Preparation of Hydrogenated Amorphous Silicon and Its Characterization by Transient Photoconductivity

Preparation of Hydrogenated Amorphous Silicon and Its Characterization by Transient Photoconductivity PDF Author: Christopher M. Walker
Publisher:
ISBN:
Category : Amorphous semiconductors
Languages : en
Pages : 320

Book Description


Preparation and Characterization of Hydrogenated Amorphous Silicon Films

Preparation and Characterization of Hydrogenated Amorphous Silicon Films PDF Author: Hwa Chao
Publisher:
ISBN:
Category : Amorphous semiconductors
Languages : en
Pages : 81

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The Physics of Hydrogenated Amorphous Silicon I

The Physics of Hydrogenated Amorphous Silicon I PDF Author: J.D. Joannopoulos
Publisher: Springer
ISBN: 9783540128076
Category : Science
Languages : en
Pages : 312

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With contributions by numerous experts

Preparation and Characterization of Hydrogenated Amorphous Silicon

Preparation and Characterization of Hydrogenated Amorphous Silicon PDF Author: James Jackson Sluss
Publisher:
ISBN:
Category : Amorphous substances
Languages : en
Pages : 110

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The Physics of Hydrogenated Amorphous Silicon I

The Physics of Hydrogenated Amorphous Silicon I PDF Author: J. D. Joannopoulos
Publisher:
ISBN: 9783662308578
Category :
Languages : en
Pages : 308

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Low Temperature Photoconductivity of Hydrogenated Amorphous Silicon (a-Si:H) Thin Flims

Low Temperature Photoconductivity of Hydrogenated Amorphous Silicon (a-Si:H) Thin Flims PDF Author: Gökhan Erdoğan
Publisher:
ISBN:
Category :
Languages : en
Pages : 166

Book Description
In this study low temperature photoconductivity of undoped hydrogenated amorphous silicon(a-Si:H) thin films have been studied to investigate the effect of native and Staebler-Wronski defects. The study covers undoped a-Si:H films prepared by various deposition techniques such as DC glow discharge, RF-PECVD with and without H-dilution, RF magnetron sputtering and hot-wire(HW) CVD.In the annealed state, the samples were characterized using temperature dependence of dark conductivity, steady-state photoconductivity, .ph, versus light intensity at room temperature and steady-state photoconductivity versus temperature down to 90 0K at three different intensities. Activation energy ,EF, of the samples changes from 0.60 eV to 1.0 eV. .ph shows a few orders of magnitude higher values from the dark conductivity and its magnitude is sample dependent due to differences in deposition conditions. The intensity dependence of .ph ,., (.ph . F.) is close to unity and varies between 0.70 to 0.90, indicating recombination kinetics through the midgap defect states in the bandgap of a-Si:H. Low temperature photoconductivity versus 1000/T spectrum shows three distinctly different regions. In Region I, .ph decreases with temperature until a transition temperature. Then Region II begins, where .ph begins to increase resulting a peak in spectrum or remains to be unchanged until a second transition temperature to Region III, where .ph continuously decreases with T. Transition temperatures and the degree of increase in .ph in Region II is sample dependent. These results indicate the presence of at least two different types of midgap defect states in the bandgap and exponential tail state present in the annealed state.In the light soaked state, Staebler-Wronski effect (SWE) was investigated after exposing the samples to white light illumination of a few suns intensity. The characterization involves dark conductivity and steady-state photoconductivity at room temperature and .ph versus temperature down to 90 0K for different intensities. Dark conductivity values decreased a certain factor indicating a slight shift in EF through midgap. .ph values decreased substantially from its annealed values due to creation of Steabler-Wronski defects in the bandgap. The intensity dependence of .ph become almost equal and close to unity for all the films even it shows slight variation in the annealed state. The shape of low temperature photoconductivity spectra becomes almost the same for all samples even drastic differences were observed in the annealed state. The spectrum is mainly dominated by only two regions.Region I dominates from room temperature down to 170 0K, where .ph decreases with a constant slope as T decreases. After that temperature, Region II sets in. .ph remains to be constant until temperature used in this study. Region III can only be detected at higher intensity and temperatures lower than 90 0K. Results indicate that more defects around the midgap are created by light, which decrease .ph and relatively less defects are created away from midgap and closer to band edge, which improve .ph instead of decreasing it as temperature decreases. The defect states in Region I responsible for decreasing .ph are more likely that they are neutral silicon dangling bond defects ,D0, and those in Region II responsible for increasing .ph are non-D0 defect states. They act as photosensitising defects with a very low capture cross-sections for electrons. They could be charged silicon dangling bonds ,D+ and D-, or floating bonds results in defect models proposed for a-Si:H.

The Physics of Hydrogenated Amorphous Silicon

The Physics of Hydrogenated Amorphous Silicon PDF Author: John D. Joannopoulos
Publisher: Springer
ISBN: 9780387128085
Category : Silicon
Languages : en
Pages : 385

Book Description


Characterization of Hydrogenated Amorphous Silicon Using the Constant Photocurrent Method

Characterization of Hydrogenated Amorphous Silicon Using the Constant Photocurrent Method PDF Author: Jin Miao Shen
Publisher:
ISBN:
Category : Absorption spectra
Languages : en
Pages : 94

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Preparation and Characterization of Hydrogenated Amorphous Silicon

Preparation and Characterization of Hydrogenated Amorphous Silicon PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 12

Book Description


SERI Photovoltaic Advanced Research and Development Bibliography, 1982-1985

SERI Photovoltaic Advanced Research and Development Bibliography, 1982-1985 PDF Author:
Publisher:
ISBN:
Category : Photovoltaic power generation
Languages : en
Pages : 180

Book Description