DEDICATED TO PROFESSOR DR. MARIANNE BAUDLER ON THE OCCASION OF HER 80TH BIRTHDAY 6 Li and 7 Li MAS NMR spectra including 1D-EXSY (exchange spectroscopy) and inversion recovery experiments of fast ionic conducting Li 2 MgCl 4 , Li 2+x Cu x MgCl 4 , Li 2+x Na x MgCl 4 , and Li 2 ZnCl 4 have been recor
Electrical conductivity and 6,7Li NMR studies of Li1 + yCoO2
β Scribed by M. Carewska; S. Scaccia; Fausto Croce; S. Arumugam; Y. Wang; S. Greenbaum
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 819 KB
- Volume
- 93
- Category
- Article
- ISSN
- 0167-2738
No coin nor oath required. For personal study only.
β¦ Synopsis
The battery cathode material LiCoO, was synthesized with a deliberate excess of Li, according to Li, +,CoOz, where y = 0.08 and 0.35 (nominally). The effect of divalent doping with Mg" was also explored for some samples, with y values of 0.0 (stoichiometric) and 0.08. Electrical conductivity measurements of the stoichiometric material, without Mg, as functions of oxygen partial pressure and temperature exhibit p-type semiconducting behaviour and suggest that the defects primarily responsible for the generation of holes are cobalt ion vacancies. Excess Li increases the electrical conductivity, while the incorporation of Mg leads to a more dramatic enhancement in conductivity, the latter interpreted as a transition to metallic behaviour. NMR spectroscopic measurements of both 6S7Li isotopes suggest that only a small fraction ( < 20%) of the excess, Li in the y = 0.35 material enters the structure ionically while reducing the formal Co valence. Most of the excess consists of L&CO, and possibly other impurity phases, the former also having been identified by X-ray diffraction. Another small portion of the excess Li (about 10%) appears to enter interstitial sites in close proximity to paramagnetic Co'+ ions.
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The room and high temperature structures of Li,UI, have been determined using the neutron powder diffraction. It has been shown that at 300 K, the compound crystallizes in trigonal unit cell with a = b = 7.3927( 8), c = 13.826(2) A with space group P-31~. Above the phase transition occuring at 775 K
Both Raman and 7Li NMR spectroscopic data of 0.2 M LiAICl, and LiGaCL in Iiquid sulfur dioxide indicate that ionic structuraI changes occur near 25 "C, thus supporting observations from conductivity and cyclic voltammetric studies. The solvation number of the lithium cation is 4 for both salts of in
Calculated ro-vibrational energy levels (J ~< 4) and transition intensities are presented for the two most abundant isotopomers of Li~. The calculations use the recent ab initio potential energy surface of ~EARLES et al. (Spectrochim. Acta 43A, 699 (1987); 44A~ 505 (198~;); 44A, 985 (1988))β’ The rot