2014
DOI: 10.1016/j.jpcs.2013.12.005
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Physical properties of the cubic spinel LiMn2O4

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Cited by 17 publications
(10 citation statements)
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“…Figure 3 shows the XRD patterns of the spinel LiMn2O4 synthesized from LiOH.H2O and MnOx by conventional and MA methods, measured at temperature range from room temperature down to 93K. Previous works [19,20] showed that at room temperature, stoichiometric spinel oxide, LiMn2O4, display a cubic, normal spinel structure (space group Fd-3m). The transformation should start at near room temperature (~290 K) and is shown by peak splitting of the spinel diffraction lines with decreasing temperature.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 3 shows the XRD patterns of the spinel LiMn2O4 synthesized from LiOH.H2O and MnOx by conventional and MA methods, measured at temperature range from room temperature down to 93K. Previous works [19,20] showed that at room temperature, stoichiometric spinel oxide, LiMn2O4, display a cubic, normal spinel structure (space group Fd-3m). The transformation should start at near room temperature (~290 K) and is shown by peak splitting of the spinel diffraction lines with decreasing temperature.…”
Section: Resultsmentioning
confidence: 99%
“…(1) 2g ) are associated with motion of Li and O atoms, and S11 (~644 cm −1 ; A 1g ) originates from the symmetric stretching vibration of Mn-O bond in the MnO 6 octahedra. In addition, the appearance of low frequency mode S1-167 cm −1 in the spectrum may be speculated due to the scattering of the acoustic mode from other parts of Brillouin zone, as the phonon dispersion of LiMn 2 O 4 spinel shows the value close to this frequency at X-point in the Brillouin zone [41]. Also, the observed weak shoulder mode S12 may be attributed to the second order modes or second order IR modes become Raman active [42,43].…”
Section: Inelastic Light (Raman) Scattering Studymentioning
confidence: 88%
“…78 For the 16d−48f−16d hops in Figure 3 (Hops 3−5), electrostatic effects are more dominant than for the tet−oct−tet hops (Hops 1, 2), primarily due to the intermediate 48f edgesharing with an 8a. Indeed, the cation centers in edge-sharing tetrahedra are closer (∼2.15 Å experimentally between 48f and 8a in an ideal LiMn 2 O 4 -spinel 79 ) than in edge-sharing octahedra (∼2.88 Å between 16c and 16d). Consequently, the Mg barriers are consistently lower with a vacant edge-8a (Hop 5, Figure 3) compared to Mg/Mn-filled edge-8a (Hops 3, 4 in Figure 3).…”
Section: Discussionmentioning
confidence: 98%