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Journal Articles

Neutron diffraction study of field-cooling effects on the relaxor ferroelectric Pb[(Zn$$_{1/3}$$Nb$$_{2/3}$$)$$_{0.92}$$Ti$$_{0.08}$$]O$$_3$$

Owada, Kenji; Hirota, Kazuma*; Rehrig, P. W.*; Fujii, Yasuhiko*; Shirane, Gen*

Physical Review B, 67(9), p.094111_1 - 094111_8, 2003/03

 Times Cited Count:105 Percentile:94.38(Materials Science, Multidisciplinary)

High-temperature ($$T$$) and high-electric-field ($$E$$) effects on Pb[(Zn$$_{1/3}$$Nb$$_{2/3}$$)$$_{0.92}$$Ti$$_{0.08}$$]O$$_{3}$$ (PZN-8%PT) were studied comprehensively by neutron diffraction in the ranges $$300 le T le 550$$~K and $$0 le E le 15$$~kV/cm. We have focused on how phase transitions depend on preceding thermal and electrical sequences. In the field cooling process (FC, $$E parallel [001] ge 0.5$$~kV/cm), a successive cubic (C) $$rightarrow$$ tetragonal (T) $$rightarrow$$ monoclinic (M$$_{rm C}$$) transition was observed. In the zero field cooling process (ZFC), however, we have found that the system does ${em not}$ transform to the rhombohedral (R) phase as widely believed, but to a new, unidentified phase, which we call X. X gives a Bragg peak profile similar to that expected for R, but the $$c$$-axis is always slightly shorter than the $$a$$-axis. As for field effects on the X phase, it transforms into the M$$_{rm C}$$ phase via another monoclinic phase (M$$_{rm A}$$) as expected from a previous report [Noheda ${it et al.}$$ Phys. Rev. B {bf 65}$, 224101 (2002)].

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