1972
DOI: 10.1002/pol.1972.160100711
|View full text |Cite
|
Sign up to set email alerts
|

Pulsed photoconductivity and current oscillations in poly(vinyl chloride)

Abstract: SynopsisTransient photocurrents in poly(viny1 chloride) films are shown to be due to photoinjection of electrons from metallic cathodes. Most of the injected electrons are promptly trapped, but some drift across the sample to the anode under the inhence of an external electric field. The mobility of these electrons, determined by transient photoconductivity techniques, is 4.7 f 0.5 X 10-4 cma/V-sec at 27"C, and rises to 3.4 f 0.5 X 10-8 cma/V-sec at 43"C, the measuring cell having been evacuated to a pressure … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0
1

Year Published

1972
1972
1995
1995

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 11 publications
(2 citation statements)
references
References 26 publications
(1 reference statement)
0
1
0
1
Order By: Relevance
“…The time tT for which thermalised electrons will travel before being trapped is ( N m ) " (Bube 1974, p 333), where Nis the density of unoccupied electron traps, a i s the electron trap capture cross-section and U is the thermal velocity of electrons. Taking N = 10" cm-3 (Reiser et a1 1969, Creswell and Perlman 1970, Boustead and Charlesby 1970, a = lo-" cm2 and U = 10' cm S -' , we obtain tT = S. On the other hand, several pulsed radiation-induced-conductivity measurements on amorphous dielectrics show currents falling, due to trapping of electrons and holes, within a few ps of the end of the irradiation pulse (Szymanski and Labes 1969, Tabak 1970. Ranicar and Fleming 1972.…”
Section: Pseudo First-order Kinetics From Geminate Electron-hole Reco...mentioning
confidence: 94%
“…The time tT for which thermalised electrons will travel before being trapped is ( N m ) " (Bube 1974, p 333), where Nis the density of unoccupied electron traps, a i s the electron trap capture cross-section and U is the thermal velocity of electrons. Taking N = 10" cm-3 (Reiser et a1 1969, Creswell and Perlman 1970, Boustead and Charlesby 1970, a = lo-" cm2 and U = 10' cm S -' , we obtain tT = S. On the other hand, several pulsed radiation-induced-conductivity measurements on amorphous dielectrics show currents falling, due to trapping of electrons and holes, within a few ps of the end of the irradiation pulse (Szymanski and Labes 1969, Tabak 1970. Ranicar and Fleming 1972.…”
Section: Pseudo First-order Kinetics From Geminate Electron-hole Reco...mentioning
confidence: 94%
“…[1,2,3] ; la nature des porteurs, le mécanisme de leur déplacement et les effets de surface sont encore mal connus. Le chlorure de polyvinyle [4,5] (PVC) semble un matériau très intéressant pour ce type d'étude, son comportement étant très caractéristique. Le travail que nous exposons ici concerne des échantillons de PVC industriel (Plymouth).…”
unclassified