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dc.contributor.author
Kopprio, Leonardo Hugo  
dc.contributor.author
Longeaud, Christophe  
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Schmidt, Javier Alejandro  
dc.date.available
2018-03-06T17:15:14Z  
dc.date.issued
2017-08  
dc.identifier.citation
Kopprio, Leonardo Hugo; Longeaud, Christophe; Schmidt, Javier Alejandro; Obtainment of the density of states in the band tails of hydrogenated amorphous silicon; American Institute of Physics; Journal of Applied Physics; 122; 8; 8-2017; 857021-8570210  
dc.identifier.issn
0021-8979  
dc.identifier.uri
http://hdl.handle.net/11336/37954  
dc.description.abstract
In this work, we present two new pairs of formulas to obtain a spectroscopy of the density of states (DOS) in each band tail of hydrogenated amorphous silicon (a-Si:H) from photoconductivity-based measurements. The formulas are based on the knowledge of the small-signal recombination lifetime τ′, the characteristic decay time of the concentration of trapped carriers generated in excess by the illumination, and that can be measured by methods like the Oscillating Photocarrier Grating (OPG) or Moving Grating Technique (MGT). First, we deduce the formulas and test their accuracy by numerical simulations using typical a-Si:H parameters. Next, we characterize an a-Si:H sample using well-known methods, like Fourier transform photocurrent spectroscopy to evaluate the valence band tail and modulated photoconductivity to measure the conduction band tail. We also performed measurements of steady-state photoconductivity, steady-state photocurrent grating and MGT, for a range of generation rates. From these measurements - and taking typical values for the capture coefficients, the extended states mobilities and the DOS at the band edges - we apply the new formulas to get the band tails. We find that the results obtained from the application of our formulas are in good agreement with those found with the traditional methods for both band tails. Moreover, we show that MGT/OPG measurement to get τ′ can be avoided if one of the band tails is measured by one of the traditional methods, since the known band tail can be used to evaluate τ′ with one pair of equations, and then the other pair can be applied to get the other band tail.  
dc.format
application/pdf  
dc.language.iso
eng  
dc.publisher
American Institute of Physics  
dc.rights
info:eu-repo/semantics/embargoedAccess  
dc.rights.uri
https://creativecommons.org/licenses/by/2.5/ar/  
dc.subject
Photoconductivity  
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Amorphous Silicon  
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Density of States  
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Condensed  
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Solar Cells  
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Band Structure  
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Computer Simulation  
dc.subject.classification
Astronomía  
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Ciencias Físicas  
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CIENCIAS NATURALES Y EXACTAS  
dc.title
Obtainment of the density of states in the band tails of hydrogenated amorphous silicon  
dc.type
info:eu-repo/semantics/article  
dc.type
info:ar-repo/semantics/artículo  
dc.type
info:eu-repo/semantics/publishedVersion  
dc.date.updated
2018-03-05T20:44:23Z  
dc.journal.volume
122  
dc.journal.number
8  
dc.journal.pagination
857021-8570210  
dc.journal.pais
Estados Unidos  
dc.description.fil
Fil: Kopprio, Leonardo Hugo. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Santa Fe. Instituto de Física del Litoral. Universidad Nacional del Litoral. Instituto de Física del Litoral; Argentina  
dc.description.fil
Fil: Longeaud, Christophe. Universite Pierre et Marie Curie; Francia. Centre National de la Recherche Scientifique; Francia  
dc.description.fil
Fil: Schmidt, Javier Alejandro. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Santa Fe. Instituto de Física del Litoral. Universidad Nacional del Litoral. Instituto de Física del Litoral; Argentina. Universidad Nacional del Litoral. Facultad de Ingeniería Química; Argentina  
dc.journal.title
Journal of Applied Physics  
dc.rights.embargoDate
2018-09-01  
dc.relation.alternativeid
info:eu-repo/semantics/altIdentifier/url/http://aip.scitation.org/doi/10.1063/1.4999626  
dc.relation.alternativeid
info:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1063/1.4999626