Fourier-transform infrared and time-domain THz dielectric spectroscopy measurements on KTa(1-x)Nb(x)O(3) crystals for x = 0.018 and 0.022 were performed. The temperature behaviour of the soft mode frequency and damping have been determined above the ferroelectric phase transition. No dielectric dispersion in the frequency range below the polar phonon absorption is observed down to kHz frequencies at temperatures from room temperature down to 60 K. At lower temperatures the KTa(1-x)Nb(x)O(3) samples become opaque due to additional losses, which persist down to liquid helium temperatures. This supports the nanoscopic dipolar glassy state rather than macroscopic ferroelectricity at low temperatures.
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http://dx.doi.org/10.1088/0953-8984/17/25/L04 | DOI Listing |
Rev Sci Instrum
July 2024
Research Institute of Electrical Communication, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Miyagi 980-8577, Japan.
Potassium tantalate niobate (KTa1-xNbxO3, KTN) single crystals have a very large relative permittivity εr (>104) just above the paraelectric to ferroelectric phase transition temperature (TC). The quadratic electro-optic coefficient and the electro-strictive coefficient are also very large because of their proportionality to εr2. However, the local relative permittivity can easily vary spatially due to the incongruently melting nature of KTN.
View Article and Find Full Text PDFControlling the space charge distributions in a crystal is indispensable for controlling a KTa₁₋xNbxO₃(KTN) optical beam deflector. The space charge is built up by applying a voltage and injecting electrons into the KTN crystal. Although a homogeneous distribution is preferable, we observed experimentally that the injected electrons concentrated in the vicinity of the cathode and for some samples the concentration was much lower around the anode.
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