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Materials Science Forum Vols. 527-529
Paper Title Page
Abstract: Dislocations were tracked from 4H-SiC epilayer to the substrate by a new method based
on combination of molten KOH etching and Reactive Ion Etching. It was found that basal plane
dislocations (BPDs) with dislocation lines parallel (or approximately parallel) to the off-cut
direction might propagate as BPDs into the epilayer, while those with dislocation lines forming
large angles (>10º) with the off-cut direction will get converted to threading edge dislocations
(TEDs). A model is proposed to explain the observations.
419
Abstract: Propagations of dislocations in 4H-SiC were evaluated three-dimensionally by a planar
mapping EBIC method with the control of accelerating voltages. Screw dislocation (SD), edge
dislocation (ED), and basal plane dislocation (BPD) were clearly observed through the 20nm-thick
Ni Schottky contact on SiC. From the analysis of BPD extended on {0001}, the intensity of EBIC
signals was proportional to the depth position of defect. In addition, the information of the
decomposition and combination for dislocations can be obtained from the fluctuation of EBIC signal
along the scanning position.
423
Abstract: In this work, we investigated the effect of crystal defects on reverse I-V characteristics of
avalanche photodiodes (APDs) using electron-beam induced current (EBIC) mode of SEM. Two
types of SiC APD structures (I and II) were fabricated using 2 inch p-doped substrates with n-doped
epilayers and 3 inch n-doped substrates with p- and n- epilayers. Areas of the formed diodes were
approximately 1 mm2. The devices without any kind of electrically active 3-D structural defects
demonstrated breakdown voltages close to theoretical values, ~500 V for the APD Type I and
~1200 V for Type II APD. Stability of Type I devices was tested by applying a short pulse of high
voltage (~800 V). EBIC images, taken prior to and after the failure test, showed new defects in the
dislocation free area, which, presumably, were caused by thermal breakdown.
427
Abstract: 3C-SiC p-type epilayers were grown to thicknesses of 1.5, 3, 6 and 10 μm on 2.5° off-axis
Si(001) substrates by chemical vapor deposition (CVD). Silane and propane were used as precursors.
Structural analysis of epilayers was performed using transmission electron microscopy (TEM),
high-resolution x-ray diffractometry (HRXRD), and Raman spectroscopy. TEM showed defect
densities (stacking faults, twins and dislocations) decreasing with increasing distance from the SiC/Si
interface as the lattice mismatch stress is relaxed. This observation was corroborated by a monotonic
decrease in HRXRD peak width (FWHM) from 780 arcsecs (1.5 μm thick epilayer) to 350 arcsecs (10
μm thick epilayer). Significant further reduction in x-ray FWHM is possible because the minimum
FWHM detected is greater than the theoretical FWHM for SiC (about 12 arcsecs). Raman
spectroscopy also indicates that the residual biaxial in-plane strain decreases with increasing epilayer
thickness initially, but becomes essentially constant between 6 and 10 μm. Structural defect density
shows the most significant reduction in the first 2 μm of growth. Phosphorus implantation was used
to generate n+/p junctions for the measurement of the critical electric field in 3C-SiC. Based on
current-voltage analyses, the critical electric field in p-type 3C-SiC with a doping of 2x1017 cm-3 is
1.3x106 V/cm.
431
Abstract: Recently, in some silicon carbide single crystals, some micropipes associated with
screw dislocation have been observed by X-ray topography and the strain field around them
produced images similar to those of screw dislocations with a very large Burgers vector, about
667 nm. The radius of the hole in the centre of the micropipe is less than 10 'm. This value
and the theoretical predictions by Frank (about 7.8 mm) using the Burgers vector magnitude
show a large discrepancy. In this paper we present Atomic Force Microscopy experiments
around this kind of defects. The Burgers vector magnitude of the screw dislocation and the
value of the radius have been measured by this technique. Not only one dislocation, but
several have been observed around the micropipe. We concluded that it is in better agreement
with the Frank theory modified by Cabrera and Levine concerning kinetic effects during the
growth.
435
Abstract: More than fifty years ago Frank proposed that a dislocation with a Burgers vector larger
than a critical value would have an open core. Since then, there has been controversy as to whether
micropipes in SiC are examples of open core screw dislocations. In this work open core dislocations
in 4H-SiC material are investigated by AFM. The results are interpreted on the basis of Frank’s
theory and the surface energy of SiC is estimated from the critical value of Burgers vector. Finally,
the extracted surface energy is compared with the results of other research.
439
Abstract: Micropipe density (MPD) is a crucial parameter for silicon carbide (SiC) substrates
that determines the quality, stability and yield of the semiconductor devices built on these
substrates. The importance of MPD is underscored by the fact that all existing specifications for
6H- and 4H-SiC substrates set upper limits for it. Several methods for measuring the MPD are
known, however, their reliability and applicability to various types of substrates (e.g. semiinsulating,
conducting, etc.) has not been systematically studied.
The subject of this paper is a comparative study of various techniques used for the MPD
measurement accompanied by statistical analysis of the results. The study was initiated by several
organizations working in the immediate field of silicon carbide or in closely related fields and
included SiC substrate manufacturers, substrate consumers, equipment manufacturers and
universities. The study represented a round robin experiment in which MPD was measured on
thirty SiC wafers of various pedigrees. The values of MPD have been determined using both
destructive and non-destructive techniques. The repeatability of each technique is analyzed and
compared with that of other techniques.
443
Abstract: Micropipes are considered to be a major device killer in SiC wafers. Developing a
method to count and map micropipes efficiently and accurately has been a challenging task to date.
In this work, a new method based on KOH etching and full wafer, high resolution digital imaging is
developed to map and count micropipes in both conductive and semi-insulating SiC wafers. This
method is also compared with a non-destructive method based on laser light scattering and a good
agreement between the two methods is demonstrated.
447
Abstract: 4H-SiC single crystal with a diameter of 1.5’’ has been grown by the seed sublimation
method. Regions of mixed polytypes are assessed by high resolution X-ray diffractometry with the
asymmetrical diffraction geometry. Multiple reflections are observed from the rocking curve
measurements of a longitudinal cut 4H-SiC slice. Those reflections are indexed to be 2131 and
2131 of 4H-SiC, 2130 , 2131 , 2131 , 2132 and 2132 of 6H-SiC, 2131 , 2132 , 2134 , 2135 and
2137 of 15R-SiC respectively based on the lattice constants of different polytypes in SiC crystal. It
is believed that the polytypes can be identified by high resolution X-ray diffractometry.
451
Abstract: Semi-insulating SiC grown by the HTCVD technique are studied by luminescence and
absorption measurements and the results are compared to PAS and SIMS results. We have found
that metal impurities are present but only in very small concentrations. The semi-insulating
properties are instead determined by the intrinsic defects, mostly the silicon vacancy in hydrocarbon
rich grown material and the carbon vacancy in the hydrocarbon poor grown material. The
hydrocarbon poor material is stable upon annealing both from a vacancy concentration point of view
and from a resistivity point of view. The hydrocarbon rich grown material does not stand the
annealing at 1600 °C and the resistivity is decreased; from the absorption and PAS measurements
we have observed that the decrease in silicon vacancy concentration fits the growth of the vacancy
clusters.
455