Phase Transition Behavior of Barium Titanate Nanoparticles

2006 ◽  
Vol 320 ◽  
pp. 131-134 ◽  
Author(s):  
Takuya Hoshina ◽  
Hirofumi Kakemoto ◽  
Takaaki Tsurumi ◽  
Masatomo Yashima ◽  
Yoshihiro Kuroiwa ◽  
...  

Almost impurity-free, defect-free and dense barium titanate (BaTiO3) fine particles with various sizes from 20 to 430 nm were prepared by the 2-step thermal decomposition method and post-heating treatment. The crystal structures of these particles in the range from -150 to 150 °C were investigated using synchrotron radiation XRD measurement. The crystal structure refinement using Rietveld method revealed that BaTiO3 particles with the size over 40 nm were composed of two parts; (a) cubic shell and (b) core with successive phase transitions. The crystal structure of the core component can be related to the dielectric properties at room temperature. Moreover, it was revealed that the phase transition behavior of BaTiO3 nanoparticles was different from that of the BaTiO3 single crystal.

Author(s):  
Takuya Hoshina ◽  
Hirofumi Kakemoto ◽  
Takaaki Tsurumi ◽  
Masatomo Yashima ◽  
Yoshihiro Kuroiwa ◽  
...  

2004 ◽  
Vol 174 (1-4) ◽  
pp. 193-203 ◽  
Author(s):  
T SHIBASAKI ◽  
T FURUYA ◽  
S WANG ◽  
T HASHIMOTO

2006 ◽  
Vol 301 ◽  
pp. 27-30 ◽  
Author(s):  
Satoshi Wada ◽  
Takuya Hoshina ◽  
Hiroaki Yasuno ◽  
Masanori Ohishi ◽  
Hirofumi Kakemoto ◽  
...  

Powder dielectric measurement of barium titanate (BaTiO3) fine particles from 17 to 1,000 nm revealed a maximum dielectric constant at a certain particle size. The sizes with maximum dielectric constants were strongly dependent on preparation methods. When BaTiO3 fine particles were prepared in vacuum of 10-2 torr, a dielectric maximum of 15,000 was observed at 70 nm. On the other hand, when BaTiO3 fine particles were prepared in air, a dielectric maximum of 5,000 was observed at 140 nm. Structure refinement of BaTiO3 particles using a Rietveld method revealed that all of BaTiO3 particles were composed of two parts; (a) surface cubic layer and (b) bulk tetragonal layer. Moreover, a thickness of surface cubic layer for BaTiO3 particles prepared in vacuum was much thinner than that for BaTiO3 particles prepared in air. To explain the differences, a new model on the basis of “surface relaxation” was proposed.


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