2006
DOI: 10.1016/j.jlumin.2006.08.004
|View full text |Cite
|
Sign up to set email alerts
|

Silicon nanocrystals in silica—Novel active waveguides for nanophotonics

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
5
0

Year Published

2007
2007
2017
2017

Publication Types

Select...
5
1
1

Relationship

0
7

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 21 publications
0
5
0
Order By: Relevance
“…It is almost certain that within the duration of the excitation pulse, nonlinear recombination processes (both radiative and non-radiative) occur in the excited Si-ncs, since, estimating the absorption cross section of Si-ncs at 400 nm for the samples with 20% excess Si concentration to be σ ≈ 2 × 10 −16 cm 2 [9,10] and considering the pump energy density of ∼10 mJ cm −2 , we get the initial mean number of electronhole pairs per nanocrystal as high as 3-5 (nevertheless, we were checking carefully that the pump power density was always below the threshold for irreversible sample changes, i.e. below the threshold for writing down a 'permanent grating' [11]). These nonlinear recombination processes in principle can be described by nonlinear terms in the relevant kinetic equations dealing with the time evolution of the LIG carrier population [4,12] and could manifest themselves through a non-exponential decay of the LIG diffraction efficiency in time.…”
Section: Resultsmentioning
confidence: 99%
“…It is almost certain that within the duration of the excitation pulse, nonlinear recombination processes (both radiative and non-radiative) occur in the excited Si-ncs, since, estimating the absorption cross section of Si-ncs at 400 nm for the samples with 20% excess Si concentration to be σ ≈ 2 × 10 −16 cm 2 [9,10] and considering the pump energy density of ∼10 mJ cm −2 , we get the initial mean number of electronhole pairs per nanocrystal as high as 3-5 (nevertheless, we were checking carefully that the pump power density was always below the threshold for irreversible sample changes, i.e. below the threshold for writing down a 'permanent grating' [11]). These nonlinear recombination processes in principle can be described by nonlinear terms in the relevant kinetic equations dealing with the time evolution of the LIG carrier population [4,12] and could manifest themselves through a non-exponential decay of the LIG diffraction efficiency in time.…”
Section: Resultsmentioning
confidence: 99%
“…The presence of excess silicon increases the refractive index of silicon dioxide and can therefore be used to define a waveguide structure [55]. The near-Gaussian depth distribution produced by silicon implantation is well suited to such applications as it naturally forms an asymmetric slab waveguide that confines light at a known depth beneath the surface.…”
Section: Waveguides and All-optical Amplifiersmentioning
confidence: 99%
“…Optical gain has been reported in ion-implanted silicon nanocrystal composites [42,43]. The waveguiding properties of silicon nanocrystal layers have been extensively investigated [44] and the relevant optical cross sections are well known (e.g., [45]). …”
Section: Light-emitting Materialsmentioning
confidence: 99%