In Situ SEM Observations and Electrical Measurements During the Annealing of Si/Ni Contacts to SiC

2003 ◽  
Vol 764 ◽  
Author(s):  
Matthew H. Ervin ◽  
Kenneth A. Jones ◽  
Michael A. Derenge ◽  
Tsvetanka S. Zheleva ◽  
Mark C. Wood

AbstractNickel (Ni) contacts to n-type silicon carbide (n-SiC) are annealed to ∼950°C in order to achieve their good ohmic properties through the reaction of the Ni with Si from the SiC to form nickel silicides. Unfortunately, the physical contact, and therefore the reliability, is poor. A possible cause is that the silicidation reaction liberates C from the SiC, which then diffuses throughout the contact. The reaction also produces a poor morphology and voids form at the metal-SiC interface. To try to understand the processes that produce the good electrical properties and at the same time improve the physical properties, we studied the reactions of Si/Ni contacts with 1:1 and 1:2 stoichiometric ratios as well as Ni-only contacts on n- and p-type SiC, both visually and electrically in situ using a hot stage and microprobe-equipped scanning electron microscope (SEM). The visual observations of the Ni-only film show that it does not react with the SiC until the temperature reaches 500–550°C. For the n-type SiC, the electrical measurements show a decrease in contact resistivity as the anneal temperature is increased from 500°C to 650°C. Increasing the anneal temperature further increases the resistivity until it begins to drop precipitously as the temperature approaches 950°C and higher. The visual observations of the Si/Ni contacts show that the Si and Ni are reacting at ∼600°C, with phases nucleating and then growing laterally. The electrical measurements for the n-type samples show that the contact resistance initially drops at 100–300°C indicating that there may be reactions, unseen by the SEM, at lower temperatures. The resistance continues to rise and fall over the intervening temperatures but begins to consistently and significantly fall at temperatures above 850°C, and then reaches ohmic values at 900–950°C. Because the silicidation reactions are seen to occur at temperatures far below those required to achieve ohmic properties, it is clear that silicide formation, while it may be necessary, is not sufficient for the formation of Ni-ohmic contacts to n-SiC. In this work, it has been observed that reaction of the Ni with the SiC appears to be necessary for achieving ohmic properties. While this may form a more intimate contact, it is proposed that damaging the SiC surface with this reaction is an important part of ohmic contact formation, possibly through increased current tunneling through interface defect states.

1993 ◽  
Vol 318 ◽  
Author(s):  
Patrick W. Leech ◽  
Geoffrey K. Reeves

ABSTRACTOhmic contacts to p-type InP with an In0.47Ga0.53As buffer layer and an interposed superlattice of 50 Å In0.47Ga0.53As/ 50 Å InP have been investigated. Initial studies of contacts to In0.47Ga0.53As/ InP without the superlattice structure have shown that Pd/Zn/Pd/Au metallization produced a lower specific contact resistance (pc = 1.1 × 10−4 Ω cm2) than Pd/Ge/Au, and over a wider range of anneal temperature than Au/Zn/Au. The incorporation of the superlattice in the p-In0.47Ga0.53As/ InP structure resulted in Pd/Zn/Pd/Au contacts with pc of 3.2 × 10−5 Ω cm2 as-deposited and 7.5 × 10−6 Ω.cm2 after a 500 °C anneal. The presence of Pd/Zn in the metallization was shown as important in reducing pc. Significant intermixing of the metal layers and In0.47Ga0.53As occured at ≥ 350 °C, as revealed by Rutherford backscattering spectrometry.


2004 ◽  
Vol 815 ◽  
Author(s):  
Z. Tian ◽  
N.R. Quick ◽  
A. Kar

AbstractLaboratory prototype SiC diodes are fabricated using a combination of gas immersion laser doping (GILD) and laser direct write (LDW) in situ metallization in a commercial SiC wafer. Trimethylaluminum (TMA) and nitrogen are the precursors used to produce p-type and n-type SiC, respectively. Using these techniques, a 150 nm p-type doped junction is fabricated in semiinsulating 6H-SiC and n-doped 4H-SiC wafers. Ohmic contacts are created by laser direct metallization producing carbon rich conductive phases in these doped materials. Alternatively an excimer laser can be used to create silicon rich Schottky contacts. The geometry of the diodes can be vertical or planar to the wafer surface and the laser processes are thought to reduce defect densities in the irradiated areas. These laser-processed diodes are intended for use in high temperature, high voltage and high frequency switching and sensing applications.


2001 ◽  
Vol 680 ◽  
Author(s):  
Agustinus Sutandi ◽  
P. Paul Ruden ◽  
Kevin F. Brennan

ABSTRACTThe physics of bulk wurtzite-structure III-nitride materials and of III-nitride heterostructures includes many phenomena that can be modulated by the application of stress. In particular, p- type material is expected to display a rich variety of piezo-resistive and piezo-optic effects that originate from the stress-induced modulation of lattice polarization charges, of valence band energies, and of bulk, surface, and interface defect states in the band gap. Here we focus on the expected effects of in-plane uniaxial on p-channel AlGaN/GaN heterostructures grown along the hexagonal axis on sapphire substrates. The valence band structure in the channel region is calculated self-consistently in the framework of a six-band Rashba-Sheka-Pikus (RSP) Hamiltonian. Stress-effects are included (in linear elastic theory) through deformation potentials and through the modulation of interfacial polarization charges associated with the piezoelectric nature of the constituent materials.


1995 ◽  
Vol 382 ◽  
Author(s):  
M.W. Cole ◽  
W.Y. Han ◽  
K.A. Jones

ABSTRACTInterfacial microstructure and phase composition of PtTiGePd ohmic contacts to heavily C doped AlGaAs were investigated as a function of annealing temperature. Results of the material analyses were used to explain the specific contact resistances measured for each thermal treatment. Evidence of interdiffusion and compound formation between AIGaAs and Pd was visible in a Ga rich Pd-Ga-As reaction zone prior to heat treatment. This phase is critical for the formation of Ga vacancies, which upon heating are occupied by in-diffusing Ge. As the annealing temperature was elevated, from 530 - 600°C, As began to out-diffuse. This As out-diffusion, which is critical to the formation of good p-type ohmic contacts, contributed to the creation and development of the two phase TiAs/Pd12Ga2Ge5 interfacial region overlying the AlGaAs substrate. In response to the enhanced As out-diffusion at 600°C, the interfacial region became laterally continuous, compositionally uniform, and the specific contact resistance achieved its minimum value. Athigher annealing temperatures, ∼650°C, the electrical measurements degraded in response to intensive chemical diffusion and development of a broad, non-uniform multi-phased interfacial region.


2010 ◽  
Vol 645-648 ◽  
pp. 729-732 ◽  
Author(s):  
Bang Hung Tsao ◽  
Jacob W. Lawson ◽  
James D. Scofield ◽  
Javier Francisco Baca

Improved AlNi-based ohmic contacts to p-type 4H-SiC have been achieved using low energy ion (Al+)implantation, the addition of a thin Ti layer, and a novel two-step implant activation anneal process. AlNi/Au contacts with and without Ti were studied, which resulted in contact resistivities around 1.8x10-4 -cm2 and 2.0x10-3 -cm2 respectively. Even though these values were higher than those of the Ti/AlNi/W system, which was the focus of previous studies, the reduced anneal temperature (650 to 700°C) implies that Ti/AlNi/Au is a promising composite configuration. Cross-sectional TEM and EDX were used to investigate the interfacial structure of the contacts. One possible mechanism for the improved ohmic contact behavior is that the addition of Au and Ti resulted in a reduction barrier height.


1989 ◽  
Vol 148 ◽  
Author(s):  
N. Newman ◽  
W.E. Spicer ◽  
E.R. Weber ◽  
Z. Liliental-Weber

We have carried out a systematic study of the electrical properties of Schottky barriers formed on atomically-clean and contaminated n-type and p-type GaAs surfaces[1-11]. Diodes were fabricated by in-situ deposition on clean GaAs (110) surfaces prepared by cleavage in ultrahigh vacuum and on contaminated surfaces prepared by cleavage and exposure to the atmosphere[1-4]. The consistent and reproducible barrier height determinations from the electrical measurements of unannealed and annealed diodes, when combined with results of transmission electron microscopy (TEM)[5,6] and surface sensitive studies on identically prepared samples[7,8], are found to be a particularly critical test of models of Schottky barrier formation. A strong correlation between annealing-induced changes in the Schottky barrier height and the stoichiometry of the near interfacial GaAs is found.


2006 ◽  
Vol 911 ◽  
Author(s):  
Bang-Hung Tsao ◽  
Jacob Lawson ◽  
James Scofield

AbstractImproved AlNi-based ohmic contacts to p-type 4H-SiC have been achieved using low energy ion (Al+) implantation, the addition of a thin Ti layer, and a novel two-step implant activation anneal process. Resistivities sometimes as low as 5×10−5 Ω-cm2 were reached by doping the surface region of lightly p-doped 4H-SiC epilayers via low energy Al+ implantation. Acceptor activation was achieved by annealing the samples with a 1400+1700°C two-step sequence in an Ar atmosphere, which also yielded improved surface morphology when implanted samples were capped with photo resist during the anneals. In this study, Ti/AlNi/W contacts on implanted layers were compared to Ti/AlNi/Au contacts. Even though the resistivities are higher than those of the Ti/AlNi/W system, the reduced anneal temperature, 650°C for Ti/AlNi/Au compared to 950°C for Ti/AlNi/W implies that Ti/AlNi/Au is a promising stacking configuration. Furthermore, the effects of a longer 30 minute anneal time at 600 − 700°C, in atmospheric pressure Ar ambients was observed. Namely, the 2 minute annealing cycle used for the Ti/AlNi/W study resulted in higher anneal temperatures before ohmic characteristics were seen. This same anneal time was not sufficient for the Ti/AlNi/Au samples, whereas increasing the cycle time to 30 minutes resulted in ohmic behavior at a much lower temperature. Increasing the anneal time however, had little or no impact on reducing the required anneal temperature of the Ti/AlNi/W.


2000 ◽  
Vol 637 ◽  
Author(s):  
Agustinus Sutandi ◽  
P. Paul Ruden ◽  
Kevin F. Brennan

AbstractThe physics of bulk wurtzite-structure III-nitride materials and of III-nitride heterostructures includes many phenomena that can be modulated by the application of stress. In particular, p-type material is expected to display a rich variety of piezo-resistive and piezo-optic effects that originate from the stress-induced modulation of lattice polarization charges, of valence band energies, and of bulk, surface, and interface defect states in the band gap. Here we focus on the expected effects of in-plane uniaxial on p-channel AlGaN/GaN heterostructures grown along the hexagonal axis on sapphire substrates. The valence band structure in the channel region is calculated self-consistently in the framework of a six-band Rashba-Sheka-Pikus (RSP) Hamiltonian. Stress-effects are included (in linear elastic theory) through deformation potentials and through the modulation of interfacial polarization charges associated with the piezoelectric nature of the constituent materials.


Author(s):  
Georgia Andra Boni ◽  
Cosmin M. Istrate ◽  
Christina Zacharaki ◽  
Polychronis Tsipas ◽  
Stefanos Chaitoglou ◽  
...  

2006 ◽  
Vol 957 ◽  
Author(s):  
Gary S. Tompa ◽  
S. Sun ◽  
C. E. Rice ◽  
L. G. Provost ◽  
D. Mentel

ABSTRACTZnO thin films are of interest for an array of applications; including: light emitters, photovoltaics, sensors and transparent contacts among others. Of particular interest is the potential to produce p-type layers from which p-n junction devices could be routinely produced. While it is fairly routine for MOCVD to produce n-type films with doping concentrations in the 10E20 cm-3 range and resistivities below 10E-3 ohm-cm; it is very difficult to produce measurable p-type ZnO. We report on our efforts with doping films p-type using N gas sources and metalorganic sources of P, As, and Sb. Films showing acceptor bands by photoluminescence have been demonstrated; however reliable electrical measurements remain difficult. Specific problems include achieving low resistance ohmic contacts, accounting for the photo-responsiveness of ZnO films and sensitivity limits in Hall measurements of low-doped and compensated materials. The presentation will review deposition parameters, produced and processed films and material characteristics.


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