Browsing by Author "LIOU, DC"
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Item type:Item, A NOVEL TECHNIQUE FOR LOW-THRESHOLD AND HIGH-POWER INGAAS/GAAS STRAINED-LAYER 0.98-MU-M BURIED HETEROSTRUCTURE LASER FABRICATION(1992-02-01) ;LIOU, DC ;CHIANG, WH ;LEE, CP ;CHANG, KHLIU, DGA novel fabrication technique has been developed for InGaAs/GaAs strained-layer buried heterostructure lasers. Dielectric masks and Zn diffusion are not required in this technique. This novel fabrication process is much easier than the conventional approach and yields excellent laser results. A low threshold of 3 mA and high-power operation for lasing wavelength of 9800 +/- 20 angstrom have been achieved with graded index separate confinement heterostructure devices using this novel technique.Item type:Item, BEHAVIOR OF THE 1ST LAYER GROWTH IN GAAS MOLECULAR-BEAM EPITAXY(1990-10-01) ;LIU, DG ;LEE, CP ;CHANG, KH ;WU, JSLIOU, DCItem type:Item, CHARACTERIZATION OF IMPROVED ALGAAS/GAAS RESONANT TUNNELING HETEROSTRUCTURE BIPOLAR-TRANSISTORS(1991-02-01) ;WU, JS ;CHANG, CY ;LEE, CP ;CHANG, KHLIU, DGWe report on the fabrication of AlGaAs/GaAs resonant tunneling heterostructure bipolar transistors (RTHBT's). The devices exhibit a current peak in the transfer characteristics, with peak-to-valley current ratios of 1.7 and 9 at 300 K and 77 K, respectively. The common-emitter small signal current gains at 300 K and 77 K reach 40 and 28, respectively. They are the best results to date for AlGaAs/GaAs resonant tunneling transistors. Because the double barriers are placed in the emitter and far from the emitter-base interface, and the heterostructure emitter suppresses the hole injection from the base to the emitter, the occurrence of the negative differential resistance (NDR) in the device characteristics is governed by the emitter current but not by the base current. The operation mechanism of the NDR behavior in the common-emitter output characteristics is discussed.Item type:Item, DELTA-DOPED QUANTUM-WELL STRUCTURES GROWN BY MOLECULAR-BEAM EPITAXY(1990-10-29) ;LIU, DG ;LEE, CP ;CHANG, KH ;WU, JSLIOU, DCItem type:Item, DIRECT OBSERVATION OF SI DELTA-DOPED GAAS BY TRANSMISSION ELECTRON-MICROSCOPY(1992-05-25) ;LIU, DG ;FAN, JC ;LEE, CP ;TSAI, CMCHANG, KHDirect observation of the Si delta-doped layer in GaAs has been achieved by high resolution transmission electron microscopy. Samples with different Si doses, from half a monolayer to two monolayers, were studied. The observed spreading of the delta-doped layer showed that Si atoms are largely confined in five monolayers at most (in the highest dose case), indicating excellent confinements of dopants in GaAs. From the images, the Si atoms were uniformly distributed in the doped layer, no cluster formation was observed. For delta-doped GaAs grown at low temperature (480-degrees-C), stacking faults originated from the doped layers were observed. These faults were thought to be caused by the large unrelaxed strain in the low-temperature grown GaAs.Item type:Item, FUNDAMENTAL MODE-OPERATION OF HIGH-POWER INGAAS/GAAS/ALGAAS LASER ARRAYS(1993-05-01) ;TSANG, JS ;LIOU, DC ;TSAI, KL ;CHEN, HRTSAI, CMA new ridge waveguide laser array with stable fundamental mode operation has been fabricated. By introducing absorption regions in all the laser stripes except for the central one, the electric field distribution of the laser arrays and the modal gains of the array supermodes are changed, resulting in fundamental mode operation. The threshold current of an array with five elements is typically 40 mA and the maximum output power is higher than 150 mW. The single-lobed far-field pattern centered at 0-degrees with full width at half maximum of 2-degrees is obtained at 1.5 times of the threshold current (I(th)).Item type:Item, HIGH-QUALITY ALGAAS LAYERS GROWN BY MOLECULAR-BEAM EPITAXY AT LOW-TEMPERATURES(1992-03-01) ;CHANG, KH ;WU, JS ;LIU, DG ;LIOU, DCLEE, CPLow-temperature (approximately 600-degrees-C) molecular beam epitaxy (MBE) growth of AlGaAs has been studied. It was found that the quality of AlGaAs grown at low temperatures can be as good as that grown at high temperatures ( > 700-degrees-C) if the source materials and the growth chamber are very clean. The threshold currents of Al0.6Ga0.4As/Al0.15Ga0.85As/Al0.6Ga0.4As double heterostructure (DH) lasers grown at low temperatures and high temperatures are almost the same. The material quality can be further improved with a proper amount of indium doping. Photoluminescence (PL) linewidths of 3.1 meV and 1.7 meV have been measured for In-doped Al0.42Ga0.58As and Al0.18Ga0.82As at 4 K, respectively. They are the narrowest linewidths for the MBE-grown AlGaAs with comparable Al contents at any growth temperature. With a proper amount of In doping, double-barrier resonant tunnelling diodes have also shown improved peak-to-valley current ratios.Item type:Item, IMPROVED ALGAAS/GAAS DOUBLE-BARRIER RESONANT TUNNELING STRUCTURES USING 2-DIMENSIONAL SOURCE ELECTRONS(1991-01-15) ;WU, JS ;LEE, CP ;CHANG, CY ;CHANG, KHLIU, DGWe report the enhancement of peak-to-valley current ratios (PVCRs) of double-barrier resonant tunneling structures (DBRTSs) based on the AlGaAs/GaAs material system. The PVCRs as high as 25.4 and 18 have been obtained at 77 K for superlattice and alloy barrier structures with 0.2-mu-m undoped electrodes, respectively. These are the largest PVCRs to date for AlGaAs/GaAs DBRTSs. The large band bending across the undoped electrodes causes size quantization of the accumulation layer, resulting in better resonant tunneling characteristics.Item type:Item, INFLUENCE OF INDIUM DOPING ON ALGAAS LAYERS GROWN BY MOLECULAR-BEAM EPITAXY(1990-10-15) ;CHANG, KH ;LEE, CP ;WU, JS ;LIU, DGLIOU, DCItem type:Item, INTRINSIC AND EXTRINSIC EFFECTS ON PERFORMANCE LIMITATION OF ALGAAS/GAAS DOUBLE-BARRIER RESONANT TUNNELING STRUCTURES(1992-05-01) ;WU, JS ;LEE, CP ;CHANG, CY ;CHANG, KHLIU, DGThe performance limitations of negative differential resistance (NDR) in AlGaAs/GaAs double-barrier resonant tunneling structures (DBRTSs) have been investigated by varying the barrier thickness and quantum well (QW) width, and by doping In into the barrier layers. For devices with thick barriers (greater-than-or-equal-to 70 angstrom), the scattering in the material is believed to cause the saturation of the peak-to-valley current ratio (PVCR). The dependence of PVCR on the well width, however, is found to be, to the first-order, not related to the scattering mechanisms or other material properties. It is rather an inherent property of the tunneling process under different conditions. On the other hand, it was found that a proper amount of In doping into the barrier layers can increase the PVCR, because of the lower defect concentration, resulting in lower scattering rate in the active region.Item type:Item, INVESTIGATION OF INDIUM DOPING AND INCORPORATION IN ALGAAS/GAAS DOUBLE-BARRIER RESONANT TUNNELING STRUCTURES(1991-02-28) ;WU, JS ;CHANG, KH ;LEE, CP ;CHANG, CYLIU, DGIn doping and incorporation in the barrier layers of AlGaAs/GaAs double-barrier resonant tunnelling structures (DBRTSs) have been studied. It was found that the peak-to-valley current ratio (PVCR) can be improved by the proper amount of In doping. This is attributed to the improvement in the quality of the AlGaAs barrier layers due to the high surface migration rate of In atoms that reduces group III vacancies. Also pseudomorphic In(x)(Al0.5Ga0.5)(1-x)As/GaAs (x = 0.12) strained-layer DBRTSs have been fabricated by incorporating a sufficient amount of In into the AlGaAs barrier layers. PVCRs as high as 27.5 at 77 K have been obtained. This is the first realisation of such DBRTSs with lattice-mismatched quaternary barrier layers.Item type:Item, PRECISE DETERMINATION OF ALUMINUM CONTENT IN ALGAAS(1991-11-01) ;CHANG, KH ;LEE, CP ;WU, JS ;LIU, DGLIOU, DCThe Al composition of AlGaAs has been determined by four methods: high-resolution transmission electron microscopy (HRTEM), reflection high-energy electron diffraction (RHEED), photoluminescence (PL), and double-crystal x-ray diffraction (DCXRD). HRTEM is direct and the most accurate method because it does not involve any formula or extrapolation. Using the result obtained from HRTEM as a standard, we have calibrated the results from other methods. RHEED intensity oscillation is found to be accurate and reliable, if the growth conditions are correctly chosen. Comparing the PL results with those determined from HRTEM and RHEED, we suggest three formulas to determine the Al contents at different temperatures. We also proposed a polynomial to determine the Al concentration using the DCXRD measurement.Item type:Item, QUANTUM EFFECT IN THE ACCUMULATION LAYER ON FIELD-INDUCED PHOTOLUMINESCENCE OF DOUBLE-BARRIER RESONANT TUNNELING STRUCTURES(1991-07-01) ;WU, JS ;CHANG, KH ;LEE, CP ;CHANG, CYLIU, DGThe photoluminescence (PL) of double-barrier resonant tunneling structures (DBRTSs) with undoped electrodes under bias has been studied. The strong band bending across the cathode causes the quantum size effect in the accumulation layer. The resonant tunneling of electrons from the first excited quantum level in the accumulation layer produces a kink in the current-voltage characteristic. It is found that the PL intensity from the quantum well (QW) as a function of bias sharply peaks at the voltage corresponding to the kink. This provides evidence of the interaction between the first excited quantum state in the accumulation layer and the resonant state in the QW.Item type:Item, REPETITION OF NEGATIVE DIFFERENTIAL RESISTANCE IN VERTICALLY INTEGRATED DOUBLE-BARRIER RESONANT TUNNELING STRUCTURES(1990-05-01) ;WU, JS ;LEE, CP ;CHANG, CY ;CHANG, KHLIU, DGItem type:Item, RESONANT TUNNELING OF ELECTRONS FROM QUANTIZED LEVELS IN THE ACCUMULATION LAYER OF DOUBLE-BARRIER HETEROSTRUCTURES(1990-11-26) ;WU, JS ;CHANG, CY ;LEE, CP ;CHANG, KHLIU, DGItem type:Item, TRANSMISSION ELECTRON-MICROSCOPY STUDY OF HEAVILY DELTA-DOPED GAAS GROWN BY MOLECULAR-BEAM EPITAXY(1993-01-15) ;LIU, DG ;FAN, JC ;LEE, CP ;CHANG, KHLIOU, DCN-type and p-type delta-doped GaAs grown by molecular beam epitaxy with rather significantly high doses of Si and Be have been investigated by transmission electron microscopy (TEM). The amount of doses ranged from half a monolayer to two monolayers. The microscopic structures of the delta-doped regions and the adjacent epilayers were directly observed by TEM. The effect of impurity spreading on the heterointerfaces and superlattices was also studied. Si atoms present in Si delta-doped samples were confined to within a few atomic layers. The Be atoms present in Be delta-doped samples, however, spread over a quite wide region and caused rough heterointerfaces and wavy superlattices to form. Spreading of Be was attributed to segregation and diffusion which occurred during growth. Stacking faults were found in the delta-doped samples when they were grown at low temperatures. They could be attributed to local strain caused by heavy doping.