing metal atoms on the irradiated surface of graphene or nanotubes and by raising then the temperature in such a way that the adatoms become mobile, and the defects will pin the adatoms.…”
Section: Engineering Carbon Nanostructures With a Focused Electron Beammentioning
confidence: 99%
“…Recently, graphene has gathered tremendous attention due to its unique electronic and mechanical properties for nanoscale electronics 5 . As a candidate material for spintronic devices, transition-metal-atom-decorated graphene (denoted as TM-graphene hereafter) has been studied extensively in theory 6-9 and experiment [10][11][12][13][14][15] , manifesting some remarkable electronic and magnetic behaviors. Thus, developing a novel method to tune the magnetism of TM-graphene system is quite urgent for future spintronics applications.…”
Section: Introductionmentioning
confidence: 99%