The Effect of Implantation and Annealing Conditions on the Fe Profile in Semi-Insulating InP.

1986 ◽  
Vol 74 ◽  
Author(s):  
G. Bahir ◽  
J. L. Merz ◽  
J. R. Abelson ◽  
T. W. Sigmon
Keyword(s):  
Mass Spectrometry ◽  
Rapid Thermal Annealing ◽  
Thermal Processing ◽  
Depth Distribution ◽  
Secondary Ion Mass Spectrometry ◽  
Furnace Annealing ◽  
Depth Profiles ◽  
Annealing Conditions ◽  
Residual Damage ◽  
Secondary Ion

AbstractThe Fe depth distribution has been measured in semi-insulating (SI) InP implanted with Si as a function of implant temperature and post-implant annealing technique (either furnace annealing or rapid thermal annealing). Depth profiles obtained by secondary ion mass spectrometry and Rutherford backscattering measurements of the damage demonstrate that Fe redistributes into regions of residual damage during thermal processing. These results are interpreted in terms of implantation-related damage effects and the stoichiometry imbalance induced by the Si implantation.

Dissociation of Deuterium-Defect Complexes in Ion-Implanted Epitaxial 4H-SiC

1998 ◽  
Vol 513 ◽  
Author(s):  
M. Janson ◽  
M. K. Linnarsson ◽  
A. Hallén ◽  
B. G. Svensson
Keyword(s):  
Experimental Data ◽  
Mass Spectrometry ◽  
Monte Carlo ◽  
Depth Distribution ◽  
Secondary Ion Mass Spectrometry ◽  
Depth Profiles ◽  
Defect Complexes ◽  
Induced Defects ◽  
Secondary Ion ◽  
Anneal Time

ABSTRACTEpitaxial layers of low doped 4H-SiC are implanted with 20 keV 2H+ ions to a dose of 1×1015 cm−2. The samples are subsequently annealed at temperatures ranging from 1040 to 1135 °C. Secondary ion mass spectrometry is used to obtain the concentration versus depth profiles of the atomic deuterium in the samples. It is found that the concentration of implanted deuterium decreases rapidly in the samples as a function of anneal time.The experimental data are explained by a model where the deuterium migrates rapidly and becomes trapped and de-trapped at implantation-induced defects which exhibit a slightly shallower depth distribution than the implanted deuterium ions. Computer simulations using this model, in which the damage profile is taken from Monte Carlo simulations and the surface is treated as a perfect sink for the diffusing deuterium atoms, are performed with good results compared to the experimental data. The complexes are tentatively identified as carbon-deuterium at a Si-vacancy and a dissociation energy (ED) of approximately 4.9 eV is extracted for the deuterium-vacancy complexes.

Residual damage in B+ and –implanted Si

1985 ◽  
Vol 63 (6) ◽  
pp. 863-869 ◽  
Author(s):  
W. Vandervorst ◽  
D. C. Houghton ◽  
F. R. Shepherd ◽  
M. L. Swanson ◽  
H. H. Plattner ◽  
...  
Keyword(s):  
Electron Microscopy ◽  
Mass Spectrometry ◽  
Transmission Electron Microscopy ◽  
Secondary Ion Mass Spectrometry ◽  
Nuclear Reaction Analysis ◽  
Furnace Annealing ◽  
Projected Range ◽  
Transmission Electron ◽  
Residual Damage ◽  
Secondary Ion

The residual damage left after furnace-annealing Si wafers implanted with 30-keV B+ or 120-keV [Formula: see text] ions has been investigated for doses of 3–5 × 1015 ions∙cm−2. Transmission electron microscopy, Rutherford backscattering, and channeling were used to study the morphology and distribution of the damage while the B and F content and their depth distributions were determined by nuclear reaction analysis and secondary-ion mass spectrometry. For B+-implanted samples the residual damage is concentrated in a band at a depth corresponding to the B projected range. For [Formula: see text]-implanted samples the residual damage is located mainly in the region of the as-implanted amorphous–crystalline interface.

Behaviour of Implanted Hydrogen in Gallium Phosphide Single Crystals

1988 ◽  
Vol 144 ◽  
Author(s):  
J. M. Zavada ◽  
R. G. Wilson ◽  
S. W. Novak ◽  
S. J. Pearton ◽  
A. R. Von Neida
Keyword(s):  
Mass Spectrometry ◽  
Single Crystals ◽  
Diffusion Coefficients ◽  
Gallium Phosphide ◽  
Secondary Ion Mass Spectrometry ◽  
Furnace Annealing ◽  
Higher Temperature ◽  
Redistribution Of Hydrogen ◽  
Secondary Ion ◽  
Post Implantation

ABSTRACTIn this paper we report on the depth distributions of implanted hydrogen in GaP crystals and the subsequent changes produced by post- implantation furnace annealing. A sulfur doped n+ GaP wafer has been implanted with 333 keV protons to a fluence of 5E15/cm+2. A similar wafer was implanted with 350 keV deuterons to the same fluence. Portions of each wafer have been furnace annealed at temperatures up to 500°C. The implanted hydrogen and the dopant S atoms were then depth profiled using secondary ion mass spectrometry (SIMS). The measurements show that the redistribution of hydrogen begins with annealing at about 300°C and proceeds both towards the surface and deeper into the substrate. The overall behavior is similar to that found previously for hydrogen in GaAs. However, in GaP crystals this redistribution begins at a higher temperature and proceeds more slowly in the implanted region. Based on the SIMS profiles, diffusion coefficients for hydrogen migrating into substrate are obtained.

The Correlation between the Reduction of Interface State Density at the SiO2/SiC Interface and the NO Post-Oxide-Annealing Conditions

2019 ◽  
Vol 954 ◽  
pp. 104-108
Author(s):  
Heng Yu Xu ◽  
Cai Ping Wan ◽  
Jin Ping Ao
Keyword(s):  
Mass Spectrometry ◽  
Secondary Ion Mass Spectrometry ◽  
Interface State ◽  
State Density ◽  
Interface State Density ◽  
Mos Capacitors ◽  
Annealing Conditions ◽  
N Concentration ◽  
Higher Temperature ◽  
Secondary Ion

We fabricated SiO2/4H-SiC (0001) MOS capacitors with oxidation temperature at 1350°C, followed by post-oxide-annealing (POA) in NO simply by the control of POA temperatures and times. A correlation between the reduction of interface state density and the increasing of N concentration at the interface has been indicated by C-ψs measurement and secondary ion mass spectrometry (SIMS). The SiO2/4H-SiC interface density decreased when POA temperature was elevated, and the sample annealed at 1300°C for 30min showed the lowest interface state density about 1.5×1012 cm-2eV-1 at Ec-E=0.3 eV when the N concentration is 11.5×1020 cm-3. Meanwhile, the SiO2 /4H-SiC interface annealed at 1200°C for 120min showed the highest N concentration at the 4H-SiC/SiO2 interface is 12.5×1020 cm-3, whereas the interface state density is 2.5×1012 cm-2eV-1 at Ec-E=0.3 eV higher than 1300°C for 30min. The results suggested that higher temperature POA might be much more efficiency in decreased the 4H-SiC MOS interface density with increasing the N area concentration.

Effects of Cryogenic Sample Analysis on Molecular Depth Profiles with TOF-Secondary Ion Mass Spectrometry

2010 ◽  
Vol 82 (19) ◽  
pp. 8291-8299 ◽  
Author(s):  
Alan M. Piwowar ◽  
John S. Fletcher ◽  
Jeanette Kordys ◽  
Nicholas P. Lockyer ◽  
Nicholas Winograd ◽  
...  
Keyword(s):  
Mass Spectrometry ◽  
Secondary Ion Mass Spectrometry ◽  
Sample Analysis ◽  
Depth Profiles ◽  
Ion Mass Spectrometry ◽  
Secondary Ion

Quantitation of Secondary Ion Mass Spectrometry (SIMS) for HgCdTe.

1983 ◽  
Vol 25 ◽  
Author(s):  
Lawrence E. Lapides ◽  
George L. Whiteman ◽  
Robert G. Wilson
Keyword(s):  
Mass Spectrometry ◽  
Ion Implantation ◽  
Ionization Potential ◽  
Electron Affinity ◽  
Secondary Ion Mass Spectrometry ◽  
Relative Sensitivity ◽  
Depth Profiles ◽  
Ion Mass Spectrometry ◽  
Sensitivity Factors ◽  
Secondary Ion

ABSTRACTQuantitative depth profiles of impurities in LPE layers of HgCdTe have been determined using relative sensitivity factors calculated from ion implantation profiles. Standards were provided for Li, Be, B, C, F, Na, Mg, Al, Si, P, S, Cl, Cu, Ga, As, Br, and In. Relative sensitivity factors as a function of ionization potential for O2+ primary ion SIMS and electron affinity for Cs+ primary ion SIMS have been calculated in order to extend quantitation to elements not yet implanted. Examples of depth profiles for implant standards and unimplanted layers are given.

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