1980
DOI: 10.1143/jjap.19.l90
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Preparation and Properties of PbF2-AlF3Glass

Abstract: A PbF2–AlF3 fluoride system has been vitrified in the shape of a ribbon using roller quenching over the composition range 30 to 60 mol% AlF3. The infrared absorption edge of the glass originates from the absorption band of AlF3 in PbF2 around a wavelength of 18 µm. The crystallization temperature is determined by DTA to be 280–350°C, and increases with increasing AlF3 content in the glass. The activation energy of crystallization is found to be about 80 kcal/mol for the PbF2–30 mol% AlF3 glass.

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Cited by 46 publications
(64 citation statements)
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“…In our discussion, we closely follow the standard description of its electronic eigenstates as a complex doublet. [19,20] We are not discussing the symmetry of the JT Hamiltonian in real space, which implicitly assumes the octahedral O h point group. Nevertheless, we take advantage of the effective form by using the r i matrices in which the orbital doublet represents a basis set.…”
Section: Comparison Of the Counterpartsmentioning
confidence: 99%
“…In our discussion, we closely follow the standard description of its electronic eigenstates as a complex doublet. [19,20] We are not discussing the symmetry of the JT Hamiltonian in real space, which implicitly assumes the octahedral O h point group. Nevertheless, we take advantage of the effective form by using the r i matrices in which the orbital doublet represents a basis set.…”
Section: Comparison Of the Counterpartsmentioning
confidence: 99%
“…This requires a strong electronphonon coupling in the model, which is the so-called JT coupling. 54 There are two phonon modes which strongly couple with e g orbital degrees of freedom. 55,56 In this work, lattice degrees of freedom are treated in a classical or addiabatic approximation, that is, kinetic energy of phonons is neglected.…”
Section: B Jahn-teller Couplingmentioning
confidence: 99%
“…In the following discussion, we denote the F atom at the longest, intermediate and shortest distances from a central Cu atom as F l, F m and F s, respectively. The distortion is attributed to a cooperative Jahn-Teller effect (Kanamori, 1960), and the directions of the displacements of the F(2) atoms alternate along the c axis, doubling the c period of the cubic perovskite structure. A refinement of the structure was recently performed by Tanaka, Konishi & Marumo (1977) and large negative peaks were found around the Cu atom on the final difference Fourier map, which seemed to indicate the distribution of the hole on the Cu 2+ ion in an octahedral field distorted by the Jahn-Teller effect.…”
Section: Introductionmentioning
confidence: 99%