Si-On-Sapphire and Si Implanted with Zr Ions: Lattice Location, Solid Phase Epitaxial Regrowth, and Electrical Properties

1982 ◽  
Vol 14 ◽  
Author(s):  
I. Golecki ◽  
I. Suni

ABSTRACTZr ions have been implanted at 300 keV (Rp= 1400Å) and doses of 3×1012 − 3×l015 Zr/cm2 into Si-implanted, amorphous Sip layers on (100) bulk Si and Sion- sapphire. Rutherford backscattering and channeling spectrometry was used to study the Zr distribution and lattice location during solid-phase regrowth of the Si layers. The regrowth at 500—550°C stops at 3.4хl020 Zr/cm3, and Zr exhibits interface trapping and surface segregation effects. In this temperature range, Zr is essentially non-substitutional, and inactive electrically.

1988 ◽  
Vol 100 ◽  
Author(s):  
W. O. Adekoya ◽  
M. Hage-Ali ◽  
J. C. Muller ◽  
P. Siffert

ABSTRACTWe have studied the solid phase epitaxial regrowth (SPER) of implantation (31P+11B+ (73Ge+ preamorphized)) amorphized silicon in the temperature range 500–600°C induced by Rapid Thermal Annealing (RTA) using Rutherford Backscattering and channeling measurements (RBS). Our results show rate enhancements (≃ 3.5–6.5) of the velocities of regrowth in all studied cases with respect to literature-reported values for furnace-induced SPER. Also, the ratio VB/VP (velocity of regrowth in the presence of boron with respect to phosphorus) gives a value of approximately 3 in both RTA and furnace-induced kinetics. These results are explained by a model which takes into account the role of electrically-active interfacial defect sites during SPER.


2012 ◽  
Vol 101 (10) ◽  
pp. 103113 ◽  
Author(s):  
F. Panciera ◽  
K. Hoummada ◽  
M. Mastromatteo ◽  
D. De Salvador ◽  
E. Napolitani ◽  
...  

2000 ◽  
Vol 647 ◽  
Author(s):  
X. T. Ren ◽  
M. B. Huang

AbstractThe 1.5 µm luminescence from Si:Er is known to strongly depend on impurities (e.g. carbon) in silicon. In this work, we investigate the effect of carbon co-doping on the lattice location of Er atoms in Si by Rutherford backscattering(RBS)/channeling techniques. A float-zone (FZ) Si (100) wafer was first amorphized to a depth of ~ 0. 3 µm by Si ions implanted to a dose of ~ 1×1015cm2 at liquid nitrogen temperature. Carbon ions were then implanted into the amorphous silicon, which was recrystallized via solid phase epitaxial growth (SPEG) at 600°C following C implant. Finally Er ions were implanted into the C-doped and C-free Si crystals, with the substrate temperature at 25°C and 300°C respectively. The RBS/channeling results show that the Er redistribution and Si crystallinity are strongly affected by C co-doping. The incorporation of C into Si can significantly suppress Er surface segregation, and modify the lattice location of Er atoms in Si. We discuss these effects in terms of the formation of Er-C defect complexes.


2001 ◽  
Vol 78-79 ◽  
pp. 345-348
Author(s):  
I. Tsunoda ◽  
T. Nagata ◽  
Taizoh Sadoh ◽  
A. Kenjo ◽  
Masanobu Miyao

1975 ◽  
Vol 53 (3) ◽  
pp. 303-309 ◽  
Author(s):  
A. B. Campbell ◽  
J. B. Mitchell ◽  
J. Shewchun ◽  
D. A. Thompson ◽  
J. A. Davies

The radiation damage, implanted atom location, and electrical properties of nitrogen implanted germanium have been studied following anneals in the temperature range of 300–700 °C. Helium ion backscattering was used to measure the damage while two nuclear reactions, the 14N(d, α)12C and the 15N(p, α)12C, were used together with channeling techniques for the atom site location study. The results indicate that ~85% of the implanted nitrogen was located on nonsubstitutional sites, and also that the nitrogen did not outdiffuse from the germanium for anneals as high as 700 °C. The I–V characteristics of mesa structures formed in the implanted germanium indicate that, nitrogen had not become a donor in germanium.


1988 ◽  
Vol 3 (5) ◽  
pp. 914-921 ◽  
Author(s):  
T. Sands ◽  
E. D. Marshall ◽  
L. C. Wang

The solid-phase epitaxial regrowth of a III–V compound semiconductor by a two-stage reaction between a two-layer metallization and a compound semiconductor substrate is described. The regrowth process begins with a low-temperature reaction between a metal M (e.g. Ni, Pd, or Pt) and a compound semiconductor substrate, AB, to produce an intermediate M, AB or MB, phase. A subsequent reaction at a higher temperature between an overlayer of Si, Ge, Al, or In and the intermediate phase results in the decomposition of the intermediate phase and the epitaxial regrowth of a layer of the compound semiconductor. This regrowth mechanism is verified experimentally for the specific case of the Si/Ni/GaAs system. Rutherford backscattering spectrometry and transmission electron microscopy data show that the ternary phase Nix GaAs, formed during the initial stage of the reaction, decomposes toNiSi and GaAs by reaction with the Si overlayer. The incorporation of the overlayer element into the regrown semiconductor layer is proposed as a mechanism to explain the formation of Ohmic contacts in Si/Pd/n-GaAs, In/Pd/n-GaAs, In/Pt/n-GaAs, and similar two-layer metallization systems on n-GaAs.


1988 ◽  
Vol 100 ◽  
Author(s):  
S. Roorda ◽  
S. Saito ◽  
W. C. Sinke

ABSTRACTMicrocrystalline Si, as produced by explosive crystallization of an amorphous Si layer on (100) Si, shows a two-stage annealing behaviour. Initially, solid phase epitaxial regrowth occurs very rapidly at temperatures at, or above 800°C. After a few seconds, the regrowth rate slows down to the value typical for alignment of poly-Si. Solid phase epitaxial regrowth of microcrystalline Si is suggested to be strongly dependent on grain size and structure.


1994 ◽  
Vol 75 (8) ◽  
pp. 3936-3943 ◽  
Author(s):  
Z. Atzmon ◽  
M. Eizenberg ◽  
Y. Shacham‐Diamand ◽  
J. W. Mayer ◽  
F. Schäffler

2011 ◽  
Vol 88 (7) ◽  
pp. 1265-1268
Author(s):  
A. Ohata ◽  
Y. Bae ◽  
T. Signamarcheix ◽  
J. Widiez ◽  
B. Ghyselen ◽  
...  

1989 ◽  
Vol 54 (1) ◽  
pp. 42-44 ◽  
Author(s):  
B. T. Chilton ◽  
B. J. Robinson ◽  
D. A. Thompson ◽  
T. E. Jackman ◽  
J.‐M. Baribeau

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