Ten glass samples in the system xFe(2)O(3).(20-x)BaO.80B(2)O(3)(0.0 le
ss than or equal to x less than or equal to 2.0 mol%) were fabricated,
and pulsed NMR measurements were performed at room temperature as fol
lows: (1) a B-11 NMR spectrum was obtained for each sample; and (2) N-
4, the fraction of 4-coordinated borons, was determined by integrating
the area of the narrow line and broad line spectra. N-4 values were a
nalyzed in terms of changes in the boron-oxygen configuration. A two-r
egion behavior was exhibited by the N-4; that is, N-4 values in the fi
rst region (0.5 mol% Fe2O3 and below) increased, but N-4 values in the
second region (above 0.5 mol% Fe2O3) decreased with increasing Fe2O3.
In this study, it was found that, in the first region, our glasses ha
d only the symmetric structures and, in the second region, symmetric a
nd asymmetric structures. However, the number of asymmetric structures
was too small to be observed by B-11 NMR. The asymmetry parameter eta
and the quadrupole coupling constant Q(cc), of pure B2O3 glass were a
pproximately 0.26 and 2.94 MHz, respectively, and these values are a b
it higher than the values of CW-NMR measurements, eta similar to 0.13
and Q(cc)similar to 2.6 MHz. However,slightly higher values of the asy
mmetry parameter are expected in pulsed NMR measurements at a high res
onance frequency of 64.19 MHz.