Dielectric double layers of thermal silicon dioxide–chemical vapour deposition (CVD) silicon nitride are found to produce excellent passivation of silicon surfaces by combining a chemical reduction of surface defect states, with a field effect reduction of carriers at the surface due to charge in the dielectrics. The charge present in such double-layers has previously been attributed to be characteristic of the interface between the two. However, experimental evidence shows this is indirect and inconclusive. This manuscript reports direct measurements that show the charge lies within 10 nm of the interface between passivating double layers of thermal silicon dioxide–plasma CVD silicon nitride. In addition, the passivation efficiency of oxid...
The surface passivation of p- and n-type silicon by different chemically grown SiO2 films (prepared ...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
In this article, field-effect surface passivation is characterised as either intrinsic or extrinsic,...
Passivation of silicon surfaces remains a critical factor in achieving high conversion efficiency in...
AbstractSurface recombination of carriers in solar cells can cause a significant reduction in their ...
Surface recombination of carriers in solar cells can cause a significant reduction in their efficien...
For the passivation of p-type silicon surfaces, we investigate layer systems consisting of a thin la...
Surface passivation continues to be a significant requirement in achieving high solar-cell efficienc...
AbstractSurface recombination of carriers in solar cells can cause a significant reduction in their ...
Surface passivation continues to be a significant requirement in achieving high solar-cell efficienc...
In this work we investigated the properties of silicon oxide (SiOy) and silicon nitride (SiNx) layer...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
Effective reduction of front surface carrier recombination is essential for high efficiency silicon ...
AbstractSurface passivation by double layers made of hydrogenated amorphous silicon (a-Si:H) and hyd...
The surface passivation of p- and n-type silicon by different chemically grown SiO2 films (prepared ...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
In this article, field-effect surface passivation is characterised as either intrinsic or extrinsic,...
Passivation of silicon surfaces remains a critical factor in achieving high conversion efficiency in...
AbstractSurface recombination of carriers in solar cells can cause a significant reduction in their ...
Surface recombination of carriers in solar cells can cause a significant reduction in their efficien...
For the passivation of p-type silicon surfaces, we investigate layer systems consisting of a thin la...
Surface passivation continues to be a significant requirement in achieving high solar-cell efficienc...
AbstractSurface recombination of carriers in solar cells can cause a significant reduction in their ...
Surface passivation continues to be a significant requirement in achieving high solar-cell efficienc...
In this work we investigated the properties of silicon oxide (SiOy) and silicon nitride (SiNx) layer...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
Effective reduction of front surface carrier recombination is essential for high efficiency silicon ...
AbstractSurface passivation by double layers made of hydrogenated amorphous silicon (a-Si:H) and hyd...
The surface passivation of p- and n-type silicon by different chemically grown SiO2 films (prepared ...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...
Recombination at the semiconductor surface continues to be a major limit to optoelectronic device pe...