Structural, Optical, and Thermophysical Properties of Mesoporous Silicon Layers: Influence of Substrate Characteristics

In this paper, the structural, optical, and thermal properties of n-type (100), p-type (100), and (111) mesoporous silicon (MePSi) are reported. The mesoporous silicon was prepared by an electrochemical process from the bulk silicon wafer. Depending on the etching depth, analyses show that the poros...

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Published in:Journal of physical chemistry. C Vol. 121; no. 14; pp. 7821 - 7828
Main Authors: Melhem, Amer, De Sousa Meneses, Domingos, Andreazza-Vignolle, Caroline, Defforge, Thomas, Gautier, Gaël, Sauldubois, Audrey, Semmar, Nadjib
Format: Journal Article
Language:English
Published: American Chemical Society 13-04-2017
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Abstract In this paper, the structural, optical, and thermal properties of n-type (100), p-type (100), and (111) mesoporous silicon (MePSi) are reported. The mesoporous silicon was prepared by an electrochemical process from the bulk silicon wafer. Depending on the etching depth, analyses show that the porosity of p-type (111) increased by 32 to 40% compared to p-type (100) which, in turn, increased by 22 to 48% compared to n-type (100). The structure morphology and the abundance of Si–O x and Si–H y also depended heavily on the type and crystal orientation of MePSi. The thermal properties of the MePSi layers such as thermal conductivity (κ), volumetric heat capacity (ρC p), and thermal contact resistance (R th) were determined using the pulsed photothermal method. The thermal conductivity of bulk silicon dropped sharply after etching, decreasing by more than 20-fold in the case of n-type (100) and by over 45-fold for p-type (100) and (111). According to the percolation model depending on both porosity and phonon confinement, the drop in thermal conductivity was mainly due to the nanostructure formation after etching. Thermal investigations showed that the volumetric heat capacity (ρC p) followed the barycentric model which depends mainly on the porosity. The thermal contact resistances of MePSi layers were estimated to be in the range of 1 × 10–8 to 1 × 10–7 K·m2·W–1.
AbstractList In this paper, the structural, optical, and thermal properties of n-type (100), p-type (100), and (111) mesoporous silicon (MePSi) are reported. The mesoporous silicon was prepared by an electrochemical process from the bulk silicon wafer. Depending on the etching depth, analyses show that the porosity of p-type (111) increased by 32 to 40% compared to p-type (100) which, in turn, increased by 22 to 48% compared to n-type (100). The structure morphology and the abundance of Si–O x and Si–H y also depended heavily on the type and crystal orientation of MePSi. The thermal properties of the MePSi layers such as thermal conductivity (κ), volumetric heat capacity (ρC p), and thermal contact resistance (R th) were determined using the pulsed photothermal method. The thermal conductivity of bulk silicon dropped sharply after etching, decreasing by more than 20-fold in the case of n-type (100) and by over 45-fold for p-type (100) and (111). According to the percolation model depending on both porosity and phonon confinement, the drop in thermal conductivity was mainly due to the nanostructure formation after etching. Thermal investigations showed that the volumetric heat capacity (ρC p) followed the barycentric model which depends mainly on the porosity. The thermal contact resistances of MePSi layers were estimated to be in the range of 1 × 10–8 to 1 × 10–7 K·m2·W–1.
Author Sauldubois, Audrey
Defforge, Thomas
Andreazza-Vignolle, Caroline
De Sousa Meneses, Domingos
Gautier, Gaël
Semmar, Nadjib
Melhem, Amer
AuthorAffiliation Université François Rabelais de Tours
ICMN-UMR 7374-CNRS
University of Orleans
GREMI-UMR 7344-CNRS
CEMHTI-UPR 3079-CNRS
CME
CNRS, CEA, INSA-CVL, GREMAN UMR 7347
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