Stanislav Kamba et al 2004 J. Phys. D: Appl. Phys. 37 1980 doi:10.1088/0022-3727/37/14/014
Stanislav Kamba1, Hana Hughes2, Dmitri Noujni1, Santhi Surendran1, Robert C Pullar3, Polina Samoukhina1, Jan Petzelt1, Robert Freer2, Neil McN Alford3 and David M Iddles4
Show affiliationsThe dielectric properties of (1 − x)Ba(Zn1/3Nb2/3)O3–xBa (Ga1/2Ta1/2)O3 (BZN–xBGT) microwave (MW) ceramics, with x between 0 and 0.2, and those of 0.9Ba(Zn0.6Co0.4)1/3Nb2/3O3–0.1Ba(Ga0.5Ta0.5)O3 (BZCN–BGT) were studied at MW, terahertz (THz) and infrared (IR) frequencies at temperatures from 10 to 300 K. At room temperature, the temperature coefficient of resonance frequency (τf) near 3 GHz decreases from 28 ppm K−1 in undoped BZN to 2 ppm K−1 in BZN–0.2BGT and reduces to zero in BZCN–BGT. The addition of BGT to BZN depresses the dielectric Q value, but incorporation of Co improves the Q values, yielding Q ~ 30 000 at 3 GHZ in BZCN–BGT. The relative permittivity (ε') exhibits only limited variation with composition (ε' values in the range 34.4–36.0). IR and THz spectra as well as the low-temperature MW dielectric measurements revealed a weak dielectric relaxation below phonon frequencies, possibly arising from charges caused by inhomogeneous distribution of the B-site ions with differing valences. The IR reflectivity spectrum of BZN–0.2BGT is significantly different (smeared) compared with other compositions, which may be caused by disorder on the B sites and by an amorphous phase at the grain boundaries.
77.84.Dy Niobates, titanates, tantalates, PZT ceramics, etc.
77.22.Gm Dielectric loss and relaxation
Issue 14 (21 July 2004)
Received 30 March 2004
Published 30 June 2004
Stanislav Kamba et al 2004 J. Phys. D: Appl. Phys. 37 1980
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