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纤锌矿GaN/ZnO量子阱中的界面声子 被引量:1

Interface-Optical-Phonon Modes in Wurtzite GaN/ZnO Quantum Wells
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摘要 根据介电连续模型和单轴晶体模型,运用传递矩阵的方法研究了纤锌矿量子阱中的界面声子,并且计算和讨论了纤锌矿GaN/ZnO单量子阱和耦合量子阱中的界面声子的色散关系。计算结果表明纤锌矿晶体的各向异性对界面声子模有大的影响:界面声子模出现在两个能量区域中,分别是:[ω⊥,TZnO,ωz,TGaN]和[ω⊥,LZnO,ωz,LGaN];界面声子随波数q⊥的减小色散越发明显、随波数q⊥增大分别趋近于54.32meV和86.56meV两个定值;当波数q⊥值非常小时,出现界面声子的色散消失现象,消失部分将穿越界面声子的能量区域转化为准受限声子或半空间声子。 Based on the dielectric continuum model and Loudon's uniaxial crystal model, the interface-optical-phonon (IOP) modes in wurtzite multilayer heterostructures were investigated by using the transfer matrix method. The dispersions of the IOP in wurtzite GaN/ZnO symmetric single quantum well and coupled quantum wells were calculated and discussed. The results indicated that the anisotropic effects of wurtzite crystal have a large influence on the behaviors of IOP modes. It was found that the IOP modes exist in frequency ranges [ω⊥.TZnO,ωz,TGaN] and [ω⊥.LZnO,ωz,LGaN].The IOP modes with small wave number q ⊥ have strong dispersions, and that with large wave number q⊥ converge to the two definite limiting values 54.32 meV and 86.56 meV, respectively. For very small value of q⊥, appearance of disappearing dispersion of the IOP mode, the IOP mode transforms to the quasiconfined mode or the halfspace mode after going beyond the IOP frequency ranges.
出处 《液晶与显示》 CAS CSCD 北大核心 2008年第2期132-136,共5页 Chinese Journal of Liquid Crystals and Displays
基金 国家自然科学基金(No.10674042) 河南省自然科学基金(No.0611053800)
关键词 界面声子 色散关系 量子阱 interface-optical-phonon dispersion relation quantum well
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  • 1Hong S, Hanada T, Makino H, et al. Band alignment at a ZnO/GaN (0001) heterointerface[J].Appl. Phys. Lett., 2001, 78(21) :3349-3351.
  • 2Yarelha D A, Vicet Am Perona A, et al. High efficiency GalnSbAs/GaSb type-Ⅱ quantum well continuous wave lasers [J].Semicond. Sci. Technol. , 2000, 15(4):390-394.
  • 3Knobel R, Smorchkova I P, Samarth N. Fabrication and characterization of a two dimensional electron gas in modulation doped ZnTe/Cd1-xMnxSe quantum wells [J]. J. Vac. Sci. Technol. B, 1999, 17(3):1147 -1150.
  • 4Hu J, Xu X G, Stotz J A H, et al. Type Ⅱ photoluminescence and conduction band offsets of GaAsSb/InGaAs and GaAsSb/InP heterostructures grown by metalorganic vapor phase epitaxy [J]. Appl. Phys. Lett. , 1998, 73(19): 2799-2801.
  • 5Loudon R. The roman effect in crystals [J]. Adv. Phys. , 1964, 13(7):429- 434.
  • 6Fuchs R, Kliewer K L. Optical Modes of Vibration in an Ionic Crystal Slab [J]. Phys. Rev., 1965,140(6A): A2076-A2088.
  • 7Gleize J, Renucci M A, Frandon J, et al. Anisotropy effects on polar optical phonons in wurtzite GaN/AIN superlattices [J]. Phys. Rev. B, 1999, 60(23):15985-15992.
  • 8Komirenko S M, Kim K W, Stroscio M A, et al. Dispersion of polar optical phonons in wurtzite quantum wells [J]. Phys. Rev. B, 1999, 59(7):5013(1-3).
  • 9Shi J J. Interface optical-phonon modes and electron-interface-phonon interaction in wurtzite GaN/AIN quantum wells [J]. Phys. Rev. B, 2003, 68(16):165335(1-7).
  • 10Shi J J, Chu X L, Goldys E M. Propagating optical-phonon modes and their electron-phonon interactions in wurtzite GaN/AlxGa1-xN quantum wells [J].Phys. Rev. B, 2004, 70(11):115318(1-8).

二级参考文献32

  • 1康凌,刘宝林,蔡加法,潘群峰.掺硅InGaN和掺硅GaN的光学性质的研究[J].液晶与显示,2004,19(4):266-269. 被引量:5
  • 2危书义,黄文登.GaN/AlN量子阱中的准受限声子[J].液晶与显示,2005,20(4):309-313. 被引量:6
  • 3危书义,赵旭,吴花蕊,夏从新.内建电场对GaN/AlGaN单量子点发光性质的影响[J].液晶与显示,2006,21(2):139-144. 被引量:6
  • 4Nakamura S, Chichibu S F. Introduction to Nitride Semiconductor Blue Laser and Light Emitting Diodes[M]. London: Taylor & Francis, 2000.2-12 .
  • 5Kittel C. Introduction to Solid State Physics[M]. New York:John Wiley & Sons, 1996.2-16.
  • 6Lee B C, Kim K W, Strroscio M A ,et al. Optical-phonon confinement and scattering in wurtzite heterostructures[J]. Phys. Rev. B, 1998, 58(8):4860(1-2).
  • 7Komirenko S M, Kim K W, Stroscio M A ,et al. Dispersion of polar optical phonons in wurtzite quantum wells[J].Phys. Rev. B, 1999, 59(7):5013(1-3).
  • 8Wendler L. Electron-phonon interaction in dielectric bilayer systems[J]. Phys.Status Solidi B, 1985, 129(2):513-520.
  • 9Baroni S, Giannozzi P, Molinari E. Phonon spectra of ultrathin GaAs/AlAs superlattices:An ab initio calculation[J]. Phys. Rev. B, 1990, 41(6):3870(2-6).
  • 10Loudan R. The Raman effect in crystals[J]. Adv. Phy., 1964.13(7):429-434.

共引文献9

同被引文献14

  • 1王志军,李守春,吕有明,唐胜,王丽红,田云霞,刘嘉宜,王连元.变分方法研究ZnO量子点中激子的基态特性[J].发光学报,2006,27(2):225-228. 被引量:2
  • 2危书义,杨艳岭,夏从新,吴花蕊,赵旭.耦合GaN/Al_xGa_(1-x)N量子点的非线性光学性质[J].液晶与显示,2007,22(3):240-244. 被引量:5
  • 3Debasis Bera, Lei Qian, Subir Sabui, et al. Photoluminescence of ZnO quantum dots produced by a sol-gel process [J]. Optical Materials, 2008, 30(8) :1233 1239.
  • 4Sun L L, Cheng W J. Lin F T, et al. Changes of structure and optical energy gap induced by oxygen pressure during the deposition of ZnO films [J]. Phys. B, 2006, 381(16) : 109-112.
  • 5Xia C X, Shi J J, Wei S Y. Exciton states in wurtzite InGaN coupled quantum dot [J]. China Phys. Lett. , 2004, 21 (8) : 1620-1623.
  • 6Kayanuma Y. Wannier excitons in low-dimension microstructures: Shape dependence of the quantum size effect [J]. Phys. Rev. B, 1991, 44 (23):13085-13088.
  • 7Vurgaftman I, Meyer J R. Band parameters for Ⅲ-Ⅴ compound semiconductors and theiralloys [J]. J. Appl. Phys. , 2001, 89(11):5815-5875.
  • 8Zhang B P, Kang J Y, Yu J Z, etal. Growth and optical properties of ZnO films and quantum wells [J]. Chin. J. Semiconductors, 2006, 27(4):613-622.
  • 9Seoung-Hwan Park,Doyeol Ahn. Crystal orientation effects on electronic and optical properties of wurtzite ZnO/ MgZnO quantum well lasers [J]. Optical and Quantum Electronics, 2006, 38(12):935-952.
  • 10Wei S Y, Wei L L, Xia C X. Exciton states and interband optical transitions in ZnO/MgZnO quantum dots [J]. J. Lumin., 2008,128:1285-1290.

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