Resonant and Non-Resonant Impurity States Related to GaAs/AlGaAs Quantum Well Sub-Bands

被引:0
|
作者
Akimov, Volodymyr [1 ,2 ]
Tulupenko, Viktor [2 ,3 ]
Demediuk, Roman [4 ]
Tiutiunnyk, Anton [5 ]
Duque, Carlos A. [2 ]
Morales, Alvaro L. [2 ]
Laroze, David [6 ]
Mora-Ramos, Miguel Eduardo [7 ]
机构
[1] Univ Medellin, Fac Ciencias Bas, Medellin 050026, Colombia
[2] Univ Antioquia UdeA, Fac Ciencias Exactas & Nat, Grp Mat Condensada UdeA, Inst Fis, Medellin 050010, Colombia
[3] Donbas State Engn Acad, Phys Dept, UA-84313 Kramatorsk, Ukraine
[4] Donbas State Pedag Univ, Phys Dept, UA-84100 Sloviansk, Ukraine
[5] Univ Tarapaca, Dept Fis, FACI, Casilla 7D, Arica 1000000, Chile
[6] Univ Tarapaca, Inst Alta Invest, Casilla 7D, Arica 1000000, Chile
[7] Univ Autonoma Estado Morelos, Ctr Invest Ciencias IICBA, Cuernavaca 62209, Mexico
关键词
semiconductor heterostructures; hydrogenic impurity states; expansion method; FANO RESONANCES; ENERGY-LEVELS; INVERSION; NANOWIRES; DONORS;
D O I
10.3390/ma18010017
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The energy positions and wave function shapes of the ground and excited states of impurities, including resonance states, are studied using the expansion of the impurity wave function in basis functions. The structures under study are rectangular GaAs/AlGaAs quantum wells with four different widths. In all cases, the impurity binding energy (relative to the corresponding sub-band) has a maximum at or near the center of the quantum well, decreases as the heterointerface is approached, and apparently has a limit of 0 if the impurity moves deeper into the barrier. If the impurity moves away from the center of the quantum well, then the "center of mass" of the electron charge of non-resonant impurity states follows the impurity atom, and the "center of mass" of the electron charge of the resonant impurity states moves away from it. The effect is more pronounced for the ground and first resonance states for wider quantum wells, and the shifts reach a maximum when the impurity atom is positioned near the midpoint of the path between the quantum well center and the heterointerface.
引用
收藏
页数:17
相关论文
共 50 条
  • [1] Density of impurity states in coaxial GaAs/AlGaAs quantum well wires under non-resonant intense laser fields
    Radu, A.
    ADVANCED TOPICS IN OPTOELECTRONICS, MICROELECTRONICS, AND NANOTECHNOLOGIES V, 2010, 7821
  • [2] RESONANT AND NON-RESONANT TUNNELING IN GAAS/ALAS MULTI QUANTUM WELL STRUCTURES
    SCHNEIDER, H
    VONKLITZING, K
    PLOOG, K
    SUPERLATTICES AND MICROSTRUCTURES, 1989, 5 (03) : 383 - 396
  • [4] Resonant impurity and exciton states in a narrow quantum well
    Monozon, BS
    Schmelcher, R
    PHYSICAL REVIEW B, 2005, 71 (08)
  • [5] RESONANT IMPURITY STATES IN QUANTUM-WELL STRUCTURES
    PRIESTER, C
    ALLAN, G
    LANNOO, M
    PHYSICAL REVIEW B, 1984, 29 (06): : 3408 - 3411
  • [7] Quantum well sub-bands probed by photo-excited, capacitance-sensitive resonant tunneling spectrum
    LiGuo Wang
    HouZhi Zheng
    KangKang Meng
    JianHua Zhao
    Science China Physics, Mechanics and Astronomy, 2012, 55 : 1362 - 1365
  • [8] Quantum well sub-bands probed by photo-excited, capacitance-sensitive resonant tunneling spectrum
    Wang LiGuo
    Zheng HouZhi
    Meng KangKang
    Zhao JianHua
    SCIENCE CHINA-PHYSICS MECHANICS & ASTRONOMY, 2012, 55 (08) : 1362 - 1365
  • [9] Resonant magnetopolaron effects in GaAs/AlGaAs multiple quantum well structures
    Wang, YJ
    Nickel, HA
    McCombe, BD
    Peeters, FM
    Shi, JM
    Hai, GQ
    Wu, XG
    Eustis, TJ
    Schaff, W
    PHYSICA E, 1998, 2 (1-4): : 161 - 165
  • [10] Resonant tunneling in GaAs/AlGaAs quantum well system for solar photovoltaics
    Klemmer, P. S.
    Mityagin, Yu A.
    Telenkov, M. P.
    Nagaraja, K. K.
    Elantsev, D. A.
    Amiri, Sh
    SUPERLATTICES AND MICROSTRUCTURES, 2020, 140