1999
DOI: 10.1002/(sici)1521-3951(199901)211:1<287::aid-pssb287>3.0.co;2-c
|View full text |Cite
|
Sign up to set email alerts
|

Raman Scattering in CuCl under Pressure

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

1
1
0

Year Published

2004
2004
2022
2022

Publication Types

Select...
4
2

Relationship

1
5

Authors

Journals

citations
Cited by 10 publications
(2 citation statements)
references
References 17 publications
(30 reference statements)
1
1
0
Order By: Relevance
“…The band at 480 cm −1 can be attributed to S−S stretching vibrations, as it was reported for the 475 cm −1 band of CuS films and nanoparticles [22,23]. The band at 373 cm −1 was not reported among the Raman bands of CuCl [29,30] and CuS. We suppose that the Raman data generally verify the formation of polymeric one-dimensional CuS as a part of the hybrid interpolymeric PVA-CuS compound.…”
Section: Resultssupporting
confidence: 57%
“…The band at 480 cm −1 can be attributed to S−S stretching vibrations, as it was reported for the 475 cm −1 band of CuS films and nanoparticles [22,23]. The band at 373 cm −1 was not reported among the Raman bands of CuCl [29,30] and CuS. We suppose that the Raman data generally verify the formation of polymeric one-dimensional CuS as a part of the hybrid interpolymeric PVA-CuS compound.…”
Section: Resultssupporting
confidence: 57%
“…This resonance can be lifted by applying pressure. The TO phonon shifts up in frequency considerably faster than the LA + TA structure (because of the negative γ TA ), and at about 3 GPa the Fermi resonance has all but disappeared [46]: A nice Lorentzian peak appears at the frequency ω 0 . Similar effects can be produced by isotopic substitution since ω 0 shifts approximately like M Cl -1/2 , whereas the LA and TA frequencies shift like M Cu -1/2 [47].…”
Section: Pressure Dependence Of Phonon Lineshapesmentioning
confidence: 99%