Abstract:Polycrystalline samples of MnIn2(1—z)Ga2zSe4 system were prepared by the melt and anneal technique. Low‐field measurements of magnetic susceptibility χ were made as a function of temperature in the range 2 to 300 K. Values of TN, the Nöel temperature, were obtained from the cusp in the χ versus T curves. The 1/χ versus T curves indicated that for 0 < z < 0.30, the Mn is randomly distributed over the cation sublattice and the compound MnIn2Se4 (z = 0) was found to be spin‐glass, with Tg = 2.75 K and θ = —94 K. … Show more
“…Despite this relatively strong exchange coupling, the material does not exhibit AFM ordering, in agreement with the previous reports. 35–39 The lack of AFM ordering is explained both by the spin frustration, due to the triangular arrangement of Mn spins, and the antisite disorder of the Mn and In atoms. The AC susceptibility measurements revealed a frequency-dependent maximum in the temperature dependence of χ ′ (Fig.…”
We report liquid-phase exfoliation (LPE) of bulk layered-structure semiconductor, MnIn2Se4, to nanoscale thick sheets by ultrasonication followed by sequential centrifugation at 2000, 5000, and 7500 rpm. The nanosheets exfoliated by...
“…Despite this relatively strong exchange coupling, the material does not exhibit AFM ordering, in agreement with the previous reports. 35–39 The lack of AFM ordering is explained both by the spin frustration, due to the triangular arrangement of Mn spins, and the antisite disorder of the Mn and In atoms. The AC susceptibility measurements revealed a frequency-dependent maximum in the temperature dependence of χ ′ (Fig.…”
We report liquid-phase exfoliation (LPE) of bulk layered-structure semiconductor, MnIn2Se4, to nanoscale thick sheets by ultrasonication followed by sequential centrifugation at 2000, 5000, and 7500 rpm. The nanosheets exfoliated by...
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