Damage calibration concept and novel B cluster reaction model for B transient enhanced diffusion over thermal process range from 600°C (839 h) to 1100°C (5 s) with various ion implantation doses and energies

Author(s):  
K. Suzuki ◽  
T. Miyashita ◽  
Y. Tada ◽  
A. Hoefler ◽  
N. Strecker ◽  
...  
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.


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

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.


1998 ◽  
Vol 532 ◽  
Author(s):  
Ning Yu ◽  
Amitabh Jain ◽  
Doug Mercer

ABSTRACTThe SIA roadmap predicts that junction depths of 500 angstroms are required for CMOS technology nodes of 0.18 μm or beyond by the year 2001. There are several ultra-shallow junction doping techniques currently under investigation. These include beamline ion implantation, plasma immersion ion implantation, and gas immersion laser doping. This study was based on beamline ion implantation of B, P, and As into single-crystal Si wafers at 0.25-2 keV to doses of (2- 10)×1014 at./cm2 with minimized beam energy contamination. Rapid thermal annealing was applied to the implanted wafers at 1000-1050 °C for 10-15 sec at ramp rates of 35- 50 °C/s in a N2 ambient. Transient enhanced diffusion was observed for all three implant species. For example, the depth of 0.25 keV B measured by SIMS increases from 250 to 520 A at a concentration level of l×1017 at./cm3 upon RTA. To minimize the TED, several schemes of defect engineering were applied prior to low energy implantation, including pre-amorphization and implantation of other species. A comparison of TED for different implantation conditions is given with the aim of process development for minimizing TED. The impact of energy contamination on ultra shallow junctions is also addressed.


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