1982
DOI: 10.1143/jpsj.51.2233
|View full text |Cite
|
Sign up to set email alerts
|

Anisotropy of Lattice Dynamical Properties in ZrS2 and HfS2

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

2
35
0

Year Published

1983
1983
2022
2022

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 33 publications
(37 citation statements)
references
References 21 publications
2
35
0
Order By: Relevance
“…The local environment of the tc-TMDs gives rise to two values of each component of the Born effective charge. 34 where we also provide the indirect band gap energy and compare to experimental data 75,77,79,[83][84][85]87,[102][103][104][105][106][107][108][109][110] .…”
Section: Structural and Electro-mechanical Propertiesmentioning
confidence: 99%
“…The local environment of the tc-TMDs gives rise to two values of each component of the Born effective charge. 34 where we also provide the indirect band gap energy and compare to experimental data 75,77,79,[83][84][85]87,[102][103][104][105][106][107][108][109][110] .…”
Section: Structural and Electro-mechanical Propertiesmentioning
confidence: 99%
“…Earlier studies have attributed the shoulder to the coupling of IR and Raman active modes due to a resonance effect, or, as mentioned above, to non-stoichiometry. 22,61,63,64 More recent studies have suggested nonharmonic effects such as the emission of low-energy acoustic phonon by optical phonon as the reason to the broadening 62 For the the IR active E u and A 2u modes, the splitting in Longitudinal optical (LO) and…”
Section: Ir/raman Spectramentioning
confidence: 99%
“…So far, however, the high-pressure effects on the vibrational properties of bulk HfS 2 have been investigated neither theoretically nor experimentally. With regard to ambient pressure conditions, several works dealing with the resonant and non-resonant Raman spectrum of bulk 1T-HfS 2 have been published in the literature 16 18 . All the previous studies report the first-order A 1 g and E g Raman-active modes, but there is some discrepancy with regard to a weak feature that appears at ~325 cm −1 as a low-frequency shoulder of the intense A 1 g peak.…”
Section: Introductionmentioning
confidence: 99%
“…All the previous studies report the first-order A 1 g and E g Raman-active modes, but there is some discrepancy with regard to a weak feature that appears at ~325 cm −1 as a low-frequency shoulder of the intense A 1 g peak. While some authors 16 , 18 assign this feature to a Raman-forbidden E u (LO) mode, Roubi and co-workers 17 attribute it to a forbidden A 2u (LO) mode. It should be noted, however, that half the frequency of this mode (~162 cm −1 ) is very close to the frequency of the zone-center E u (TO) measured by Lucovsky and co-workers (166 cm −1 ) with infrared (IR) reflectance spectroscopy 19 .…”
Section: Introductionmentioning
confidence: 99%