Recombination, multiplication, and transfer of electron-hole pairs in silicon nanocrystals: Effects of quantum confinement, doping, and surface chemistry

2021 ◽  
Vol 233 ◽  
pp. 117904
Author(s):  
N.V. Derbenyova ◽  
A.A. Konakov ◽  
V.A. Burdov
2010 ◽  
Vol 1 (13) ◽  
pp. 1957-1961 ◽  
Author(s):  
Navneethakrishnan Salivati ◽  
Nimrod Shuall ◽  
Joseph M. McCrate ◽  
John G. Ekerdt

2007 ◽  
Vol 204 (5) ◽  
pp. 1491-1496 ◽  
Author(s):  
A. Sa'ar ◽  
M. Dovrat ◽  
J. Jedrzejewsky ◽  
I. Popov ◽  
I. Balberg

2008 ◽  
Author(s):  
Anoop Gupta ◽  
Folarin Erogbogbo ◽  
Mark T. Swihart ◽  
Hartmut Wiggers

2019 ◽  
Author(s):  
Nathan Neale ◽  
Michael Carroll ◽  
Rens Limpens ◽  
Lance Wheeler ◽  
Gregory Pach

Author(s):  
H.S. Mavi ◽  
S. Rath ◽  
Arun Shukla

Laser-induced etching of silicon is used to generate silicon nanocrystals. The pore structure depends on the substrate type and etching laser wavelength. Porous silicon (PS) samples prepared by Nd:YAG laser (1.16 eV) etching of n-type substrate showed a fairly uniform and highly interconnected network of nearly circular pores separated by thin columnar boundaries, while no circular pits were produced by argon- ion laser (2.41 eV) etching under similar conditions. The size and size distribution of the nanocrystals are investigated by Raman and photoluminescence spectroscopies and analyzed within the framework of quantum confinement models.


1999 ◽  
Vol 588 ◽  
Author(s):  
S. Manotas ◽  
F. Agulló-Rueda ◽  
J. D. Moreno ◽  
R. J. Martín-Palma ◽  
R. Guerrero-Lemus ◽  
...  

AbstractWe have measured micro-photoluminescence (PL) and micro-Raman spectra on the cross section of porous silicon multilayers to sample different layer depths. We find noticeable differences in the spectra of layers with different porosity, as expected from the quantum confinement of electrons and phonons in silicon nanocrystals with different average sizes. The PL emission band gets stronger, blue shifts, and narrows at the high porosity layers. The average size can be estimated from the shift. The Raman phonon band at 520 cm−1 weakens and broadens asymmetrically towards the low energy side. The line shape can be related quantitatively with the average size by the phonon confinement model. To get a good agreement with the model we add a band at around 480 cm−1, which has been attributed to amorphous silicon. We also have to leave as free parameters the bulk silicon phonon frequency and its line width, which depend on temperature and stress. We reduced laser power to eliminate heating effects. Then we use the change of frequency with depth to monitor the stress. At the interface with the substrate we find a compressive stress in excess of 10 kbar, which agrees with the reported lattice mismatch. Finally, average sizes are larger than those estimated from PL.


2002 ◽  
Vol 80 (25) ◽  
pp. 4834-4836 ◽  
Author(s):  
G. Ledoux ◽  
J. Gong ◽  
F. Huisken ◽  
O. Guillois ◽  
C. Reynaud

2011 ◽  
Vol 248 (11) ◽  
pp. 2724-2727 ◽  
Author(s):  
M. Dossot ◽  
P. Miska ◽  
H. Rinnert ◽  
M. Vergnat ◽  
B. Humbert

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