or glassy state. On cooling from T
g
to room temperature, the linear
thermal expansion is the result of changes in bond lengths, whereas above T
g
,
a thermal expansion coefficient, which is at least twice as great, is due to
structural rearrangements and to bond length changes. For materials such as
silica, silicates, and some chalcogenides, upon reheating through T
g
and up to
the melting point, there is little probability of crystallization when heating at
reasonable rates. Other glasses such as the HMFs may rather easily crystallize on
either reheating or on the initial cooling. Thus, in such glasses, care must be
taken to ensure that no crystallization occurs. In particular, surface-nucleated
crystallization may be a problem both mechanically and