1986
DOI: 10.1080/00018738600101871
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Properties of II–VI semiconductors associated with moving dislocations

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Cited by 151 publications
(101 citation statements)
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“…The average charge density was found to be close to -2← → 10 −10 Cm −1 for the dislocation bands predominantly consisting of S(g) dislocations and +1← →10 −10 Cm −1 for the dislocation bands predominantly consisting of Zn(g) dislocations, respectively. The former charge density is similar to the value of -3← →10 −10 Cm −1 found by Petrenko and Whitworth (1980) on moving S(g) dislocations in ZnS using the method of dislocation currents (Osip'yan et al 1986). Thus, the electric charges of resting Zn and S dislocations were determined quantitatively for the first time.…”
supporting
confidence: 63%
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“…The average charge density was found to be close to -2← → 10 −10 Cm −1 for the dislocation bands predominantly consisting of S(g) dislocations and +1← →10 −10 Cm −1 for the dislocation bands predominantly consisting of Zn(g) dislocations, respectively. The former charge density is similar to the value of -3← →10 −10 Cm −1 found by Petrenko and Whitworth (1980) on moving S(g) dislocations in ZnS using the method of dislocation currents (Osip'yan et al 1986). Thus, the electric charges of resting Zn and S dislocations were determined quantitatively for the first time.…”
supporting
confidence: 63%
“…The primary slip system is <110>{111} and the Burgers' vectors of perfect dislocations are a/2<110> (Holt 1962). The moving dislocations in the ZnS are Shockley partials with Burgers' vectors of a/6 <112> (Zaretskii et al 1983), which have a component of to along [110], and they move on the planes of the glide set (Osip'yan et al 1986). Another important feature of the sphalerite structure of ZnS is that dislocations with an edge component can be of two kinds, depending on whether the extra half-plane terminates in a row of metal or nonmetal atoms (Haasen 1957).…”
Section: Methodsmentioning
confidence: 99%
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