Fig. 4. The inverse dielectric cons

Fig. 4. The inverse dielectric constant (1 / ε) as a function of temperature at 100 kHz for Ba(ZrxTi1−x)O3 with x=1.00, 0.95, 0.90 and 0.85 (the symbols: experimental
data; the solid line: fitting to the Curie–Weiss law). The insets show the plot of ln(1 / ε−1/εm) vs. ln(T−Tm) for Ba(ZrxTi1−x)O3 with x=0.95, 0.90 and 0.85 (the

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fig. Four. the inverse dielectric constant (1 / ε) as a function of temperature at 100 khz for ba (zrxti1-x) o3 with x = 1.00, 0.95, 0.90 and 0.85 (the symbols: experimental
data; the solid line: fitting to the. curie-weiss law). the insets show the plot of ln (1 / ε-1/εm) vs. ln (t-tm) for ba (zrxti1-x) o3 with x = 0.95, 0.90 and 0.85 (the.

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Fig. 4. The inverse dielectric constant (1/ε), as a function of temperature at 100 kHz for Ba (ZrxTi − 1 x) 3 O with X = 1.00, 0.95, 0.90 and 0.85 (the symbols:
experimental data; the solid line: fitting to the Curie - Weiss law). The insets show the plot of ln(1/ε − 1/ε m) vs. ln (T − Tm) for Ba (ZrxTi − 1 X), O with 3 X = 0.95, 0.90 and 0.85 (the