2011
DOI: 10.1103/physrevb.83.201401
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Transport anomaly at the ordering transition for adatoms on graphene

Abstract: We analyze a manifestation of the partial ordering transition of adatoms on graphene in resistivity measurements. We find that Kekule mosaic ordering of adatoms increases sheet resistance of graphene, due to a gap opening in its spectrum, and that critical fluctuations of the order parameter lead to a non-monotonic temperature dependence of resistivity, with a cusp-like minimum at T=T_c.Comment: 4 pages, 1 figur

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Cited by 15 publications
(23 citation statements)
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References 18 publications
(30 reference statements)
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“…At the scale of an entire graphene device, however, the observation of significant macroscopic transverse charge currents due to scattering with a large ensemble of top-position adatoms appears more challenging than the observation of a large SHE due to hollow-position adatoms because of the necessity of having an imbalance between the A and B sublattices. Nevertheless, it should be noted that sublattice ordering driven by Ruderman-Kittel-Kasuya-Yosida (RKKY) -type interactions below a critical temperature was predicted by several authors [48][49][50][51], so that the above-discussed CHE may in principle be observed in an experiment.…”
Section: Scattering With Top-position Adatomsmentioning
confidence: 99%
“…At the scale of an entire graphene device, however, the observation of significant macroscopic transverse charge currents due to scattering with a large ensemble of top-position adatoms appears more challenging than the observation of a large SHE due to hollow-position adatoms because of the necessity of having an imbalance between the A and B sublattices. Nevertheless, it should be noted that sublattice ordering driven by Ruderman-Kittel-Kasuya-Yosida (RKKY) -type interactions below a critical temperature was predicted by several authors [48][49][50][51], so that the above-discussed CHE may in principle be observed in an experiment.…”
Section: Scattering With Top-position Adatomsmentioning
confidence: 99%
“…(11) into Eq. (10) gives (13) Therefore, the binding energy change has the form (14) The initial parameters of the problem for single layer graphene are given in Table 1. The values of for a single layer graphene are given in Fig.…”
Section: Energy Of Substitution Of Atoms 877mentioning
confidence: 99%
“…This can simply be achieved using adsorption or intercalation (see, for example, references to works in [9][10][11], published before 2011, and also recent works in this field [12][13][14][15]). In [16], a method of direct doping was proposed: formation of substitutional defects by replacing car bon atoms with Group III and V atoms.…”
Section: Introductionmentioning
confidence: 99%
“…There is much to be learned about this unusual electronic structure by considering the change in the LDOS and the FO in the excess charge density due to a well localized impurity. Results of these considerations have implications for the LDOS in disordered graphene [4,5], for the interaction between adatoms in graphene [6][7][8], or in case of magnetic adatoms [9] for the corresponding RKKY interaction [10,11]. Research on topological insulators also profit from the ideas developed for graphene due to similarities in their electronic structure [12].…”
Section: Basics Of Graphenementioning
confidence: 95%
“…Using (7) in (6) we obtain ρ(ε, r) = πuρ 2 0 (ε)Img 2 (kr) (8) for the change in the LDOS. Moreover, from (3) and (8) the change in the electron density (FO) at zero temperature is evaluated for large distances (k F r 1) from the impurity as…”
Section: Free Electronsmentioning
confidence: 98%