2006
DOI: 10.1103/physrevb.74.184207
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Inelastic collective dynamics of liquid rubidium with increasing temperature by neutron scattering studies

Abstract: Although the collective dynamics of liquid alkali metals are rather well understood near the melting point, there is not much research on these dynamics at temperatures higher than the melting temperature. We carried out a set of neutron scattering experiments on liquid rubidium, an alkali metal, to study the effects of temperature on the collective dynamics. In particular, we determined the dispersion relations at different temperatures from the current correlation spectra functions and from the evolution in … Show more

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Cited by 22 publications
(35 citation statements)
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“…However, the experimentally obtained second moment exceeds the calculated one. Simple liquids, like alkali metals, exhibit a good agreement [19] and we conclude an already much more emphasized inelastic response around Q ≈ 2.0 Å K1 in that associated liquid, which seems to be not covered by the second moment. Fig.…”
Section: Resultsmentioning
confidence: 54%
“…However, the experimentally obtained second moment exceeds the calculated one. Simple liquids, like alkali metals, exhibit a good agreement [19] and we conclude an already much more emphasized inelastic response around Q ≈ 2.0 Å K1 in that associated liquid, which seems to be not covered by the second moment. Fig.…”
Section: Resultsmentioning
confidence: 54%
“…More experimental details can be found in [9,12,23]. Furthermore, inelastic experiments to follow the collective excitations at 320 K, 420 K, 500 K and 600 K have been performed and analysed [11]. More details about the extensive data analysis and comparison with MD-simulations can be found there.…”
Section: Methodsmentioning
confidence: 99%
“…Near the melting point the dynamics has been related to high frequency elastic moduli of liquid rubidium [30]. Previously we analysed the inelastic collective dynamics of liquid rubidium in detail and derived from spectra of the current correlation functions dispersion curves over a wide range of momentum vectors [11]. From these dispersion curves phase velocities c(Q) = ω/Q can be calculated for the acoustic-type excitations.…”
Section: Lam-16mentioning
confidence: 99%
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