1982
DOI: 10.1016/0022-3093(82)90164-8
|View full text |Cite
|
Sign up to set email alerts
|

Structure of amorphous and glassy Sb2S3 and its connection with the structure of As2X3 arsenic chalcogenide glasses

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

3
39
0

Year Published

1997
1997
2018
2018

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 86 publications
(42 citation statements)
references
References 20 publications
3
39
0
Order By: Relevance
“…In agreement with the study of Cervinka and Hruby (32), we demonstrated the existence of weak bonds around 3.0 A > in the antimony environments. This present study confirms that the sequence of pyramidal coordination patterns leads to the gradual transition from layer-like to a random network in this system.…”
Section: Resultssupporting
confidence: 91%
See 1 more Smart Citation
“…In agreement with the study of Cervinka and Hruby (32), we demonstrated the existence of weak bonds around 3.0 A > in the antimony environments. This present study confirms that the sequence of pyramidal coordination patterns leads to the gradual transition from layer-like to a random network in this system.…”
Section: Resultssupporting
confidence: 91%
“…These weak bonds provide the cohesion between the successive layers. Cervinka and Hruby (32) have constructed a simple model of vitreous Sb S . In this model the explanation of the non-zero electron density of the radial electron density distribution curve in the region of 3 A > , was achieved by a suitable mutual orientation of elementary SbS E units shown in Fig.…”
Section: Vitreous Compoundsmentioning
confidence: 99%
“…This type of connection between the IRO and the thermal stability of the glass, observed in this work, was reported for As±Se glasses [43] where the inhibition of crystallization ability is accompanied by the growth of a FSDP. It was also reported for the excellent glass-former B 2 O 3 [29] for which the FSDP is the strongest peak in the diffraction pattern, for the poor glass-former Sb 2 S 3 [44] which exhibits a small FSDP in its diffraction pattern, and for Ge±Se [45], a very poor glassformer, where the FSDP is virtually eliminated.…”
mentioning
confidence: 50%
“…At Z=2.4, the layer structure is fully developed, exhibiting the maximal diffraction peak intensity, which decreases further with increasing the number of cross-linked sites [16]. The peak value of 2θ=40º is the shortest distance between Sb-S atoms suggesting the triple pyramid, Sb 2 S 3, units represent the basic building block of the network structure [17]. The grain size of the peak around 2θ=40º (Sb 2 S 3 phase) was calculated from XRD patterns by using Deby-Scherrer's formula; L=0.9λ/Bcosθ, where, B is the full-width at half-maximum (FWHM).…”
Section: Results and Discussion: Structural Characterizationsmentioning
confidence: 99%