2 research outputs found

    Magnetocrystalline Anisotropy and Magnetocaloric Effect Studies on the Room-temperature 2D Ferromagnetic Cr4_4Te5_5

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    We present a thorough study on the magnetoanisotropic properties and magnetocaloric effect in the layered ferromagnetic Cr4_4Te5_5 single crystals by performing the critical behaviour analysis of magnetization isotherms. The critical exponents Ξ²\beta=0.485(3), Ξ³\gamma=1.202(5), and Ξ΄\delta=3.52(3) with a Curie temperature of TCβ‰ˆ340.73(4)T_C \approx 340.73(4) K are determined by the modified Arrott plots. We observe a large magnetocrystalline anisotropy Ku_u=330 kJ/m3m^3 at 3 K which gradually decreases with increasing temperature. Maximum entropy change -Ξ”SMmax\Delta S_{M}^{max} and the relative cooling power (RCP) are found to be 2.77 J/kgβˆ’KJ/kg-K and 88.29 J/kgJ/kg, respectively near TCT_C when the magnetic field applied parallel to ab\it{ab}-plane. Rescaled -Ξ”SM(T,H)\Delta S_M (T, H) data measured at various temperatures and fields collapse into a single universal curve, confirming the second order magnetic transition in this system. Following the renormalization group theory analysis, we find that the spin-coupling is of 3D Heisenberg-type, {d:n}={3:3}\{d:n\}=\{3:3\}, with long-range exchange interactions decaying as J(r)=rβˆ’(d+Οƒ)=rβˆ’4.71J (r) = r^{-(d+\sigma)}= r^{-4.71}.Comment: 10 pages, 7 figure

    Investigation of the Anomalous and Topological Hall Effects in Layered Monoclinic Ferromagnet Cr2.76_{2.76}Te4_4

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    We studied the electrical transport, Hall effect, and magnetic properties of monoclinic layered ferromagnet Cr2.76_{2.76}Te4_4. Our studies demonstrate Cr2.76_{2.76}Te4_4 to be a soft ferromagnet with strong magnetocrystalline anisotropy. Below 50 K, the system shows an antiferromagnetic-like transition. Interestingly, between 50 and 150 K, we observe fluctuating magnetic moments between in-plane and out-of-plane orientations, leading to non-coplanar spin structure. On the other hand, the electrical resistivity data suggest it to be metallic throughout the measured temperature range, except a kinkkink at around 50 K due to AFM ordering. The Rhodes-Wohlfarth ratio ΞΌeffΞΌs=1.89(>1)\frac{\mu_{eff}}{\mu_{s}}=1.89 (>1) calculated from our magnetic studies confirms that Cr2.76_{2.76}Te4_4 is an itinerant ferromagnet. Large anomalous Hall effect has been observed due to the skew-scattering of impurities and the topological Hall effect has been observed due to non-coplanar spin-structure in the presence of strong magnetocrystalline anisotropy. We examined the mechanism of anomalous Hall effect by employing the first principles calculations.Comment: 9 pages, 6 figures, To appear in Physical Review Material
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