1994
DOI: 10.1103/physrevb.50.1489
|View full text |Cite
|
Sign up to set email alerts
|

π bonding versus electronic-defect generation: An examination of band-gap properties in amorphous carbon

Abstract: The electronic properties of amorphous carbon structures with varying microscopic mass densities, ranging from 2.0 to 3.52 g/cm, are analyzed. Using a semiempirical density-functional approach the model structures were generated by molecular dynamics performing a simulated cooling of liquid carbon clusters, containing 128 atoms, within periodically arranged cubic supercells. By investigation of properties related to chemical bonding we find a strong control of the band gap by the balance between x bonding and … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

4
38
0

Year Published

1996
1996
2018
2018

Publication Types

Select...
8
1
1

Relationship

1
9

Authors

Journals

citations
Cited by 108 publications
(42 citation statements)
references
References 34 publications
4
38
0
Order By: Relevance
“…4 -7 The common feature of these films is the C bonding degeneracy, leading to the various concentration of nondiamond ͑mainly sp 2 ) bonded carbon. This fact has a significant influence not only on the film structure but also on the film electronic properties such as the width of the band gap and the density of states in it 8 and consequently to the electric transport and optical properties. 9 As a rule, the spin density in the band gap is often more then 10 18 cm Ϫ3 in the a-C films 10 and results in pinning of the Fermi level thus making it difficult to change electronic properties by doping.…”
Section: Introductionmentioning
confidence: 99%
“…4 -7 The common feature of these films is the C bonding degeneracy, leading to the various concentration of nondiamond ͑mainly sp 2 ) bonded carbon. This fact has a significant influence not only on the film structure but also on the film electronic properties such as the width of the band gap and the density of states in it 8 and consequently to the electric transport and optical properties. 9 As a rule, the spin density in the band gap is often more then 10 18 cm Ϫ3 in the a-C films 10 and results in pinning of the Fermi level thus making it difficult to change electronic properties by doping.…”
Section: Introductionmentioning
confidence: 99%
“…First, we describe the electronic and optical properties of FCVA deposited a-C as a function of the ion energy and relate them to models of electronic structure. [16][17][18][19] We also report on the effect of deposition temperature on the structural characteristics of FCVA deposited a-C films with particular reference to the optical and electronic properties. Related studies have been carried out on a-C prepared by other methods.…”
mentioning
confidence: 99%
“…This structural change would occur when the distorted bonds are relaxed during the deposition, because the misorientation between orbitals corresponding to a bent or twisted bond creates paramagnetic defects. 19,20 For example, relaxation of the highly distorted sp 2 clusters results in a decreasing number of unpaired electrons and thus a smaller ESR signal. Relaxation of the twisted sp 2 bonds would also reduce the ESR signal.…”
Section: Resultsmentioning
confidence: 99%