The electron spin resonance (ESR) spectra of device quality poly-Si films (N-d = 7.8 x 10(16)/cm(3)) made by hot wire chemical vapor deposition show only an inhomogeneously broadened single line at g = 2.0055 +/- 0.0003 and peak to peak line width (Delta H-pp) of 0.76 mT. This line from the sample with the smaller concentration of defects is due to isolated defects with a g-tensor anisotropy with diagonal elements g(xx) = 2.0040 +/- 0.0003, g(yy) = 2.0030 +/- 0.0003, g(zz) = 2.0090 +/- 0.0003. However, for films with a larger defect density, the line width is less. A computer simulation of this ESR line shows that then are two contributions i.e., (1) a line with larger width as found for the smaller defect density materials and (2) a Lorentzian line with g = 2.005 +/- 0.0003 and Delta H-pp = 0.5 +/- 0.01 mT. We suggest that there are two types of spin systems in the material. The temperature dependence of the magnetic susceptibility, chi, shows that there are two contributions; (i) isolated defects (dangling bonds) which follow a simple Curie function and (ii) paired spins with anti-ferromagnetic coupling with a Weiss temperature of -136.4 i;;. The exchange coupling energy, J, in the interaction energy between the two spins in the dimer (E = -J S_1 S_2), is estimated to be 9.91 meV. We propose that there are regions at the grain boundary where the defects are clustered and are close enough to allow exchange interaction. The poly-Si:H films thus appear to have such a compact structure that the defects that have to be accommodated in the region between columns have a tendency to form clusters.

Clustered defects in hot wire chemical vapor deposited poly-silicon films

BARBON, ANTONIO;
2000

Abstract

The electron spin resonance (ESR) spectra of device quality poly-Si films (N-d = 7.8 x 10(16)/cm(3)) made by hot wire chemical vapor deposition show only an inhomogeneously broadened single line at g = 2.0055 +/- 0.0003 and peak to peak line width (Delta H-pp) of 0.76 mT. This line from the sample with the smaller concentration of defects is due to isolated defects with a g-tensor anisotropy with diagonal elements g(xx) = 2.0040 +/- 0.0003, g(yy) = 2.0030 +/- 0.0003, g(zz) = 2.0090 +/- 0.0003. However, for films with a larger defect density, the line width is less. A computer simulation of this ESR line shows that then are two contributions i.e., (1) a line with larger width as found for the smaller defect density materials and (2) a Lorentzian line with g = 2.005 +/- 0.0003 and Delta H-pp = 0.5 +/- 0.01 mT. We suggest that there are two types of spin systems in the material. The temperature dependence of the magnetic susceptibility, chi, shows that there are two contributions; (i) isolated defects (dangling bonds) which follow a simple Curie function and (ii) paired spins with anti-ferromagnetic coupling with a Weiss temperature of -136.4 i;;. The exchange coupling energy, J, in the interaction energy between the two spins in the dimer (E = -J S_1 S_2), is estimated to be 9.91 meV. We propose that there are regions at the grain boundary where the defects are clustered and are close enough to allow exchange interaction. The poly-Si:H films thus appear to have such a compact structure that the defects that have to be accommodated in the region between columns have a tendency to form clusters.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11577/1332957
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