Kamali K, Ravindran T R
Materials Science Group, Indira Gandhi Centre for Atomic Research , Kalpakkam 603 102, India.
J Phys Chem A. 2016 Mar 31;120(12):1971-7. doi: 10.1021/acs.jpca.5b12117. Epub 2016 Mar 22.
LiZr2(PO4)3 (LZP) belongs to the NASICON family of compounds whose ionic conductivity can be tuned by substitution of different cations or by increasing the temperature or pressure. Besides its conductivity, thermal and electrochemical stability makes it useful as a cathode material for lithium-ion energy storage devices. Temperature dependent Raman spectroscopic studies were carried out on the monoclinic (β') phase of LZP in the temperature range 298-853 K. A reversible structural phase transition driven by disorder in lithium sites is observed at 603 K. The spectral data enable an understanding of dynamics of the mobile Li ion and PO4 internal modes across the orthorhombic structural phase transition. On the basis of these studies, a reported change in the conductivity around 600 K is explained. High pressure Raman spectroscopic measurements on β'-LiZr2(PO4)3 reveal the onset of a structural phase transformation at 3.8 GPa and amorphization above 10 GPa. On decompression from 26 GPa, the amorphous phase remains unchanged, indicating irreversible nature of pressure-induced amorphization. Three low frequency Raman modes at 100, 124, and 144 cm(-1), which soften with an increase in pressure could be the driving force for the phase transition at 3.8 GPa. Pressure-induced phase transition prior to amorphization in β'-LiZr2(PO4)3 could be due to collapse of Zr-O-P bond angles. Pressure-induced amorphization in this compound might be due to kinetic hindrance of equilibrium decomposition.
LiZr2(PO4)3(LZP)属于NASICON族化合物,其离子电导率可通过不同阳离子的取代、升高温度或压力来调节。除了其导电性外,热稳定性和电化学稳定性使其成为锂离子储能装置的有用阴极材料。在298 - 853 K的温度范围内,对LZP的单斜(β')相进行了温度依赖拉曼光谱研究。在603 K观察到由锂位点无序驱动的可逆结构相变。光谱数据有助于理解在正交结构相变过程中移动锂离子和PO4内部模式的动力学。基于这些研究,解释了报道的600 K左右电导率的变化。对β'-LiZr2(PO4)3的高压拉曼光谱测量揭示了在3.8 GPa时结构相变的开始以及在10 GPa以上的非晶化。从26 GPa减压后,非晶相保持不变,表明压力诱导非晶化的不可逆性质。在100、124和144 cm(-1)处的三个低频拉曼模式随着压力增加而软化,可能是3.8 GPa时相变的驱动力。β'-LiZr2(PO4)3在非晶化之前的压力诱导相变可能是由于Zr - O - P键角的塌陷。该化合物中的压力诱导非晶化可能是由于平衡分解的动力学阻碍。