Distribution of Excess Charge Carriers in Bilateral Macroporous Silicon with Different Thicknesses of Porous Layers

Authors V.F. Onyshchenko
Affiliations

V.Ye. Lashkaryov Institute of Semiconductor Physics of National Academy of Sciences of Ukraine, 41, Nauky Ave, 03028 Kyiv, Ukraine

Е-mail onyshchenkovf@isp.kiev.ua
Issue Volume 13, Year 2021, Number 6
Dates Received 07 October 2021; revised manuscript received 01 December 2021; published online 20 December 2021
Citation V.F. Onyshchenko, J. Nano- Electron. Phys. 13 No 6, 06010 (2021)
DOI https://doi.org/10.21272/jnep.13(6).06010
PACS Number(s) 73.50.Pz
Keywords Bilateral macroporous silicon, Porous silicon (3) , Excess charge carriers.
Annotation

The paper presents a system of equations describing the distribution of excess charge carriers in bilateral macroporous silicon with different thicknesses of porous layers. The system contains equations, which are the general solution to the diffusion equation written for a monocrystalline substrate and each porous layer. Also, it contains equations describing the boundary conditions on two surfaces of a bilateral macro-porous silicon sample and on the boundaries of a monocrystalline substrate with macroporous layers. It was taken into account that light propagates through the pores and illuminates the monocrystalline substrate through the bottom of the pores. We calculated the distribution of excess charge carriers in bilateral macroporous silicon with different thicknesses of porous layers, provided that excess charge carriers are generated by light with wavelengths of 0.95 and 1.05 m. At these wavelengths, the generation of excess charge carriers was uniform and non-uniform over the sample, respectively. The calculations were carried out for the cases when one layer of macropores had a thickness of 100 m, while the other varied from zero to 400 m. It is shown that one or two maxima are observed in the distribution of excess charge carriers in bilateral macroporous silicon with different thicknesses of porous layers. The maximum can be located near surfaces that are illuminated by light or in the middle of a monocrystalline substrate. The maxima decrease due to the diffusion of charge carriers to the recombination surfaces. The distribution of excess charge carriers in bilateral macroporous silicon with different thicknesses of porous layers is affected by the recombination of excess charge carriers on the pore surface of each macroporous layer and the diffusion of excess charge carriers from the substrate to the recombination surfaces in porous layers.

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