2010
DOI: 10.1016/j.physb.2010.08.050
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Structural and magnetic properties of LiMn1.5Fe0.5O4 spinel oxide

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Cited by 10 publications
(10 citation statements)
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“…It is worth noting that the DM interactions in single Mn­(IV) 3 Mn­(III) tetrahedron are asymmetric due to the difference in the magnitude between the Dzyaloshinskii vectors within the Mn­(III)–O–Mn­(IV) bond and within the Mn­(IV)–O–Mn­(IV) bond and the difference between the distinct spin states for Mn ions (see Figure S8 for details). In the Heisenberg antiferromagnets of CdCr 2 O 4 and the x = 0.07 phase, having symmetrical tetrahedral structures, a spin-Peierls-like lattice distortion stabilizes the collinear or coplanar magnetic ground state. , It has been reported that a spinel Li 0.5 Mn­(IV)­Mn­(III) 0.5 Fe­(III) 0.5 O 4 exhibits an AFM order with a similar anomaly in χ′ –T curves . In particular, the isotopological Cu 2 OSeO 3 , whose space group ( P 2 1 3) is the same as that of Li 0.50 Mn 2 O 4 , gives rise to a complex noncollinear ferrimagnetic configuration; the DM interactions in this space group with the absence of both inversion and mirror symmetries result in a chiral skyrmionic helimagnet. , …”
Section: Resultsmentioning
confidence: 99%
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“…It is worth noting that the DM interactions in single Mn­(IV) 3 Mn­(III) tetrahedron are asymmetric due to the difference in the magnitude between the Dzyaloshinskii vectors within the Mn­(III)–O–Mn­(IV) bond and within the Mn­(IV)–O–Mn­(IV) bond and the difference between the distinct spin states for Mn ions (see Figure S8 for details). In the Heisenberg antiferromagnets of CdCr 2 O 4 and the x = 0.07 phase, having symmetrical tetrahedral structures, a spin-Peierls-like lattice distortion stabilizes the collinear or coplanar magnetic ground state. , It has been reported that a spinel Li 0.5 Mn­(IV)­Mn­(III) 0.5 Fe­(III) 0.5 O 4 exhibits an AFM order with a similar anomaly in χ′ –T curves . In particular, the isotopological Cu 2 OSeO 3 , whose space group ( P 2 1 3) is the same as that of Li 0.50 Mn 2 O 4 , gives rise to a complex noncollinear ferrimagnetic configuration; the DM interactions in this space group with the absence of both inversion and mirror symmetries result in a chiral skyrmionic helimagnet. , …”
Section: Resultsmentioning
confidence: 99%
“…45,46 It has been reported that a spinel Li 0.5 Mn(IV)Mn(III) 0.5 Fe(III) 0.5 O 4 exhibits an AFM order with a similar anomaly in χ′−T curves. 47 In particular, the isotopological Cu 2 OSeO 3 , whose space group (P2 1 3) is the same as that of Li 0.50 Mn 2 O 4 , gives rise to a complex noncollinear ferrimagnetic configuration; the DM interactions in this space group with the absence of both inversion and mirror symmetries result in a chiral skyrmionic helimagnet. 48,49 The spin-glass state is absent in the x = 0.07 sample, but a sharp, frequency-independent peak occurs at T N = 30 K in the χ′−T plots (see Figure 3c).…”
Section: ■ Introductionmentioning
confidence: 99%
“…[ 1–4 ] Among the components of LIBs, the cathode material is the main provider of Li‐ion and the key factor that affects the performance of the battery. [ 5,6 ] Therefore, the modification of the cathode material plays a key role in improving the electrochemical performance of LIBs.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, synthesizing high-quality spinel LiCoTiO 4 crystals simply and cost-effectively remains a challenge. Although various lithium-containing spinel crystals (including LiMn 1.5 Ni 0.5 -O 4 , 1,17 LiMn 2 O 4 , 4,18 LiCr 0.5 Mn 1.5 O 4 , 19 LiMn 1.5 Fe 0.5 O 4 , 20 etc.) usually with special (truncated) octahedral morphologies have been obtained, detailed investigations of the corresponding formation mechanisms are still needed.…”
Section: Introductionmentioning
confidence: 99%