1989
DOI: 10.1002/crat.2170240425
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Comparative infrared lattice vibration study of LiGaO2 and LiInO2 (I) experimental results

Abstract: Experimental ResultsInfrared reflectivity spectra of LiGaO, and LiInO, samples pressed from powdered niaterial are measured at room temperature in the wavenumber range from 180 to 4000 cm-l. The optical mode frequencies found for LiGaO, agree with measurements on single crystals. I n LiInO, four vibrational modes are found. Comparing the results for LiGaO, and LiInO, some conclusions are made with regard to the Li-0 bond related vibrational modes.Infrarot-Reflexionsspektren von aus pulverformigem Material herg… Show more

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Cited by 10 publications
(8 citation statements)
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“…Following the arguments of SOBOTTA et al (1989) this wurtzite-like mode in LiGaO, is ascribed to G a -0 bond vibrations. Experimental and theoretical studies of the lattice vibrations of P-Ga203 support this point of view.…”
Section: Analysis Of Experimental Datamentioning
confidence: 69%
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“…Following the arguments of SOBOTTA et al (1989) this wurtzite-like mode in LiGaO, is ascribed to G a -0 bond vibrations. Experimental and theoretical studies of the lattice vibrations of P-Ga203 support this point of view.…”
Section: Analysis Of Experimental Datamentioning
confidence: 69%
“…To solve this problem it has been tentatively assumed that the Li-0 bond related modes have higher frequencies than the G a -0 bond related modes (NEUMANN 1986b), in agreement with the trends observed in LiInS, ), LiInSe, (SOBOTTA et al 1987) and LiInTe, ( K~N et al) exhibiting frequencies of the Li-Cvl bond related modes that are distinctly higher than those of the In-C" bond related modes. However, considering the results of a recent infrared reflectivity study of the lattice vibrations of LiInO, (SOBOTTA et al 1989) and In,O, (SOBOTTA et al 1990) it is obvious that this supposition must be abandoned in the case of the LiB"'0, compounds. In the present work the lattice vibration data of LiGaO, are reconsidered, and revised force constants are proposed for the Li-0 and G a -0 bonds.…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, the relative change of mode frequencies is small, and it can be expected that the temperature variation of the mode frequency can be well represented by a rapidly converging power series expansion in the temperature T. Secondly, it follows from the nonlinear temperature dependence of the thermal expansion coefficient [15] that the mode frequency will also be a nonlinear function of temperature. Then, taking into account that the mode Grüneisen parameters can also depend on temperature the anharmonic contribution to the heat capacity at constant volume becomes In principle, ∆C V (T) can be calculated with (13) provided that all the vibrational mode frequencies ω s (q) and the corresponding mode Grüneisen parameters γ(s,q) are known, for instance from accurate inelastic neutron scattering experiments as a function of pressure and temperature. However, because of the lack of related experimental data for LiGaO 2 further approximations are required.…”
Section: VImentioning
confidence: 99%
“…Exceptions are the optical modes with lowest frequency [34][35][36][37][38][39][40] and, in particular, the acoustic modes [43][44][45] exhibiting very small and partly negative mode Grüneisen parameters with a pronounced dependence on the wave vector q [44,45]. Therefore, the contribution of these modes to ∆C V (T) can only be calculated using relation (13) with summation over the frequency range from ω = 0 to ω = ω l . However, it has been established experimentally that, within the usual experimental accuracy of heat capacity measurements, anharmonicity effects remain negligibly in the temperature range characteristic of thermal excitation of these modes only [22,46,47].…”
Section: B Cmentioning
confidence: 99%
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