On the Influence of Boron-Interstitial Complexes on Transient Enhanced Diffusion

1999 ◽  
Vol 568 ◽  
Author(s):  
D. Stiebel ◽  
P. Pichler ◽  
H. Ryssel

ABSTRACTWe present new experimental results on the transient enhanced diffusion (TED) of boron after ion implantation. The investigation is focussed on effects that influence TED of shallow profiles in the absence of {311}-defects. Under these conditions, TED is mainly determined by the formation of boron-interstitial complexes (BIC). In addition, effects from the proximity of the surface become more and more important. Insight into the behavior of the dopant atoms is obtained by the comparison with simulations.

1995 ◽  
Vol 67 (15) ◽  
pp. 2158-2160 ◽  
Author(s):  
J. Ravi ◽  
Yu. Erokhin ◽  
G. A. Rozgonyi ◽  
C. W. White

1999 ◽  
Vol 86 (11) ◽  
pp. 6039-6042 ◽  
Author(s):  
I. O. Usov ◽  
A. A. Suvorova ◽  
V. V. Sokolov ◽  
Y. A. Kudryavtsev ◽  
A. V. Suvorov

2000 ◽  
Vol 610 ◽  
Author(s):  
L. S. Robertson ◽  
P. N. Warnes ◽  
K. S. Jones ◽  
S. K. Earles ◽  
M. E. Law ◽  
...  

AbstractThe interaction between boron and excess silicon interstitials caused by ion implantation hinders the formation of ultra-shallow, low resistivity junctions. Previous studies have shown that fluorine reduces boron transient enhanced diffusion, however it is unclear whether this observed phenomenon is due to the fluorine interacting with the boron atoms or silicon self-interstitials. Amorphization of a n-type Czochralski wafer was achieved with a 70 keV Si+ implantation at a dose of 1×1015/cm2. The Si+ implant produced a 1500Å deep amorphous layer, which was then implanted with 1.12 keV 1×1015/cm2 B+. The samples were then implanted with a dose of 2×1015/cm2F+ at various energies ranging from 2 keV to 36 keV. Ellipsometry measurements showed no increase in the amorphous layer thickness from either the boron or fluorine implants. The experimental conditions allowed the chemical species effect to be studied independent of the implant damage caused by the fluorine implant. Post-implantation anneals were performed in a tube furnace at 750° C. Secondary ion mass spectrometry was used to monitor the dopant diffusion after annealing. Transmission electron microscopy (TEM) was used to study the end-of-range defect evolution. The addition of fluorine reduces the boron transient enhanced diffusion for all fluorine energies. It was observed that both the magnitude of the boron diffusivity and the concentration gradient of the boron profile vary as a function of fluorine energy.


2000 ◽  
Vol 610 ◽  
Author(s):  
P. H. Keys ◽  
R. Brindos ◽  
V. Krishnamoorthy ◽  
M. Puga-Lambers ◽  
K. S. Jones ◽  
...  

AbstractThe release of interstitials from extended defects after ion implantation acts as a driving force behind transient enhanced diffusion (TED). Implantation of Si+ ions into regions of phosphorus-doped silicon provides experimental insight into the interaction of silicon interstitials and dopant atoms during primary damage annealing. The presence of phosphorus influences the morphology of secondary defects during initial nucleation. Transmission electron microscopy (TEM) is used to differentiate between defect types and quantify the interstitials trapped in extended defects. This analysis reveals that phosphorus results in a reduction of interstitials trapped in observable extended defects. The interstitial flux released from the implanted region is also affected by the phosphorus doping. This phenomenon is closely studied using secondary ion mass spectrometry (SIMS) to monitor diffusion enhancements of dopant layers. Shifts in diffused dopant profiles are correlated with the different morphologies of the extended defects and the decay of the silicon interstitial supersaturation. This correlation is used to understand the interaction of excess silicon interstitials with phosphorus atoms.


1998 ◽  
Vol 73 (14) ◽  
pp. 2015-2017 ◽  
Author(s):  
Aditya Agarwal ◽  
H.-J. Gossmann ◽  
D. C. Jacobson ◽  
D. J. Eaglesham ◽  
M. Sosnowski ◽  
...  

1998 ◽  
Vol 54 (1-3) ◽  
pp. 80-83 ◽  
Author(s):  
Norihiro Shimada ◽  
Takaaki Aoki ◽  
Jiro Matsuo ◽  
Isao Yamada ◽  
Kenichi Goto ◽  
...  

1996 ◽  
Vol 79 (5) ◽  
pp. 2352-2363 ◽  
Author(s):  
H. S. Chao ◽  
S. W. Crowder ◽  
P. B. Griffin ◽  
J. D. Plummer

1994 ◽  
Vol 9 (11) ◽  
pp. 2987-2992
Author(s):  
Naoto Shigenaka ◽  
Shigeki Ono ◽  
Tsuneyuki Hashimoto ◽  
Motomasa Fuse ◽  
Nobuo Owada

A new process for ion implantation into silicon wafers was proposed. This process has an additional implantation step to form an amorphous phase. At first self-ions are implanted into a cooled wafer (< −30 °C) to form the amorphous phase, and subsequently dopant atoms are implanted to form a doped layer within the amorphous layer. After annealing above 650 °C, the silicon wafer is completely recrystallized, and no defects with sizes detectable by TEM are present near the doped layer. There is indeed a defect layer in the wafer; however, it lies along the amorphous/crystal interface that is behind the doped layer. The concentration profile of the dopant atoms is not changed during epitaxial recrystallization, and further dopant atom diffusion during annealing is limited to about 0.05 μm, because defect-enhanced diffusion does not occur. The double implantation method is considered to be effective for doped layer formation in the VLSI fabrication process.


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