High dose dopant implantation to heated Si substrate without amorphous layer formation

Author(s):  
Hiroshi Onoda ◽  
Yoshiki Nakashima ◽  
Tsutomu Nagayama ◽  
Shigeki Sakai
1996 ◽  
Vol 35 (Part 1, No. 3) ◽  
pp. 1857-1861 ◽  
Author(s):  
Mitsuyasu Yatsuzuka ◽  
Yoshiyuki Hashimoto ◽  
Tohru Yamasaki ◽  
Hitoshi Uchida

1998 ◽  
Vol 525 ◽  
Author(s):  
L. P. Ren ◽  
P. Liu ◽  
G. Z. Pan ◽  
Jason C. S. Woo

ABSTRACTA novel low temperature self-aligned Ti silicidation with Ge+ pre-amorphization implant (PAI) is presented. Compared to conventional high temperature PAM silicidation, the advantages of Ti salicidation at temperatures below the recrystallization of a pre-amorphized layer are: (1) C49 TiSi2 silicide formation occurs only in the pre-amorphized layer so that the silicide depth can be well controlled, forming a very sharp interface between the silicide and the Si substrate; (2) Ti just reacts with the amorphous layer, avoiding the so-called bridging issue in which the silicide grows laterally over the isolation or spacer; (3) the effects of metal thickness and substrate doping on silicide formation are suppressed.


2016 ◽  
Vol 22 (S3) ◽  
pp. 144-145
Author(s):  
Michael Presley ◽  
Jacob Jensen ◽  
Dan Huber ◽  
Hamish Fraser

2000 ◽  
Vol 610 ◽  
Author(s):  
R. Annunziata ◽  
R. Bottini ◽  
P. Colpani ◽  
C. Cremonesi ◽  
G. Ghidini ◽  
...  

AbstractIn this paper we show that dopant decoration of process-induced defects is responsible for a failure mechanism of memory devices. From the electrical point-of-view, the defect-related failure consists in a source-to-drain resistive path formed by junction piping. This mechanism is made active by the very close spacing which is typical of present device structures. A device-like test structure is used for defect detection. This structure proves to be a very effective tool for studying the impact of various process steps on defect generation, in that it allowes statistical data about the formation of these defects to be collected. TEM analyses are extensively used for studying the evolution of end-of-range defects during subsequent thermal treatments and for measuring the amorphous layer width under various implantation conditions.The role of high dose implantations in the generation of this sort of defects is discussed. Even if the amorphous layer is completely recovered by a suitable recristallization annealing, residual defects grow and become dopant-decorated during post-implantation thermal treatments. Defect density is increased by oxidizing treatments. In this case point defect injection is active both in enhancing dopant diffusion and in growing defects.Defect formation is suppressed if the amorphous layer is made very shallow (≤ 50 nm) by suitable choices of the screen oxide and of the implantation energy. A binary collision code is used in order to estimate the dependence on energy of the self-interstitial excess outside the amorphous region. The results of these calculations indicate that defect suppression can be tentatively explained by point defect annihilation at the silicon surface.


1986 ◽  
Vol 74 ◽  
Author(s):  
Alice E. White ◽  
K. T. Short ◽  
L. N. Pfeiffer ◽  
K. W. West ◽  
J. L. Batstone

AbstractFrom the early work on high dose oxygen implantation for buried SiO2 formation, it is apparent that the temperature of the Si substrate during the implant has a strong influence on the quality of both the SiO2 layer and the overlying Si. This, in turn, can be related to the damage from the oxygen implant. For substrate temperatures < ∼ 300°C, amorphous Si is created during the implant and leads to the formation of twins or polycrystalline Si during the subsequent high temperature (>1300°C) anneal. At higher substrate temperatures (<∼400°C), dynamic annealing eliminates the amorphous Si, but the implanted oxygen appears to segregate during the implant leading to oxygen-rich amorphous regions imbedded in regions of crystalline material. As the amorphous regions start to coalesce and form SiO2 during the high temperature anneal, they trap crystalline Si which cannot escape by diffusion. This process can be circumvented by using a randomizing Si implant to change the damage structure from the oxygen implant before annealing. We have seen these effects clearly in sub-stoichiometric implants, and believe they are also operative during stoichiometric implants.


1993 ◽  
Vol 316 ◽  
Author(s):  
Robert Simonton ◽  
Jinghong Shi ◽  
Ted Boden ◽  
Philippe Maillot ◽  
Larry Larson

ABSTRACTWe implanted <100> silicon 200mm wafers with 20keV 11B+ to a fluence of 5×1015 atoms/ cm2 using beam currents from 1-7mA, which produced flux of about 50-350µA/cm2. The implant temperature of all wafers rose no more than five degrees above room temperature, regardless of flux. Cross sectional TEM images (as-implanted) of the highest flux samples revealed a continuous amorphous layer from the implanted surface to a depth of about 530Å. The high flux and <30°C implantation temperature allowed amorphous layer formation even with this moderate boron fluence, as was suggested by Jones, et.al.1. We observed a strong dependence of as-implanted damage on boron flux, as previously reported by Eisen and Welch2. After 900°C, 20 sec RTA, the highest flux samples had 50% lower sheet resistance than the lowest flux samples, due to better activation, as observed in SRP. When a 1050°C, 15 sec RTA was employed, this sheet resistance and activation dependence on flux disappeared. Cross sectional TEM images revealed that the size and number of the Type II end of range defects , which were centered near the amorphous and crystalline as-implanted interface, in the highest flux samples were smaller than the Type 1 dislocation loops centered about the peak disorder in the lowest flux samples after RTA. SIMS and SRP profiles indicated that transient enhanced diffusion during the 900°C, 20 sec RTA may have been reduced in the highest flux samples. Based on these observations and on previous reports, we conclude that sufficiently high flux during room temperature boron implantation will produce a continuous amorphous layer with doses that are appropriate for p-type source/drain formation. The amorphous layer will produce improved activation and damage annealing behavior in subsequent RTA, particularly as the RTA temperature is reduced.


1996 ◽  
Vol 439 ◽  
Author(s):  
S. Tian ◽  
M. Morris ◽  
S. J. Morris ◽  
B. Obradovic ◽  
A. F. Tasch

AbstractWe present for the first time a physically based ion implantation damage model which successfully predicts both the as-implanted impurity range profiles and the damage profiles for a wide range of implant conditions for arsenic, boron, phosphorus, and BF2 implants into single-crystal (100) silicon. In addition, the amorphous layer thicknesses predicted by this damage model for high dose implants are also generally in excellent agreement with experiments. This damage model explicitly simulates the defect production and its subsequent evolution into the experimentally observable profiles for the first time. The microscopic mechanisms for damage evolution are further discussed.


1994 ◽  
Vol 354 ◽  
Author(s):  
J.K.N. Lindner ◽  
A. Frohnwieser ◽  
B. Rauschenbach ◽  
B. Stritzker

AbstractHomogenous, epitaxial buried layers of 3C-SÍC have been formed in Si(100) and Si(lll) by ion beam synthesis (IBS) using 180 keV high dose C ion implantation. It is shown that an annealing temperature of 1250 °C and annealing times of 5 to 10 h are sufficient to achieve well-defined Si/SiC/Si layer systems with abrupt interfaces. The influence of dose, annealing time and temperature on the layer formation is studied. The favourable dose is observed to be dependent on the substrate orientation. IBS using 0.8 MeV C ions resulted in a buried SiC precipitate layer of variable composition.


2006 ◽  
Author(s):  
Roisin Doherty ◽  
Brendan Mc Comb ◽  
Richard Ting ◽  
Yu Chin Cheng

1994 ◽  
Vol 9 (10) ◽  
pp. 2695-2702 ◽  
Author(s):  
N. Jiang ◽  
B.W. Sun ◽  
Z. Zhang ◽  
Z. Lin

A high resolution electron microscopic (HREM) study of interface structure between diamond film and its silicon substrate is presented. The HREM images reveal that there is an amorphous intermediate layer between the diamond film and its substrate for samples grown by hot filament chemical vapor deposition (HF-CVD). In some cases, β-SiC crystallites and a few graphite microcrystallites may be embedded in this amorphous layer. The HREM images obtained from cross-sectional specimens reveal that the diamond crystallites nucleate directly either on the amorphous intermediate layer, at diamond seed crystallites that were left during pretreatment of Si substrate by diamond paste,β-SiC particles, or at some scratches of the Si substrate. HREM images also reveal that the quantity, distribution, and the size of β-SiC particles in the intermediate layer are different for different processes. Some β-SiC crystallites have certain orientation relationships with the Si substrate. A HREM study of cross-sectional specimens indicates that twins and microtwins in the HF-CVD diamond film are formed during nucleation of the film either from diamond seeds, β-SiC crystallites, or the amorphous intermediate layer. Multiple twins formed from different β-SiC crystallites have also been observed. High densities of “V” shaped microtwins formed during the initial growth of the diamonds and the formation mechanism of these twins are discussed.


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