Tuning the Photoluminescence Peak Position of Si Nanocrystals by Chemical Etching

Author(s):  
J. R. Chen ◽  
D. C. Wang ◽  
M. Lu ◽  
C. Zhang ◽  
Y. Q. Zhang
2014 ◽  
Vol 116 (12) ◽  
pp. 123501 ◽  
Author(s):  
Mindaugas Karaliunas ◽  
Edmundas Kuokstis ◽  
Shao-Ying Ting ◽  
Jeng-Jie Huang ◽  
C. C. Yang

2009 ◽  
Vol 24 (7) ◽  
pp. 2259-2267 ◽  
Author(s):  
Fang Fang ◽  
Wei Zhang ◽  
Jian Sun ◽  
Ning Xu ◽  
Jiang Zhu ◽  
...  

Photoluminescence (PL) properties of SiOx thin films deposited by pulsed laser ablation of Si in a reactive oxygen ambient and annealed in a nitrogen atmosphere were studied at room temperature. Raman spectroscopy, Fourier transform infrared spectroscopy, and optical transmission measurements were used to characterize the deposited films before and after annealing and complement the PL studies. Strong PL due to quantum confinement was observed at room temperature from Si nanocrystals with an average diameter of approximately 5 nm at 325-nm light excitation. An apparent dependence of PL on the oxygen pressure for film deposition was observed. A detailed analysis of the effects of the annealing temperature revealed a significant PL evolution in luminescence intensity, spectrum profile, peak position, and spectrum range with the annealing temperature ranging from 300 to 1200 °C. Structural variations induced by thermal annealing of the films deposited at different oxygen pressures were also discussed on the basis of their correlation with the PL evolution.


2019 ◽  
Vol 19 (6) ◽  
pp. 3604-3609
Author(s):  
F Severiano ◽  
V. L Gayou ◽  
G García ◽  
J. A Luna-López ◽  
H. Martínez Gutiérrez ◽  
...  

In this article, physical characteristics of porous silicon (PS) obtained by electro chemical etching using HAuCl4 in the electrolyte are described. The morphological and optical features of PS decorated with gold-nanoparticles (AuNPs) were analyzed in function of the chemical etching time. The insertion of AuNPs inside the PS were performed simultaneously with the formation of the porous silicon layer. Scanning electron microscopy (SEM) analysis showed the formation and incorporation of AuNPs with an average size of 20 nm in the PS structure, which has a pore size of 1.5 μm. Also, it was possible to observe the loss of Si in function of the etching time. Photoluminescence spectroscopy analysis shows a decreasing of the PL intensity, which can be related to the presence of oxygen in the samples. Raman spectroscopy was used to estimate the size of the Si nanocrystals in the PS structure, which suffers a reduction in size due to the presence of HAuCl4 in the electrolyte.


Author(s):  
B. Monemar ◽  
J. P. Bergman ◽  
J. Dalfors ◽  
G. Pozina ◽  
B.E. Sernelius ◽  
...  

We present a study of the radiative recombination in In0.15Ga0.85N/GaN multiple quantum well samples, where the conditions of growth of the InGaN quantum layers were varied in terms of growth temperature (< 800 °C) and donor doping. The photoluminescence peak position varies strongly (over a range as large as 0.3 eV) with delay time after pulsed excitation, but also with donor doping and with excitation intensity. The peak position is mainly determined by the Stark effect induced by the piezoelectric field. In addition potential fluctuations, originating from segregation effects in the InGaN material, from interface roughness, and the strain fluctuations related to these phenomena, play an important role, and largely determine the width of the emission. These potential fluctuations may be as large as 0.2 eV in the present samples, and appear to be important for all studied growth temperatures for the InGaN layers. Screening effects from donor electrons and excited electron-hole pairs are important, and account for a large part of the spectral shift with donor doping (an upward shift of the photoluminescence peak up to 0.2 eV is observed for a Si donor density of 2 × 1018 cm−3 in the well), with excitation intensity and with delay time after pulsed excitation (also shifts up to 0.2 eV). We suggest a two-dimensional model for electron- and donor screening in this case, which is in reasonable agreement with the observed data, if rather strong localization potentials of short range (of the order 100 Å) are present. The possibility that excitons as well as shallow donors are impact ionized by electrons in the rather strong lateral potential fluctuations present at this In composition is discussed


2015 ◽  
Vol 9 (1) ◽  
pp. 91-94
Author(s):  
Wang Xiaoyang ◽  
Ren Keming ◽  
Zhou Zhen

The ZnCuO (x=6.27%) films under different annealing were prepared by the sol-gel method on grass. Using the X-ray diffraction (XRD), atomic force microscopy to study the influence of annealing on the microstructure and surface morphology of the film, the result of which shows that the annealing temperature did not change the wurtzite structure of ZnO and the film density under 400 degree annealing is evened out and is the best one.In the transmission spectra of zinc oxide (ZnO) films, the transmittance in the visible light range changes little with the shift of the annealing temperature, and the absorption edge assumes a hypsochromic shift. From the point of light spectrum at room temperature, annealing temperature changes photoluminescence peak position, not significantly changing the luminescence peak position of ZnO film, but make zinc deficiency increased with annealing and the obvious enhancement in the visible region photoluminescence peak.


2013 ◽  
Vol 1617 ◽  
pp. 81-84
Author(s):  
E. Vergara Hernandez ◽  
B. Perez Miltan ◽  
J. Jedrzejewski ◽  
I. Balberg

ABSTRACTThe effect of thermal annealing on the optical properties of Al2O3 films with different Si content was investigated by the photoluminescence method. Si-rich Al2O3 films were prepared by RF magnetron co-sputtering of the silicon and alumina targets on long quarts glass substrates. Photoluminescence (PL) spectra of freshly prepared Si-rich Al2O3 films are characterized by three PL bands with the peak positions at 2.97-3.00, 2.25-2.29 and 1.50 eV. The thermal annealing of the films at 1150 °C during 30 min stimulates the formation of Si nanocrystals (NCs) in the film area with Si content exceeded 60%. After the thermal annealing the PL intensity of all mentioned PL bands decreases and the new PL band appears with the peak position at 1.67 eV. The new PL band is attributed to the photo currier recombination inside of Si NCs. The size of NCs estimated from the PL peak position 1.67 eV of Si NC emission is about ∼-4.5-5.0 nm.The temperature dependences of PL spectra of Si-rich Al2O3 films have been studied in the range of 10-300K with the aim to reveal the mechanism of recombination transitions for mentioned above PL bands 2.97-3.00, 2.25-2.29 and 1.50 eV in freshly prepared films. The thermal activation of PL intensity and permanent PL peak positions in the temperature range 10-300K permit to assign these PL bands to defect related emission in Al2O3 matrix.


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