Ohmic Contacts to Gallium Aluminum Arsenide for High Temperature Applications


Book Description

A new approach for fabricating nonalloyed ohmic contacts to gallium arsenide was developed. The approach uses ultrathin layers of heavily doped germanium or silicon in contact with gallium arsenide to alter the Schottky barrier height(phi B) at the gallium arsenide interface. For n-type gallium arsenide phi B could be varied from about 0.3 to 1.0 eV. The low barriers are useful for tunneling ohmic contacts to n-gallium arsenide while the high barriers should be useful for p-gallium arsenide ohmic contacts and for Field Effect Transistor (FET) gate applications. In some instances it was necessary to interpose a thin nonmetallic electrically conducting barrier between the contact metal and the thin germanium or silicon layer to preserve optimum contact properties. Specific contact resistivity measurements indicated that contact resistivity




Ohmic Contracts to Gallium Aluminum Arsenide for High Temperature Applications


Book Description

A method of modifying the Gallium Arsenides (100) interface Fermi level position (EF) has been investigated. For tunnel ohmic contacts the contact resistance depends exponentially on the energy difference between the conduction band minimum and EF; thus, stable contacts with small values of this energy difference (large values of EF) could be important in designing nonalloyed ohmic contacts. Very thin (approx. 10A) epitaxial layers of Gallium that incorporate Arsenic have been found to produce exceptionally large values of EF, 1.0-1.2 eV relative to the valence band maximum (as determined by x-ray photoelectron spectroscopy). Thick model contacts that include layered structures of Au, Ge, and Ni in various combinations have been used to establish conditions under which these large EF values can be preserved (as determined by current-voltage measurements). The results question the usual assumption of a near mid-gap EiF position for the widely used alloyed AuGeNi ohmic contact and offer an alternative explanation for the mechanism of ohmic contact formation.
















Materials for High-Temperature Semiconductor Devices


Book Description

Major benefits to system architecture would result if cooling systems for components could be eliminated without compromising performance. This book surveys the state-of-the-art for the three major wide bandgap materials (silicon carbide, nitrides, and diamond), assesses the national and international efforts to develop these materials, identifies the technical barriers to their development and manufacture, determines the criteria for successfully packaging and integrating these devices into existing systems, and recommends future research priorities.







Demand Bibliography


Book Description




Ohmic Contact to Ion Implanted Gallium Arsenide Antimonide for Application to Indium Aluminum Arsenide/Gallium Arsenide Antimonide Heterostructure Insulated-Gate Field Effect Transistors


Book Description

The p-channel In(0.52)Al(0.48)As/GaAs(1-x)Sb(x) heterostructure insulated-gate field effect transistor (p-HIGFET) is a candidate for complementary integrated circuits due to superior cutoff characteristics and low gate leakage current. Advancement of the In(0.52)Al(0.48)As/GaAs(1-x)Sb(x) p-HIGFET requires improved source/drain design. Five main tasks were accomplished to achieve this goal. First, thermal limits of the In(0.52)Al(0.48)As/GaAs(0.51)Sb(0.49) HIGFET were investigated. Second, the temperature dependence of band gap and impurity energies were determined for beryllium doped GaAs(0.51)Sb(0.49). Third, high acceptor concentrations were obtained on GaAs(1-x)Sb(x) using beryllium ion implantation. Fourth, Au/Zn/Au and Ti/Pt/Au were compared as ohmic contact metallizations to these highly doped layers. Finally, In(0.52)Al(0.48)As/GaAs(0.51)Sb(0.49) HIGFETs were fabricated and characterized using Ti/Pt/Au metallization and Be implantation. An array of characterization methods were employed to thoroughly characterize materials and devices including: transmission line measurements (TLM), electrochemical profiling, photoluminescence (PL), atomic force microscopy (AFM), secondary ion mass spectroscopy (SIMS), Auger electron spectroscopy (AES), X-ray diffraction (XRD), cross-sectional transmission electron microscopy (XTEM), selected area diffraction (SAD) and energy dispersive X-ray analysis (EDX). jg p.25.