Analysis of temperature dependent optical gain of strained quantumwell taking account of carriers in the SCH layer

The temperature dependence of optical gain in strained quantum well is analyzed taking account of carriers in the separate confinement heterostructure (SCH) layer. Taking account of these carriers in the SCH layer can explain to a considerable extent the difference in the temperature performance between the λ=0.98 μm laser and λ=1.3 μm laser. It is shown that well depth plays a crucial role for the temperature dependence of optical gain. A strained quantum well on an InGaAs ternary substrate is shown to give a high gain with a small temperature dependence     

High-performance strain-compensated InGaAs-GaAsP-GaAs(λ=1.17 μm) quantum well diode lasers

This letter reports studies on highly strained and strain-compensated InGaAs quantum-well (QW) active diode lasers on GaAs substrates, fabricated by low-temperature (550°C) metal-organic chemical vapor deposition (MOCVD) growth. Strain compensation of the (compressively strained) InGaAs QW is investigated by using either InGaP (tensile-strained) cladding layer or GaAsP (tensile-strained) barrier layers. High-performance λ=1.165 μm laser emission is achieved from InGaAs-GaAsP strain-compensated QW laser structures, with threshold current densities of 65 A/cm² for 1500-μm-cavity devices and transparency current densities of 50 A/cm². The use of GaAsP-barrier layers are also shown to significantly improve the internal quantum efficiency of the highly strained InGaAs-active laser structure. As a result, external differential quantum efficiencies of 56% are achieved for 500-μm-cavity length diode lasers     

Strained InGaAs quantum well lasers with small-divergence anglesfor high-power pump modules

Epitaxial structures were designed for high-power strained InGaAs/AlGaAs quantum well lasers with low vertical-divergence emitting angles. The vertical divergence angles achieved were down to ~20°. High power output 1.02 μm pump modules with well-designed strained quantum well lasers have been developed for a 1.3 μm band Pr⁺ -doped fibre amplifier. A maximum optical fibre output of 157 mW was obtained     

Fabrication of In0.25Ga0.75As/InGaAsPstrained SQW lasers on In0.05Ga0.95As ternarysubstrate

A uniform In_0.05Ga_0.95As ternary substrate was grown by using liquid encapsulated Czochralski (LEC) technique with a method of supplying GaAs source material at a constant temperature, and InGaAs/InGaAsP strained single quantum well (SQW) lasers were fabricated on the substrate for the first time. The lasers lased at 1.03 μm and exhibited low threshold current density of 222 A/cm² and excellent characteristic temperature of 221 K, showing that the ternary substrate has a sufficient quality for laser fabrication     

Broadband tuning (170 nm) of InGaAs quantum well lasers

The wavelength tuning properties of strained InGaAs quantum well lasers using an external grating for feedback is reported. Tunable laser oscillation has been observed over a range of 170 nm, between 840 and 1010 nm, under pulsed current excitation. The optimal conditions for broadband tunability for the InGaAs lasers are different from GaAs lasers, which is attributed to a difference in spectral gain curves. Together with an optimised GaAs quantum well laser the entire region between 740 and 1010 nm is spanned.<>     

Strained-layer InGaAs-GaAs-InGaP buried-heterostructurequantum-well lasers on a low-composition InGaAs substrate byselective-area MOCVD

Aluminum-free buried-heterostructure quantum-well lasers have been successfully fabricated on low-composition InGaAs substrates. Selective-area metalorganic chemical vapor deposition (MOCVD) was utilized to investigate a variety of InGaAs quantum wells with a wide range of composition and thickness. Compressively strained quantum wells can be deposited thicker on substrates of InGaAs than GaAs before the generation of misfit dislocations. These deeper potential wells enable laser diodes with longer wavelengths (1.1504 μm) than GaAs-based emitters and higher characteristic temperatures (145 K) than InP-based devices     

Very low threshold current density room temperature continuous-wavelasing from a single-layer InAs quantum-dot laser

Continuous-wave (CW) lasing operation with a very low threshold current density (J_th=32.5 A/cm²) has been achieved at room temperature by a ridge waveguide quantum-dot (QD) laser containing a single InAs QD layer embedded within a strained InGaAs quantum well (dot-in-well, or DWELL structure). Lasing proceeds via the QD ground state with an emission wavelength of 1.25 μm when the cavity length is longer than 4.2 mm. For a 5-mm long QD laser, CW lasing has been achieved at temperatures as high as 40°C, with a characteristic temperature T₀ of 41 K near room temperature. Lasers with a 20 μm stripe width have a differential slope efficiency of 32% and peak output power of >10 mW per facet (uncoated)     

Strained layer InxGa1-xAs/GaAs and InxGa1-xAs/InyGa1-yPmultiple-quantum-well optical modulators grown by gas-source MBE

The first results on low-power p-i-n diode modulator structures using strained multiple quantum wells (MQW's) of InGaAs/InGaP grown by gas-source molecular beam epitaxy (MBE) on GaAs are presented. A comparison of transmission, reflection, and photocurrent spectra for these nonresonant devices with those fabricated from InGaAs/GaAs indicates larger modulation, with a maximum change in reflection of >42% observed at 5-V bias at a wavelength of 0.96 μm     

InGaAs/AlGaAs半导体激光器二维阵列

用金属有机化合物气相淀积 (MOCVD)技术外延生长了InGaAs/AlGaAs分别限制应变单量子阱激光器材料。利用该材料制成半导体激光器一维线阵列 ,然后再串联组装成二维阵列 ,在 1 0 0 0 μs的输入脉宽下 ,输出峰值功率达到 730W (77A) ,输出光功率密度为 4 87W/cm2 ,中心激射波长为 90 3nm ,光谱半宽 (FWHM )为 4 4nm。在此条件下可以稳定工作 86 0 0h以上     

Chemical beam epitaxy and laser-modified chemical beam epitaxy of InGaAs using tris-dimethylaminoarsenic

The growth of In_xGaj_1−xAs (x = 0.13–0.25) on GaAs by chemical beam epitaxy (CBE) and laser-modified CBE using trimethylindium (TMIn), triethylgallium (TEGa), and tris-dimethylaminoarsenic (TDMAAs) has been studied. Reflection high-energy electron diffraction measurements were used to investigate the growth behavior of InGaAs at different conditions. X-ray rocking curve and lowtemperature photoluminescence (PL) measurements were used to characterize the InGaAs/GaAs pseudomorphic strained quantum well structures. Good InGaAs/GaAs interface and optical property were obtained by optimizing the growth condition. As determined by the x-ray simulation, laser irradiation during the InGaAs quantum well growth was found to enhance the InGaAs growth rate and reduce the indium composition in the substrate temperature range studied, 440–500°C, where good interfaces can be achieved. These changes, which are believed to be caused by laser-enhanced decomposition of TEGa and laser-enhanced desorption of TDMAAs, were found to depend on the laser power density as well. With laser irradiation, lateral variation of PL exciton peaks was observed, and the PL peaks became narrower.     

1.75 μm strained InGaAs multiquantum well laser grown on InAs0.08P0.92 ternary substrate

The authors have demonstrated a strained InGaAs multiquantum well laser grown on an InAs_0.08P_0.92 ternary substrate. The epitaxial structure was grown using metal organic vapour phase epitaxy (MOVPE). The InAsP wafers were characterised using room temperature photoluminescence, X-ray diffraction and X-ray topography. Pulsed power levels of 60 mW/facet at h=1.75 μm were measured at T=250 K. A characteristic temperature of T₀=46 K was observed over a temperature range of 78-250 K     

Carrier-dependent nonlinearities and modulation in an InGaAs SQWwaveguide

The authors report measurements of optically induced carrier-dependent refractive index changes and their saturation in an InGaAs single quantum well centered within a linear multiple quantum well guided-wave Fabry-Perot resonator using diode laser sources. A low-excitation nonlinear refractive cross-section, σ_n=-1×10^-19 cm³, was deduced for probe wavelengths near the TM (transverse magnetic) absorption edge, falling only to σ_n=-3.1×10^-20 cm³, at over 0.16 μm from the band edge. For an incident irradiance of 18 kW/cm ², refractive index changes in the InGaAs quantum well as large as -0.16 were deduced near the absorption edge, while the index change at a wavelength 0.16 μm from the absorption edge was -0.055. This large off-resonant index change is attributed to an enhanced free-carrier contribution within a 2D system     

Optical properties of InGaAs/InGaAlAs quantum wells for the 1520–1580 nm spectral range

The optical properties of elastically strained semiconductor heterostructures with InGaAs/InGaAlAs quantum wells (QWs), intended for use in the formation of the active region of lasers emitting in the spectral range 1520–1580 nm, are studied. Active regions with varied lattice mismatch between the InGaAs QWs and the InP substrate are fabricated by molecular beam epitaxy. The maximum lattice mismatch for the InGaAs QWs is +2%. The optical properties of the elastically strained InGaAlAs/InGaAs/InP heterostructures are studied by the photoluminescence method in the temperature range from 20 to 140°C at various power densities of the excitation laser. Investigation of the optical properties of InGaAlAs/InGaAs/InP experimental samples confirms the feasibility of using the developed elastically strained heterostructures for the fabrication of active regions for laser diodes with high temperature stability.     

On the gain properties of “thin” elastically strained InGaAs/InGaAlAs quantum wells emitting in the near-infrared spectral region near 1550 nm

The results of experimental studies of the gain properties of “thin” (3.2 nm thick) elastically strained InGaAs/InGaAlAs quantum wells emitting in the near-infrared spectral region near 1550 nm are presented. The results of studying the threshold and gain characteristics of stripe laser diodes with active regions based on “thin” quantum wells with a lattice–substrate mismatch of +1.0% show that the quantum wells under study exhibit a high modal gain of 11 cm^–1 and a low transparency current density of 46 A/cm² per quantum well.     

Monolithic serial InGaAs-GaAs-AlGaAs laser diode arrays

Top-contact monolithic serially-biased InGaAs-GaAs-AlGaAs (λ~0.93 μm) broad area strained-layer quantum well laser arrays have been fabricated on a semi-insulating GaAs substrate. The laser array consists of four individual laser diodes and operates up to 2.8 W at 3.6 A (supply limited) per uncoated facet under pulsed conditions (15 kHz, 2 μs). The threshold current is ~0.5 A, and the peak slope efficiency and the peak electrical-to-optical conversion efficiency of an individual laser element are ~0.53 W/A and 14%, respectively. The near-field intensity distribution is shown to be broad enough to fill the entire active region under the p-metal stripe (125 μm) of the individual laser diodes at high current levels     

Gain in injection lasers based on self-organized quantum dots

The analytical form of the dependence of the gain on pump current density for lasers with an active region based on self-organized quantum dots is derived in a simple theoretical model. The proposed model is shown to faithfully describe experimental data obtained for laser diodes based on InGaAs quantum dots in an AlGaAs/GaAs matrix, as well as InAs quantum dots in an InGaAs/InP matrix. The previously observed gain saturation and switching of the lasing from the ground state to an excited state of the quantum dots are studied. The influence of the density of quantum-dot arrays on the threshold characteristics of lasers based on them is examined on the basis of this model. Fiz. Tekh. Poluprovodn. 33, 215–223 (February 1999)     

High-power InAlGaAs-GaAs laser diode emitting near 731 nm

High-power, reliable operation of an InAlGaAs-based QW laser diode structure emitting near 731 nm and having a strained InAlGaAs active region is described. Threshold currents for coated 100 μm×1000 μm devices are 281 mA, and a peak power conversion efficiency of 41% is measured. Internal losses are measured to be 1.2 cm^-1. A system for fiber-coupling two-dimensional continuous-wave (CW) arrays of these devices is demonstrated     

Proposal of a GaInAs/GaInAsP/InP antiguided filter laser arrayoperating in single longitudinal mode

The authors propose a type of in-phase lateral- and single-longitudinal-mode laser array, the so-called antiguided filter laser array (AFLA), in which an antiguided filter region is inserted between a positive-index-guided multiple-strip array region with a shallow corrugation grating and a high-reflectivity region with deep corrugation. Threshold current as low as 100 mA was obtained for a five-element laser array with active region length of 300 μm and total emitter width of 18 μm, using five-pairs of Ga_0.3In _0.7As (3 nm)/GaInAsP (10 nm) compressively strained quantum wells     

Submicrometre gate length scaling of inversion channelheterojunction field effect transistor

The scaling to 0.5 μm of the inversion channel HFET with a single strained InGaAs quantum well is described. A unity current gain frequency of 40 GHz, g_m=205 mS/mm and V_TH=-0.34 V have been obtained for 0.5×100 μm² devices. For shorter gate lengths, threshold shifts are sizeable so that in order to scale further, modifications to the growth and processing are required     

Calculated performances of 1.3-μm vertical-cavitysurface-emitting lasers on InGaAs ternary substrates

1.3-μm vertical-cavity surface-emitting lasers (VCSEL's) on InGaAs ternary substrates are proposed and designed, It is shown that a deep potential well on the ternary substrate enlarges optical gain of a strained quantum well in the wavelength region of 1.3 μm. A higher reflectivity distributed Bragg reflector (DBR) is also obtained by the use of the ternary substrate because materials with a large refractive-index difference can be used for the DBR. Calculated threshold current density of 1.3-μm VCSEL's on the ternary substrates is much lower than those on the conventional InP substrates. The possibility of extremely low threshold current density below 200 A/cm ² and temperature-insensitive operation are described