Bulletin of the Chinese Ceramic Society, Volume. 41, Issue 11, 3826(2022)
Phase Boundary and Energy Storage Performance of La2O3 Doped SiO2B2O3Nb2O5 Complex Phase GlassCeramics
La2O3 doped SiO2B2O3Nb2O5 (SBN) complex phase glassceramics were prepared by controlled crystallization method. The effects of La2O3 doping on structure and energy storage performance of SBN complex phase glassceramics were characterized by DSC, Raman, XRD, SEM, ferroelectric and dielectric tests. The results show that La2O3 doping can effectively improve the thermal stability of complex phase glassceramics. With the increase of La2O3 content, the crystallization barrier of the system increases, the thermal expansion coefficient decreases first and then increases,the valence bond vibration intensifies, the dielectric constant increases first and then decreases, and the dielectric loss decreases first and then increases. When doped with 1.00% (mole fraction) La2O3, the energy storage density and energy storage efficiency of complex phase glassceramics under 40 kV/cm are the highest, which are 0.031 J·cm-3 and 77.6%, respectively. The energy storage performance is mainly evaluated by the synergistic effect of dielectric constant and breakdown field strength. La2O3 can improve the dielectric constant by improving structure stability and reducing dielectric loss. When La2O3 is introduced into the system, it is in the voids of glass network, which can effectively enhance the breakdown resistance of material. The complex phase glassceramic structure can increase structural disorder, thereby reducing relaxation loss and effectively improving the energy storage performance of material.
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GUO Hongwei, BAI Yun, CHI Longxing, ZHAO Zhilong, LIU Shuai, WANG Yi, LI Rongyue. Phase Boundary and Energy Storage Performance of La2O3 Doped SiO2B2O3Nb2O5 Complex Phase GlassCeramics[J]. Bulletin of the Chinese Ceramic Society, 2022, 41(11): 3826
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Received: Jul. 25, 2022
Accepted: --
Published Online: Dec. 26, 2022
The Author Email: Hongwei GUO (03guohongwei@163.com)
CSTR:32186.14.