Magnetic behavior of Ni substituted LiCoO2, magnetization and electron paramagnetic resonance studies
Magnetic behavior of Ni substituted LiCoO2, magnetization and electron paramagnetic resonance studies
复制标题
DOI:
10.1016/j.matchemphys.2017.06.019
复制
发表时间:
2016-11
期刊:
影响因子:
--
通讯作者:
Mofasser Mallick;S. Vitta
中科院分区:
文献类型:
--
作者:
Mofasser Mallick;S. Vitta
Abstract Single phase Ni substituted LiCo 1-x Ni x O 2 solid solutions with x≤ 0.15 have been synthesized to study the effect of substitution on the magnetic behavior. Two different techniques, magnetic susceptibility and electron paramagnetic resonance (EPR) which provide information in two different time windows have been used. The solid solutions have been found to be single phase with large grains conforming to R 3¯ m rhombohedral structure. The lattice parameters ‘c’and ‘a’increase with increasing Ni substitution but with a nearly constant c/a ratio of≈ 4.99 in all the cases indicating that the CoO 6 and LiO 6 octahedra do not undergo any Jahn-Teller distortions. The room temperature EPR absorption spectra clearly shows a peak in all the compounds at a field of 314 mT corresponding to a g-factor of 2.14. The peak width however is found to be a strong function of Ni substitution; increasing with increasing Ni from 3.6 mT to 6.5 mT for x= 0.08. The magnetization increases with decreasing temperature in all the compounds, a paramagnetic behavior, unlike Li-deficient compounds which show a Pauli paramagnetic susceptibility. Also, the magnetization exhibits thermal irreversibility which vanishes at large magnetic fields in all the compounds. The unsubstituted compound has discontinuities at 200 K and 50 K corresponding to magnetic transitions which disappear on substitution with 2% Ni for Co. The effective magnetic moment μ eff is found to increase from 0.32 μ B to 0.66 μ B on increasing the substitution to 0.15. The unique feature however is that all the compounds exhibit a clear magnetic hysteresis at room temperature with a finite coercivity. The coercivity increases from 31 Oe to 168 Oe for x= 0.04 and then decreases on further increasing of x. A deconvolution of the hysteresis loops clearly shows an increasing paramagnetic component with substitution.