Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access
  • Access by Xinjiang University

Numerical simulation of a two-dimensional Blume-Capel ferromagnet in an oscillating magnetic field with a constant bias

Celeste Mendes* and Gloria M. Buendía

Per Arne Rikvold

  • *Contact author: 17-10374@usb.ve
  • Contact author: buendia@usb.ve
  • Contact author: p.a.rikvold@fys.uio.no

Phys. Rev. E 110, 044133 – Published 22 October, 2024

DOI: https://doi.org/10.1103/PhysRevE.110.044133

Abstract

We perform a numerical study of the kinetic Blume-Capel (BC) model to find if it exhibits the metamagnetic anomalies previously observed in the kinetic Ising model for supercritical periods [P. Riego et al., Phys. Rev. Lett. 118, 117202 (2017); G. M. Buendía et al., Phys. Rev. B 96, 134306 (2017)]. We employ a heat-bath Monte Carlo (MC) algorithm on a square lattice in which spins can take values of ±1,0, with a nonzero crystal field, subjected to a sinusoidal oscillating field in conjunction with a constant bias. In the ordered region, we find an equivalent hysteretic response of the order parameters with its respective conjugate fields between the kinetic and the equilibrium model. In the disordered region (supercritical periods), we observed two peaks, symmetrical with respect to zero bias, in the susceptibility and scaled variance curves, consistent with the numerical and experimental findings on the kinetic Ising model. This behavior does not have a counterpart in the equilibrium model. Furthermore, we find that the peaks occur at higher values of the bias field and become progressively smaller as the density of zeros, or the amplitude of the oscillating field, increases. Using nucleation theory, we demonstrate that these fluctuations, as in the Ising model, are not a critical phenomenon, but that they are associated with a crossover between a single-droplet (SD) and a multidroplet (MD) magnetization switching mechanism. For strong (weak) bias, the SD (MD) mechanism dominates. We also found that the zeros concentrate on the droplets' surfaces, which may cause a reduced interface tension in comparison with the Ising model [M. Schick et al., Phys. Rev. B 34, 1797 (1986)]. Our results suggest that metamagnetic anomalies are not particular to the kinetic Ising model, but rather are a general characteristic of spin kinetic models, and provide further evidence that the equivalence between dynamical phase transitions and equilibrium ones is only valid near the critical point.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (71)

  1. M. Blume, V. J. Emery, and R. B. Griffiths, Ising model for the λ transition and phase separation in He3He4 mixtures, Phys. Rev. A 4, 1071 (1971).
  2. H. W. Capel, On the possibility of first-order phase transitions in Ising systems of triplet ions with zero-field splitting, Physica (Utrecht) 32, 966 (1966).
  3. I. D. Lawrie and S. Sarbach, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic Press, New York, 1984), Vol. 9.
  4. J. B. Collins, P. A. Rikvold, and E. T. Gawlinski, Finite-size scaling analysis of the S=1 Ising model on the triangular lattice, Phys. Rev. B 38, 6741 (1988).
  5. N. B. Wilding, Coexistence curve singularities at critical end points, Phys. Rev. Lett. 78, 1488 (1997).
  6. W. Selke and J. Oitmaa, Monte Carlo study of mixed-spin S=(1/2,1) Ising ferrimagnets, J. Phys.: Condens. Matter 22, 076004 (2010).
  7. D. Silva, G. M. Buendía, and P. A. Rikvold, Multicritical bifurcation and first-order phase transitions in a three-dimensional Blume-Capel antiferromagnet, Phys. Rev. E 108, 024122 (2023).
  8. W. Kwak, J. Jeong, J. Lee, and D. H. Kim, First-order phase transition and tricritical scaling behavior of the Blume-Capel model: A Wang-Landau sampling approach, Phys. Rev. E 92, 022134 (2015).
  9. A. Malakis, P. Kalozoumis, and N. Tyraskis, Monte Carlo studies of the square Ising model with next-nearest-neighbor interactions, Eur. Phys. J. B 50, 63 (2006).
  10. C. J. Silva, A. A. Caparica, and J. A. Plascak, Wang-Landau Monte Carlo simulation of the Blume-Capel model, Phys. Rev. E 73, 036702 (2006).
  11. J. Zierenberg, N. G. Fytas, M. Weigel, W. Janke, and A. Malakis, Scaling and universality in the phase diagram of the 2D Blume-Capel model, Eur. Phys. J.: Spec. Top. 226, 789 (2017).
  12. J. G. Brankov, J. Przystawa, and E. Praveczki, Effect of crystal field anisotropy on the Curie temperature of an Ising ferromagnet: HTS expansion method, J. Phys. C 5, 3387 (1972).
  13. T. W. Burkhardt and H. J. F. Knops, Renormalization-group results for the Blume-Capel model in two and three dimensions, Phys. Rev. B 15, 1602 (1977).
  14. W. M. Ng and J. H. Barry, Cluster-variation method applied in the pair approximation to the S=1 Ising ferromagnet having additional single-ion-type uniaxial anisotropy, Phys. Rev. B 17, 3675 (1978).
  15. T. Balcerzak and J. Tucker, The spin 1 Blume-Capel model with RKKY interactions, J. Magn. Magn. Mater. 278, 87 (2004).
  16. A. Zaim, Y. E. Amraoui, M. Kerouad, and H. Arhchoui, Monte Carlo study of the spin-1 Blume-Capel Ising film, J. Magn. Magn. Mater. 320, 1030 (2008).
  17. J. Lajzerowicz and J. Sivardière, Spin-1 lattice-gas model. I. Condensation and solidification of a simple fluid, Phys. Rev. A 11, 2079 (1975).
  18. P. A. Rikvold, J. B. Collins, G. D. Hansen, and J. D. Gunton, Three-state lattice gas on a triangular lattice as a model for multicomponent adsorption, Surf. Sci. 203, 500 (1988).
  19. J. Sivardière and J. Lajzerowicz, Spin-1 lattice-gas model. II. Condensation and phase separation in a binary fluid, Phys. Rev. A 11, 2090 (1975).
  20. J. Sivardière and J. Lajzerowicz, Spin-1 lattice-gas model. III. Tricritical points in binary and ternary fluids, Phys. Rev. A 11, 2101 (1975).
  21. M. Schick and W. H. Shih, Spin-1 model of a microemulsion, Phys. Rev. B 34, 1797 (1986).
  22. Y. Benhouria, I. Essaoudi, A. Ainane, R. Ahuja, and F. Dujardin, Hysteresis loops and dielectric properties of a mixed spin Blume-Capel Ising ferroelectric nanowire, Phys. A (Amsterdam) 506, 499 (2018).
  23. A. N. Berker and M. Wortis, Blume-Emery-Griffiths-Potts model in two dimensions: Phase diagram and critical properties from a position-space renormalization group, Phys. Rev. B 14, 4946 (1976).
  24. N. S. Branco and B. M. Boechat, Real-space renormalization-group study of the two-dimensional Blume-Capel model with a random crystal field, Phys. Rev. B 56, 11673 (1997).
  25. M. Kaufman, R. B. Griffiths, J. M. Yeomans, and M. E. Fisher, Three-component model and tricritical points: A renormalization-group study. Two dimensions, Phys. Rev. B 23, 3448 (1981).
  26. D. P. Snowman, Blume-Capel Ising ferromagnet with competing crystal-field interactions, Phys. Rev. E 79, 041126 (2009).
  27. J. D. Kimel, P. A. Rikvold, and Y. L. Wang, Phase diagram for the antiferromagnetic Blume-Capel model near tricriticality, Phys. Rev. B 45, 7237 (1992).
  28. T. Fiig, B. M. Gorman, P. A. Rikvold, and M. A. Novotny, Numerical transfer-matrix study of a model with competing metastable states, Phys. Rev. E 50, 1930 (1994).
  29. J. A. Plascak, J. G. Moreira, and F. C. sáBarreto, Mean field solution of the general spin Blume-Capel model, Phys. Lett. A 173, 360 (1993).
  30. H. Ez-Zahraouy and A. Kassou-Ou-Ali, Phase diagrams of the spin-1 Blume-Capel film with an alternating crystal field, Phys. Rev. B 69, 064415 (2004).
  31. A. K. Jain and D. P. Landau, Monte Carlo study of the fcc Blume-Capel model, Phys. Rev. B 22, 445 (1980).
  32. N. Boccara, A. Elkenz, and M. Saber, Mean-field theory of the spin-1 Ising model with a random crystal field, J. Phys.: Condens. Matter 1, 5721 (1989).
  33. Y.-L. Wang and J. D. Kimel, Multicrtitical behavior in the antiferromagnetic Blume-Capel model, J. Appl. Phys. 69, 6176 (1991).
  34. A. Malakis, A. N. Berker, I. A. Hadjiagapiou, N. G. Fytas, and T. Papakonstantinou, Multicritical points and crossover mediating the strong violation of universality: Wang-Landau determinations in the random-bond d=2 Blume-Capel model, Phys. Rev. E 81, 041113 (2010).
  35. A. Malakis, A. N. Berker, N. G. Fytas, and T. Papakonstantinou, Universality aspects of the d=3 random-bond Blume-Capel model, Phys. Rev. E 85, 061106 (2012).
  36. E. N. M. Cirillo and E. Olivieri, Metastability and nucleation for the Blume-Capel model. Different mechanisms of transition, J. Stat. Phys. 83, 473 (1996).
  37. E. N. M. Cirillo, V. Jacqier, and C. Spitoni, Homogeneous and heterogeneous nucleation in the three-state Blume-Capel model, Phys. D (Amsterdam) 461, 134125 (2024).
  38. G. M. Buendía and E. Machado, Kinetics of a mixed Ising ferrimagnetic system, Phys. Rev. E 58, 1260 (1998).
  39. M. Keskin, O. Canko, and Ü. Temizer, Dynamic phase transition in the kinetic spin-1 Blume-Capel model under a time-dependent oscillating external field, Phys. Rev. E 72, 036125 (2005).
  40. M. Keskin, O. Canko, and Ü. Temizer, Dynamic phase transition in the kinetic spin-1 Blume-Capel model: Phase diagrams in the temperature and crystal-field interaction plane, J. Exp. Theor. Phys. 104, 936 (2007).
  41. X. Shi and G. Wei, Effective-field and Monte Carlo studies of a kinetic Blume-Capel model, Phys. Scr. 89, 075805 (2014).
  42. M. Acharyya and A. Halder, Blume-Capel ferromagnet driven by propagating and standing magnetic field wave: Dynamical modes and nonequilibrium phase transition, J. Magn. Magn. Mater. 426, 53 (2017).
  43. E. Vatansever and N. G. Fytas, Dynamic phase transition of the Blume-Capel model in an oscillating magnetic field, Phys. Rev. E 97, 012122 (2018).
  44. P. Riego, P. Vavassori, and A. Berger, Metamagnetic anomalies near dynamic phase transitions, Phys. Rev. Lett. 118, 117202 (2017).
  45. D. T. Robb, P. A. Rikvold, A. Berger, and M. A. Novotny, Conjugate field and fluctuation-dissipation relation for the dynamic phase transition in the two-dimensional kinetic Ising model, Phys. Rev. E 76, 021124 (2007).
  46. D. T. Robb, Y. H. Xu, O. Hellwig, J. McCord, A. Berger, M. A. Novotny, and P. A. Rikvold, Evidence for a dynamic phase transition in [Co/Pt]3 magnetic multilayers, Phys. Rev. B 78, 134422 (2008).
  47. S. W. Sides, P. A. Rikvold, and M. A. Novotny, Kinetic Ising model in an oscillating field: Finite-size scaling at the dynamic phase transition, Phys. Rev. Lett. 81, 834 (1998).
  48. G. M. Buendía and P. A. Rikvold, Dynamic phase transition in the two-dimensional kinetic Ising model in an oscillating field: Universality with respect to the stochastic dynamics, Phys. Rev. E 78, 051108 (2008).
  49. H. Park and M. Pleimling, Surface criticality at a dynamic phase transition, Phys. Rev. Lett. 109, 175703 (2012).
  50. O. Idigoras, P. Vavassori, and A. Berger, Mean field theory of dynamic phase transitions in ferromagnets, Phys. B: Condens. Matter 407, 1377 (2012).
  51. H. Park and M. Pleimling, Dynamic phase transition in the three-dimensional kinetic Ising model in an oscillating field, Phys. Rev. E 87, 032145 (2013).
  52. G. M. Buendía and P. A. Rikvold, Fluctuations in a model ferromagnetic film driven by a slowly oscillating field with a constant bias, Phys. Rev. B 96, 134306 (2017).
  53. J. M. Marín Ramírez, E. Oblak, P. Riego, G. Campillo, J. Osorio, O. Arnache, and A. Berger, Experimental exploration of dynamic phase transitions and associated metamagnetic fluctuations for materials with different Curie temperatures, Phys. Rev. E 102, 022804 (2020).
  54. M. Quintana, C. Martín Valderrama, and A. Berger, Metamagnetic fluctuation characteristics near dynamic phase transitions, Phys. Rev. E 108, 064121 (2023).
  55. Y. Yüksel, Dynamic phase transition properties and metamagnetic anomalies of kinetic Ising model in the presence of additive white noise, Phys. A (Amsterdam) 580, 126172 (2021).
  56. Y. Yüksel, Exploring the equilibrium and dynamic phase transition properties of the Ising ferromagnet on a decorated triangular lattice, Phys. Rev. E 108, 034125 (2023).
  57. X. Shi and P. Liu, Metamagnetic anomalies in the kinetic Ising model, Phys. A (Amsterdam) 536, 120998 (2019).
  58. M. Bati, Mixed spin (1, 5/2) Ising ferromagnetic Blume-Capel model under time-dependent sinusoidal magnetic field: An effective-field theory analysis, J. Supercond. Novel Magn. 31, 821 (2017).
  59. Y. Yüksel, Ü. Akinci, and E. Vatansever, Metamagnetic anomalies in the kinetic Blume-Capel model with arbitrary spin, Phys. A (Amsterdam) 603, 127867 (2022).
  60. E. Vatansever and N. G. Fytas, Dynamic phase transitions in the presence of quenched randomness, Phys. Rev. E 97, 062146 (2018).
  61. Y. Yüksel, Dynamic phase transition and universality in a quasi 2D system: Bilayer Ising/Blume-Capel ferromagnet on a honeycomb lattice, J. Magn. Magn. Mater. 513, 167249 (2020).
  62. A. Vasilopoulos, Z. D. Vatansever, E. Vatansever, and N. G. Fytas, Monte Carlo study of the two-dimensional kinetic Blume-Capel model in a quenched random crystal field, Phys. Rev. E 104, 024108 (2021).
  63. P. Riego, P. Vavassori, and A. Berger, Towards an understanding of dynamic phase transitions, Phys. B: Condens. Matter 549, 13 (2018).
  64. P. A. Rikvold, H. Tomita, S. Miyashita, and S. W. Sides, Metastable lifetimes in a kinetic Ising model: Dependence on field and system size, Phys. Rev. E 49, 5080 (1994).
  65. H. Tomita and S. Miyashita, Statistical properties of the relaxation processes of metastable states in the kinetic Ising model, Phys. Rev. B 46, 8886 (1992).
  66. H. L. Richards, S. W. Sides, M. A. Novotny, and P. A. Rikvold, Magnetization switching in nanoscale ferromagnetic grains: Description by a kinetic Ising model, J. Magn. Magn. Mater. 150, 37 (1995).
  67. A. Kolmogorov, A statistical theory for the recrystallization of metals, Bull. Acad. Sci. USSR, Phys. Ser. 1, 355 (1937).
  68. W. Johnson and R. Mehl, Reaction kinetics in processes of nucleation and growth, Trans. Am. Inst. Min. Metall. Eng. 135, 416 (1939).
  69. M. Avrami, Kinetics of phase change. I General theory, J. Chem. Phys. 7, 1103 (1939); Kinetics of phase change. II Transformation‐time relations for random distribution of nuclei, 8, 212 (1940); Granulation, phase change, and microstructure kinetics of phase change. III, 9, 177 (1941).
  70. S. W. Sides, P. A. Rikvold, and M. A. Novotny, Kinetic Ising model in an oscillating field: Avrami theory for the hysteretic response and finite-size scaling for the dynamic phase transition, Phys. Rev. E 59, 2710 (1999).
  71. G. Korniss, C. J. White, P. A. Rikvold, and M. A. Novotny, Dynamic phase transition, universality, and finite-size scaling in the two-dimensional kinetic Ising model in an oscillating field, Phys. Rev. E 63, 016120 (2000).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation