Fig. 4: Pockels coefficients of LN and BTO. | Nature Materials

Fig. 4: Pockels coefficients of LN and BTO.

From: Barium titanate and lithium niobate permittivity and Pockels coefficients from megahertz to sub-terahertz frequencies

Fig. 4

a, Pockels coefficient measurements for LN, with r33 in dark blue, r42 in light blue and linear fits to the data in solid lines. The fitted values are r33 = 26.9 pm V–1 and 1/2(r13 + 2r42) = 15.0 pm V–1. b, Pockels coefficient measurements for BTO, with r33 in dark green, r42 in light green and model fits to the data in solid lines. The r42 data are fit to a Debye model with γ0 = 565 MHz, σ = 0.06, SR = 75 pm V–1 and r = 60 pm V–1. The 1/2(r13 + 2r42) value is fit using equation (5), where ε is calculated from the Debye model of equation (2) using the same coefficients as the measured permittivity (Table 1). The data points are the result of fitting the measured reff data from n = 15–20 devices to equation (4), as described in Supplementary Information. The error bars represent two standard errors of the fit. Note that typically 2r42r13 so that r13 + 2r42 ≈ 2r42. We, therefore, plot this parameter as 1/2(r13 + 2r42) ≈ r42.

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