Channeling Contrast Microscopy: A Powerful Tool for Examining Semiconductor Structures

1986 ◽  
Vol 69 ◽  
Author(s):  
J. C. McCallum ◽  
R. A. Brown ◽  
E. Nygren ◽  
J. S. Williams ◽  
G. L. Olson

AbstractChanneling contrast microscopy with a He+ microbeam has been employed to measure 3-dimensional damage distributions and impurity profiles in ion implanted laser annealed silicon. Refinements to the technique are described, involving construction of a precision goniometer to allow accurate orientation of the microbeam with respect to micron-scale- sample features. We have found that indium diffusion in amorphous silicon is significantly less for laser annealing than with lower temperature furnace annealing. Lateral variations in the extent of crystal growth have also been observed across laser irradiated areas less than 100μm.

1980 ◽  
Vol 1 ◽  
Author(s):  
Nobuyoshi Natsuaki ◽  
Takao Miyazaki ◽  
Makoto Ohkura ◽  
Toru Nakamura ◽  
Masao Tamura ◽  
...  

ABSTRACTBipolar transistors with laser annealed base and emitter, as well as those with furnace annealed base and laser annealed emitter, have been successfully fabricated using Q-switched ruby laser pulse irradiation. The performance of laser asannealed transistors is rather poor. However, it can be improved, to some extent, by relatively low temperature furnace annealing after laser irradiation. DC and RF characteristics of laser annealed transistors are presented in conjunction with laser irradiation effects on the characteristics of conventionally fabricated transistors.


1996 ◽  
Vol 420 ◽  
Author(s):  
Kwon-Young Choi ◽  
Jae-Hong Jeon ◽  
Min-Koo Han ◽  
Yong-Sang Kim

AbstractThe performance of polysilicon thin film transistors fabricated by two-step annealing, which consists of furnace annealing and subsequent excimer laser annealing, is described. It was found that the average grain size of low temperature furnace annealed polysilicon films was several times larger than that of excimer laser annealed polysilicon films while the density of in-grain defect in low temperature furnace annealed films was much higher than that of excimer laser annealed film. The device characteristics of the low temperature furnace annealed polysilicon thin film transistors were improved significantly by postannealing, such as high temperature furnace annealing and excimer laser annealing, due to the effective elimination of in-grain defects. The density of trap states, which was extracted from the transfer curves of polysilicon thin film transistors, was used to demonstrate the effects of modifying the deep and tail trap levels by two-step annealing.


1983 ◽  
Vol 23 ◽  
Author(s):  
T. P. Smith ◽  
P. J. Stiles ◽  
W. M. Augustyniak ◽  
W. L. Brown ◽  
D. C. Jacobson ◽  
...  

ABSTRACTFormation of buried insulating layers and redistribution of impurities during annealing are important processes in new semiconductor device technologies. We have studied pulsed ruby laser and furnace annealing of high dose (D>1017 N/cm2) 50 KeV nitrogen implanted silicon. Using He Back scattering and channeling, X-ray diffraction, transmission electron microscopy, and infrared transmission spectroscopy, we have compared liquid and solid phase regrowth, diffusion, impurity segregation and nitride formation. As has been previously reported, during furnace annealing at or above 1200C nitrogen redistributes and forms a polycrystalline silicon nitride (Si3N4 ) layer. [1–4] In contrast, pulsed laser annealing produces a buried amorphous silicon nitride layer filled with voids or bubbles below a layer of polycrystalline silicon.


1985 ◽  
Vol 53 ◽  
Author(s):  
R. Sundaresan ◽  
P.-H. Chang ◽  
S.D.S. Malhi ◽  
H.W. Lam

ABSTRACTSolid-phase epitaxial regrowth of polysilicon films. amorphized by a room-temperature silicon implant. has been achieved using a (low temperature) furnace anneal or a (high temperature) rapid thermal anneal. Lateral extension of the growth onto an oxide layer, 4 μm wide, has also been observed. The electrical properties of the films were examined by building MO2S devices in them. Average electron mobilities of 520 cm2/v-sec and 200 cm2/v-sec have been measured for films regrown on top of silicon and oxide respectively.


Shinku ◽  
2000 ◽  
Vol 43 (12) ◽  
pp. 1120-1125 ◽  
Author(s):  
Naoto MATSUO ◽  
Hisashi ABE ◽  
Naoya KAWAMOTO ◽  
Ryouhei TAGUCHI ◽  
Tomoyuki NOUDA ◽  
...  

2006 ◽  
Vol 45 (5B) ◽  
pp. 4344-4346 ◽  
Author(s):  
Shinji Munetoh ◽  
Takahide Kuranaga ◽  
Byoung Min Lee ◽  
Teruaki Motooka ◽  
Takahiko Endo ◽  
...  

2008 ◽  
Vol 5 (10) ◽  
pp. NA-NA
Author(s):  
N. Misra ◽  
L. Xu ◽  
M. S. Rogers ◽  
S. H. Ko ◽  
C. P. Grigoropoulos

1993 ◽  
Vol 316 ◽  
Author(s):  
Hajime Shibata ◽  
Yunosuke Makita ◽  
Kawakatsu Yamada ◽  
Yutaka Uchida ◽  
Sabro Satoh

ABSTRACTThe capability of discharge-pumped vacuum ultraviolet F2 molecular laser for laser annealing of heavily ion implanted semiconductor was demonstrated for the first time using Se+ heavily ion implanted GaAs. Cr-doped semi-insulationg GaAs wafers were used as the substrates, and the Se+ implantation energy and dose were controlled to 100 keV and 1× 1015 cm-2, respectively. Samples were annealed using a F2 molecular laser ( wavelength = 157 nm ) with a single pulse ( width ~ 20 ns ) in the energy density range from 200 to 800 mJ/cm2 in a nitrogen atmosphere. In addition, furnace annealing was done on separate samples at 850 ºC for 20 minutes in a purified hydrogen atmosphere for comparison. Characterization of the samples was carried out using Raman scattering and ellipsometry. The laser annealed samples exhibited intense Raman scattering LO phonon peaks whose intensity increased with increasing laser power density, whereas the furnace annealed samples exhibited a very weak LO phonon peak. It was demonstrated for the first time that VUV photons can be very effective in annealing ion implantation damage as compared with conventional furnace annealing. The behavior of Raman scattering spectra as a function of laser energy density was explained quantitatively by a “spatial correlation” model. The model made it possible to estimate the average size of the recovered crystal regions in samples for any given laser energy density.


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