MESFET-like transferred-electron devices in In/sub 0.53/Ga/sub 0.47/As

In/sub 0.53/Ga/sub 0.47/As transferred-electron devices with Schottky-gate electrodes were fabricated. These devices can be used in optoelectronic circuits on InP or as millimetre wave oscillators. For the realisation of the gate electrode several enhancement layers were tested to increase the Schottky barrier height on In/sub 0.53/Ga/sub 0.47/As. The triggering of single dipole domains in the device was demonstrated.<>     

Metal-semiconductor-metal photodetector on p-type In/sub 0.53/Ga/sub 0.47/As

An MSM Schottky barrier photodetector based on p-type In/sub 0.53/Ga/sub 0.47/As suitable for detection in the 0.8-1.7 wavelength range is reported. Aluminium metallisation was used. The large area devices exhibited responsivity of about 0.4 A/W at 1.3 mu m and tau /sub on/>     

Threshold voltage of submicron Ga/sub 0.47/In/sub 0.53/As HIGFETs

Presents threshold voltage data for Al/sub 0.48/In/sub 0.52/As/Ga/sub 0.47/In/sub 0.53/As/InP heterostructure insulated gate FETs (HIGFETs) with gate lengths from 1.2 mu m to 0.4 mu m. The refractory-gate, self-aligned fabrication process was applied to MBE-grown structures with 300 AA Ga/sub 0.47/In/sub 0.53/As channels and semi-insulating superlattice buffers to achieve sharp pinchoff with excellent threshold uniformity. HIGFETs with L/sub g/=1.2 mu m showed a threshold voltage of -0.076+or-0.019 V, making them well-suited to application in direct-coupled FET logic (DCFL) circuits.<>     

Temperature dependence of breakdown and avalanche multiplication in In/sub 0.53/Ga/sub 0.47/As diodes and heterojunction bipolar transistors

The avalanche multiplication and impact ionization coefficients in In/sub 0.53/Ga/sub 0.47/As p-i-n and n-i-p diodes over a range of temperature from 20-400 K were measured and shown to have negative temperature dependence. This is contrary to the positive temperature dependence of the breakdown voltage measured on InP/In/sub 0.53/Ga/sub 0.47/As heterojunction bipolar transistors (HBTs) in this and previous works. It is shown that the collector-base dark current and current gain can be the overriding influence on the temperature dependence of breakdown in InP/In/sub 0.53/Ga/sub 0.47/As HBTs and could explain previous anomalous interpretations from the latter.     

Transferred-electron oscillations in In0.53Ga0.47As

Transferred-electron oscillations were observed and investigated in planar devices of In0.53Ga0.47As. The peak-to-peak magnitude of oscillations with respect to the device current at threshold field was as high as 70%, indicating the peak-to-valley velocity ratio of 3.3:1 for this material. The domain velocity was estimated from the oscillation frequency (2 GHz) and the corresponding device length (40 ?m) to be 8×106 cms?1. The results presented in the letter show a promising prospect for TED applications of this ternary alloy.     

Transferred-electron effect in In0.53Ga0.47As

The transferred-electron effect in In0.53Ga0.47As is demonstrated by observation for the first time in the travelling-domain mode. Current pulses of more than 70% are found. From velocity/field characteristics the peak velocity is determined as (2.2 ± 0.3) × 107 cm/s. The temperature dependence of the peak current is measured.     

High-performance In/sub 0.53/Ga/sub 0.47/As thermophotovoltaic devices grown by solid source molecular beam epitaxy

In/sub 0.53/Ga/sub 0.47/As-based monolithic interconnected modules (MIMs) of thermophotovoltaic (TPV) devices lattice-matched to InP were grown by solid source molecular beam epitaxy. The MIM device consisted of ten individual In/sub 0.53/Ga/sub 0.47/As TPV cells connected in series on an InP substrate. An open-circuit voltage (V/sub oc/) of 4.82 V, short-circuit current density (J/sub sc/) of 1.03 A/cm/sup 2/ and fill factor of /spl sim/73% were achieved for a ten-junction MIM with a bandgap of 0.74 eV under high intensity white light illumination. Device performance uniformity was better than 1.5% across a full 2-in InP wafer. The V/sub oc/ and J/sub sc/ values are the highest yet reported for 0.74-eV band gap n-p-n MIM devices.     

Direct optical injection locking of monolithically integrated In/sub 0.53/Ga/sub 0.47/As/In/sub 0.52/Al/sub 0.48/As MODFET oscillators

The authors have fabricated monolithically integrated In/sub 0.53/Ga/sub 0.47/As/In/sub 0.52/Al/sub 0.48/As 0.25 mu m gate modulation-doped field effect transistor (MODFET) oscillators. The results of direct optical subharmonic injection locking of these oscillator circuits at 10.159 and 19.033 GHz are presented.<>     

Bit rate dependence of receiver sensitivities in Ga0.47In0.53As photoconductive detectors

We report the bit rate dependence of the sensitivities of a Ga0.47In0.53As photoconductive detector/GaAs FET hybrid receiver and compare the results with a theoretical calculation.     

Ohmic contacts on p-type Ga0.47In0.53As/InP

Ohmic contacts of Au and Ag based Zn containing alloys on p-type Ga_0.47In_0.53As have been studied using intermediate layers of Ti and Ni, respectively. Low specific contact resistance in the order of 10⁻⁵ Ωcm² are achieved. In case of AuZn alloy, the Ti intermediate metal layer causes higher contact resistances together with a worse contact morphology in contrast to Ni intermediate layers. However for AgZn contacts Ti adherent layers improve the contact resistances, especially for lower alloying temperatures. Moreover these contacts exhibit significant smoother interfaces as revealed by TEM micrographs. Thus AgZn contacts apply best to low resistive contacting of very thin p-layers forming e.g. the base of a ballistic device.     

Long-wavelength In/sub 0.53/Ga/sub 0.47/As-In/sub 0.52/Al/sub 0.48/As large-area avalanche photodiodes and arrays

Large-area (500-/spl mu/m diameter) mesa-structure In/sub 0.53/Ga/sub 0.47/As-In/sub 0.52/Al/sub 0.48/As avalanche photodiodes (APDs) are reported. The dark current density was /spl sim/2.5/spl times/10/sup -2/ nA//spl mu/m/sup 2/ at 90% of breakdown; low surface leakage current density (/spl sim/4.2 pA//spl mu/m) was achieved with wet chemical etching and SiO/sub 2/ passivation. An 18 /spl times/ 18 APD array with uniform distributions of breakdown voltage, dark current, and multiplication gain has also been demonstrated. The APDs in the array achieved 3-dB bandwidth of /spl sim/8 GHz at low gain and a gain-bandwidth product of /spl sim/120 GHz.     

InP衬底AlAs/In0.53Ga0.47As RTD的研制

报道了InP衬底AlAs/In0.53Ga0.47As/AlAs两垒一阱结构共振隧穿二极管(RTD)器件的研制.结构材料由分子束外延制备,衬底片为(001)半绝缘InP单晶片,器件制作选用台面结构.测得室温下的峰值电流密度为1.06×105 A/cm2,峰-谷电流比为7.4,是国内报道的首例InP材料体系RTD器件.     

InP衬底AlAs/In0.53Ga0.47As RTD的研制

报道了InP衬底AlAs/In0.53Ga0.47As/AlAs两垒一阱结构共振隧穿二极管(RTD)器件的研制.结构材料由分子束外延制备,衬底片为(001)半绝缘InP单晶片,器件制作选用台面结构.测得室温下的峰值电流密度为1.06×105 A/cm2,峰-谷电流比为7.4,是国内报道的首例InP材料体系RTD器件.     

Low dark current quasi-Schottky barrier MSM-photodiode structures on n-Ga/sub 0.47/In/sub 0.53/As with p/sup +/-Ga/sub 0.47/In/sub 0.53/As cap layer

The p/sup +/-cap layer was used to fabricate a metal-semiconductor-metal (MSM) interdigitated photodetector on Ga/sub 0.47/In/sub 0.53/As. The measured barrier height was Phi /sub Bn=/0.52 V, the ideality factor n=1.1 and average dark current density 2 mA/cm/sup 2/. A rise time of 45 ps at lambda =1.3 mu m under 2 V bias was measured for an MSM photodiode with 3 mu m finger width and finger gaps and an active area of 100*100 mu m/sup 2/.<>     

Longitudinal photoeffect in In0.53Ga0.47As p-n junctions

A longitudinal photoeffect in In_0.53Ga_0.47As p-n junctions was investigated: the dependence of the longitudinal photoemf V _{ph 1} on the coordinates of the light spot, the temperature, and the magnetic field. The dependences on the coordinates of the light spot were found to be linear; the theoretical values of V _{ph 1} agree with the experimental values. The temperature variation of V _{ph 1} in the interval 100–300 K is explained by the variation of the current-carrier mobility as a result of thermal scattering by the lattice. In a magnetic field, V _{ph 1} is observed to increase as a result of the photomagnetic effect. Fiz. Tekh. Poluprovodn. 31, 864–865 (July 1997)     

Geiger mode operation of an In/sub 0.53/Ga/sub 0.47/As-In/sub 0.52/Al/sub 0.48/As avalanche photodiode

Low-temperature photon counting with gated mode quenching is demonstrated with separate absorption, charge, and multiplication avalanche photodiodes that have an In/sub 0.52/Al/sub 0.48/As multiplication layer. A minimum of ten dark counts per second and single-photon detection efficiency of 16% were achieved at 130 K.     

High-performance Al/sub 0.48/In/sub 0.52/As/Ga/sub 0.47/In/sub 0.53/As MSM-HEMT receiver OEIC grown by MOCVD on patterned InP substrates

Reports the first demonstration of a new long-wavelength receiver OEIC comprising an AlInAs/GaInAs MSM detector and an AlInAs/GaInAs HEMT preamplifier. The layer structure was grown by LP-MOCVD on patterned InP substrates, which allowed independent optimisation of the MSM detector and HEMT preamplifier. The MSM detector showed the lowest leakage current yet reported and the HEMT exhibited a transconductance of 260 mS/mm. An excellent receiver response to 1.7 Gbit/s NRZ signals has been obtained.<>     

Current instabilities in Ga0.47In0.53As transferred-electron devices

Time-resolved measurements of the device current in Ga0.47In0.53As transferred-electron devices are presented. The current drop, usually attributed to domain nucleation shows an unexpected behaviour because a drop of the device current of up to 90% is observed. This cannot be explained solely by the model of domain formation caused by electron transfer. The influence of transport properties of the central valley is discussed, giving rise to the assumption of its dominant effect on domain nucleation.     

Ultralow leakage In/sub 0.53/Ga/sub 0.47/As p-i-n photodetector grown on linearly graded metamorphic In/sub x/Ga/sub 1-x/P buffered GaAs substrate

A novel top-illuminated In/sub 0.53/Ga/sub 0.47/As p-i-n photodiodes (MM-PINPD) grown on GaAs substrate by using linearly graded metamorphic In/sub x/Ga/sub 1-x/P (x graded from 0.49 to 1) buffer layer is reported. The dark current, optical responsivities, noise equivalent power, and operational bandwidth of the MM-PINPD with aperture diameter of 60 /spl mu/m are 13 pA, 0.6 A/W, 3.4/spl times/10/sup -15/ W/Hz/sup 1/2/, and 7.5 GHz, respectively, at 1550 nm. The performances of the MM-PINPD on GaAs are demonstrated to be comparable to those of a similar device made on InGaAs-InP substrate.     

Dark noise of Ga0.47 In0.53As photoconductive detectors

We have studied the dark noise of planar, interdigitated Ga0.47In0.53As photoconductive detectors by measuring the statistical distribution of the dark current under DC bias. The measurements reveal two interesting results: (i) the probability distribution of the dark current around its DC level is Gaussian and (ii) the standard deviation of the probability distribution grows exponentially with increasing bias voltage. Utilising these data an optimum bias level was calculated to maximise the receiver sensitivity of the detector.