摘要We theoretically investigate the electronic properties of p-type δ-doped GaAs inserted into a quantum well under the electric field, at T=0K. We will investigate the influence of the electric field on the δ-doping concentration for a uniform distribution. The depth of confining potential, the density profile, the Fermi level, the subband energies and the subband populations calculate by solving the Schrodinger and Poisson equations self consistently. It is found that the changes of the electronic properties are quite sensitive to the applied electric field and the doping concentration. As different from single n-type δ-doped structure, we see a replace between the ground light-hole (lh1) subband and the first excited heavy-hole (hh2) subband whenever the external electric field reaches a critical value. We find the abrupt changing of the subband energies and the subband populations whenever the applied electric field reaches a certain value. Also, it is found that the heavy-hole subbands contain many more energy states than the light-hole ones, the population of the heavy-hole levels represent approximately 91% of all the carriers.
Abstract:We theoretically investigate the electronic properties of p-type δ-doped GaAs inserted into a quantum well under the electric field, at T=0K. We will investigate the influence of the electric field on the δ-doping concentration for a uniform distribution. The depth of confining potential, the density profile, the Fermi level, the subband energies and the subband populations calculate by solving the Schrodinger and Poisson equations self consistently. It is found that the changes of the electronic properties are quite sensitive to the applied electric field and the doping concentration. As different from single n-type δ-doped structure, we see a replace between the ground light-hole (lh1) subband and the first excited heavy-hole (hh2) subband whenever the external electric field reaches a critical value. We find the abrupt changing of the subband energies and the subband populations whenever the applied electric field reaches a certain value. Also, it is found that the heavy-hole subbands contain many more energy states than the light-hole ones, the population of the heavy-hole levels represent approximately 91% of all the carriers.
[1] Schubert E F 1990 J. Vac. Sci. Technol. A 82980 [2] Ploog K, Hauser M and Fischer A 1998 Appl. Phys. A 45 233 [3] Ioriatti L 1990 Phys. Rev. B 41 8340 [4] Ke M L et al 1992 Phys. Rev. B 45 14114 [5] Dominguez-Adame F, Mendez B and Macina F 1994 Semicond. Sci. Technol. 9 263 [6] Nakazato K, Blaikie R J and Ahmed H 1994 J. Appl.Phys. 75 5123 [7] Osvald J 2004 Physica E 23 147 Osvald J 2004 J. Phys. D 37 2655 [8] Chico L, Garcia-Moliner F and Velasco V R 1993 Phys.Rev. B 48 11 427 [9] Ozturk E and Sokmen I 2003 J. Phys. D: Appl. Phys. 36 2457 Ozturk E and Sokmen 2003 Solid State Commun. 126 605 Ozturk E, Ergun Y, Sari H and Sokmen I 2001 Appl.Phys. A 73 749 Ozturk E, Sari H, Ergun Y and Sokmen I 2005 Appl.Phys. A 80 167 [10] Zrenner A, Koch F, Williams R L, Stradling R A, Ploog Kand Weinmann G 1988 Semicond. Sci. Technol. 3 1203 [11] Schubert E F, Chiu T H, Cunningham J E, Telland B andStark J B 1988 J. Electron. Mater. 17 527 [12] Schubert E F, Fischer A and Ploog K 1986 IEEE Trans.Electron Devices 33 625 [13] Shibli S M, Scolfaro L M, Leite J R, Mendon\c{ca C A C,Plentz F and Meneses A 1992 Appl. Phys. Lett. 60 2895 [14] Ozturk E, Ergun Y, Sari H and Sokmen 2000 Superlattices and Microstructure 28 35 Ozturk E, Ergun Y, Sari H and Sokmen 2002 J. Appl.Phys. 91 2118 [15] Gaggero-Sager L M and Mora-Ramos M E 2000 Solid-State Electron. 44 175 [16] Gaggero-Sager L M 2002 Phys. Status Solidi 231 243 [17] Rosa A L et al 1998 Microelectronic Engineering 43-44 489 [18] Henning J C and Ansems J P 1987 Semicond. Sci.Technol. 2 1 [19] Kortus J and Monecke J 1994 Phys. Rev. B 4917216 [20] Ben Jazia A, Mejri H, Maaref H and Souissi K 1997 Semicond. Sci. Tech. 12 1388 [21] Cuesta J A, Sanchez A and Domingez-Adame F 1995 Semicond. Sci. Tech. 10 1303 [22] Domingez-Adame F, Mendez B and Macia F 1994 Semicond. Sci. Tech. 9 263 Domingez-Adame F and Mendez B 1994 Phys. Rev. B 49 11471 [23] Mezrin O A et al 1992 Semicond. Sci. Tech. 7664 [24] Ozturk E et al 2001 Semicond. Sci. Technol. 16 421 [25] Gaggero-Sager L M and Perez-Alvarez R 1996 J. Appl.Phys. 79 3351