Please use this identifier to cite or link to this item:
https://apo.ansto.gov.au/dspace/handle/10238/4616
Title: | The magnetocaloric effect and critical behaviour of the Mn0.94Ti0.06CoGe alloy |
Authors: | Shamba, P Wang, JL Debnath, JC Kennedy, SJ Zeng, R Din, MFM Hong, F Cheng, ZX Studer, AJ Dou, SX |
Keywords: | X-ray diffraction Magnetization Entropy Nickel Titanium Silicon Phase transformations Orthorhombic lattices Ferromagnetism |
Issue Date: | 6-Feb-2013 |
Publisher: | IOP Publishing Ltd. |
Citation: | Shamba, P., Wang, J. L., Debnath, J.C., Kennedy, S.J., Zeng, R., Md Din, M.F., Hong, F., Cheng, Z.X., Studer, A.J., & Dou, S.X. (2013). The magnetocaloric effect and critical behaviour of the Mn0.94Ti0.06CoGe alloy. Journal of Physics-Condensed Matter, 25 (5), 56001. doi:10.1088/0953-8984/25/5/056001 |
Abstract: | Structural, magnetic and magnetocaloric properties of the Mn(0.94)Ti(0.06)CoGe alloy have been investigated using x-ray diffraction, DC magnetization and neutron diffraction measurements. Two phase transitions have been detected, at T(str) = 235 K and T(C) = 270 K. A giant magnetocaloric effect has been obtained at around Tstr associated with a structural phase transition from the low temperature orthorhombic TiNiSi-type structure to the high temperature hexagonal Ni(2)In-type structure, which is confirmed by neutron study. In the vicinity of the structural transition, at T(str), the magnetic entropy change, -Delta S(M) reached a maximum value of 14.8 J kg(-1) K(-1) under a magnetic field of 5 T, which is much higher than that previously reported for the parent compound MnCoGe. To investigate the nature of the magnetic phase transition around T(C) = 270 K from the ferromagnetic to the paramagnetic state, we performed a detailed critical exponent study. The critical components gamma, beta and delta determined using the Kouvel-Fisher method, the modified Arrott plot and the critical isotherm analysis agree well. The values deduced for the critical exponents are close to the theoretical prediction from the mean-field model, indicating that the magnetic interactions are long range. On the basis of these critical exponents, the magnetization, field and temperature data around T(C) collapse onto two curves obeying the single scaling equation M(H, epsilon) = epsilon(beta)f +/- (H/epsilon(beta+gamma)). © 2013 IOP Publishing LTD |
Gov't Doc #: | 4895 |
URI: | http://dx.doi.org/10.1088/0953-8984/25/5/056001 http://apo.ansto.gov.au/dspace/handle/10238/4616 |
ISSN: | 0953-8984 |
Appears in Collections: | Journal Articles |
Files in This Item:
There are no files associated with this item.
Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.