Pulsed Ion-Beam Induced Reactions of Ni And Co With Amorphous and Single Crystal Silicon

1984 ◽  
Vol 35 ◽  
Author(s):  
J. O. Olowolafe ◽  
R. Fastow
Keyword(s):  
Amorphous Silicon ◽  
Ion Beam ◽  
Single Crystal Silicon ◽  
Reaction Rates ◽  
Rutherford Backscattering ◽  
Thin Layers ◽  
X Ray Diffraction ◽  
Furnace Annealing ◽  
Crystal Silicon ◽  
Transmission Electron

ABSTRACTThin layers (~1,000 A ) of Ni and Co have been reacted with both (100) and amorphous silicon (a-Si) using a pulsed ion beam. Samples were analyzed using Rutherford backscattering, x-ray diffraction, and transmission electron microscopy. Rutherford backscattering showed that the metal/a-Si and metal/(100)-Si reaction rates were comparable. Both reactions began at the composition of the lowest eutectic. For comparison. furnace annealing of the same structures showed that the reaction rate of Ni with amorphous silicon was greater than with (100) Si; Co reacted nearly identically with both substrates. Diffraction data suggest that pulsed ion beam annealing crystallizes the amorphous silicon before the metal/a-Si reaction begins.

Single Crystal Silicon Carbide On Silicon Using A Supersonic Gas Jet Of Methylsilane

1997 ◽  
Vol 483 ◽  
Author(s):  
S. A. Ustin ◽  
C. Long ◽  
L. Lauhon ◽  
W. Ho
Keyword(s):  
Growth Rate ◽  
Growth Rates ◽  
Single Crystal Silicon ◽  
Maximum Growth ◽  
X Ray Diffraction ◽  
Crystal Silicon ◽  
Cross Sectional ◽  
Supersonic Molecular Beam ◽  
Transmission Electron

AbstractCubic SiC films have been grown on Si(001) and Si(111) substrates at temperatures between 600 °C and 900 °C with a single supersonic molecular beam source. Methylsilane (H3SiCH3) was used as the sole precursor with hydrogen and nitrogen as seeding gases. Optical reflectance was used to monitor in situ growth rate and macroscopic roughness. The growth rate of SiC was found to depend strongly on substrate orientation, methylsilane kinetic energy, and growth temperature. Growth rates were 1.5 to 2 times greater on Si(111) than on Si(001). The maximum growth rates achieved were 0.63 μm/hr on Si(111) and 0.375μm/hr on Si(001). Transmission electron diffraction (TED) and x-ray diffraction (XRD) were used for structural characterization. In-plane azimuthal (ø-) scans show that films on Si(001) have the correct 4-fold symmetry and that films on Si(111) have a 6-fold symmetry. The 6-fold symmetry indicates that stacking has occurred in two different sequences and double positioning boundaries have been formed. The minimum rocking curve width for SiC on Si(001) and Si(111) is 1.2°. Fourier Transform Infrared (FTIR) absorption was performed to discern the chemical bonding. Cross Sectional Transmission Electron Microscopy (XTEM) was used to image the SiC/Si interface.

Synthesis and Selected Micro-Mechanical Properties of Titanium Nitride Thin Films by the Pyrolysis of Tetrakis Titanium in Ammonia.

1994 ◽  
Vol 363 ◽  
Author(s):  
Y. W. Bae ◽  
W. Y. Lee ◽  
T. M. Besmann ◽  
P. J. Blau ◽  
L. Riester
Keyword(s):  
Thin Films ◽  
Titanium Nitride ◽  
Electron Spectroscopy ◽  
Single Crystal Silicon ◽  
Chemical Vapor ◽  
Silicon Substrates ◽  
X Ray Diffraction ◽  
Crystal Silicon ◽  
Transmission Electron ◽  
Chemical Vapor Deposited

AbstractThin films of titanium nitride were chemical vapor deposited on (100)-oriented single-crystal silicon substrates from tetrakis (dimethylamino) titanium, Ti((CH3)2N)4, and ammonia gas mixtures in a cold-wall reactor at 623 K and 655 Pa. The films were characterized by Auger electron spectroscopy, X-ray diffraction, and transmission electron spectroscopy. The nano-scale hardness of the film, measured by nanoindentation, was 12.7±0.6 GPa. The average kinetic friction coefficient against unlubricated, type- 440C stainless steel was determined using a computer-controlled friction microprobe to be ∼0.43.

Epitaxial Silicon-Carbon Alloy Growth by Laser Induced Melting and Solidification

1995 ◽  
Vol 398 ◽  
Author(s):  
Kenneth M. Kramer ◽  
Michael O. Thompson
Keyword(s):  
Single Crystal ◽  
Secondary Ion Mass Spectrometry ◽  
Single Crystal Silicon ◽  
Epitaxial Silicon ◽  
X Ray Diffraction ◽  
Crystal Silicon ◽  
Silicon Carbon ◽  
Transmission Electron ◽  
Excimer Laser Irradiation ◽  
Secondary Ion

ABSTRACTIon implantation of carbon into single-crystal silicon followed by excimer laser irradiation was used to create supersaturated, epitaxial SixC1-x. films. Crystallization proceeded from the underlying single-crystal silicon through the carbon containing layers at velocities of approximately 5 m/s. Characterization by high-resolution x-ray diffraction and Fourier-transform infrared absorption indicate that the carbon is found predominantly on substi-tutional lattice sites for concentrations up to 1.4 at.% C. Secondary-ion mass spectrometry profiles and numerical mass transfer calculations were used to estimate the diffusion coefficient of carbon in the liquid as 2-3 × 10−4cm2/s with a segregation coefficient greater than 0.4. Unusual diffusion behavior was observed for the carbon at 1.4 at.% C. At higher concentrations, evidence of SiC precipitates was observed in transmission electron microscope images and FTIR absorption spectra.

Recrystallization of Amorphous Silicon Using Rapid Thermal Processing, Laser Annealing and Furnace Heating

1994 ◽  
Vol 342 ◽  
Author(s):  
J. Viatella ◽  
R.K. Singi ◽  
R.P.S. Thiakur ◽  
G. Sandhu ◽  
S.D. Harkness
Keyword(s):  
Amorphous Silicon ◽  
Laser Annealing ◽  
Laser Wavelength ◽  
X Ray Diffraction ◽  
Incoherent Light ◽  
Furnace Annealing ◽  
X Ray ◽  
Pulsed Laser Annealing ◽  
Conventional Furnace ◽  
Transmission Electron

ABSTRACTRecrystallization of amorphous silicon has been investigated using conventional furnace annealing, incoherent light-based rapid thermal annealing (RTA) and pulsed laser annealing using excimner laser (wavelength=248 nm, energy density = 0.1−0.6 J/cm2) at a pulse width of approximately 20 nanoseconds. The effects of annealing methods are characterized for grain growth and crystallized orientation using transmission electron microscopy (TEM) and X-ray diffraction analysis. The various recrystallization methods are compared based on the structural properties of the resulting film and optimized thermal budgets for each heating mechanism are discussed.

An Epitaxial Si/insulator/Si Structure Prepared by Vacuum Deposition of CaF2 and Silicon

1981 ◽  
Vol 10 ◽  
Author(s):  
T. Asano ◽  
H. Ishiwara
Keyword(s):  
Substrate Temperature ◽  
Silicon Film ◽  
Single Crystal Silicon ◽  
Rutherford Backscattering ◽  
Film Deposition ◽  
Silicon Substrates ◽  
Optimum Conditions ◽  
Crystal Silicon ◽  
Transmission Electron ◽  
Substrate Temperatures

Heteroepitaxial CaF2/Si and Si/CaF2/Si structures were prepared by conventional vacuum evaporation of CaF2 and silicon onto silicon substrates. The optimum conditions for obtaining good epitaxial films were investigated by changing the silicon substrate orientation, the film thickness and the substrate temperature during film deposition. From Rutherford backscattering and channelling spectroscopy it was found that CaF2 films with excellent film quality were obtained on Si(111), Si(110) and Si(100) substrates at substrate temperatures of 600– 800°C, 800°C and 500–600°C respectively. It was also found from Rutherford backscattering and channelling spectroscopy and from transmission electron microscopy that single-crystal silicon films are formed on a CaF2/Si(111) structure at a substrate temperature of 700°C. From measurements of the electrical properties of the top silicon film after the implantation of phosphorus ions at 2 ×1015 cm−2 and subsequent annealing at 750°C, an electron Hall mobility of 69cm2 V−1 s−1 was obtained.

Furnace and Rapid Thermal Annealing of P–Implanted Silicon for Solar Cell Fabrication

1985 ◽  
Vol 45 ◽  
Author(s):  
H.B. Harrison ◽  
Y.H. Lee ◽  
A. Pogany ◽  
M.J. Kenny
Keyword(s):  
Light Source ◽  
Void Formation ◽  
Single Crystal Silicon ◽  
Incoherent Light ◽  
Furnace Annealing ◽  
Crystal Silicon ◽  
Transmission Electron ◽  
Cell Fabrication ◽  
Isothermal Mode ◽  
Initial Results

ABSTRACTSingle crystal silicon has been implanted with low energy (20 keV) phosphorus ions and a comparison made of furnace annealing (which produces excellent solar cells) and rapid annealing using a radiant incoherent light source. The light source is used to anneal and activate implanted layers in the isothermal mode on a time scale of the order of seconds compared with the much longer furnace annealing times of several hours.Initial results using the incoherent light source show a high dark current and inferior photoresponse. However a subsequent thermal treatment at 600°C for 10–15 minutes shows that the resultant photoresponse can approach that of the longer time furnace anneal. Transmission electron microscopy shows the formation of large voids (20–100 nm) after the initial annealing phase. These reduce in size after furnace annealing. This photoresponse may be related to this void formation.

TEM characterization of Au/Polysilicon interactions

1990 ◽  
Vol 48 (4) ◽  
pp. 650-651
Author(s):  
N. David Theodore ◽  
Leslie H. Allen ◽  
C. Barry Carter ◽  
James W. Mayer
Keyword(s):  
Solid Phase ◽  
Single Crystal Silicon ◽  
Chemical Vapor ◽  
Electrical Contacts ◽  
Silicon Substrates ◽  
Crystal Silicon ◽  
Transmission Electron ◽  
Polysilicon Films ◽  
The Stability

Metal/polysilicon investigations contribute to an understanding of issues relevant to the stability of electrical contacts in semiconductor devices. These investigations also contribute to an understanding of Si lateral solid-phase epitactic growth. Metals such as Au, Al and Ag form eutectics with Si. reactions in these metal/polysilicon systems lead to the formation of large-grain silicon. Of these systems, the Al/polysilicon system has been most extensively studied. In this study, the behavior upon thermal annealing of Au/polysilicon bilayers is investigated using cross-section transmission electron microscopy (XTEM). The unique feature of this system is that silicon grain-growth occurs at particularly low temperatures ∽300°C).Gold/polysilicon bilayers were fabricated on thermally oxidized single-crystal silicon substrates. Lowpressure chemical vapor deposition (LPCVD) at 620°C was used to obtain 100 to 400 nm polysilicon films. The surface of the polysilicon was cleaned with a buffered hydrofluoric acid solution. Gold was then thermally evaporated onto the samples.

scholarly journals The Influence of Wire Speed on Phase Transitions and Residual Stress in Single Crystal Silicon Wafers Sawn by Resin Bonded Diamond Wire Saw

Micromachines ◽  
2021 ◽  
Vol 12 (4) ◽  
pp. 429
Author(s):  
Tengyun Liu ◽  
Peiqi Ge ◽  
Wenbo Bi
Keyword(s):  
Residual Stress ◽  
Surface Layer ◽  
Phase Transitions ◽  
Single Crystal ◽  
Amorphous Silicon ◽  
Silicon Wafer ◽  
Single Crystal Silicon ◽  
Silicon Wafers ◽  
Crystal Silicon ◽  
Diamond Wire

Lower warp is required for the single crystal silicon wafers sawn by a fixed diamond wire saw with the thinness of a silicon wafer. The residual stress in the surface layer of the silicon wafer is the primary reason for warp, which is generated by the phase transitions, elastic-plastic deformation, and non-uniform distribution of thermal energy during wire sawing. In this paper, an experiment of multi-wire sawing single crystal silicon is carried out, and the Raman spectra technique is used to detect the phase transitions and residual stress in the surface layer of the silicon wafers. Three different wire speeds are used to study the effect of wire speed on phase transition and residual stress of the silicon wafers. The experimental results indicate that amorphous silicon is generated during resin bonded diamond wire sawing, of which the Raman peaks are at 178.9 cm−1 and 468.5 cm−1. The ratio of the amorphous silicon surface area and the surface area of a single crystal silicon, and the depth of amorphous silicon layer increases with the increasing of wire speed. This indicates that more amorphous silicon is generated. There is both compressive stress and tensile stress on the surface layer of the silicon wafer. The residual tensile stress is between 0 and 200 MPa, and the compressive stress is between 0 and 300 MPa for the experimental results of this paper. Moreover, the residual stress increases with the increase of wire speed, indicating more amorphous silicon generated as well.

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