Time-resolved photoluminescence in porous silicon

1997 ◽  
Vol 72-74 ◽  
pp. 347-349 ◽  
Author(s):  
J. Kudrna ◽  
P. Bartošek ◽  
F. Trojánek ◽  
I. Pelant ◽  
P. Malý
2016 ◽  
Vol 70 (12) ◽  
pp. 1974-1980 ◽  
Author(s):  
Justin M. Reynard ◽  
Nathan S. Van Gorder ◽  
Caley A. Richardson ◽  
Richie D. Eriacho ◽  
Frank V. Bright

We report new instrumentation for rapidly and reliably measuring the temperature-dependent photoluminescence response from porous silicon as a function of analyte vapor concentration. The new system maintains the porous silicon under inert conditions and it allows on-the-fly steady-state and time-resolved photoluminescence intensity and hyper-spectral measurements between 293 K and 450 K. The new system yields reliable data at least 100-fold faster in comparison to previous instrument platforms.


1997 ◽  
Vol 71 (1) ◽  
pp. 13-20 ◽  
Author(s):  
X. Wu ◽  
R. White ◽  
U. Hömmerich ◽  
F. Namavar ◽  
A.M. Cremins-Costa

1998 ◽  
Vol 43 (4) ◽  
pp. 423-426 ◽  
Author(s):  
Yu. P. Piryatinskii ◽  
V. A. Semenovich ◽  
N. I. Klyui ◽  
A. G. Rozhin

2010 ◽  
Vol 506 (2) ◽  
pp. 496-499 ◽  
Author(s):  
M. Rahmani ◽  
H. Ajlani ◽  
A. Moadhen ◽  
M.-A. Zaïbi ◽  
L. Haji ◽  
...  

2001 ◽  
Vol 686 ◽  
Author(s):  
K. W. Cheah ◽  
Ling Xu ◽  
Xinfan Huang

Nano-ZnS was deposited into porous silicon. By varying the concentration of Zn2+ ion solution during nano-ZnS formation, the amount of nano-ZnS in porous silicon host can be controlled. The doped porous silicon exhibited a gradual shift in its photoluminescence peak from red to blue as a function of the nano-ZnS coverage. At an optimum doping, white light photoluminescence was obtained. A study in the luminescence lifetime showed that the radiative recombination at the blue end of the visible spectrum was due to nano-ZnS, whereas, luminescence emission at the red end of the visible spectrum came from porous silicon. The latter luminescence was due to in part tunneling of excited electrons from nanoZnS into porous silicon and in part direct excitation of porous silicon layer. Time-resolved photoluminescence also showed that radiative recombination was effectively dominated by the nano-ZnS. Photoluminescence excitation result revealed the presence of two excitation levels; one belonged to nano-ZnS at near uv region, and another at about 520 nm from the surface states of porous silicon and nano-ZnS. The doping of nano-ZnS into porous silicon demonstrates that luminescence color tuning is possible when an appropriate functional material is introduced into porous silicon.


1996 ◽  
Vol 198-200 ◽  
pp. 965-968 ◽  
Author(s):  
Shuji Komuro ◽  
Takitaro Morikawa ◽  
Patrick O'Keeffe ◽  
Yoshinobu Aoyagi

1994 ◽  
Vol 358 ◽  
Author(s):  
Julie M. Rehm ◽  
George L. McLendon ◽  
Leonid Tsybeskov ◽  
Philippe M. Fauchet

ABSTRACTWe have investigated the sensitivity of blue (PLmax = 480 nm) and red (PLmax = 660 nm) emitting porous silicon samples to various chemical adsorbates. Steady-state and time-resolved photoluminescence measurements and FTIR spectroscopy were employed to characterize the photophysical and optical effects induced by chemical exposure. The red samples, which are hydrogen terminated, exhibit quenching and recovery of photoluminescence intensity and broadening of the Si-Hx stretch bands upon exposure to liquid methanol. This behavior is attributed to the ability of the Si-Hx specie on the surface of the PSI to interact with the solvent molecules which temporarily traps the electrons and causes PL loss and Si-Hx broadening. The blue samples, which are oxygen terminated, display similar sensitivity to methanol. This sensitivity is attributed to the solvent's ability to change the surface passivation and thereby introduce competitive radiative and nonradiative recombination channels. The origin of the blue PL is discussed.


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