Skip to main page content
U.S. flag

An official website of the United States government

Dot gov

The .gov means it’s official.
Federal government websites often end in .gov or .mil. Before sharing sensitive information, make sure you’re on a federal government site.

Https

The site is secure.
The https:// ensures that you are connecting to the official website and that any information you provide is encrypted and transmitted securely.

Access keys NCBI Homepage MyNCBI Homepage Main Content Main Navigation
. 2022 Jan 11;15(2):526.
doi: 10.3390/ma15020526.

Impurity-Induced Magnetization of Graphene

Affiliations

Impurity-Induced Magnetization of Graphene

Michał Inglot et al. Materials (Basel). .

Abstract

We present a model of impurity-induced magnetization of graphene assuming that the main source of graphene magnetization is related to impurity states with a localized spin. The analysis of solutions of the Schrödinger equation for electrons near the Dirac point has been performed using the model of massless fermions. For a single impurity, the solution of Schrödinger's equation is a linear combination of Bessel functions. We found resonance energy levels of the non-magnetic impurity. The magnetic moment of impurity with a localized spin was accounted for the calculation of graphene magnetization using the Green's function formalism. The spatial distribution of induced magnetization for a single impurity is obtained. The energy of resonance states was also calculated as a function of interaction. This energy is depending on the impurity potential and the coupling constant of interaction.

Keywords: graphene; impurity; localized states; magnetism; resonant states; spintronics.

PubMed Disclaimer

Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
(a) First Brillouin zone in graphene with marked points, (b) Γ—center of the zone, M—center of the edge, K and K are the nonequivalent Dirac points.
Figure 2
Figure 2
Single-node doping in graphene, (a) a new atom instead of a carbon atom, (b) a gap in the graphene lattice.
Figure 3
Figure 3
Dependence of resonant energy levels ε of a state localized on a non-magnetic impurity with the potential V0 Equation (16), where εc=2/(mea02), Vc=εca02, me is the mass of electron, and a0 is the distance between carbon atoms. Localized states without magnetic correlations.
Figure 4
Figure 4
Induced local magnetization Mz(ϱ) as a function of the distance from the impurity center ϱ.
Figure 5
Figure 5
Interaction energy Eint as the function of impurity potential V0. ×—the results obtained for the interaction energy in the first iteration step (see the blue dashed line (Figure 6)). Solutions marked with a circles correspond to Eint in the last iteration step of the self-reconciliation procedure. Colors denote different values of the constant gc.
Figure 6
Figure 6
Resonant energy levels ε with consideration of magnetic interaction Eint as a function of renormalized impurity potential V0 for different values of coupling constant gc.

References

    1. Li Y., He J., Kong X., Kou S.-P. Vacancy-induced intrinsic magnetic impurity with quasilocalized spin moment in graphene. Phys. Rev. B. 2014;90:201406. doi: 10.1103/PhysRevB.90.201406. - DOI
    1. Zhong M., Li S., Duan H.-J., Hu L.-B., Yang M., Wang R.-Q. Effect of impurity resonant states on optical and thermoelectric properties on the surface of a topological insulator. Sci. Rep. 2017;7:3971. doi: 10.1038/s41598-017-04360-x. - DOI - PMC - PubMed
    1. Inglot M., Dugaev V.K. Impurity states in graphene with intrinsic spin–orbit interaction. J. Appl. Phys. 2011;109:123709. doi: 10.1063/1.3598130. - DOI
    1. Skrypnyk Y.V., Loktev V.M. Impurity effects in a two-dimensional system with the dirac spectrum. Phys. Rev. B. 2006;73:241402. doi: 10.1103/PhysRevB.73.241402. - DOI
    1. Noori K., Quek S.Y., Rodin A. Hydrogen adatoms on graphene: The role of hybridization and lattice distortion. Phys. Rev. B. 2020;102:19541. doi: 10.1103/PhysRevB.102.195416. - DOI

LinkOut - more resources