Glass, Volume 1 |
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Page 128
the two - phase structure . Suppose that the higher viscosity phase of the phase -
separated glass is continuous . Then at the temperature at which the glass rod is
stretched , the pulling load must be borne essentially by the higher viscosity ...
the two - phase structure . Suppose that the higher viscosity phase of the phase -
separated glass is continuous . Then at the temperature at which the glass rod is
stretched , the pulling load must be borne essentially by the higher viscosity ...
Page 138
At the same time , the distribution of the dispersed phase becomes anisotropic .
After the postpulling heat treatment at 564°C , the prolate spheroids return to their
initial spherical shape but stay at the same position and the overall specimen ...
At the same time , the distribution of the dispersed phase becomes anisotropic .
After the postpulling heat treatment at 564°C , the prolate spheroids return to their
initial spherical shape but stay at the same position and the overall specimen ...
Page 151
In this section we describe a totally different type of microstructural birefringence
which was encountered during leaching of phase - separated glasses . The
origin of this birefringence is not completely clear , but the phenomenon is of ...
In this section we describe a totally different type of microstructural birefringence
which was encountered during leaching of phase - separated glasses . The
origin of this birefringence is not completely clear , but the phenomenon is of ...
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absorption alkali annealing applied assumed atoms band birefringence bleaching bond borate glasses Bray Brillouin calculations caused Ceram charge Chem coefficient color composition concentration conductivity considered constant containing coordination copper crystal crystalline curve darkening density dependence described detailed determined dielectric diffusion discussed distribution effect electron energy equation equilibrium et al experimental fading field fluctuations frequency function given gives heat treatment hole increased indicated intensity ions levels light liquid material measured mole negative observed obtained optical oxide oxygen particles phase photochromic Phys polarization positive present probably produce properties range ratio reduced relaxation reported respectively sample scattering separation shift shown in Fig silicate glasses silver halide similar SiO2 sodium Solids spectra spectrum strain stretching structural studied Taylor techniques temperature term thermal tion transition trapped units unpublished wavelengths York