Abstract.
Numerical simulations of the field dependence of the isothermal remanent moment (IRM) and the thermoremanent moment (TRM) are presented, based on a Preisach formalism which decomposes the free energy landscape into an ensemble of thermally activated, temperature dependent, double well subsystems, each characterized by a dissipation field H d and a bias field H s . The simulations show that the TRM approaches saturation much more rapidly than the corresponding IRM and that, as a consequence, the characteristics of the IRM are determined primarily by the distribution of dissipation fields, as defined by the mean field \(\bar {H}_d (T)\) and the dispersion \(\sigma_d (T)\), while the characteristics of the TRM are determined primarily by a mixture of the mean dissipation field \(\bar {H}_d (T)\) and the dispersion of bias fields \(\sigma_s (T)\). The simulations also identify a regime \(\bar {H}_d \gg\sigma_s \), where the influence of \(\bar {H}_d (T)\) on the TRM is negligible, and hence where the TRM and the IRM provide essentially independent scans of the Preisach distribution along the two orthogonal H s and H d directions, respectively. The systematics established by the model simulations are exploited to analyze TRM and IRM data from a mixed ferromagnetic perovskite Ca0.4Sr0.6RuO3, and to reconstruct the distribution of characteristic fields H d and H s , and its variation with temperature.
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Received: 16 April 2004, Published online: 12 August 2004
PACS:
75.60.Ej Magnetization curves, hysteresis, Barkhausen and related effects - 75.60.-d Domain effects, magnetization curves, and hysteresis
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Roshko, R.M., Viddal, C. Interpreting remanence isotherms: a Preisach-based study. Eur. Phys. J. B 40, 145–151 (2004). https://doi.org/10.1140/epjb/e2004-00253-3
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DOI: https://doi.org/10.1140/epjb/e2004-00253-3