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Showing papers by "Dany Carlier published in 2004"


Journal ArticleDOI
TL;DR: In this paper, short-range ordering in Li[Ni x Mn ( 2 - x ) / 3 Li ( 1 - 2 x )/3 ]O 2 was investigated with 6 Li NMR and first principles structure computations.
Abstract: Short-range ordering in Li[Ni x Mn ( 2 - x ) / 3 Li ( 1 - 2 x ) / 3 ]O 2 was investigated with 6 Li NMR and first principles structure computations. NMR indicates that the tendency for Ni 2 + to replace Li + in the Li + layers decreases with decreasing nickel content. Li in the Ni/Mn layers preferentially occupies sites near Mn 4 + and avoids the Ni 2 + ions, leading to nonrandom configurations. Calculations indicate that the ground state of Li(Ni 0 . 5 Mn 0 . 5 )O 2 contains zigzag rows of Ni 2 + and Mn 4 + ions. Although a disordering temperature of approximately 1000 K is calculated, ordered fragments persist above the phase transition and these materials contain significant short-range order, even when quenched from high temperature.

183 citations


Journal ArticleDOI
TL;DR: In this article, a model was proposed to describe the exchange reaction of sodium by lithium in P2 crystals, where the exchange consists on the formation of nucleation centers and then on the growth of O2 domains.

37 citations


Journal ArticleDOI
TL;DR: This work studied the metastable O2-LiCoO(2) phase from a structural viewpoint using X-ray and neutron diffraction (ab initio method) and discusses the possibility of this T(#)2 phase to exhibit stacking faults, whose amount depends on the method used to prepare this deintercalated phase.
Abstract: The metastable O2-LiCoO(2) phase undergoes several reversible phase transitions upon lithium deintercalation. The first transition leads to an unusual oxygen stacking in such layered compounds. This stacking is found to be stable for 0.52 < x < or = 0.72 in Li(x)()CoO(2) and is called T(#)2. We studied this phase from a structural viewpoint using X-ray and neutron diffraction (ab initio method). The new stacking derives from the O2 one by gliding every second CoO(2) slab by (1/3, 1/6, 0). The lithium ions are found to occupy very distorted tetrahedral sites in this structure. We also discuss the possibility of this T(#)2 phase to exhibit stacking faults, whose amount depends on the method used to prepare this deintercalated phase.

29 citations


01 Jan 2004
TL;DR: In this article, the short-range ordering in Li O2 was investigated with Li NMR and first principles structure computations, and it was shown that Ni 21 and Mn 41 preferentially occupied sites near Mn 41 and avoided the Ni 21 ions, leading to nonrandom configurations.
Abstract: Short-range ordering in Li @NixMn(22x)/3Li (122x)/3#O2 was investigated with Li NMR and first principles structure computations. NMR indicates that the tendency for Ni 21 to replace Li 1 in the Li layers decreases with decreasing nickel content. Li in the Ni/Mn layers preferentially occupies sites near Mn 41 and avoids the Ni 21 ions, leading to nonrandom configurations. Calculations indicate that the ground state of Li(Ni 0.5Mn0.5)O2 contains zigzag rows of Ni 21 and Mn ions. Although a disordering temperature of approximately 1000 K is calculated, ordered fragments persist above the phase transition and these materials contain significant short-range order, even when quenched from high temperature. © 2004 The Electrochemical Society. @DOI: 10.1149/1.1737711 # All rights reserved.

24 citations


01 Mar 2004
TL;DR: Two-level fluctuations of the magnetization state of pseudo-spin-valve pillars embedded in electrodeposited nanowires are triggered by spin-polarized currents of 10(7) A/cm(2) at room temperature.
Abstract: Two-level fluctuations of the magnetization state of pseudo-spin-valve pillars Co(10 nm)/Cu(10 nm)/Co(30 nm) embedded in electrodeposited nanowires ( approximately 40 nm in diameter, 6000 nm in length) are triggered by spin-polarized currents of 10(7) A/cm(2) at room temperature. The statistical properties of the residence times in the parallel and antiparallel magnetization states reveal two effects with qualitatively different dependences on current intensity. The current appears to have the effect of a field determined as the bias field required to equalize these times. The bias field changes sign when the current polarity is reversed. At this field, the effect of a current density of 10(7) A/cm(2) is to lower the mean time for switching down to the microsecond range. This effect is independent of the sign of the current and is interpreted in terms of an effective temperature for the magnetization.

3 citations