Low energy boron implantation profiles in silicon from junction depth measurements

1971 ◽  
Vol 7 (1-2) ◽  
pp. 7-15 ◽  
Author(s):  
P. Sebillotte ◽  
M. Badanoiu ◽  
V. B. Ndocko ◽  
P. Siffert
1998 ◽  
Vol 525 ◽  
Author(s):  
E. J. H. Collart ◽  
G. de Cock ◽  
A. J. Murrell ◽  
M. A. Foad

ABSTRACTThe effects of ramp-up rate during rapid thermal processing of ultra-shallow boron implants have been investigated. Ramp-up rates were varied between 25 °C and 200 °C for two types of anneals: soak anneals and spike anneals. It was found that the ramp-up rate had very little influence on junction depth or electrical activation for both types of anneals. Spike anneals did produce shallower profiles than soak anneal for a comparable electrical activation and may be an option for future processes.


Author(s):  
E.J.H Collart ◽  
K Weemers ◽  
N.E.B Cowern ◽  
J Politiek ◽  
P.H.L Bancken ◽  
...  

2004 ◽  
Vol 96 (4) ◽  
pp. 1891-1898 ◽  
Author(s):  
Antonio F. Saavedra ◽  
Kevin S. Jones ◽  
Mark E. Law ◽  
Kevin K. Chan ◽  
Erin C. Jones

1988 ◽  
Vol 128 ◽  
Author(s):  
Gary A. Ruggles ◽  
Shin-Nam Hong ◽  
Jimmie J. Wortman ◽  
Mehmet Ozturk ◽  
Edward R. Myers ◽  
...  

ABSTRACTLow energy (6 keV) BF2 implantation was carried out using single crystal, Ge-preamorphized, and Si-preamorphized silicon substrates. Implanted substrates were rapid thermal annealed at temperatures from 600°C to 1050'C and boron channeling, diffusion, and activation were studied. Ge and Si preamorphization energies were chosen to produce nearly identical amorphous layer depths as determined by TEM micrographs (approximately 40 nm in both cases). Boron segregation to the end-of-range damage region was observed for 6 keV BF2 implantation into crystalline silicon, although none was detected in preamorphized substrates. Junction depths as shallow as 50 nm were obtained. In this ultra-low energy regime for ion implantation, boron diffusion was found to be as important as boron channeling in determining the junction depth, and thus, preamorphization does not result in a significant reduction in junction depth. However, the formation of junctions shallower than 100 rmu appears to require RTA temperatures below 1000°C which can lead to incomplete activation unless the substrate has been preamorphized. In the case of preamorphized samples, Hall measurements revealed that nearly complete electrical activation can be obtained for preamorphized samples after a 10 second rapid thermal anneal at temperatures as low as 600°C.


2002 ◽  
Vol 717 ◽  
Author(s):  
Srinivasan Chakravarthi ◽  
Chidambaram P.R. ◽  
Charles Machala ◽  
Amitabh Jain ◽  
Xin Zhang

SummaryIn summary, we find it is possible to model the extent of arsenic diffusion during front-end and back-end processes that define the final junction depth. The key features of the model can be summarised as: (a) Interstitials from implant damage play a diminished role as implant energies are scaled; (b) As4V formation and precipitation at high concentrations is critical to accurate modeling of ultra-shallow arsenic junctions. These models when used with device simulations help optimize transistor performance/tradeoffs.We would like to thank Pavel Fastenko and Scott T. Dunham (University of Washington) for details and discussion regarding their modeling results.


1999 ◽  
Author(s):  
T. Sugii ◽  
K. Goto ◽  
T. Tanaka ◽  
J. Matsuo ◽  
I. Yamada

2004 ◽  
Vol 810 ◽  
Author(s):  
H. Graoui ◽  
M. Hilkene ◽  
B. McComb ◽  
M. Castle ◽  
S. Felch ◽  
...  

ABSTRACTThe main challenges for PMOS ultra shallow junction formation remain the transient enhanced diffusion (TED) and the solid solubility limit of boron in silicon. It has been demonstrated that low energy boron implantation and spike annealing are key in meeting the 90 nm technology node ITRS requirements. To meet the 65 nm technology requirements many studies have used fluorine co-implantation with boron and Si+ or Ge+ pre-amorphization (PAI) and spike annealing. Although using BF+2 can be attractive for its high throughput, self-amorphization and the presence of fluorine, many studies have shown that for the fluorine to successfully reduce TED its energy needs to be well optimized with respect to the boron's, therefore BF+2 does not present the right fluorine/boron energy ratio for the optimum junction formation. In this work we optimize the fluorine energy when a deep or shallow PAI is used. We also demonstrate that the fluorine dose needs to be carefully optimized otherwise a reverse effect can be observed. We will also show that the optimized junction depends less on the Ge+ energies between 2 keV and 20 keV and when HF etch is implemented after Ge+ PAI, improvements in both the junction depth and the sheet resistance are observed.


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