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Correlation between the results of charge deep-level transient spectroscopy and ESR techniques for undoped hydrogenated amorphous silicon
Author(s) -
Vojtěch Nádaždy,
R. Durný,
I. Thurzo,
Emil Pinčík,
Akihiko Nishida,
Junichi Shimizu,
Minoru Kumeda,
Tatsuo Shimizu
Publication year - 2002
Publication title -
physical review. b, condensed matter
Language(s) - English
Resource type - Journals
eISSN - 1095-3795
pISSN - 0163-1829
DOI - 10.1103/physrevb.66.195211
Subject(s) - deep level transient spectroscopy , materials science , amorphous silicon , amorphous solid , silicon , spectroscopy , spectral line , atomic physics , band gap , semiconductor , charge (physics) , charge carrier , electron paramagnetic resonance , analytical chemistry (journal) , molecular physics , condensed matter physics , nuclear magnetic resonance , crystalline silicon , optoelectronics , chemistry , physics , crystallography , quantum mechanics , astronomy , chromatography
Results of charge deep-level transient spectroscopy (DLTS) and electron spin resonance (ESR) measurements on undoped hydrogenated amorphous silicon (a-Si:H) clearly demonstrate that a group of gap states with a mean energy of 0.82 eV as observed in charge DLTS experiments for a-Si:H based metal/oxide/semiconductor structure is the same as the g=2.0055 ESR defect (the Dz component). This correlation provides a distinct marker for charge DLTS technique. We obtained a very good fit to spectra obtained on undoped a-Si:H in the annealed state whilst there is some discrepancy between the experimental and simulated spectra for the light-soaked state. The first quantitative comparison of defect pool model with gap states directly observed by charge DLTS offers not only additional data for more accurate identification of all the intrinsic and light-induced defects. This also renders distinct counter-evidence to recently published conjectures about the creation of another charged defect during early stage of Staebler-Wronski effect. By contrast, our presented results clearly argue for opposite process, i.e., decay of positively charged defect states Dh

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