A noncommutative space approach to confined Dirac fermions in graphene

被引:21
|
作者
Dayi, Oemer F. [1 ,3 ]
Jellal, Ahmed [2 ,4 ]
机构
[1] Istanbul Tech Univ, Fac Sci & Letters, Dept Phys, TR-34469 Istanbul, Turkey
[2] King Faisal Univ, Coll Sci, Dept Phys, Alahsa 31982, Saudi Arabia
[3] Feza Gursey Inst, TR-34349 Istanbul, Turkey
[4] Chouaib Doukkali Univ, Fac Sci, Theoret Phys Grp, El Jadida 24000, Morocco
关键词
D O I
10.1063/1.3442719
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A generalized algebra of noncommutative coordinates and momenta embracing non-Abelian gauge fields is proposed. Through a two-dimensional realization of this algebra for a gauge field including electromagnetic vector potential and two spin-orbit-like coupling terms, a Dirac-like Hamiltonian in noncommutative coordinates is introduced. We established the corresponding energy spectrum and from that we derived the relation between the energy level quantum number and the magnetic field at the maxima of Shubnikov-de Haas oscillations. By tuning the noncommutativity parameter theta in terms of the values of magnetic field at the maxima of Shubnikov de Haas oscillations, we accomplished the experimentally observed Landau plot of the peaks for graphene. Accepting that the experimentally observed behavior is due to the confinement of carriers, we conclude that our method of introducing noncommutative coordinates provides another formulation of the confined massless Dirac fermions in graphene. (C) 2010 American Institute of Physics. [doi:10.1063/1.3442719]
引用
收藏
页数:12
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