2008
DOI: 10.1016/j.crhy.2007.10.017
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High-resolution inelastic x-ray scattering to study the high-frequency atomic dynamics of disordered systems

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Cited by 7 publications
(4 citation statements)
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“…Within the context of large literature about intermolecular vibrational dynamics of glass-forming liquids, the band at ∼20 cm –1 seen in low-frequency Raman spectra of the glassy phase of ionic liquids (see Figure ) is the so-called boson peak. , ,, It has been pointed out that the boson peak vibrations remain in the liquid state even though the peak is hidden under the intense quasi-elastic scattering of the low-frequency Raman spectrum. In an OKE spectroscopy study of 1-ethyl-3-methylimidazolium tosylate, Li et al assigned to the boson peak dynamics the oscillatory component with period of ∼2.0 ps (i.e., ∼17 cm –1 ) seen in the time domain data a few degrees above the glass transition temperature ( T g = 201 K). The partial nature of longitudinal and transverse acoustic modes of the intermolecular dynamics in the spatial range of wavevectors 0.1 < k < 1.0 Å –1 and frequency range 0 < ω < 100 cm –1 in viscous glass-forming liquids has been established in many studies by inelastic X-ray scattering spectroscopy and MD simulations. Although the exact origin of the boson peak is yet a lively debated issue, several studies have been pointing to the nature of transverse acoustic vibrations of high wave-vectors (i.e., soundlike modes of short wavelength). It is worth stressing that projecting into soundlike modes recovers only part of the intermolecular vibrations of liquids because the other part is random phase motion ,,, and eventually molecular-like normal modes in high temperature molten salts in which complexes survive for a relatively long time. , …”
Section: Vibrational Spectroscopy Of Pure Ionic Liquids In the Low-fr...mentioning
confidence: 99%
“…Within the context of large literature about intermolecular vibrational dynamics of glass-forming liquids, the band at ∼20 cm –1 seen in low-frequency Raman spectra of the glassy phase of ionic liquids (see Figure ) is the so-called boson peak. , ,, It has been pointed out that the boson peak vibrations remain in the liquid state even though the peak is hidden under the intense quasi-elastic scattering of the low-frequency Raman spectrum. In an OKE spectroscopy study of 1-ethyl-3-methylimidazolium tosylate, Li et al assigned to the boson peak dynamics the oscillatory component with period of ∼2.0 ps (i.e., ∼17 cm –1 ) seen in the time domain data a few degrees above the glass transition temperature ( T g = 201 K). The partial nature of longitudinal and transverse acoustic modes of the intermolecular dynamics in the spatial range of wavevectors 0.1 < k < 1.0 Å –1 and frequency range 0 < ω < 100 cm –1 in viscous glass-forming liquids has been established in many studies by inelastic X-ray scattering spectroscopy and MD simulations. Although the exact origin of the boson peak is yet a lively debated issue, several studies have been pointing to the nature of transverse acoustic vibrations of high wave-vectors (i.e., soundlike modes of short wavelength). It is worth stressing that projecting into soundlike modes recovers only part of the intermolecular vibrations of liquids because the other part is random phase motion ,,, and eventually molecular-like normal modes in high temperature molten salts in which complexes survive for a relatively long time. , …”
Section: Vibrational Spectroscopy Of Pure Ionic Liquids In the Low-fr...mentioning
confidence: 99%
“…Momentum-resolved Inelastic X-ray Scattering (IXS) with meV energy resolution provides a powerful technique for studying vibrational dynamics and excitations in condensed matter systems [1]. The scientific objective of the IXS beamline of NSLS-II is focused on very high-resolution (1 meV ~ 0.1 meV) IXS experiments.…”
Section: Introductionmentioning
confidence: 99%
“…With the 0.1 meV energy resolution, we anticipate improved understanding of the low-energy excitations in liquid, disordered and bio-molecular systems, where atomic motions due to the naturally occurring inhomogeneity and/or density fluctuations dominate the scattering at low momentum transfer (Q), for which very high Q resolution (< 0.1 nm -1 ) would also be required. Achieving these goals would allow the NSLS-II IXS beamline to bridge, at least partially, the dynamic gap (0.1 nm -1 < Q < 2 nm -1 and 0.1 meV < E < 5 meV) between various existing inelastic scattering probes [1]. This is an area where potential new science may be expected.…”
Section: Introductionmentioning
confidence: 99%
“…Similarly to what happens in single crystals, at a given pressure, the dependence of the acoustic excitation energy on momentum transfer can be plotted in a diagram and follows a dispersing curve, the so-called longitudinal acoustic dispersion relation for the amorphous material. The dispersion relation has an almost linear dependence on Q when Q tends to zero and its slope at this limit corresponds to the macroscopic longitudinal sound velocity [39]. The dispersion curves behave like a typical sinusoidal function that peaks at momentum transfers between 10 and 12 nm −1 , depending on the applied pressure.…”
Section: Mechanical Propertiesmentioning
confidence: 94%