Blue Light Emission from Porous Silicon

1992 ◽  
Vol 283 ◽  
Author(s):  
X. Y. Hou ◽  
G. Shi ◽  
W. Wang ◽  
F. L. Zhang ◽  
P. H. Hao ◽  
...  

ABSTRACTThrough a post treatment of light emitting porous silicon in boilingwater, a large blue shift of its photoluminescence (PL) spectrum hasbeen observed and a stable blue-green light emission at the peak wavelength down to 500 nm is achieved. The effect of boiling water treatment is suggested to be a kind of oxidation, which could reduce thesize of the Si column, fill up some micropores and strengthen the Siskeleton. The photoluminescence microscopic observation shows that the surface of blue light emitting porous silicon is composed of manysmall uniformly light-emitting domains at the size of several tens of μm. Fourier transform infrared reflection (FTIR) measurements show that the formation of Si-H bonds is not responsible for the visible luminescence in the very thin Si wires.

1994 ◽  
Vol 08 (02) ◽  
pp. 69-92 ◽  
Author(s):  
XUN WANG

In this review article, we give a new insight into the luminescence mechanism of porous silicon. First, we observed a “pinning” characteristic of photoluminescent peaks for as-etched porous silicon samples. It was explained as resulting from the discontinuous variation of the size of Si nanostructures, i.e. the size quantization. A tight-binding calculation of the energy band gap widening versus the dimension of nanoscale Si based on the closed-shell Si cluster model agrees well with the experimental observations. Second, the blue-light emission from porous silicon was achieved by using boiling water treatment. By investigating the luminescence micrographic images and the decaying behaviors of PL spectra, it has been shown that the blue-light emission is believed to be originated from the porous silicon skeleton rather than the surface contaminations. The conditions for achieving blue light need proper size of Si nanostructures, low-surface recombination velocity, and mechanically strong skeleton. The fulfillment of these conditions simultaneously is possible but rather critical. Third, the exciton dynamics in light-emitting porous silicon is studied by using the temperature-dependent and picosecond time-resolved luminescence spectroscopy. A direct evidence of the existence of confined excitons induced by the quantum size effect has been revealed. Two excitation states are found to be responsible for the visible light emission, i.e. a higher lying energy state corresponding to the confined excitons in Si nanostructures and a lower lying state related with surfaces of Si wires or dots. A picture of the carrier transfer between the quantum confined state and the surface localized state has been proposed. Finally, we investigated the transient electroluminescence behaviors of Au/porous silicon/Si/Al structure and found it is very similar to that of an ordinary p-n junction light-emitting diode. The mechanism of electroluminescence is explained as the carrier injection through the Au/porous silicon Schotky barrier and the porous silicon/p-Si heterojunction into the corrugated Si wires, where the radiative recombination of carriers occurs.


2016 ◽  
Vol 24 (13) ◽  
pp. 15071 ◽  
Author(s):  
Cunlong Li ◽  
Zhigang Zang ◽  
Weiwei Chen ◽  
Zhiping Hu ◽  
Xiaosheng Tang ◽  
...  

1994 ◽  
Vol 33 (Part 1, No. 11) ◽  
pp. 6075-6077 ◽  
Author(s):  
Peter Steiner ◽  
Frank Kozlowski ◽  
Marek Wielunski ◽  
Walter Lang

1999 ◽  
Vol 588 ◽  
Author(s):  
Xingsheng Liu ◽  
Jesus Noel Calata ◽  
Houyun Liang ◽  
Wangzhou Shi ◽  
Xuanyin Lin ◽  
...  

AbstractThrough a comparative study of the light emission and light excitation property of porous silicon (PS) and Si oxide, photoluminescence (PL) and photoluminescence excitation (PLE) mechanisms for blue-light-emitting PS are analyzed. Strong blue light (445nm) and ultraviolet light (365nm) emission from silicon-rich silicon oxynitride films at room temperature were observed. An analysis of the PL and PLE spectra of PS and Si oxide indicated that for blue-light emission from PS, there are two types of photoexcitation processes: photo-excitation occurring in nanometer Si particles (NSP's) and in the Si oxide layers covering NSPs, and radiative recombination of electron-hole pairs taking place in luminescence centers (LCs) located on the interfaces between NSP's and Si oxide and those inside Si oxide layers. The PL spectra of silicon-rich silicon oxynitride films implies that the PL originated from some LCs in SiOx and SiOxNy:H, while PLE spectra indicates that photoexcitation occurs in NSPs, SiOx and SiOxNy:H. The 365 nm band is attributed to the former two photoexcitation processes and the 445 nm one to the third process. As such, the quantum confinement/luminescence center model appears to be a satisfactory model in explaining the experimental results.


2001 ◽  
Vol 78 (1) ◽  
pp. 37-39 ◽  
Author(s):  
Weili Liu ◽  
Miao Zhang ◽  
Chenglu Lin ◽  
Zhaoming Zeng ◽  
Lianwei Wang ◽  
...  

2005 ◽  
Vol 252 (4) ◽  
pp. 1065-1069 ◽  
Author(s):  
Yue Zhao ◽  
Deren Yang ◽  
Dongsheng Li ◽  
Minghua Jiang

1996 ◽  
Vol 45 (1) ◽  
pp. 121
Author(s):  
LIN JUN ◽  
ZHANG LI-ZHU ◽  
CHEN ZHI-JIAN ◽  
SONG HAI-ZHI ◽  
YAO DE-CHENG ◽  
...  

Nanoscale ◽  
2019 ◽  
Vol 11 (47) ◽  
pp. 22899-22906 ◽  
Author(s):  
Miao He ◽  
Chunyun Wang ◽  
Jingzhou Li ◽  
Jiang Wu ◽  
Siwei Zhang ◽  
...  

All-inorganic perovskite CsPbBr3–Cs4PbBr6 composite nanocrystals (NCs) were synthesized via a convenient solution process without inert gas protection and systematically studied as green phosphors for light emitting diode (LED) applications.


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