2003
DOI: 10.1063/1.1542414
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Elastic properties and phonon spectra of quasi-two-dimensional VSe2

Abstract: A recently developed method is used to make acoustic measurements of VSe2 single crystals. The components of the elastic constant tensor are determined from the data of these measurements. The experimental data are used to calculate the total and partial phonon densities of VSe2, which permit an explanation of the vibrational spectra of this compound.

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Cited by 10 publications
(8 citation statements)
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“…Using mean field theory, we estimated the Curie temperature of the bulk structure to be approximately 39 K and 17 K without a Hubbard-U and with U eff = 1.0 eV, respectively, which is significantly below the charge density transition temperature of 100 -110 K (see Table S1 and the corresponding text in the Supplemental Information). [40][41][42][43][44][45][46] A ferromagnetic ground state is thus not inconsistent with experimental evidence since undistorted 1T-VSe 2 is not stable in the temperature regime in which it would be ferromagnetic.…”
Section: A Stability Of Undistorted Vse2 Layers Withmentioning
confidence: 86%
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“…Using mean field theory, we estimated the Curie temperature of the bulk structure to be approximately 39 K and 17 K without a Hubbard-U and with U eff = 1.0 eV, respectively, which is significantly below the charge density transition temperature of 100 -110 K (see Table S1 and the corresponding text in the Supplemental Information). [40][41][42][43][44][45][46] A ferromagnetic ground state is thus not inconsistent with experimental evidence since undistorted 1T-VSe 2 is not stable in the temperature regime in which it would be ferromagnetic.…”
Section: A Stability Of Undistorted Vse2 Layers Withmentioning
confidence: 86%
“…For the 1Tpolytype, T c is predicted to be 35 K for optPBE and U eff = 1.0 eV, and 14 K for optB86b and U eff = 2.5 eV (∆E mag = 11 meV), which is below the experimentally observed charge density wave (CDW) transition temperature of 100 -110 K (onset). [40][41][42][43][44][45][46][52][53][54][55][56] This means that the magnetic transformation in the 1T-structure is unlikely to be observable as the 1T-polytype is unstable at such low temperatures.…”
Section: Monolayer Bilayermentioning
confidence: 99%
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“…It has been proposed that the presence of charge density waves could cause the quenching of monolayer ferromagnetism due to the band gap opening induced by Peierls distortion 19 . Phonon spectra of several VSe 2 and similar systems were also considered theoretically 20,21 . This modeling motivates us to study interplay between magnetism and structural phase transitions in VSe 2 .…”
Section: Introductionmentioning
confidence: 99%
“…This value is close to the previously reported value of 2.67 km/s. [52] In general, defects and imperfect contact can reduce the coherence of acoustic waves and induce different frequencies, which is independent of the material thickness. [49,53] Moreover, as shown in Fig.…”
Section: Interfacial Coherent Acoustic Phonon (Cap) Dynamics In Vbhsmentioning
confidence: 99%