Impurity cyclotron resonance in InGaAs/AlAs superlattice under ultra high magnetic fields

We have carried out cyclotron resonance (CR) measurements of (InGaAs)₈/(AlAs)₈ superlattice (SL) to investigate electronic properties of the SL under pulsed ultra-high magnetic fields. The magnetic fields up to 160 T were generated by using the single-turn-coil technique. Clear CR signals were obtained in the transmission of far-infrared laser through the SL at room temperature and lower temperature. We observed a shift of CR peak to lower magnetic field caused by transition from free-electron CR to impurity CR below 90 K. Compared with the previous works of GaAs/AlAs SL, the peak shift was small and the transition temperature was low. This result suggests that a binding energy of the impurity in the InGaAs/AlAs SL is smaller than the GaAs/AlAs SL.     

Infrared cyclotron resonance in InSb,GaAs and Ge in very high magnetic fields

Infrared cyclotron resonance was observed in n-type InSb, GaAs and Ge in very high magnetic fields up to 1.3 MOe at room temperature using a CO₂ laser. A large shift of the cyclotron mass due to the non-parabolicity of the energy band was found in each material. The band edge masses of electrons at room temperature were evaluated to be $\text{m}{}^1\text{= 0.0127 m}$ for InSb, $\text{m}{}^1\text{= 0.065}$m for GaAs and $\text{m}{}^1{}_{\mathrm{t}}\text{= 0.086}$m for Ge. The linewidth was measured in GaAs and Ge in the high fields.     

Electron-active cyclotron resonance in p-doped InMnAs in high magnetic fields

We present a theoretical and experimental study of electron-active cyclotron resonance in p-doped InMnAs in high magnetic fields. Results are based on an 8-band Pidgeon–Brown model generalized to include finite k_z effects and s(p)–d exchange interaction between itinerant carriers and Mn d-electrons. The e-active transitions in the valence band in p-doped samples take place due to the nature of multiple valence bands (heavy and light holes). We have calculated the absorption spectra in high magnetic fields and identified optical transitions which contribute to the cyclotron resonance for both e-active and h-active polarizations. Calculations show agreement with experimental results.     

低温InGaAs/InAlAs多量子阱的分子束外延生长与表征

采用气源分子束外延(GSMBE)生长了低温InGaAs材料,研究了生长温度及As压对InGaAs材料性质的影响,得到优化的生长条件为:生长温度为300 ℃、As压为77.3 kPa。通过Be掺杂,并采用In0.52Al0.48As/In0.53Ga0.47As多量子阱结构,将材料的方块电阻提高到1.632106 /Sq,载流子数密度降低至1.0581014 cm-3。X射线衍射结果表明:InGaAs多量子阱材料具有较高的晶体质量。这种Be掺杂InGaAs多量子阱材料缺陷密度大且电阻率高,是制作太赫兹光电导天线较理想的基质材料。收稿日期:; 修订日期:     

低温InGaAs/InAlAs多量子阱的分子束外延生长与表征

采用气源分子束外延(GSMBE)生长了低温InGaAs材料,研究了生长温度及As压对InGaAs材料性质的影响,得到优化的生长条件为：生长温度为300 ℃、As压为77.3 kPa。通过Be掺杂,并采用In0.52Al0.48As/In0.53Ga0.47As多量子阱结构,将材料的方块电阻提高到1.632106 /Sq,载流子数密度降低至1.0581014 cm-3。X射线衍射结果表明：InGaAs多量子阱材料具有较高的晶体质量。这种Be掺杂InGaAs多量子阱材料缺陷密度大且电阻率高,是制作太赫兹光电导天线较理想的基质材料。收稿日期:; 修订日期:     

Determination of electron effective mass from optical transition energy in InGaAs/InAlAs quantum wells

Nonparabolic effective mass of conduction subbands in InGaAs/InAlAs quantum wells (QWs), lattice-matched to InP, was quantitatively obtained by analyzing interband-optical transition spectra. Thickness of InGaAs well was 5.3, 9.4, and . Thickness of InAlAs barrier was about , and each QW was independent. Excellent agreement was obtained between experimental mass and theoretical mass predicted by Kane's three-level band theory on bulk InGaAs, in a wide energy range of from the bandedge. Method of experimental analysis on a relation between eigen energy and effective mass was described.     

Rashba spin-orbit coupling probed by the weak antilocalization analysis in InAlAs/InGaAs/InAlAs quantum wells as a function of quantum well asymmetry

We have investigated the values of the Rashba spin-orbit coupling constant alpha in In(0.52)Al(0.48)As/In(0.53)Ga(0.47)As/In(0.52)Al(0.48)As quantum wells using the weak antilocalization (WAL) analysis as a function of the structural inversion asymmetry (SIA) of the quantum wells. We have found that the deduced alpha values have a strong correlation with the degree of SIA of the quantum wells as predicted theoretically. The good agreement between the theoretical and experimental values of alpha suggests that our WAL approach for deducing alpha values provides a useful tool in designing future spintronics devices that utilize the Rashba spin-orbit coupling.     

Anomalous shape of cyclotron resonance line in n-GaP in high magnetic fields

Cyclotron resonance in n-GaP has been observed at 119 μm in pulsed magnetic fields up to 410 kG. From the experiments with the magnetic field parallel to the 〈100〉, 〈110〉 and 〈111〉 axes, it is concluded that the transverse effective mass for electron is and that the anisotropy factor of the conduction band is K = 7.9^+3.2_?2.0. An anomalous shape of the absorption curve was found in the magnetic field directions parallel to the crystal axes 〈110〉 and 〈111〉.     

Photoluminescence in GaAs/AlGaAs quantum wells associated with excited confinement subbands

We report on photoluminescence emission features which are observed from GaAs/AlGaAs multiple quantum wells only at elevated temperatures (T>10K), using weak cw laser excitation. These features have energies higher than those of the heavy and light hole excitons and are associated with interband transitions between excited confinement conduction and valence subbands. Their energies are compared with values calculated from measured well dimensions and accepted band parameters for a series of samples with well widths between 80 and 375Å.     

InAlAs/InGaAs/InAlAs量子阱高迁移率二维电子气系统中的反弱局域效应研究

研究了Si 重δ 掺杂In_0.52Al_0.48As/In_0.53Ga_0.47As/In_0.52Al_0.48As单量子阱内高迁移率二维电子气系统中的反弱局域效应. 研究表明，强的Rashba自旋轨道相互作用来源于量子阱高的结构反演不对称. 高迁移率系统中，粒子的运动基于弹道输运而非扩散输运. 因此，旧的理论模型不能用于拟合实验结果. 由于最新的模型在实际拟合中过于复杂，一种简单可行的近似用于处理实验结果，并获得了自旋分裂能Δ₀和自旋轨道耦合常数α两个重要的物理参数. 该结果与对纵向电阻的Shubnikov-de Haas—SdH振荡分析获得的结果一致. 高迁移率系统中的反弱局域效应研究表明，发展有效的反弱局域理论模型，对于利用Rashba自旋轨道相互作用来设计自旋器件尤为重要.     

Photoluminescence saturation in InGaAs/GaAs single quantum wells

Saturation of the photoluminescence associated with the 11H transition in the InGaAs single quantum wells is observed under high intensity optical excitation. At the onset of saturation, a spill-over of the photoluminescence occurs into the GaAs cladding layers as the excitation intensity is increased. The measurements are used to determine a limiting value of the quantum efficiency of the quantum-well associated photoluminescence.     

Variable-range hopping conduction in doped germanium at very low temperatures and high magnetic fields

The conductivity of doped Ge below the metal-insulator transition is measured at temperatures between 4 K and 40 mK and in magnetic fields up to 7 Tesla. In zero field the resistivity exponent diverges asT ^–1/2. In weak fields the magnetoresistance increases asB ² and becomes exponentially large in strong fields and at low temperatures. The results can be described quantitatively in terms of variable-range hopping between localized states having a Coulomb gap in the density of states at the Fermi level. The magnetoresistance is calculated for arbitrary fields by means of a quasi-classical method. A fit to the data gives the radius of the localized states and the density of states. The sample is found to be very close to the metal-insulator transition. A small increase of the binding energy is observed in strong fields.     

Intermixing behavior in InGaAs/InGaAsP multiple quantum wells with dielectric and InGaAs capping layers

The influence of the InGaAs capping layer on the intermixing behavior of dielectric-capped In_0.53Ga_0.47 As/In_0.81Ga_0.19As_0.37P_0.63 multiple quantum wells (MQWs) was investigated by measuring the change in the photoluminescence spectra after rapid thermal annealing. The magnitude of the energy shift in the transition energy from the first electronic sub-band to the first heavy- and light-hole sub-bands of the MQWs is large when SiO₂ and InGaAs hybrid capping layers are employed, but it is rather small when Si₃N₄ and InGaAs hybrid capping layers are employed. This result indicates that the InGaAs capping layer holds promise for applications involved in the fabrication of integrated photonic devices, but only when it is incorporated with the SiO₂ capping layer. The reason why the InGaAs capping layer behaves differently under the SiO₂ and Si₃N₄ capping layers is also discussed. Received: 4 December 1999 / Accepted: 26 September 2000 / Published online: 10 January 2001     

Observation of a hybridization gap in cyclotron resonance spectra of semimetallic InAs/GaSb quantum wells

Splitting of the cyclotron resonance (CR) line is observed in the electron CR spectra of InAs/GaSb heterostructures containing tunneling-coupled electron and hole layers. This splitting is interpreted to be a manifestation of a hybridization gap arising as a result of anticrossing of the Landau levels of electrons and holes when their wave functions overlap. The energy splitting of the CR lines is correlated with the magnitude of the overlap and agrees with theoretical estimates of the hybridization gap width. Pis’ma Zh. éksp. Teor. Fiz. 69, No. 4, 313–317 (25 February 1999)     

Manifestation of a semimetallic state in cyclotron resonance in low-symmetry HgTe-based quantum wells

Cyclotron-resonance measurements in 21-nm-thick HgTe/CdHgTe quantum wells of different crystallographic orientations have been performed. It has been found that, in contrast to the structures with the (001) orientation of the quantum-well plane, (013)-oriented quantum wells are semimetallic and their absorption spectra exhibit both electron and hole cyclotron-resonance lines. The simultaneous presence of the two types of charge carriers originates from an overlap between the upper heavy-hole quantum-confinement subbands hh1 and hh2. This overlap is caused by the strong interaction of these subbands with the Dyakonov-Khaetskii interface state. Calculations carried out using the eight-band kp-Hamiltonian indicate that, for known values of the band-structure parameters, the overlap between hh2 and hh1 subbands does not occur; this result is in agreement with the cyclotron-resonance data for (001)-oriented structures. The enhanced interaction between heavy-hole and interface states owing to the existence of steps at low-symmetry heterointerfaces may be the mechanism responsible for the appearance of an overlap between subbands in HgTe quantum wells with orientation different from (001).