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46. The Nonlinear Acoustoelectric Effect in a Cylindrical Quantum<br />

Wire with a Infinite Potential<br />

Nguyen Van Nghia (1), Tran Thi Thu Huong (2), Nguyen<br />

Quang Bau (2)<br />

(1) Department of physics, Water Resources University, 175 Tay Son,<br />

Dong Da, Ha Noi<br />

(2) Department of physics, Hanoi National University, 334 Nguyen<br />

Trai, Thanh Xuan, Ha Noi<br />

The nonlinear acoustoelectric effect in a cylindrical quantum wire<br />

with a infinite potential is investigated by using Boltzmann kinetic<br />

equation for an acoustic wave whose wavelength λ = 2π/q is smaller<br />

than the mean free path l of the electrons and hypersound in the<br />

region ql >> 1, (where q is the acoustic wave number). The analytic<br />

expression for the acoustoelectric current I is calculated in the case:<br />

relaxation time of momentum is constant approximation and<br />

degenerates electrons gas. The nonlinear dependence of the<br />

expression for the acoustoelectric current I on the acoustic wave<br />

numbers q and on the intensity of constant electric field E are<br />

obtained. Numerical computations are performed for AlGaAs/GaAs<br />

cylindrical quantum wire with a infinite potential. The results are<br />

compared with the normal bulk semiconductors and the<br />

superlattices to show the values of the acoustoelectric current I in<br />

the cylindrical quantum wire are different than they are in the<br />

normal bulk semiconductors and the superlattices.<br />

Báo cáo Treo<br />

Hội nghị Vật lý lý thuyết toàn quốc lần thứ 35<br />

53<br />

47. The Dependence of the Parametric Transformation Coefficient of<br />

Confined Acoustic and Confined Optical Phonons in the Rectangular<br />

Quantum Wire<br />

Luong Van Tung (1), Ngo Thi Thanh Ha (2), Nguyen Thi<br />

Thanh Nhan (2), Le Thi Thu Phuong (2), Nguyen Quang<br />

Bau (2)<br />

(1) Department of Physics, Dong Thap University, 783-Pham Huu<br />

Lau, Dong Thap, Viet Nam (2) Hanoi University of Science, 334<br />

Nguyen Trai, Thanh Xuan, Ha Noi<br />

The parametric transformation of confined acoustic and confined<br />

optical phonons in a rectangular quantum wire is theoretically<br />

studied by using a set of quantum kinetic equations for phonons.<br />

The analytic expression of parametric transformation coefficient of<br />

confined acoustic and confined optical phonons in a rectangular<br />

quantum wire is obtained. The dependence of the parametric<br />

transformation coefficient on the temperature T is numerically<br />

evaluated, plotted and discussed for a specific quantum wire<br />

GaAs/GaAsAl. All the results are compared with those for the<br />

unconfined phonons to show the difference.<br />

54<br />

Báo cáo Treo<br />

48. Rate of Phonon Excitation and Conditions for Phonon<br />

Generation in Cylindrical Quantum Wires<br />

Tran Cong Phong (1,2), Le Thi Thu Phuong (1), Tran Dinh<br />

Hien (1)<br />

(1) Department of Physics, Hue University's College of Education, 32<br />

Le Loi, Hue, Vietnam;<br />

(2) National Education Union of Vietnam, 02 Trinh Hoai Duc, Dong<br />

Da, Ha noi, Vietnam<br />

Phonon generation via the Cerenkov effect in cylindrical quantum<br />

wires (CQW) is theoretically studied based on the quantum kinetic<br />

equation for phonon population operator. Both electrons and<br />

phonons are confined in the CQW. Analytical expressions for the<br />

rate of change of the phonon population and conditions for phonon<br />

generation are obtained. Numerical results for GaAs/AlAs<br />

cylindrical quantum wires show that the amplitude of the laser field<br />

Tp. Hồ Chí Minh, 02-06/8/2010<br />

must satisfy additional conditions that are different in comparison<br />

with those of the other works. The differences between the<br />

generation of acoustic phonon and longitudinal optical phonon are<br />

considered. Comparisons between two cases of confined phonons<br />

and bulk phonons are discussed.<br />

Báo cáo Treo<br />

49. Độ linh động và điện trở của khí điện tử trong giếng lượng tử<br />

SiGe/Si/SiGe ở nhiệt độ khác không<br />

Vo Van Tai and Nguyen Quoc Khanh<br />

Trường Đại học KHTN TP HCM, 227 Nguyễn Văn Cừ, Quận 5, TP<br />

Hồ Chí Minh<br />

Chúng tôi đã tính độ linh động và điện trở của khí điện tử giả hai<br />

chiều trong giếng lượng tử Si ở nhiệt độ khác không cho cả hai<br />

trường hợp có hoặc không có từ trường song song. Mật độ hạt, bề<br />

dày lớp và nhiệt độ được chọn sao cho tán xạ tạp chất và bề mặt<br />

nhám là các cơ chế chủ yếu. Các kết quả của chúng tôi có dáng điệu<br />

phù hợp với các kết quả thực nghiệm. Chúng tôi chỉ ra rằng đối với<br />

từ trường quanh giá trị bão hòa điện trở hầu như không phụ thuộc<br />

nhiệt độ.<br />

Báo cáo Treo<br />

50. Two <strong>Ban</strong>d Model for Diluted Magnetic Semiconductors: Study of<br />

the Ferromagnetic Transition Temperature<br />

Vu Kim Thai and Hoang Anh Tuan<br />

Institute of Physics, Vietnam Academy of Science and Technology, 10<br />

Dao Tan, Ba Dinh, Ha Noi<br />

The ferromagnetic transition temperature (Tc) of a two band model<br />

for diluted magnetic semiconductors (DMS) is calculated by using<br />

the coherent potential approximation (CPA). It is shown that Tc is<br />

strongly parameter dependent such as density of the carriers,<br />

magnetic coupling constants, and the hopping terms. The maximal<br />

Tc of the two band model is found when both impurity bands fully<br />

overlap and this value is approximately twice larger than the highest<br />

Tc obtained in the single band model.<br />

Báo cáo Treo<br />

51. Density Functional Based Tight Binding Study on Wurzite Coreshell<br />

Nanowires Heterostructures ZnO/ZnS.<br />

N.T. Thuong, N.V. Minh, N.N. Tuan, V.N. Tuoc<br />

Hanoi University of Technology, 1 Dai Co Viet, Hai Ba Trung, Ha<br />

Noi<br />

We present a Density Functional Based Tight Binding study on<br />

the structural and electronic structure of II-VI wurtzite coreshell,<br />

core- multi-shell ZnO/ZnS hexagonal unsaturated<br />

nanowires of circular and hexagonal cross section shapes and<br />

examine the dependence of interface stress and formation<br />

energy on nanowire lateral size with diameter range from 20Å<br />

upto 40Å. Wire’s Young’s modulus along the axial growth<br />

direction have been estimated. Also the tensile test have been<br />

applied for various wires to show the diameter dependence’s of<br />

their mechanical properties. The electronic properties of these<br />

heterostructure nanowire (e.g. Projected <strong>Ban</strong>d Structure,<br />

Density of State, charge transfer via Mulliken population<br />

analysis) also exhibit wire’s diameter dependence behaviors.<br />

Báo cáo Treo<br />

52. Electron Scattering from Polarization Charges Bound on a<br />

Rough Interface of Uniformly-Doped ZnO/Zn1‐xMgxO<br />

Heterostructure<br />

Le Tuan (1) and Nguyen Thanh Tien (2)<br />

(1) Institute of Engineering Physics, Hanoi University of Science and<br />

Technology, 1 Dai Co Viet Road, Hanoi, Vietnam (2) College of<br />

Science, Can Tho University, 3-2 Road, Can Tho City, Vietnam<br />

We present a theory of polarization surface roughness (PSR)<br />

scattering mechanism for electrons in the conduction channel of<br />

actual ZnO/Zn 1-x Mg x O heterostructures of the both O- and Zn-polar<br />

faces in ZnO layer. In combination with the normal surface<br />

roughness (SR) scattering from roughness-induced fluctuations in<br />

the potential barrier position, the carriers must be extra scattered<br />

from the polarization charges bound on a rough interface of the<br />

heterostructure. This ad hoc scattering mechanism tends to reduce<br />

carrier mobility down to a half of value in comparison with the one<br />

Hội nghị Vật lý lý thuyết toàn quốc lần thứ 35<br />

55<br />

56<br />

Tp. Hồ Chí Minh, 02-06/8/2010

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