Hysteresis properties of a mixed ferromagnetic-ferrimagnetic ternary alloy

Year 2018, Volume: 6 Issue: 2, 94 - 102, 03.08.2018

Zeynep Demir Vatansever

https://doi.org/10.21541/apjes.345567

Cited By: 1

Abstract

In this work, we have investigated
the hysteresis properties of a mixed ferro-ferrimagnetic ternary alloy system by
Monte Carlo simulation method. The ternary alloy system contains two
interpenetrating sublattices. One of the sublattice consists of type-A magnetic
components with spin-3/2 while the other one is randomly occupied type-B and
type-C magnetic components with spin-1 and spin-5/2, respectively.  We consider both ferromagnetic and
antiferromagnetic exchange interactions between nearest-neighbor magnetic
components.  The influences of the
exchange interaction ratio, R, and the concentration value of type-B magnetic
ions, p, on the remanent magnetization, coercivity and hysteresis loops of the
system have been investigated in detail. 
It has been demonstrated that it is possible to modify the remanent
magnetization, coercivity and also the saturation magnetization of the system
by changing the concentration value and exchange interaction ratio.

Keywords

Hysteresis, Ternary alloy, Monte Carlo Simulation

Hysteresis properties of a mixed ferromagnetic-ferrimagnetic ternary alloy

Abstract

In this work, we have investigated the hysteresis properties of a mixed ferro-ferrimagnetic ternary alloy system by Monte Carlo simulation method. The ternary alloy system contains two interpenetrating sublattices. One of the sublattice consists of type-A magnetic components with spin-3/2 while the other one is randomly occupied type-B and type-C magnetic components with spin-1 and spin-5/2, respectively. We consider both ferromagnetic and antiferromagnetic exchange interactions between nearest-neighbor magnetic components. The influences of the exchange interaction ratio, R, and the concentration value of type-B magnetic ions, p, on the remanent magnetization, coercivity and hysteresis loops of the system have been investigated in detail. It has been demonstrated that it is possible to modify the remanent magnetization, coercivity and also the saturation magnetization of the system by changing the concentration value and exchange interaction ratio.

Keywords

Hysteresis, ternary alloy, Monte Carlo simulation

References

• [1] J. S. Miller and M. Drillon, Magnetism: Molecules to Materials V, Weinheim: Wiley-VCH, 2005.
• [2] S. I. Ohkoshi, O. Sato, T. Iyoda, A. Fujishima, K. Hashimoto, “Tuning of Superexchange Couplings in a Molecule-Based Ferroferrimagnet: (NiIIxMnII1-x) 1.5[CrIII(CN)6]”, Inorg. Chem., vol. 36, pp. 268-269, 1997.
• [3] S. I. Ohkoshi, O. Sato, T. Iyoda, A. Fujishima, K. Hashimoto, “Magnetic properties of mixed ferro-ferrimagnets composed of Prussian blue analogs”, Phys. Rev. B, vol. 56, pp. 11642.
• [4] S. I. Ohkoshi and K. Hashimoto, “Theoretical treatment of the mixed ferro-ferrimagnets composed of ternary-metal Prussian blue analogs in a paramagnetic region”, Phys. Rev. B, vol. 60, no 18, pp. 12820-12825, June 1999.
• [5] S. I. Ohkoshi, S. Yorozu, O. Sato, T. Iyoda and A. Fujishima, “Photoinduced magnetic pole inversion in a ferro–ferrimagnet: (Fe0.40IIMn0.60II)1.5CrIII(CN)6”, Appl. Phys. Lett., vol. 70, pp. 1040, 1997.
• [6] S. I. Ohkoshi, Y. Abe, A. Fujishima and K. Hashimoto, “Design and Preparation of a Novel Magnet Exhibiting Two Compensation Temperatures Based on Molecular Field Theory”, Phys. Rev. Lett., vol. 82, pp. 1285, 1999.
• [7] S. I. Ohkoshi, T. Hozumi, M. Utsunomiya, M. Abe and K. Hashimoto, “The observation of two compensation temperatures in a cobalt-manganese hexacyanochromate”, Physica B, vol. 329, pp. 691-692, 2003.
• [8] S. I. Ohkoshi, T. Hozumi and K. Hashimoto, “Design and preparation of a bulk magnet exhibiting an inverted hysteresis loop”, Phys. Rev. B, vol. 64, pp. 132404, 2001.
• [9] P. Bhatt, S. Banerjee, S. Anwar, M. D. Mukadam, S. S. Meena and S. M. Yusuf, “Core−Shell Prussian Blue Analogue Molecular Magnet Mn1.5 [Cr(CN)6]•mH2O@Ni1.5 [Cr(CN)6]•nH2O for Hydrogen Storage”, Appl. Mater. Interfaces, vol. 6, pp. 17579-17588, 2014.
• [10] C-H Lee, C-M Wu, E. Batsaikhan, H-C Li, C. H. Li, M. K. Peprah, D. R. Talham, M. W. Meisel and W-H Li, “Complex Magnetic Phases in Nanosized Core@Shell Prussian Blue Analogue Cubes: Rb0.48Co[Fe(CN)6] 0.75 [(H2O)6]0.25•0.34H2O@K0.36Ni[Cr(CN)6]0.74[(H2O)6]0.26•0.11H2O”, J. Phys. Chem. C, vol. 119, pp. 29138-29147, 2015.
• [11] P. Bhatt, A. Kumar, S.S. Meena, M.D. Mukadam and S.M. Yusuf, “Magnetic proximity effect in ferrimagnetic–ferromagnetic core–shell Prussian blue analogues molecular magnet”, Chem. Phys. Lett., vol. 651, pp. 155-160, 2016.
• [12] P. Zhou, D. Xue, H. Luo and X. Chen, “Fabrication, Structure, and Magnetic Properties of Highly Ordered Prussian Blue Nanowire Arrays”, Nano Lett., vol. 2, pp. 845-847, 2002.
• [13] P. H. Zhou and D. S. Xue, “Finite-size effect on magnetic properties in Prussian blue nanowire arrays”, J. Appl. Phys., vol. 96, pp. 610-614, 2004.
• [14] A. Johansson, E. Widenkvist, J. Lu, M. Boman and U. Jansson, “Fabrication of High-Aspect-Ratio Prussian Blue Nanotubes Using a Porous Alumina Template” Nano Lett., vol. 5, no 8, pp. 1603-1606, 2005.
• [15] A. Bobák, F. O. Abubrig and T. Balcerzak, “Multicritical points in the mixed ferromagnetic-ferrimagnetic ternary alloy with a single-ion anisotropy”, Phys. Rev. B, vol. 68, pp. 224405, December 2003.
• [16] A. Bobák, J. Dely and T. Balcerzak,“Compensation temperatures and susceptibility of ternary metal Prussian blue analogs”, Czech. J. Phys, vol: 54, pp. D523-D-526, June 2004.
• [17] A. Bobák, F. O. Abubrig and T. Balcerzak, “Phase diagrams of the mixed ferro-ferrimagnetic ternary alloy with a single-ion anisotropy”, J. Magn. Magn. Mater., vol. 272-276, pp. 989-990, 2004.
• [18] A. Bobák and J. Dely, “The effect of a single-ion anisotropy on the phase diagram of a mixed ferro-ferrimagnetic ternary alloy”, Physica A, vol. 341, pp. 281-298, 2004.
• [19] J. Dely and A. Bobák, “Magnetic properties of the ternary alloy with a structure of Prussian blue analogs” Physica B, vol. 388, pp. 49-58, 2007.
• [20] J. Dely and A. Bobák, “Phase diagrams of the ternary alloy with a single-ion anisotropy in the mean-field approximation”, J. Magn. Magn. Mater., vol. 305, pp. 464-466, 2006.
• [21] J. Dely, A. Bobák and D. Horváth , “Mean-Field and Monte Carlo Study of a Mixed Ferro-Ferrimagnetic Ternary Alloy”, Acta Phys. Pol. A, vol. 113, no 1, pp. 461-464, 2008.
• [22] J. Dely, A: Bobák and M. Žukovic ̌, “Critical temperature of a mixed ferro-ferrimagnetic ternary alloy”, J. Phys. Conf. Ser., vol. 200, pp. 022005, 2010.
• [23] Bobák, A. O. F. Abubrig and D. Horváth, “Magnetic properties of a mixed ferro–ferrimagnetic ternary alloy”, Physica A, vol. 312, pp. 187-207, 2002.
• [24] H. Hu, Z. Xin and W. Liu, “Magnetic properties of the mixed ferro-ferrimagnets composed of Prussian blue analogs with (AxB1–x)yC”, Phys. Lett. A, vol. 357, pp. 388-392, 2006.
• [25]J. Wei, G. H. Yu and L. V. Cheong, “Magnetization of mixed ferri-ferrimagnets composed of Prussian blue analogs A1xA21–xB”, Chin. Phys. B, vol. 20, no 5, pp. 057501, 2011.
• [26] E. Albayrak, J. Magn. Magn. Mater., “The mixed-spin ternary-alloy in the form of ABpC1-p on the Bethe lattice”, vol. 323, pp. 992-996, 2011.
• [27]B. Deviren, M. Keskin and Y. Aydin, “Compensation Temperatures, Magnetic Susceptibilities and Phase Diagrams of a Mixed Ferrimagnetic Ternary System on the Bethe Lattice”, JETP Letters, vol. 92, pp. 214-222, 2010.
• [28]G. Mert, “Green's function study of a three-sublattice mixed-spin Heisenberg ferromagnetic and ferrimagnetic system”, J. Magn. Magn. Mater., vol. 363, pp. 224-231, 2014.
• [29] G. M. Buendía and J. E. Villarroel, “Compensation temperatures of mixed ferro-ferrimagnetic ternary alloys”, J. Magn. Magn. Mater., vol. 310, pp. e495-e497, 2007.
• [30]J. Dely, A. Bobák and M. Žukovic ̌, “Compensation temperatures and magnetic susceptibility of a mixed ferro-ferrimagnetic ternary alloy”, Phys. Lett. A, vol. 373, pp. 3197-3200, 2009.
• [31] M. Žukovic ̌ and A. Bobák, “Critical and compensation phenomena in a mixed-spin ternary alloy: A Monte Carlo study”, J. Magn. Magn. Mater., vol. 322, pp. 2868, 2010.
• [32] S. Tsuji, T. Kasama and T. Idogaki, “Decoration–iteration transformation and Monte Carlo simulation for mixed ferrimagnetic ternary alloy”, J. Magn. Magn. Mater., vol. 310, pp. e471-e473, 2007.
• [33] E. K. Çam and E. Aydiner, J. Magn. Magn. Mater., “Compensation temperature of 3d mixed ferro-ferrimagnetic ternary alloy”, vol. 322, pp. 1706-1709, 2010.
• [34] E. K. Çam and E. Aydiner, “Magnetic Behavior of Ternary Prussian Blue Analog in Presence Single-Ion Anisotropy”, E. IEEE Trans. Magn., vol. 49, no 9, pp. 4951-4955, 2013.
• [35]Y. Yuksel, “Monte Carlo simulation of Prussian blue analogs described by Heisenberg ternary alloy model” J. Phys. Chem. Solids, vol. 86, pp. 207-214, 2015.
• [36] E. Vatansever, and Y. Yuksel, “Dynamic phenomena in magnetic ternary alloys”, J. Alloys Compd., vol. 689, pp. 446-450, 2016.
• [37] K. Binder, Monte Carlo Methods in Statistical Physics, Berlin: Springer, 1979.
• [38] M. E. J. Newman and G. T. Barkema, Monte Carlo Methods in Statistical Physics, Newyork: Oxford University Press, 1999.