scholarly journals Pore Morphology of Heavily Doped P-Type Porous Silicon

Proceedings ◽  
2018 ◽  
Vol 4 (1) ◽  
pp. 14 ◽  
Author(s):  
David Martín-Sánchez ◽  
Salvador Ponce-Alcántara ◽  
Jaime García-Rupérez

Tuning the pore diameter of porous silicon (PS) is essential for some applications such as biosensing, where the pore size can filter the entrance of some analytes or increase its sensitivity. However, macropore (>50 nm) formation on p-type silicon is still poorly known due to the strong dependence on resistivity. Electrochemically etching heavily doped p-type silicon usually forms micropores (<5 nm), but it has been found that bigger sizes can be achieved by adding an organic solvent to the electrolyte. In this work, we present the results of using dimethylformamide (DMF), dimethylsulfoxide (DMSO), potassium hydroxide (KOH) and sodium hydroxide (NaOH) for macropore formation in p-type silicon with a resistivity between 0.001 and 0.02 Ω∙cm, achieving pore sizes from 5 to 100 nm.

2019 ◽  
Vol 166 (2) ◽  
pp. B9-B12 ◽  
Author(s):  
David Martín-Sánchez ◽  
Salvador Ponce-Alcántara ◽  
Paula Martínez-Pérez ◽  
Jaime García-Rupérez

2013 ◽  
Vol 50 (37) ◽  
pp. 3-11
Author(s):  
E. Ossei-Wusu ◽  
J. Carstensen ◽  
E. Quiroga-Gonzalez ◽  
M. Amirmaleki ◽  
H. Foll
Keyword(s):  

1999 ◽  
Vol 146 (9) ◽  
pp. 3309-3314 ◽  
Author(s):  
R. B. Wehrspohn ◽  
F. Ozanam ◽  
J. ‐N. Chazalviel

2000 ◽  
Vol 638 ◽  
Author(s):  
Carlos Navarro ◽  
Luis F. Fonseca ◽  
Guillermo Nery ◽  
O. Resto ◽  
S. Z. Weisz

AbstractThe maximum photoresponse of a normal silicon photodetector, that uses a p-n junction as the active zone, is obtained when the incident radiation wavelength is around 750nm. This response diminishes significantly when the incident radiation is near or in the UV region. Meanwhile, nanocrystalline silicon (nc-Si) films with high transparency above 650nm and high absorbance in the UV can be prepared. By quantum confinement effects, a fraction of this absorbed UV energy is re-emitted as visible photons that can be used by the junction. We study the enhancement of the UV-photoresponse of two silicon detector prototypes with a silicon p-n junction active zone and with a photoluminescent nc-Si overlayer. One prototype is made with a porous silicon/n-type silicon/p-type silicon/p++-silicon/metal configuration and the other with an Eu-doped Si-SiO2 overlayer instead of the porous silicon one. The comparison between both prototypes and the control is presented and discussed stressing on the enhancement effect introduced by the photoluminescent overlayers, stability and reproducibility.


2002 ◽  
Vol 149 (1) ◽  
pp. G70 ◽  
Author(s):  
A. Vyatkin ◽  
V. Starkov ◽  
V. Tzeitlin ◽  
H. Presting ◽  
J. Konle ◽  
...  

1991 ◽  
Vol 234 ◽  
Author(s):  
Cronin B. Vining

ABSTRACTA model is presented for the high temperature transport properties of large grain size, heavily doped p-type silicon-germanium alloys. Good agreement with experiment (±10%) is found by considering acoustic phonon and ionized impurity scattering for holes and phonon-phonon, point defect and hole-phonon scattering for phonons. Phonon scattering by holes is found to be substantially weaker than phonon scattering by electrons, which accounts for the larger thermal conductivity values of ptype silicon-germanium alloys compared to similarly doped n-type silicongermanium alloys. The relatively weak scattering of long-wavelength phonons by holes raises the possibility that p-type silicon-germanium alloys may be improved for thermoelectric applications by the addition of an additional phonon scattering mechanism which is effective on intermediate and long-wavelength phonons. Calculations indicate improvements in the thermoelectric figure of merit up to 40% may be possible by incorporating several volume percent of 20 Å radius inclusions into p-type silicon-germanium alloys.


Author(s):  
V. N. MIRONOV ◽  
◽  
O. G. PENYAZKOV ◽  
P. N. KRIVOSHEYEV ◽  
Y. A. BARANYSHYN ◽  
...  

The ability of porous silicon to actively participate in oxidative reactions leading to combustion and explosion when interacting with reagents in the pores was established about twenty years ago [1] but because of the high propagation velocities of these physicochemical transformations (102-103 m/s), it was di©cult to understand their mechanisms.


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