Glass, Volume 1 |
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Page 284
... Displacement ( Eq . ( 5 ) ] Amplitude of displacement Diffusion coefficient when
no Electric field Amplitude of electric field Electric fields in layers 1 and 2 ,
respectively Initial electric field in layer 1 and 2 , respectively Steady state electric
field ...
... Displacement ( Eq . ( 5 ) ] Amplitude of displacement Diffusion coefficient when
no Electric field Amplitude of electric field Electric fields in layers 1 and 2 ,
respectively Initial electric field in layer 1 and 2 , respectively Steady state electric
field ...
Page 285
... modulus ” Imaginary part of “ electric modulus ” Frequency dependent variable
de - fined by Eq . ( 66 ) , or ( 66 ' ) Number of charged particles in unit volume
Number of charged particles in position 1 and 2 , respectively Number of
equivalent ...
... modulus ” Imaginary part of “ electric modulus ” Frequency dependent variable
de - fined by Eq . ( 66 ) , or ( 66 ' ) Number of charged particles in unit volume
Number of charged particles in position 1 and 2 , respectively Number of
equivalent ...
Page 286
... E2 Dielectric constant of layer 1 and 2 , respectively , at high fre - quency
Relaxation strength ( height of dielectric dispersion ) Angle between direction of
field and radius vector r in Eq . ( 153 ) Angle between path direction and jump
direction ...
... E2 Dielectric constant of layer 1 and 2 , respectively , at high fre - quency
Relaxation strength ( height of dielectric dispersion ) Angle between direction of
field and radius vector r in Eq . ( 153 ) Angle between path direction and jump
direction ...
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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