1975
DOI: 10.1071/ph750057
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Phonon Dispersion Relations for Chromium and Tantalum

Abstract: Aust. J. Phys., 1975, 28, 57-61 Phonon dispersion curves for the normal modes of vibration in chromium and tantalum are calculated along the symmetry directions [100], [110] and [111] using the five force-constant model of Behari and Tripathi (1970a). The results are compared with experimental values obtained from inelastic neutron spectroscopy and reasonably good agreement is found.

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Cited by 12 publications
(6 citation statements)
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“…for Ta [24,25]. The dispersions for the substrates follow their orientation: Γ for c-sapphire, and for Si [26,27].…”
Section: Modeling Of G For the Metal-interlayer-substrate Systemmentioning
confidence: 95%
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“…for Ta [24,25]. The dispersions for the substrates follow their orientation: Γ for c-sapphire, and for Si [26,27].…”
Section: Modeling Of G For the Metal-interlayer-substrate Systemmentioning
confidence: 95%
“…Interlayer Substrate Al Ni α-Al 2 O 3 θ D = 428 K [51] θ D = 450 K [51] θ D = 1035 K [53] ν L = 9.6 THz [52] ν L = 9.1 THz [29] ν L = 10 THz [31] ν T = 5.7 THz [52] ν T = 4.5 THz [29] ν T = 6.9 THz [31] g = 0.24 × 10 18 W (m −3 •K −1 ) [51] g = 0.36 × 10 18 W (m −3 •K −1 ) [51] ν optical = 26 THz [31] Au Ta Si θ D = 165 K [51] θ D = 225 K [55] θ D = 645 K [57] ν L = 4.6 THz [54] ν L = 5.5 THz [28] ν L = 12 THz [30] ν T = 2.8 THz [54] ν T = 2.6 THz, 3.7 THz [28] ν T = 4 THz [30] g = 0.023 × 10 18 W (m −3 •K −1 ) [51] g = 3.1 × 10 18 W (m −3 •K −1 ) [56] ν optical = 15.5 THz [30] Cr θ D = 630 K [38] ν L = 10 THz [28] ν T = 6 THz, 7.7 THz [28] g = 0.42 × 10 18 W (m −3 •K −1 ) [58]…”
Section: Top Metalmentioning
confidence: 99%
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“…Metals were 50 nm thick and interlayers 5 nm thick. [41] ν T = 6 THz, 7.7 THz [42] ν T = 6.9 THz [43] ν A = 3.4 THz ν A = 7.9 THz ν A = 7.9 THz g = 0.023 × 10 18 g = 0.42 [51] ν optical = 16 THz [50] even for materials that are not well characterized in the literature.…”
Section: Interlayer Selectionmentioning
confidence: 99%
“…These model potentials require further modifications with respect to their non-centrality and dielectric functions for yielding a good comparison between the computed and experimental dispersion data. The later studies [5][6][7][8] of these metals suffer from the deficiency of lattice instability and use extensive fitting procedures. Not only this, the first principle theories [9][10][11] to study the lattice dynamics of transition metals make use of drastic approximations to arrive at useful conclusions and increases computer time many times.…”
mentioning
confidence: 99%