New understanding of Li3VO4/C as potential anode for Li-ion batteries: Preparation, structure characterization and lithium insertion mechanism

2015 ◽  
Vol 274 ◽  
pp. 345-354 ◽  
Author(s):  
Zhiyong Liang ◽  
Zhiping Lin ◽  
Yanming Zhao ◽  
Youzhong Dong ◽  
Quan Kuang ◽  
...  
CrystEngComm ◽  
2015 ◽  
Vol 17 (32) ◽  
pp. 6163-6174 ◽  
Author(s):  
L. de Biasi ◽  
G. Lieser ◽  
J. Rana ◽  
S. Indris ◽  
C. Dräger ◽  
...  

For possible future application as cathode material in lithium ion batteries, the lithium insertion mechanism of trirutile-type LiNiFeF6 was investigated.


2018 ◽  
Vol 6 (2) ◽  
pp. 443-455 ◽  
Author(s):  
Alois Kuhn ◽  
Juan Carlos Pérez-Flores ◽  
Markus Hoelzel ◽  
Carsten Baehtz ◽  
Isabel Sobrados ◽  
...  

Sodium hexatitanate Na2Ti6O13 with a tunnel structure has been proposed to be an attractive anode material for lithium ion batteries because of its low insertion voltage, structural stability and good reversibility.


1999 ◽  
Vol 45 (1-2) ◽  
pp. 3-22 ◽  
Author(s):  
M Broussely ◽  
P Biensan ◽  
B Simon

1999 ◽  
Vol 11 (10) ◽  
pp. 2846-2850 ◽  
Author(s):  
C. Branci ◽  
J. Sarradin ◽  
J. Olivier-Fourcade ◽  
J. C. Jumas

2004 ◽  
Vol 835 ◽  
Author(s):  
P.E. Lippens ◽  
L. Aldon ◽  
C.M. Ionica ◽  
F. Robert ◽  
J. Olivier-Fourcade ◽  
...  

ABSTRACTThe Mössbauer spectroscopy is an efficient experimental tool to study lithium insertion mechanisms in negative electrodes of Li-ion batteries at the atomic scale. However, a quantitative interpretation of the experimental data is often difficult due to the complexity of the spectra and we propose to use first-principle calculations of the hyperfine parameters. Three different types of negative electrode materials are considered. First, the experimental 119Sn Mössbauer spectrum obtained for the insertion of 3.5 Li into SnO is compared to the theoretical spectrum, which clearly establishes the existence of Li-Sn stable phases. Then, the analysis of the 121Sb Mössbauer spectra for metal antimonides at the end of the first discharge shows different behaviours depending on the lithium rate. Finally, tin and iron doped titanates are considered to study changes in Ti local environments during lithium insertion.


ChemistryOpen ◽  
2015 ◽  
Vol 4 (4) ◽  
pp. 443-447 ◽  
Author(s):  
Damien Dambournet ◽  
Karena W. Chapman ◽  
Mathieu Duttine ◽  
Olaf Borkiewicz ◽  
Peter J. Chupas ◽  
...  

2003 ◽  
Vol 118 (13) ◽  
pp. 6038-6045 ◽  
Author(s):  
Michel Letellier ◽  
Frédéric Chevallier ◽  
Christian Clinard ◽  
Elzbieta Frackowiak ◽  
Jean-Noël Rouzaud ◽  
...  

2004 ◽  
Vol 60 (4) ◽  
pp. 382-387 ◽  
Author(s):  
Jonas Höwing ◽  
Torbjörn Gustafsson ◽  
John O. Thomas

The structures of Li3V6O13 and Li3+δV6O13, δ ≃ 0.3, have been determined by single-crystal X-ray diffraction. Both compounds have the space group C2/m, with very similar cell parameters. In Li3V6O13, the Li atoms are found in the Wyckoff positions 4(i) and 2(b) with multiplicities of four and two, respectively. Since Li3V6O13 exhibits no superstructure reflections, it is concluded that Li3V6O13 contains one disordered lithium ion in an otherwise ordered centrosymmetric structure. On inserting more lithium into the structure, the Li3+δV6O13 phase is formed with the homogeneity range 0 < δ < 1. It is concluded that the site for the extra inserted lithium ion is closely coupled to the position of the disordered lithium ion in Li3V6O13. A mechanism for this behaviour and for the further formation of the Li6V6O13 end-phase in the Li x V6O13 system is proposed.


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