Comment on “Optical absorption measurements of silica containing Si nanocrystals produced by ion implantation and thermal annealing” [Appl. Phys. Lett. 80, 1325 (2002)]

2002 ◽  
Vol 81 (7) ◽  
pp. 1357-1358 ◽  
Author(s):  
Leonid Khriachtchev
1995 ◽  
Vol 396 ◽  
Author(s):  
Jane G. Zhu ◽  
C. W. White ◽  
D. J. Wallis ◽  
J. D. Budai ◽  
S. P. Withrow

AbstractGaAs nanocrystals have been formed by the sequential ion implantation method. The sequence of Ga and As ion implantation (i.e., Ga + As or As + Ga) is found to affect the size distributions of GaAs nanocrystals significantly. The nanocrystal sizes are much bigger in the samples with Ga implanted first than those with As implanted first. This phenomenon is explained by the different diffusion behaviors of Ga and As species. Different precipitate regions have been observed in the samples implanted with Ga first and then As. Optical absorption measurements show that Ga particles have already formed in the as-implanted stage.


1998 ◽  
Vol 507 ◽  
Author(s):  
C. W. White ◽  
S. P. Withrow ◽  
A. Meldrum ◽  
J. D. Budai ◽  
D. M. Hembree ◽  
...  

ABSTRACTSi nanocrystals formed in SiO2 by high-dose ion implantation and annealing give rise to strong optical absorption and intense photoluminescence (PL). The dose dependence of optical absorption provides evidence for size-dependent quantum confinement in the Si nanocrystals. PL peak energies are nearly independent of dose suggesting that surface or interface states play an important role in PL. Estimates of absorption bandgaps in the nanocrystals are given.


2000 ◽  
Vol 650 ◽  
Author(s):  
Stephanie Cheylan ◽  
Robert G. Elliman

ABSTRACTThis paper explores the effect of hydrogen on the luminescence properties of silicon nanocrystals formed in silica by high-dose ion-implantation and thermal annealing. For samples implanted to low fluence (small nanocrystals), passivation is shown to result in a uniform enhancement of the PL emission for all wavelengths. However, for samples implanted to high fluence, preferential enhancement of the emission from larger nanocrystals is evident, resulting in a red-shift of emission spectra. Both the intensity enhancement and the red-shift are shown to be reversible, with spectra returning to their pre-passivation form when H is removed from the samples by annealing. The luminescence lifetime is also shown to increase after passivation, confirming that defect-containing nanocrystals luminesce.


Vacuum ◽  
2013 ◽  
Vol 89 ◽  
pp. 132-135
Author(s):  
J.X. Xu ◽  
X.H. Xiao ◽  
F. Ren ◽  
X.D. Zhou ◽  
G.X. Cai ◽  
...  

1995 ◽  
Vol 52 (2) ◽  
pp. 1405-1407 ◽  
Author(s):  
Arthur L. Ruoff ◽  
Kouros Ghandehari

1992 ◽  
Vol 72 (1) ◽  
pp. 73-77 ◽  
Author(s):  
H. B. Erzgräber ◽  
P. Zaumseil ◽  
E. Bugiel ◽  
R. Sorge ◽  
K. Tittelbach‐Helmrich ◽  
...  

1989 ◽  
Vol 147 ◽  
Author(s):  
Samuel Chen ◽  
S.-Tong Lee ◽  
G. Braunstein ◽  
G. Rajeswaran ◽  
P. Fellinger

AbstractDefects induced by ion implantation and subsequent annealing are found to either promote or suppress layer intermixing in Ill-V compound semiconductor superlattices (SLs). We have studied this intriguing relationship by examining how implantation and annealing conditions affect defect creation and their relevance to intermixing. Layer intermixing has been induced in SLs implanted with 220 keV Si+ at doses < 1 × 1014 ions/cm2 and annealed at 850°C for 3 hrs or 1050°C for 10 s. Upon furnace annealing, significant Si in-diffusion is observed over the entire intermixed region, but with rapid thermal annealing layer intermixing is accompanied by negligible Si movement. TEM showed that the totally intermixed layers are centered around a buried band of secondary defects and below the Si peak position. In the nearsurface region layer intermixing is suppressed and is only partially completed at ≤1 × 1015 Si/cm2. This inhibition is correlated to a loss of the mobile implantation-induced defects, which are responsible for intermixing.


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