Electrical Activation of Boron in B+ + C+ Implanted Si during RTA with Different Heating Rates

1994 ◽  
Vol 342 ◽  
Author(s):  
H. Boudinov ◽  
J.P. de Souza

ABSTRACTSilicon samples were single implanted with B+ (5 x 1014 cm−2, 50 keV) or co-implanted with C+ (5 x 1015 cm−2, 55 keV). Rapid thermal annealing (RTA) with heating rates (HR) of 1°C/s and 100°C/s with dwell time duration from 2 s to 15 min was used for B activation and the results compared with those provided by conventional furnace annealing (FA) for 30 min. In single implanted samples it was found that below 600°C or above 800°C the activation always increases with the annealing time. However, in the temperature range of 600-800°C and annealing times longer than 60 s a fraction of the initially activated B concentration deactivates. For temperatures in the range of 700-800°C the deactivation is followed again by another activation period. There is no noticeable difference between the activation yields after RTA with high HR for 15 min or FA for 30 min. In the C co-implanted samples the activation of boron saturates after few minutes. In addition the deactivation process is significantly reduced. A model assuming interaction of the B atoms with point defects and the C atoms with Si self- interstitial atoms is proposed to explain the results.

1983 ◽  
Vol 23 ◽  
Author(s):  
K.V. Vaidyanathan ◽  
H.L. Dunlap

ABSTRACTThis paper discusses the properties of high intensity lamp-annealed silicon or beryllium-implanted GaAs and InP samples. We find this annealing process can result in efficient activation of dopants. Conventional furnace annealing at the same temperature does not result in increased electrical activation of the dopants. High fluence silicon implants can be activated in anneal times as short as 2 seconds, while low fluence silicon implants require more extended annealing. Activation of low fluence implants in GaAs depends strongly on the properties of the bulk semiinsulating material.


1987 ◽  
Vol 92 ◽  
Author(s):  
E. Ma ◽  
M. Natan ◽  
B.S. Lim ◽  
M-A. Nicolet

ABSTRACTSilicide formation induced by rapid thermal annealing (RTA) and conventional furnace annealing (CFA) in bilayers of sequentially deposited films of amorphous silicon and polycrystalline Co or Ni is studied with RBS, X-ray diffraction and TEM. Particular attention is paid to the reliability of the RTA temperature measurements in the study of the growth kinetics of the first interfacial compound, Co2Si and Ni2Si, for both RTA and CFA. It is found that the same diffusion-controlled kinetics applies for the silicide formation by RTA in argon and CFA in vacuum with a common activation energy of 2.1+0.2eV for Co2Si and 1.3+0.2eV for Ni Si. Co and Ni atoms are the dominant diffusing species; during silicide formation by both RTA and CFA. The microstructures of the Ni-silicide formed by the two annealing techniques, however, differs considerably from each other, as revealed by cross-sectional TEM studies.


1985 ◽  
Vol 52 ◽  
Author(s):  
Thomas E. Kazior ◽  
Kamal Tabatabaie-Alavi

ABSTRACTAn Eaton Nova Rapid Optical Annealer (ROA 400) has been used to activate n and n+ Si implants for use in power and low noise FET structures for GaAs MMIC's. PECVD SiN capped 3" SI GaAs wafers were annealed at temperatures ranging from 800 to 970 °C for times ranging from 0 (transient light pulse) to 20 sec. Doping profiles were determined using a Polaron concentration profiler; FATFET's were used for measuring drift mobility; and short gate (l.0μm gate length) FET's were fabricated to establish activation uniformity and to determine d.c. and r.f. performance. Results have indicated peak implant activation as high as 90% and electron mobilities of up to 4700cm2/V-sec for carrier concentrations of 1.3×1017/cm3 – results comparable to conventional furnace annealing. The most significant improvement of optical annealing comes in device uniformity. Saturated current uniformities of < ±3% have been achieved over 3" wafers with excellent reproducibility from wafer to wafer. Power FET structures with zero bias gm of 120mS/mm with uniformities of <±5mS/mm have been measured. R.f. measurements on these devices yielded output powers of >500mW/mm with power added efficiencies as high as 35%.


1992 ◽  
Vol 283 ◽  
Author(s):  
Yoon-Ho Song ◽  
Jong-Tae Baek ◽  
Kee-Soo Nam ◽  
Sang-Won Kang

ABSTRACTA new annealing method, a combination of rapid thermal annealing (RTA) and furnace annealing, has been developed to obtain a high quality poly-Si from a-Si deposited by LPCVD. This method produces a large grain poly-Si with good uniformity, which may result from the growth of relatively defect-free nucleus generated at a high temperature by RTA. Poly-Si thin film transistors fabricated by this new annealing method have higher field effect mobility and better uniformity compared with those by the conventional furnace annealing.


2010 ◽  
Vol 44-47 ◽  
pp. 4154-4156
Author(s):  
Rui Min Jin ◽  
Ding Zhen Li ◽  
Lan Li Chen ◽  
Xiang Ju Han ◽  
Jing Xiao Lu

Amorphous silicon films prepared by PECVD on glass substrate has been crystallized by conventional furnace annealing (FA) at different temperatures. From the Raman spectra and scanning electronic microscope (SEM), it is found that the thin film grain size present quantum states with annealing temperature.


1986 ◽  
Vol 74 ◽  
Author(s):  
K. Kohlhof ◽  
S. Mantl ◽  
B. Stritzker

AbstractIon beam mixing experiments of Ti-Si layers have been performed with Kr ions of 250 keV energy and doses ranging from 7 1015 to 7 1016 cm-2 at temperatures between liquid nitrogen temperature and 450°C. At substrate temperatures below 120°C no silicide formation could be detected. Only weak mixing at the Ti-Si interface is observed. At temperatures above 120°C the formation of TiSi2 could be verified by Rutherford backscattering and X-ray diffractometry. Layers of TiSi2 produced by ion beam mixing show smooth surfaces in contrast to those prepared by conventional furnace annealing. Those display rough surfaces and interfaces.


2000 ◽  
Vol 610 ◽  
Author(s):  
Janet M. Bonar ◽  
Barry M. Mcgregor ◽  
Nick E. B. Cowern ◽  
Aihua Dan ◽  
Graham A. Cooke ◽  
...  

AbstractThe diffusion of B in Si and SiGe under the influence of point defect injection by Rapid Thermal Anneal (RTA) and conventional furnace anneal is studied in this work. B-doped regions in SiGe and Si were grown by LPCVD, and point defects were injected by RTA or furnace annealing bare, Si3N4 or SiO2 + Si3N4 covered samples in an oxygen atmosphere. Self-interstitial defects will be injected into bare Si while vacancy defects will be injected into Si3N4 covered samples, and inert annealing will occur in SiO2 + Si3N4 covered samples. The annealed and asgrown profiles were determined using SIMS analysis, and the diffusivities extracted by direct comparison of the profiles. Both interstitials and vacancies were injected during furnace annealing of SiGe, as demonstrated by the respective enhancement and retardation of the B diffusion. Enhanced B diffusion in SiGe was observed even for 5 s RTA at 1000°C, with an enhancement factor of ∼2.5. The B in Si diffusivity enhancement for interstitial injection by RTA oxidation was found to be a factor of ∼3 compared to inert anneals, close to the factor for SiGe.


2014 ◽  
Vol 32 (1-2) ◽  
pp. 43-49
Author(s):  
M. Edwin Sahayaraj ◽  
Jepas T. Winowlin Jappes ◽  
Irulappasamy Siva ◽  
Murugan Sundaram Senthil Saravanan

AbstractThis work aims at studying the corrosion behavior of electroless Ni-P coating on mild steel substrate heat-treated by microwave and conventional furnace (muffle) annealing. The corrosion behavior of the deposits has been evaluated by potentiodynamic polarization studies in 3.5 wt% sodium chloride solution. The heat treatment temperatures of both the microwave and the conventional furnace annealing were kept at regular intervals to study the corrosion performance of the coatings. Microwave heat treatment significantly improved the corrosion performance of the coatings. Further, corrosion mechanisms of as-coated, various microwave- and conventional heat-treated coatings were discussed for the consideration of phase constituents, grain sizes and microstrain.


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