Robert C. Glass
Cree Inc.
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Featured researches published by Robert C. Glass.
Materials Science Forum | 2003
Stephan G. Müller; M.F. Brady; W.H. Brixius; Robert C. Glass; H. McD. Hobgood; Jason Ronald Jenny; R.T. Leonard; David Phillip Malta; Adrian Powell; Valeri F. Tsvetkov; Scott Allen; John W. Palmour; Calvin H. Carter
In this paper we show the progression in the development of semi-insula ti g SiC grown by the sublimation technique from extrinsically doped material to hig h purity semi-insulating (HPSI) 4H-SiC bulk crystals of 2-inch and 3-inch diameter without re sorting to the intentional introduction of elemental deep level dopants, such as vanadium. Secondary ion m ass spectrometry, optical absorption, deep level transient spectroscopy and electron parama gnetic resonance data suggest that the semi-insulating behavior in HPSI material orig inates from deep levels associated with intrinsic point defects. While high temperature resistivity measurements on different high purity 4H-SiC samples indicate activation energies ranging from 0.9 to 1.6 eV, HPSI wafers with homogeneous activation energies near mid-gap are demonstrated. The roomtemperature thermal conductivity of this material approaches the theoretical maximum of ~ 5 W/cmK. Additionally, HPSI substrates exhibit micropipe densities as low as 8 cm -2 over the full diameter of a 3-inch wafer. MESFETs produced on HPSI wafers are free of backgating effects and have resulted in the best combination of power density and efficiency reported to date for SiC M ESFETs of 5.2 W/mm and 63% power added efficiency (PAE) at 3.5 GHz.
Materials Science Forum | 2004
Jason Ronald Jenny; David Phillip Malta; M.R. Calus; Stephan G. Müller; Adrian Powell; Valeri F. Tsvetkov; H. McD. Hobgood; Robert C. Glass; Calvin H. Carter
The next generation of wireless infrastructure will rely heavily upon wide band gap semiconductors owing to their unique materials properties, including: their large bandgap, high thermal conductivity, and high breakdown field. To facilitate implementation of this next generation, a significant effort is required to make SiC MESFET and GaN HEMT microwave devices more suitable for widespread application. Currently, the interest in high-purity semiinsulating (HPSI) 4H-SiC is critically tied to its influence on microwave devices, whether performance or affordability. To address these issues, we have developed high-purity 3-inch and 100 mm 4H-SiC substrates with low micropipe densities (as low as 1.4 cm -2 in 3-inch and <60 cm -2 in 100 mm) and uniform semi-insulating properties (>10 9 Ωcm) over the full wafer diameter. These wafers possess typical residual shallow level contamination less than 1x10 16 cm -3 (5x10 15 nitrogen and 3x10 15 boron) with best nitrogen values of 3x10 14 . In this paper, we will report on the development of our HPSI growth process focusing on the specific areas of the assessment of semiinsulating character and device applicability.
Materials Science Forum | 2004
H. McD. Hobgood; M.F. Brady; M.R. Calus; Jason Ronald Jenny; R.T. Leonard; David Phillip Malta; Stephan G. Müller; Adrian Powell; Valeri F. Tsvetkov; Robert C. Glass; Calvin H. Carter
The quest of driving SiC toward the realization of its full potential as a semiconductor material continues in many organizations world-wide. R&D and manufacturing efforts continue to address issues of scale-up of wafer size, improvements in wafer shape and surface characteristics, reduction of background impurities in bulk crystals, controlled uniformity of electrical properties, and reduction and control of crystalline defects. Significant progress has been made in several key areas. Increased manufacturing activity in the production of 3-inch diameter crystals has led to substrates with micropipes densities <30 cm -2 in n-type and <80 cm -2 in semi-insulating material, and R&D demonstrations of substrates exhibiting micropipe densities <0.5 cm -2 in n-type and <5 cm -2 in semi-insulating wafers. Developmental 100-mm diameter substrates exhibiting micropipe densities <60 cm -2 in both n-type and semi-insulating materials have now been demonstrated. Significant improvement in bulk crystal purity has been achieved with reduction of impurity concentrations below 5 x 10 15 cm -3 .
Materials Science Forum | 2004
Adrian Powell; R.T. Leonard; M.F. Brady; Stephan G. Müller; Valeri F. Tsvetkov; R. Trussell; Joseph J. Sumakeris; H. McD. Hobgood; Albert A. Burk; Robert C. Glass; Calvin H. Carter
The SiC power device market is predicted to grow exponentially in the next few years. In the development of substrates for this emerging commercial market, it is imperative to develop the product to meet the needs of the targeted application. In this paper we will discuss the status and requirements for SiC substrates for power devices such as Schottky and PiN diodes. For example, for the SiC Schottky device where current production is approaching 50 amp devices, there are several substrate material aspects that are key. These include: wafer diameter (3-inch and 100 mm), micropipe density (<1cm -2 for 3-inch substrates and as low as 30cm -2 for 100-mm substrates), dislocation density, and wafer cost.
MRS Proceedings | 2004
Adrian Powell; Joseph J. Sumakeris; R.T. Leonard; M.F. Brady; S. Müller; Valeri F. Tsvetkov; H. McD. Hobgood; Albert A. Burk; Michael James Paisley; Robert C. Glass; Calvin H. Carter
The performance enhancements offered by the next generation of SiC high power devices offer potential for enormous growth in SiC power device markets in the next few years. For this growth to occur, it is imperative that substrate and epitaxial material quality increases to meet the needs of the targeted applications. We will discuss the status and requirements for SiC substrates and epitaxial material for power devices such as Schottky and PiN diodes. For the SiC Schottky device where current production is approaching 50 amp devices, there are several material aspects that are key. These include; wafer diameter (3-inch and 100-mm), micropipe density ( −2 for 3-inch substrates and 16 cm −2 for 100-mm substrates), epitaxial defect densities (total electrically active defects −2 ), epitaxial doping and epitaxial thickness uniformity. For the PiN diodes the major challenge is the degradation of the Vf characteristics due to the introduction of stacking faults during the device operation. We have demonstrated that the stacking faults are often generated from basal plane dislocations in the active region of the device. Additionally we have demonstrated that by reducing the basal plane dislocation density, stable PiN diodes can be produced. At present typical basal plane dislocation densities in our epitaxial layers are 100 to 500 cm −2 ; however, we have achieved basal plane dislocation densities as low as 4 cm −2 in epitaxial layers grown on 8° off-axis 4H-SiC substrates.
Archive | 2002
David B. Slater; Robert C. Glass; Charles M. Swoboda; Bernd Keller; James Ibbetson; Brian Thibeault; Eric Tarsa
Archive | 2002
David B. Slater; Robert C. Glass; Charles M. Swoboda; Bernd Keller; James Ibbetson; Brian Thibeault; Eric Tarsa
Archive | 2004
David B. Slater; Robert C. Glass; Charles M. Swoboda; Bernd Keller; James Ibbetson; Brian Thibeault; Eric Tarsa
Materials Science Forum | 2000
H. McD. Hobgood; M.F. Brady; W.H. Brixius; George John Fechko; Robert C. Glass; D. Henshall; Jason Ronald Jenny; Robert Tyler Leonard; David Phillip Malta; Stephan G. Müller; Valeri F. Tsvetkov; Calvin H. Carter
Archive | 1997
Calvin H. Carter; Valeri F. Tsvetkov; Robert C. Glass