Please use this identifier to cite or link to this item: http://nopr.niscpr.res.in/handle/123456789/25850
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dc.contributor.authorRao, R V Gopala-
dc.contributor.authorVenkatesh, R-
dc.date.accessioned2014-01-18T07:19:12Z-
dc.date.available2014-01-18T07:19:12Z-
dc.date.issued2000-03-
dc.identifier.issn0975-0975(Online); 0376-4710(Print)-
dc.identifier.urihttp://hdl.handle.net/123456789/25850-
dc.description247-252en_US
dc.description.abstractUsing the potential function and its derivatives evaluated by Rao and Venkatesh from the experimental structure factors, the longitudinal (ωL) and transverse(ωT) phonon frequencies have been computed through the equations of Takeno and Goda. The ωL (k) maximum is found to occur midway between zero and the first peak of the structure factor. The dynamic structure factor has been calculated in the viscoelastic approximation. In the current correlation function, the position of the maximum of the current density at a particular k is designated as ωm. ωm versus k has been obtained at various wave vectors. The ωm versus k exhibits a flat portion spreading over the three peaks of the complex structure factor of liquid Te even though ωm (k) increases slowly with k.ωm gives a peak at nearly the same position as ωL(k).en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJC-A Vol.39A(01-03) [January-March 2000]en_US
dc.titleCollective excitations and dynamic structure factor of liquid telluriumen_US
dc.typeArticleen_US
Appears in Collections:IJC-A Vol.39A(01-03) [January-March 2000]

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