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Journal ArticleDOI

Photoconductivity and absorption in amorphous Si

TLDR
In this paper, the photoconductivity and absorption of Si specimens were measured at room temperature as a function of photon energy and Td in a spectral range from 0.5 eV to 3 eV and the absorption coefficient was determined for evaporated, sputtered and glow discharge specimens.
Abstract
The paper deals with photoconductivity and absorption in aSi specimens, prepared mainly by the decomposition of silane in a glow discharge. Substrate temperatures, Td, between 300 K and 650 K were used during deposition. The normalised photoresponse was measured at room temperature as a function of photon energy and Td in a spectral range from 0.5 eV to 3 eV. The absorption coefficient was determined for evaporated, sputtered and glow discharge specimens. The main features of the results are in agreement with conclusions drawn from previous electrical transport and field effect measurements and can be interpreted on the basis of the proposed model for the localised state distribution. It is confirmed that ϵc−ϵv is 1.5 to 1.6 eV, and that there is a local density of state maximum at about 1.2 eV below ϵc. At room temperature the steady photocurrent is carried predominantly by electrons in states above ϵc, whether excitation is from localized or extended states. Specimens prepared at Td > 500 K are highly photosensitive, with electron recombination lifetimes, τ, of up to 10−5s. Rise and decay times of the signal lie in the millisecond range. For Td < 500 K there is a drastic decrease in τ, which falls to 10−11 s at Td ⋍ 300 K and is even less for evaporated specimens. These results are discussed in some detail.

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Journal ArticleDOI

Reversible conductivity changes in discharge‐produced amorphous Si

TL;DR: In this paper, a new reversible photoelectronic effect was reported for amorphous Si produced by glow discharge of SiH4, where long exposure to light decreases both the photoconductivity and the dark conductivity.
Journal ArticleDOI

Amorphous silicon solar cell

TL;DR: In this article, thin film solar cells, ∼ 1 μm thick, have been fabricated from amorphous silicon deposited from a glow discharge in silane, and the cells were made in a p i n structure by using doping gases in the discharge.
Journal ArticleDOI

States in the gap and recombination in amorphous semiconductors

TL;DR: In this paper, states in the gap in amorphous silicon and chalcogenides and their effect on photoconductivity, luminescence and drift mobility are examined.
Journal ArticleDOI

Electronic properties of substitutionally doped amorphous Si and Ge

TL;DR: In this paper, it was shown that substitutional doping of an amorphous semiconductor is possible and can provide control of the electronic properties over a wide range, which corresponds to a movement of the Fermi level of 1·2 eV.
Journal ArticleDOI

Substitutional doping of amorphous silicon

TL;DR: In this article, it was shown that the electrical conductivity of a tetrahedral amorphous semiconductor can be controlled over many orders of magnitude by doping with substitutional impurities.
References
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Book

Electronic processes in non-crystalline materials

TL;DR: The Fermi Glass and the Anderson Transition as discussed by the authorsermi glass and Anderson transition have been studied in the context of non-crystalline Semiconductors, such as tetrahedrally-bonded semiconductors.
Journal ArticleDOI

Conduction in non-crystalline systems V. Conductivity, optical absorption and photoconductivity in amorphous semiconductors

TL;DR: In this article, the experimental evidence concerning the density of states in amorphous semiconductors and the ranges of energy in which states are localized is reviewed; this includes d.c and a.c. conductivity, drift mobility and optical absorption.
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