An alternative approach to understand the photoluminescence and the photoluminescence peak shift with excitation in porous silicon

2008 ◽  
Vol 104 (12) ◽  
pp. 123515 ◽  
Author(s):  
J. Anto Pradeep ◽  
Pratima Agarwal
1993 ◽  
Vol 62 (6) ◽  
pp. 642-644 ◽  
Author(s):  
Shu‐Lin Zhang ◽  
Kuok‐san Ho ◽  
Yongtian Hou ◽  
Bidong Qian ◽  
Peng Diao ◽  
...  

2015 ◽  
Vol 29 (15) ◽  
pp. 1550093 ◽  
Author(s):  
A. Cetinel ◽  
N. Artunç ◽  
G. Sahin ◽  
E. Tarhan

Effects of current density on nanostructure and light emitting properties of porous silicon (PS) samples were investigated by field emission scanning electron microscope (FE-SEM), gravimetric method, Raman and photoluminescence (PL) spectroscopy. FE-SEM images have shown that below 60 mA/cm 2, macropore and mesopore arrays, exhibiting rough morphology, are formed together, whose pore diameter, pore depth and porosity are about 265–760 nm, 58–63 μ m and 44–61%, respectively. However, PS samples prepared above 60 mA/cm 2 display smooth and straight macropore arrays, with pore diameter ranging from 900–1250 nm, porosity of 61–80% and pore depth between 63–69 μ m . Raman analyses have shown that when the current density is increased from 10 mA/cm 2 to 100 mA/cm 2, Raman peaks of PS samples shift to lower wavenumbers by comparison to crystalline silicon (c-Si). The highest Raman peak shift is found to be 3.2 cm -1 for PS sample, prepared at 90 mA/cm 2, which has the smallest nanocrystallite size, about 5.2 nm. This sample also shows a pronounced PL, with the highest blue shifting, of about 12 nm. Nanocrystalline silicon, with the smallest nanocrystallite size, confirmed by our Raman analyses using microcrystal model (MCM), should be responsible for both the highest Raman peak shift and PL blue shift due to quantum confinement effect (QCE).


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.


2020 ◽  
Author(s):  
Rabeb Layouni ◽  
Michael Dubrovsky ◽  
Mengdi Bao ◽  
Haejun Chung ◽  
Ke Du ◽  
...  

AbstractUsing porous silicon (PSi) interferometer sensors, we show the first experimental implementation of the high contrast probe cleavage detection (HCPCD) mechanism. HCPCD makes use of dramatic optical signal amplification caused by cleavage of high-contrast nanoparticle labels on probes instead of the capture of low-index biological molecules. An approximately 2 nm reflectance peak shift was detected after cleavage of DNA-quantum dot probes from the PSi surface via exposure to a 12.5 nM DNase enzyme solution for 2 hrs. This signal change is 20 times greater than the resolution of the spectrometer used for the interferometric measurements, and the interferometric measurements agree with the interferometric response predicted by simulations and fluorescence measurements. These proof of principle experiments show a clear path to real-time, highly sensitive and inexpensive point-of-care readout for a broad range of biological diagnostic assays that generate signal via nucleic acid cleavage.


1989 ◽  
Vol 71 (4) ◽  
pp. 233-236 ◽  
Author(s):  
Atsuko Yamaguchi ◽  
Tetsuya Tada ◽  
Kazuro Murayama ◽  
Toshiyuki Ninomiya

2000 ◽  
Vol 638 ◽  
Author(s):  
Z. Gaburro ◽  
G. Faglia ◽  
C. Baratto ◽  
G. Sberveglieri ◽  
L. Pavesi

AbstractWe experimentally demonstrate that porous silicon optical microcavities can be effectively used as multi-parametric gas sensors. As known, the photoluminescence intensity and electrical conduction of porous silicon are strongly dependent on environmental properties, such as the dipole moment of molecules of surrounding gases. The sensitivity is large due to the large surface/volume ratio of porous silicon. While these effects can be observed in any porous silicon structure, microcavities of porous silicon allow an additional sensing parameter, i.e. the spectral position of the resonance cavity peak. The position of the peak depends on the index of refraction of the environment, and gives independent additional information. Moreover, we show that the dynamic response of the peak shift is much faster comparing the other sensing parameters. The combined effects on the peak position, luminescence intensity and electrical conduction can allow discrimination between different substances, and therefore porous silicon optical microcavities can work as multi-parametric optical/electrical sensors. We report detection of 1 ppm of NO2 and 500 ppm of ethanol at room temperature. With NO2, the electrical conduction increases and PL quenches, but the peak does not shift, whereas the peak shifts with ethanol (no significant PL quenching is observed at 500 ppm). This suggests that discrimination between different species can be achieved.


1997 ◽  
Vol 71 (8) ◽  
pp. 1074-1076 ◽  
Author(s):  
Kai Shum ◽  
P. M. Mooney ◽  
J. O. Chu

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

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

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