Weak localization in bilayer graphene with Li-intercalation/desorption

被引:5
|
作者
Endo, Y. [1 ]
Ichinokura, S. [1 ]
Akiyama, R. [1 ]
Takayama, A. [1 ]
Sugawara, K. [2 ,3 ]
Nomura, K. [3 ,4 ]
Takahashi, T. [2 ,3 ,5 ]
Hasegawa, S. [1 ]
机构
[1] Univ Tokyo, Dept Phys, Tokyo 1130033, Japan
[2] Tohoku Univ, WPI Res Ctr, Adv Inst Mat Res, Sendai, Miyagi 9808577, Japan
[3] Tohoku Univ, Ctr Spintron Res Network, Sendai, Miyagi 9808577, Japan
[4] Tohoku Univ, Inst Mat Res, Sendai, Miyagi 9808577, Japan
[5] Tohoku Univ, Dept Phys, Sendai, Miyagi 9808578, Japan
关键词
graphene; weak localization; quantum coherent transport; intercalation; atomic layer; Berry phase; stacking structure; 2; DIMENSIONS; FIELD; MAGNETORESISTANCE; TEMPERATURE; DIFFUSION; MONOLAYER; SYSTEMS;
D O I
10.1088/1361-648X/aaccc4
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
We performed in-situ electrical transport measurements for bilayer graphene grown on SiC(0 0 0 1) substrate, Li-intercalated bilayer graphene, and after that desorbing Li atoms by heating. Bilayer graphene after desorbing intercalated Li atoms showed a higher resistivity and different behavior in magnetoconductance compared to pristine bilayer graphene. We observed the weak localization of carriers at low temperatures in all the three samples and analyzed the experimental results with the extended Hikami-Larkin-Nagaoka equation to investigate the transport properties. The result shows that the magnetoconductance of pristine bilayer graphene is described by the AB stacking structure model and the phase breaking scattering is dominated by the electron-electron scattering. The intra-valley scattering occurs most frequently probably due to dopants in SiC substrate. However, in Li-desorbed graphene, the magnetoconductance can be described by neither AB nor AA-stacking model, suggesting the coexistence of domains with several different stacking structures.
引用
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页数:7
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