Steplike behavior of photoluminescence peak energy and formation ofp‐type porous silicon

1993 ◽  
Vol 62 (6) ◽  
pp. 642-644 ◽  
Author(s):  
Shu‐Lin Zhang ◽  
Kuok‐san Ho ◽  
Yongtian Hou ◽  
Bidong Qian ◽  
Peng Diao ◽  
...  
2010 ◽  
Vol 663-665 ◽  
pp. 393-396
Author(s):  
Fu Ru Zhong ◽  
Xiao Yi Lv ◽  
Zhen Hong Jia

We have investigated the morphology and photoluminescence (PL) of Zinc Oxide (ZnO) and Zinc sulphide (ZnS) compound grown on porous silicon at room temperature. Under different excitation wavelengths (320 nm, 340nm, 370 nm), the photoluminescence (PL) spectra of PS-ZnS-ZnO composites were different, and at 550nm there is a strong photoluminescence peak. Energy dispersive spectroscopy (EDS) has been carried out to evaluate the existing of ZnO/ZnS compound. In addition, the scanning electron microscopy (SEM) observation shows that the morphology of the PS-ZnS-ZnO composites was well grown on porous silicon.


1995 ◽  
Vol 7 (3) ◽  
pp. 697-704 ◽  
Author(s):  
L Z Zhang ◽  
B Q Zong ◽  
B R Zhang ◽  
Z H Xu ◽  
J Q Li ◽  
...  

1994 ◽  
Vol 358 ◽  
Author(s):  
Adam A. Filios ◽  
Raphael Tsu

ABSTRACTPorous silicon samples prepared in the dark under "gentle" etching conditions clearly demonstrate effects of quantum confinement, such as a correlation of the photoluminescence peak energy with the downshift of the Raman line from 521 cm−1 for bulk silicon, and a blue shift in the remaining weak photoluminescence after thermal annealing. On the other hand, samples prepared under illumination as well as those heavily etched in the dark, though luminesce brightly, show no significant effects of quantum confinement, suggesting a different dominant mechanism for the observed luminescence.


1993 ◽  
Vol 298 ◽  
Author(s):  
Shulin Zhang ◽  
Kuoksan He ◽  
Yangtian Hou ◽  
Xin Wang ◽  
Jingjian Li ◽  
...  

AbstractA novel step—like and pinning behavior of photoluminescence peak energy connected with changes in the concentration of HIF and current density were for the first time observed for p— type porous silicon. Based on a theoretical calculation of the electron structure of the silicon quantum wire it is argued that these behaviors can be explained in terms of a novel formation mechanism model of porous silicon.


2021 ◽  
Vol 4 (1) ◽  
pp. 1-9 ◽  
Author(s):  
Fathallah Jabouti ◽  
Haddou El Ghazi ◽  
Redouane En-nadir ◽  
Izeddine Zorkani ◽  
Anouar Jorio

Based on the finite difference method, linear optical susceptibility, photoluminescence peak and binding energies of three first states of an exciton trapped by a positive charge donor-impurity ( ) confined in InN/AlN quantum well are investigated in terms of well size and impurity position. The electron, heavy hole free and bound excitons allowed eigen-values and corresponding eigen-functions are obtained numerically by solving one-dimensional time-independent Schrödinger equation. Within the parabolic band and effective mass approximations, the calculations are made considering the coupling of the electron in the n-th conduction subband and the heavy hole in the m-th valence subband under the impacts of the well size and impurity position. The obtained results show clearly that the energy, binding energy and photoluminescence peak energy show a decreasing behavior according to well size for both free and bound cases. Moreover, the optical susceptibility associated to exciton transition is strongly red-shift (blue-shifted) with enhancing the well size (impurity position).


1994 ◽  
Vol 332 ◽  
Author(s):  
H.Z. Song ◽  
L.Z. Zhang ◽  
B.R. Zhang ◽  
G.G. Qin

ABSTRACTIt was found that porous silicon (PS) layers formed on 0.01 Ωcm (111) and 0.02 Ωcm (100) Si substrates show high photoluminescence (PL) peak energies on both lower and higher porosity sides and a minimum of PL peak energy at the moderate porosity, while those formed on 0.8 and 10Ωcm (111) p-type Si substrates show an increase of PL peak energy with porosity on the lower side and a saturation of PL peak energy with porosity on the higher side. These experimental facts are not consistent with the quantum confinement model for light emission of PS, which predicts a monotonous increase of PL peak energy with PS porosity.


2014 ◽  
Vol 35 (9) ◽  
pp. 093001
Author(s):  
Wei Li ◽  
Peng Jin ◽  
Weiying Wang ◽  
Defeng Mao ◽  
Guipeng Liu ◽  
...  

1993 ◽  
Vol 71 (8) ◽  
pp. 1265-1267 ◽  
Author(s):  
Xun Wang ◽  
Daming Huang ◽  
Ling Ye ◽  
Min Yang ◽  
Pinghai Hao ◽  
...  

2009 ◽  
Vol 2009 ◽  
pp. 1-7 ◽  
Author(s):  
Pushpendra Kumar ◽  
Peter Lemmens ◽  
Manash Ghosh ◽  
Frank Ludwig ◽  
Meinhard Schilling

The most common fabrication technique of porous silicon (PS) is electrochemical etching of a crystalline silicon wafer in a hydrofluoric (HF) acid-based solution. The electrochemical process allows for precise control of the properties of PS such as thickness of the porous layer, porosity, and average pore diameter. The effect of HF concentration in the used electrolyte on physical and electronic properties of PS was studied by visual color observation, measuring nitrogen sorption isotherm, field emission type scanning electron microscopy, Raman spectroscopy, and photoluminescence spectroscopy. It was found that with decrease in HF concentration, the pore diameter increased. The PS sample with large pore diameter, that is, smaller nanocrystalline size of Si between the pores, was found to lead to a pronounced photoluminescence peak. The systematic rise of photoluminescence peak with increase of pore diameter and porosity of PS was attributed to quantum confinement. The changes in nanocrystalline porous silicon were also clearly observed by an asymmetric broadening and shift of the optical silicon phonons in Raman spectra. The change in electronic properties of PS with pore diameter suggests possibilities of use of PS material as a template for fundamental physics as well as an optical material for technological applications.


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