BIO. B11. and 0 17 NMR were used to study B 2 0 3 glass. BID NMR was employed to determine the most probable values and the Gaussian widths (0') of the distributions of the quadrupole coupling constant (Q,J and the asymmetry parameter (1). The resulting values are Q~, = 5.51 MHz. O'Qcc = 0.21 MHz. 1)0 = 0.12. and 0' ~ = 0.043. These values are consistent with results using B11 NMR. The 0 17 NMR spectra are obtained and analyzed using two sites: site 1 is characterized by Q~, = 4.69 MHz. 0' Qc, = 0.10 MHz. 1)0 = 0.58; site 2 is characterized by Q~, = 5.75 MHz. 1)0 = 0.4. and 0' ~ = 0.2. Only small distributions are present for site 1 and for Q" of site 2. A Townes-Daily calculation was employed. using the boroxol ring model of B 2 0 3 glass. to determine the charge distributions and the B-O-B angle outside the boroxol rings. The results are consistent with a structure composed of randomly oriented boroxol rings.(2)where y is the gyromagnetic ratio, H o is the applied magnetic field assumed to lie in the z direction, and I. is the component of the nuclear spin operator I in the direction of the applied magnetic field. H Q can be written asH 802

The NMR of 205Tl was observed in the thallium silicate, thallium germanate, and thallium borate glass systems at six operating frequencies spanning the range 8–26.5 MHz. Two sets of glasses were used for each system spanning the glass-forming region, one using 205Tl in the natural abundance (70.5%) and the other using thallium enriched to 99.5% 205Tl. Large distributions in the values of the chemical shift tensor and a large Tl–Tl exchange interaction were observed in each of the glass systems. The results for the thallium silicate glasses indicate a pairing or clustering of the thallium atoms. A variety of complicated and distorted structural groupings appear to be present in an SiO2 matrix; the groupings change in size and structure with composition and link together at compositions having more than 20 molar percent Tl2O. Data for the germanate and borate glasses are similar to each other and indicate the following conditions. (1) The environment for the thallium atoms in low thallium content glasses is ionic. (2) The thallium environment gradually changes to a covalent environment with increasing thallium content, and there appears to be a variety of thallium-rich structural units in the region of 20–35 molar percent Tl2O. (3) The thallium atoms are paired or clustered in similar covalent structural units for high thallium contents. This situation produces a strong exchange interaction and a reduction in the size of the distribution of the values of the chemical shift tensor.

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