Mott p-n junctions in layered materials

被引:17
|
作者
Charlebois, M. [1 ,2 ]
Hassan, S. R. [3 ]
Karan, R. [3 ]
Senechal, D. [1 ,2 ]
Tremblay, A. -M. S. [1 ,2 ,4 ]
机构
[1] Univ Sherbrooke, Dept Phys, Sherbrooke, PQ J1K 2R1, Canada
[2] Univ Sherbrooke, RQMP, Sherbrooke, PQ J1K 2R1, Canada
[3] Inst Math Sci, Madras 600113, Tamil Nadu, India
[4] Canadian Inst Adv Res, Toronto, ON, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
HIGH-TEMPERATURE SUPERCONDUCTIVITY; INTERFACE; INSULATOR; TRANSITION; SURFACE;
D O I
10.1103/PhysRevB.87.035137
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The p-n junction has provided the basis for the semiconductor-device industry. Investigations of p-n junctions based on Mott insulators is still in its infancy. Layered Mott insulators, such as cuprates or other transition metal oxides, present a special challenge since strong in-plane correlations are important. Here we model the planes carefully using plaquette cellular dynamical mean field theory with an exact diagonalization solver. The energy associated with interplane hopping is neglected compared with the long-range Coulomb interaction that we treat in the Hartree-Fock approximation. Within this new approach, dynamical layer theory, the charge redistribution is obtained at the final step from minimization of a function of the layer fillings. A simple analytical description of the solution, in the spirit of the Thomas-Fermi theory, reproduces quite accurately the numerical results. Various interesting charge reconstructions can be obtained by varying the Fermi energy differences between both sides of the junction. One can even obtain quasi-two-dimensional charge carriers at the interface, in the middle of a Mott insulating layer. The density of states as a function of position does not follow the simple band bending picture of semiconductors. DOI: 10.1103/PhysRevB.87.035137
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页数:7
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