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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of chemical & engineering data 22 (1977), S. 222-225 
    ISSN: 1520-5134
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of chemical & engineering data 27 (1982), S. 288-290 
    ISSN: 1520-5134
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Materials science forum Vol. 73-75 (Jan. 1991), p. 175-182 
    ISSN: 1662-9752
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 7505-7514 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular dynamics calculation for molten LiOH has been executed using a set of effective pair potentials obtained by a small modification of ab initio ones. Some experimental data on static and dynamic properties of the melt were successfully reproduced by the calculation. Anisotropic coordination structures of Li+ and OH− ions around an OH− ion have been elucidated from two-dimensional pair correlation functions, three-particle angular distribution functions, and four-particle distance distribution functions. The most probable location of a Li+ ion is on the O atom side of the OH− ion, being somewhat different from the pair potential minimum position. The correlation is strikingly large irrespective of the libration of the OH− ion. The OH− ion was found to coordinate to the neighboring OH− ion in two ways. The first one consists of a direct contact between ions on their H atom sides in spite of the large pair repulsion. The second is an indirect one on the O atom side through intervening Li+ ions which have strong Coulombic attraction to the OH− ion. This feature has a good correspondence to that of the LiOH crystal. These anisotropic structures result in an approximately isotropic coordination of the O atom around the OH− ion and give rise to a gOO(r) with a considerably sharp and large first peak and long range oscillatory correlations. This is the origin of the sharp and high first peak of the neutron structure function characteristic of the LiOH melt. It was also found that, on the average, OH− ions around a Li+ ion form a regular tetahedron, whereas the Li+ ions are located around the apexes of a square which is slightly folded downward along a diagonal just under the O atom of the OH− ion. These short range framework structures of the liquid are nearly the same with those of the crystal except that the four Li+ ions just under the OH− ion form only one plane in the crystal. Space–time correlation functions indicate that the above structures dissipate substantially in about 1 ps.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 3101-3106 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Polarized and depolarized Raman scattering measurements have been performed for the stretching vibrational mode of OH− ion in molten MOH (M= Li, Na, K, Rb, and Cs). Vibrational and rotational autocorrelation functions, Cv(t) and Cr(t), have been evaluated from Fourier transformation of the spectra. The relaxation rate of Cv(t) becomes more rapid and the asymmetry of the isotropic band becomes larger as the cation size becomes smaller. These results can be interpreted in terms of the coulombic interaction. Applying the two-parameters model based on the Kubo line shape theory to the observed spectra, it is suggested that the OH− ion apparently follows the fast modulation regime due to the libration of OH− ion. For all melts, the Cr(t) has oscillatory character caused by libration of the OH− ion at small t 〈0.1 ps. The function shows ordinary exponential decay at large t(approximately-greater-than)0.1 ps. The cation dependence of the libration at t〈 0.1 ps and the rotational diffusion process at t(approximately-greater-than)0.1 ps were investigated separately. The larger the cation size becomes, the longer and larger the period and amplitude of the libration become, respectively. This indicates that in the libration process the OH− ion seems to have more extended space in the melt as the cation size becomes larger. With respect to the rotational diffusion process, the rate shows rather small cation dependence.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 5587-5591 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Raman scattering spectra have been measured for molten LiOH at 773 K. The highly corrosive melt was held as a drop under a silver wire ring. While the Rayleigh wing spread over more than 1000 cm−1, only one distinct peak for the OH− stretching mode appeared at 3607 cm−1, the band shape being asymmetric owing to inhomogeneous broadening. The vibrational and rotational autocorrelation functions for the OH− ion, Gv(t) and Gr(t), respectively, have been evaluated from the Fourier transformation of the observed polarized and depolarized band contours. The Gv(t) is virtually of an exponential form and its decay is faster than that of the NO−3 ion in molten LiNO3. The Gr(t) can be obtained with good accuracy, whereas inhomogeneous broadening is obviously observed. The relaxation rate of Gr (t) is extremely high as compared with that for the NO−3 ion in molten LiNO3 . The difference is explained in terms of the difference mainly in the moments of inertia and partly in the temperatures. The Gr (t) has oscillatory character with a period of ∼0.04 ps at small t. This must be attributed to the precession and/or the pendulum motion of the ion, which supports the M- or J-extended rotational diffusion model rather than Debye's rotational diffusion model.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 1515-1516 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Polarized and depolarized Raman scattering spectra for the ν1 (A'i) mode of the CO2−3 ion in the molten Li2 CO3 system at 1023 K have been measured. The interference from background radiation could be eliminated by a phase detection method. Rotational and vibrational autocorrelation functions were obtained by Fourier transformation of the spectra. The rate of the rotational relaxation of the CO2−3 ion in molten Li2 CO3 at 1023 K is considerably slower than that of the NO−3 ion in molten LiNO3 at 623 K, whereas the vibrational relaxation of the former is quicker than that of the latter.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 5595-5605 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Three body forces acting on lithium, oxygen, and hydrogen atoms have been calculated directly by ab initio molecular orbital methods for more than a thousand relative intra- and interionic Li+-OH− configurations in order to evaluate the accurate interactions. The forces have been decomposed in two ways. The first method expresses the forces on O and H atoms of OH− ion in terms of the translational, the rotational, and the vibrational components. The vibrational forces have been optimized to the differential form of the Morse function and some spectroscopic parameters for OH stretching mode have been evaluated. It is clarified that they are largely dependent on the coordinating position of Li+ ion. A Li+ ion on the oxygen side causes a blue shift of the spectrum while the ion in the hydrogen side takes a red shift. These are directly related to the inhomogeneous broadening in Raman scattering and infrared absorption spectra. The second method leads the forces to a set of pairwise additive interatomic interaction forces. It has been also shown that the interatomic forces obtained here can be applied to higher order many body systems with good precision. The evaluation of the many body force is remarkably improved by considering the three body forces for the pair of the ions.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 5954-5960 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamics of ions in molten LiOH has been investigated by molecular dynamics simulation analyzing the trajectories of the particles. Rotational autocorrelation function of the OH− ion shows rapid and large oscillatory decay at small t as well as rather slow and exponential decay at large t. The function agrees well with that obtained by polarized and depolarized Raman scattering measurements. The former decay was caused by libration of the OH− ion. The latter is based on the reorientation overlapping the relatively frequent libration. It is also found that the exponential decay has a strong correlation with the structural relaxation of the liquid. The OH− ion cannot rotate without any breakdown of the structure of the surrounding ions. Significantly oscillatory translational motions have been demonstrated in terms of various one-particle and ensemble averaged autocorrelation functions. The spectrum analysis elucidated that there exists a strong correlation between the translational motion of the Li+ ion and the rotational and translational motion of the OH− ion. This is in contrast to the case of LiNO3 melt, where Li+ and NO3− ions appear to move independently, at least for the short time oscillatory motion.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 8594-8601 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Polarized and depolarized Raman scattering measurement and molecular dynamics (MD) calculations have been performed for supercritical CF3H at various densities along an isotherm higher than Tc by about 6 K in order to investigate the density dependence of rotational relaxation. The rotational autocorrelation functions obtained from both methods, which are in satisfactory agreement with each other, showed liquid-like diffusional decay for the fluid at densities higher than ρc. The function changed in shape continuously to a nearly free-rotor-like one at the lowest density going through the oscillatory ones at intermediate densities. The detailed analysis based upon the MD trajectories has been done in order to clarify the relaxation mechanism at each density. Applicability of the J-extended diffusion model was also examined. They showed that the density dependence of the rotational relaxation may be explained in terms of the states of molecular aggregation in the fluid. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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