Advances in Condensed Matter Physics

Volume 2018 (2018), Article ID 8479684, 12 pages

https://doi.org/10.1155/2018/8479684

## Frequency Variation of the AC Order Parameter Susceptibility of the Metamagnetic Ising Model

Department of Physics, Dokuz Eylül University, 35160 Izmir, Turkey

Correspondence should be addressed to Gul Gulpinar; rt.ude.ued@raniplug.lug

Received 18 January 2018; Revised 16 February 2018; Accepted 26 February 2018; Published 18 April 2018

Academic Editor: Yuri Galperin

Copyright © 2018 Gul Gulpinar. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

The extensive investigation of the absorptive and reactive parts of the AC order parameter susceptibility spectra of iron group dihalides, which is obtained on the basis of Onsager theory of irreversible processes, revealed the fact that the diagonal phenomenological rate coefficients and have an important impact on the nature of the order parameter relaxation process. The number of the relaxation peaks appearing in the double logarithmic plots of versus field frequency and the number of plateau regions in spectrum depends on the values of and . Only for does the relaxation evolve from a simple Debye exponential at high temperatures to a two-step process at lower temperatures in which there exist two long relaxation times characterizing the relaxation of staggered magnetization. In parallel with these characteristics of the order parameter relaxation, Cole-Cole plots () are shown to consist of two arcs in the metamagnetic phase and of a semicircle in the paramagnetic phase.

#### 1. Introduction

If a magnetic system is perturbed by an alternative current (AC) external magnetic field, magnetic properties of the system that are coupled to the magnetic field change accordingly. This fact lets the investigation of the AC susceptibility play an important role in the study of magnetic phase transitions and spin dynamics [1–4]. The AC susceptibility of correlated spin structures consisting of clusters or domains of various volumes is generally described by models based on linear response theory which assumes a single relaxation time or a distribution of relaxation times that measure how fast the system approaches equilibrium after a disturbance [5–7]. In the phenomenological spin-glass model prescribing a wide distribution of relaxation times, it has been reported that the imaginary part of the AC susceptibility is related to the density of relaxation times [6–8].

Metamagnetic systems are systems that have both ferromagnetic and antiferromagnetic couplings, simultaneously. They attracted much interest due to the fact that it is possible to induce novel kinds of critical behavior by forcing competition between these couplings, especially by applying a magnetic field [9, 10]. Compounds such as , , , , , and are grouped as metamagnetic substances [11]. The transitions in these materials are so-called field induced transitions which are distinguished from other magnetization processes. In particular, and are well-known Ising type metamagnets [9]. The spins of the iron ions display a ferromagnetic order in the triangular layers, perpendicular to the -axis of the crystals, with the sign of the magnetization per layer changing layer by layer: say an “up (+)” layer is followed by a “down (−)” layer in the metamagnetic phase. If one applies an external physical magnetic field , one type of layer (i.e., “”) is favored, and keeps on increasing, eventually the magnetization will be equal in all layers [12]. The corresponding phase transition is of the first order at low temperatures, while it is continuous at higher temperatures and low fields.

The aim of this study is to formulate the steady-state dynamics and investigate the frequency variance of the AC order parameter susceptibility of a metamagnetic Ising system via the phenomenological kinetic coefficients and the linear response theory. In particular, the frequency behavior of the AC staggered susceptibility of the metamagnetic Ising model near the field induced Neel point will be studied. The critical and multicritical characteristics of the relaxation times of the model are presented by studying the relaxation dynamics [13, 14]. Recently, only the temperature variations of the static and dynamic magnetic response functions for the same model Hamiltonian have been presented by studying the steady-state solutions of the kinetic equations in the existence of oscillating staggered field [15]. The AC susceptibility obtained by means of linear response theory is independent of the amplitude but dependent on the frequency of the AC field. In addition, even though the temperature dependence and critical exponents of the real and imaginary parts of the AC susceptibility characterize the relaxation process of a spin system near the critical point, the temperature variance is not a good criterion to detect the existence of long relaxation times which characterize relaxation of the order parameter [16].

A brief discussion of the mean-field equilibrium behavior of the model is given in Section 2. Section 3 is devoted to the derivation of the relaxation times and the frequency dependent AC order parameter susceptibility, . The AC order parameter susceptibility spectra and Cole-Cole plots () are presented near the critical point in Section 4. Finally, a summary and discussion of the results are given in the last section.

#### 2. Equilibrium Properties of the Model

The metamagnetic Ising model on a simple cubic lattice, setting the lattice constant equal to one, can be described by the Hamiltonianwhere Ising spin at site can take one of two values () depending on whether the spin is “up” or “down,” respectively. The first sum refers to couplings between spins and in the same - layers, the second sum denotes interactions of spins in adjacent layers, and the physical and staggered fields and act on all spins. In this spin system, there exist antiferromagnetic interlayer couplings, , and ferromagnetic intralayer interactions between neighboring spins, .

The reference spin, at site (), interacts only with its two nearest neighbors, at sites () and () in the adjacent layers above and below, with the coupling . In addition, it couples to its four nearest neighbors in its layer located at (), (), (), and () via ferromagnetic intralayer exchange coupling . Due to the existence of the antiferromagnetic coupling, it is convenient to divide the system into two sublattices ( and ) and define magnetization of each sublattice as and . In addition, one should introduce total and staggered magnetization as follows:The mean-field free energy of the system can be expressed as follows:where are the number of spins, temperature, Boltzmann constant, Bohr magneton, spin factor, total number of spins, and coordination numbers, respectively [9, 13]. As discussed above, and . Using the minimization conditions of equilibriumthe following self-consistent equations are obtained:Here, and .

As one converges to critical point, the staggered magnetization () vanishes whereas the total magnetization () stays finite [12]. Thus, is the order parameter of the metamagnetic Ising model. In the extensive theoretical review by Kincaid and Cohen, it has been reported that, depending on the ratio of the antiferromagnetic and ferromagnetic exchange interactions (), metamagnetic Ising model exhibits different kinds of phase diagrams in () plane for .

(i) If , then the phase transition between the antiferromagnetic and paramagnetic phases is discontinuous at low temperatures and strong fields while it is continuous at higher temperature regime. First- and second-order transition lines are joined at the tricritical point (see Figure of [13]).

(ii) If , then the topology of the phase diagram changes in nature: the transitions between the antiferromagnetic and paramagnetic phases are of the first order at low temperatures and strong magnetic fields while they are of the second order at high temperature regions. In addition, the phase diagram displays reentrance: a portion of the second-order transition line is masked by a first-order transition line which gives rise to an appearance of a critical endpoint where the second-order line meets two first-order lines, one of which is immersed in the ordered phase and ends at a double critical endpoint (see Figure of [13]).

#### 3. Derivation of AC Order Parameter Susceptibility

In this section, we will first discuss the relaxation behavior of the metamagnetic Ising model by investigating the relaxation process which takes place if there exists a small disturbance that removes the system slightly from equilibrium. Then, we will study the steady-state response of the system to an oscillating staggered magnetic field, which will let us obtain the frequency dependent AC order parameter susceptibility.

##### 3.1. Free Energy Production, Rate Equations, and Relaxation Times

It is well known that the metamagnetic-paramagnetic phase transition lines occur at places which are away from the axis. Since then, we have assumed that there exist small deviations in the physical and staggered magnetic fields () only for a short while, which removes the system slightly from equilibrium [9]. The near-equilibrium free energy of the system can be expressed as follows:where is the equilibrium free energy and is the production of the free energy due to the variance of the external fields. The free energy production for the metamagnetic Ising model readswherewhich are the so-called free energy production coefficients. The time derivatives of the staggered and total magnetization are treated as generalized currents conjugate to their appropriate generalized forces in the realm of the theory of irreversible thermodynamics. One obtains the generalized forces and conjugate to the generalized currents and by differentiating with respect to and :The relations between the currents and forces may be expressed in terms of a matrix of the phenomenological rate coefficients. Since both and are odd variables under time inversion, this matrix should be symmetric [13, 17]. Thus, the off-diagonal elements will be identical:

One should consider the corresponding homogeneous equations resulting when there is no external stimulation ( and ) in order to obtain two relaxation times that will govern the relaxation dynamics of the system. Then, the matrix equation given by (9) becomes

One can observe from (11) that the off-diagonal rate coefficient () couples the total and staggered magnetization currents. The kinetic equations given by (10) can be solved by assuming a form for the solution () by making use of the secular equation given below:The resulting reciprocal relaxation times can be found aswhere is given as follows:

We should emphasize that, for temperatures near the Neel temperature, the following assumption is valid:

In other words, we do not take into account the interference between the relaxation processes of staggered and total magnetization. Temperature variances of the relaxation times for finite external magnetic field values in the ordered and disordered phases for the Onsager rate coefficient sets satisfying the assumption (see (15)) were discussed in [13]. The findings of this study can be summarized as follows: for continuous phase transitions, scarcely varies with temperature in the ordered phase and rises slightly just below and above the phase transition temperatures. It should be noted that cusps are observed for the critical behavior of , whereas increases rapidly with rising temperature and diverges near the second- and the higher-order phase transition points as . In other words, is the dominant relaxation time which characterizes the critical slowing down of the staggered magnetization.

##### 3.2. Response of the System to a Time-Varying Staggered Magnetic Field

In order to derive the kinetic equations leading to complex order parameter susceptibility, let us assume that the system is stimulated by a staggered magnetic field oscillating at an angular frequency while . It is a well-known fact that all quantities will oscillate at at the steady state:

In addition, embedding (16) into the kinetic equations (10), one obtainsSolving (17) yields the following expression for :

The determinant in the denominator of (18) is the same as the secular determinant which is used for the calculation of the reciprocal relaxation times given by (11) except for the replacement of by . Hence, (18) may be written as

Now, (19) is needed in order to calculate the complex staggered susceptibility . This may be seen as follows. The total induced staggered magnetic moment per unit volume of the metamagnetic Ising model is given by

Here, is the staggered magnetization induced by a staggered field oscillating at -frequency. Further, by definition, the expression for the complex staggered susceptibility reads

Comparing (19) and (21), one may write complex staggered susceptibility as follows:

Finally, using the relationone finds

and contain a linear superposition (with a temperature dependent coefficient) of two Debye forms characterized by the two relaxation times of the metamagnetic Ising model (). In accordance with the fact that our analysis is based on linear response theory, the real and imaginary parts of are independent of the amplitude of the time-varying staggered field but dependent on the frequency of the field . On the other hand, physical interpretations of the real and imaginary parts of the complex susceptibility are different. The imaginary part can be expressed as , where is the complex conjugate of . In addition, by making use of the fact that is the inverse Fourier transform of , one obtainsEquation (25) indicates that the imaginary part of is attributable to the part of dynamic response function which is not invariant under time reversal. Namely, it arises due to dissipative irreversible processes that take place in the system. Due to the fact that is the dissipative or absorptive part of the response function, it is called the absorption factor. The same analysis as above shows that the real component is given by the following equation for the real part:Contrary to the absorption factor, the real part is invariant under time reversal and is thus related to the reversible magnetization process and stays in phase with the oscillating staggered magnetic field. Since then, has been called the dispersion factor or in-phase component of the AC staggered susceptibility [5].

#### 4. Frequency Response of the AC Order Parameter Susceptibility

It is instructive to review the zero and -frequency limits of the staggered dispersion and absorption factors first. The metamagnetic Ising model experiences the so-called phenomenon of critical slowing down characterized by the dominant relaxation time in the vacancy of the field induced Neel point [13]. Thus, is the quantity that rules the separation of the so-called low- and high-frequency regions. In addition, since as , one can choose to keep the frequency of the oscillating staggered field fixed and observe, for certain fixed frequencies, the low-frequency behaviors followed by the higher-frequency behaviors as . Since then, for any finite , one can observe the high-frequency results if the temperature considered is close enough to the critical temperature .

The investigation of the temperature variance of the staggered dispersion and absorption factors of the metamagnetic Ising model has shown that their critical characteristics in high- and low-frequency regions are quite different [15]. In the low-frequency regime, the AC staggered magnetization can readily follow the applied field since is small. In addition, due to the fact that varies as , if one approaches the Neel point, the low-frequency region corresponds to zero frequency limit for which corresponds to the isothermal staggered susceptibility:Thus, one expects to converge to static results and to vanish in the zero frequency limit. As the frequency grows, the staggered magnetization generated by the AC staggered field cannot change more rapidly than the spin-spin relaxation time, so that the AC staggered susceptibility becomes lower and lower and approaches the adiabatic staggered susceptibility in the infinite-frequency limit [18, 19]:

One should note that the reduced values of the temperature and the physical and staggered magnetic fields will be utilized:from now on. Due to the fact that metamagnetic-paramagnetic phase transition takes place for zero static staggered field, in all figures. In light of this information, the reactive and dissipative parts of the AC staggered susceptibility spectra of the metamagnetic Ising model will be presented in the paramagnetic phase first. With this aim, and versus plots are given at while , , , and , , and . We should note that the diagonal and off-diagonal coefficients of the kinetic matrix satisfy the condition which is valid through our analysis as already discussed in Section 2. Denoted by the black curve, becomes the isothermal staggered susceptibility, whereas vanishes for . These results are in accordance with the temperature variances of and in the low-frequency region: follows the scaling law for temperatures converging and varies as and vanishes in the limit [15]. Finally, zero frequency limit of is comparable with the static results of iron group dihalides in static fields where increases rapidly with rising temperature and diverges at the critical and multicritical points [9, 20].

As shown in Figure 1, adopts a maximum value, undergoes a step-like change just for , and separates the so-called low- and high-frequency regions as a signature of the Debye type relaxation [18]. One can see from Figure 1 that both and vanish as . This implies that for and is in accordance with the fact that the adiabatic susceptibility is zero for vanishing static fields [18]. Parallel with these findings, the constant frequency thermal variance of of the metamagnetic Ising model is reported to display a local minimum equal to zero at and vary as for temperatures slightly below and above for frequencies that satisfy the condition . In addition, has two frequency dependent local maxima in paramagnetic and antiferromagnetic phases while displays a minimum at the phase transition point whose amplitude decreases with increasing frequency [15].