Stability of graphene band structures against an external periodic perturbation: Na on graphene

被引:24
作者
Hwang, C. G. [1 ,4 ]
Shin, S. Y. [1 ]
Choi, Seon-Myeong [1 ]
Kim, N. D. [1 ,5 ]
Uhm, S. H. [1 ]
Kim, H. S. [1 ]
Hwang, C. C. [2 ]
Noh, D. Y. [3 ]
Jhi, Seung-Hoon [1 ]
Chung, J. W. [1 ]
机构
[1] Pohang Univ Sci & Technol, Dept Phys, Pohang 790784, South Korea
[2] Pohang Accelerator Lab, Beamline Res Div, Pohang 790784, South Korea
[3] Gwangju Inst Sci & Technol, Dept Mat Sci & Engn, Kwangju 500712, South Korea
[4] Univ Calif Berkeley, Lawrence Berkeley Lab, Div Mat Sci, Berkeley, CA 94720 USA
[5] Columbia Univ, Dept Phys, New York, NY 10027 USA
关键词
adsorption; band structure; buffer layers; charge exchange; crystallisation; diffusion; Fermi level; graphene; hopping conduction; photoelectron spectra; silicon compounds; sodium; MASSLESS DIRAC FERMIONS; CARBON NANOTUBES; BACK SCATTERING; BERRYS PHASE; TRANSITION; GRAPHITE; DYNAMICS; ABSENCE;
D O I
10.1103/PhysRevB.79.115439
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The electronic structure of Na-adsorbed graphenes formed on the 6H-SiC(0001) substrate was studied using angle-resolved photoemission spectroscopy with synchrotron photons and ab initio pseudopotential calculations. It was found that the band of the graphenes sensitively changes upon Na adsorption especially at low temperature. With increasing Na dose, the pi band appears to be quickly diffused into the background at 85 K whereas it becomes significantly enhanced with its spectral intensity at room temperature (RT). A new parabolic band centered at k similar to 1.15 A(-1) also forms near Fermi energy with Na at 85 K while no such band was observed at RT. Such changes in the band structure are found to be reversible with temperature. The changes in the pi band of graphene are mainly driven by the Na-induced potential especially at low temperature where the potential becomes periodic due to the crystallized Na overlayer. The new parabolic band turns out to be the pi band of the underlying buffer layer partially filled by the charge transfer from Na adatoms. The increase in the hopping rate of Na adatoms at RT by 5 orders of magnitude prevents such a charge transfer, explaining the absence of the new band at RT.
引用
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页数:5
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