Research Article  Open Access
Temperature Dependence of the Tilt Angle for the Smectic ASmectic Transition in a Mixture of C770PDOB Ferroelectric Liquid Crystals near the Tricritical Point
Abstract
The temperature dependence of the tilt angle is studied in the smectic phase near the smectic Asmectic tricritical point for a mixture of 70PD0B in the ferroelectric liquid crystal C7 (). The meanfield models with the biquadratic ( is the spontaneous polarization) and (bilinear) coupling terms in the free energy expansion are used to analyze the experimental data for the tilt angle in this binary mixture. From our analysis, the coefficients given in the free energy expansion of the meanfield models are determined. Our results show that the meanfield theory explains adequately the observed behaviour of the C770PD0B mixture near the tricritical point.
1. Introduction
Smectic transitions in ferroelectric liquid crystals have been the subject of various experimental and theoretical studies. In particular, smectic A and C (or ) transitions have been investigated and reported in the literature.
In the smectic A phase, the liquid molecules are oriented along the director (orientational order parameter) and they show a transitional order in layers, whereas in the smectic C (or ) phase, additionally they make a tilt angle with the director which is perpendicular to the smectic layers. If the chiral molecules, which are optically active, exist in the liquid crystalline material, then the smectic phase occurs.
The smectic Asmectic () transition has been predicted by de Gennes [1] as the transition which belongs to the threedimensional universality class (,). This has not been confirmed by some early experiments which are in agreement with a Landau meanfield theory of the transition [2–7]. Some experimental [8–13] and theoretical [3, 14, 15] studies have shown that from the firstorder to a second order transition, there occurs a tricritical point (TCP). In our recent studies, tricritical behaviour of mixtures of C7+10.04 [16] and SCE9+SCE10 [17, 18] has been shown using the meanfield models. Meanfield models are applicable to many liquid crystalline systems and they predicted adequately the observed behaviour of those materials exhibiting phase transitions. The physical quantities measured to high accuracy can then be analyzed by a meanfield model and the type of transition (first order, second order, or tricritical) can be characterized. From this point of view, meanfield model is a more realistic theoretical model to be applicable to the experiments.
The meanfield models which describe the AC (or ) transitions have the free energy expanded in terms of the order parameters (tilt angle and the spontaneous polarization ) and their bilinear () and/or biquadratic () couplings [3, 14, 19, 20]. Dipolar interactions ( coupling) are of a chiral character which becomes importantly close to the transition, whereas quadrupolar interactions ( coupling) are of a nonchiral one which covers a wide range of temperatures below the transition temperature in the smectic C or phase. On the basis of our earlier meanfield models with the biquadratic coupling (), recently we have calculated tilt angle and the temperature shifts as a function of concentration for a mixture of 10.04+C7 [16] and the temperature dependence of the spontaneous polarization and the tilt angle for a mixture of SCE9+SCE10 [17, 18] for the transition. Very recently, we have studied the dielectric constant as a function of temperature for the transition in 4(3methyl2chlorobutanoyloxy)4′heptyloxybiphenly (A7) [21] and we have calculated a generalized smectichexatic phase diagram in various mixtures of liquids crystals [22].
In this study, we focus on the temperature dependence of the tilt angle for a mixture of C770PDOB ferroelectric liquid crystal close to the tricritical point (TCP). The ferroelectric material 4(3methyl2chlorobutanoyloxy)4′heptyloxy biphenly (C7) exhibits a large spontaneous polarization [11]. It undergoes a firstorder transition. When adding a second compound of 4heptyloxy4′decloxybenzoate (7OPDOB), this transition is driven towards a second order by passing through a tricritical point (TCP) [9]. The transition temperatures of C7 for the relevant phases are as follows: (53.9°C) and SmA (54.06°C) [8]. The transition temperatures of a binary mixture of C7+7OPDOB depending on the values (mol percent of 7OPDOB) [9] are given in Table 1. Ferroelectric liquid crystals with large spontaneous polarizations such as C7 can be used in switching display devices and liquid crystals devices. Their carbon13 nuclear magnetic resonance can be obtained experimentally to determine the temperature dependence of order parameter. In our previous study [21], we used our meanfield model with the coupling and calculated the dielectric constant (dielectric susceptibility) at various temperatures under constant electric field for A7. Our calculation for the tilt angle (order parameter) as a function of temperature was performed [21] using the molecular field theory [23] for A7. The experimental data for the dielectric constant of A7 [24] was then analyzed according to the expression derived from the meanfield model [21]. Similarly, we have used our meanfield model with the quadratic couplings ( is the orientational order parameter and is the tilt angle) for the smectichexatic phase transitions in various mixtures of liquid crystals in our recent study [22]. By expanding the free energy in terms of the order parameters ( and ), we derived the phase line equations and calculated a generalized phase diagram () on the basis of the experimental data [25].

In the present study, not only the quadric coupling but also coupling in the free energy of our meanfield model is considered and the temperature dependence of the tilt angle is derived in both cases. Instead of using the temperature dependence of the order parameter from the order parameter, from the molecular field theory [23], as we have also needed in our recent study [21], the versus relation derived here is directly used to analyze the experimental data [9]. This is more general in the sense that the experimental data can be analyzed freely with the fitted parameters determined, whereas the molecular field theory [23] predicts the temperature dependence of the order parameter according to the critical exponent . This, however, can restrict the analysis of the experimental data for various mixtures of liquid crystals. In order to get good fits, our versus expression is favorable. On this basis, we have fitted to the experimental data [9] the expression for the tilt angle as a function of temperature, which we derive from the meanfield models with the and couplings for the transition close to the TCP. Coefficients given in the meanfield energy are calculated from our fits and they are interpreted within the transition in this mixture of C770PDOB.
In Section 2, we give an outline of our meanfield models, where the temperature dependence of the tilt angle and the spontaneous polarization are derived. In Section 3, the tilt angle expression is fitted to the experimental data and the results are presented. Sections 4 and 5 give our discussion and conclusions, respectively.
2. Theory
The free energy of the smectic phase can be expanded in terms of the tilt angle and the spontaneous polarization for the transition in ferroelectric liquid crystals. By considering the quadrupolar interaction between the and (biquadratic coupling ), the free energy can be expressed as in the presence of the electric field , where , , , , and are constants. is the transition temperature, is the static dielectric susceptibility, and is the permittivity in free space. In the free energy expansion, the tilt angle is taken as the primary order parameter which does not exist in the smectic A phase. The spontaneous polarization is the secondary order parameter which is defined in both the smectic A and phases. We have introduced this model in our previous study [19].
In order to describe the transition, the energy is minimized with respect to the order parameters and . By minimizing the free energy with respect to the spontaneous polarization , we get at the zero electric field (), Also, by minimizing the free energy with respect to the tilt angle , we find that Equations (2) and (3) give the temperature dependence of the spontaneous polarization and tilt angle, respectively. By substituting (2) into (3), the temperature dependence of the primary order parameter (tilt angle) can be written as In (4) the temperature shifts, were used for a firstorder transition [19]. In (5) denotes the experimentally measured transition.
The free energy of the smectic phase can also be expanded in terms of the tilt angle and the spontaneous polarization by considering both the dipolar interactions (bilinear coupling ) and the quadrupolar interactions (biquadratic coupling ) for the transition in ferroelectric liquid crystals. The free energy can then be expressed as By minimizing the free energy with respect to the spontaneous polarization and the tilt angle as before, one gets respectively. By substituting (7) into (8), the temperature dependence of the tilt angle can be written as Using (1) and (6) with the and coupling in the free energies, respectively, the temperature dependence of the tilt angle can be predicted for the transition in ferroelectric liquid crystals.
3. Calculations and Results
The temperature dependence of the tilt angle was calculated for the transition of a binary mixture of 70PDOB in C7 near the tricritical point (). The value is the mol percent (mol %) of 70PDOB in C7, as given in Table 1 [9]. For this calculation, (4) was fitted to the experimental data [9] and the coefficients were determined. Table 2 gives values of the coefficients with the uncertainties from (4) according to the biquadratic coupling () for this mixture of 70PDOB+C7 when the tricritical concentration of 70PDOB is for the transition. We plot versus in Figure 1. We also calculated the temperature dependence of the tilt angle by fitting (9) to the experimental data [9] in the case of both biquadratic () and bilinear () couplings. Coefficients with the uncertainties and plots of versus are given in Table 2 and Figure 2, respectively.

4. Discussion
The tilt angle was calculated as a function of temperature in the phase for the transition near the tricritical concentration of 70PDOB () in C7 using the meanfield models with the (1) and (6) couplings, as shown in Figures 1 and 2, respectively. Both equations, (4) with the coupling and (9) with the , when fitted to the experimental data [9], describe the observed behaviour of the tilt angle near the tricritical point (TCP) satisfactorily. We also calculated the standard deviations of the fitted parameters for both meanfield models, as given in Table 2. The uncertainties in the coefficients of the free energies ((1) and (6)) are comparatively small in most cases (Table 2). However, these uncertainties can be significant for the coefficients in the free energies for both models since the critical behaviour of the mesomorphic mixture depends on those coefficients, in particular the coefficients of the coupling terms ( and ). For the mesomorphic mixture studied here, regarding the values of and (Table 2) for the second meanfield model (6), the bilinear coupling is dominant in comparison with the biquadratic coupling . However, considering all the values of the fitted parameters in the free energy expansion (Table 1), the meanfield model with the coupling (1) can still be preferred since (4) provides the values of the fitted parameters which are physically meaningful. This then indicates that the dominant mechanism of the smectic transition near the tricritical point is due to quadratic interactions for a mixture of 70PDOP+C7. In (1) the biquadratic coupling terms () characterizes the nonchiral properties and induces a transverse quadrupolar ordering. This is the dominant term in a wide temperature range far away from . To stabilize the mesomorphic mixture for far away , we included the term, which has also been considered in the generalized meanfield model for the smectic Achiralsmectic C phase transition in the case of p(ndecyloxybenzylidence)pamino(2methylbutly) cinnamate (DOBAMBC) in an earlier study [3]. Since the bilinear coupling term () characterizes the chiral properties close to the , the mesomorphic mixture is already stabilized with the biquadratic coupling term () and, no additional term such as is required, in (6). So that the free energy of the smectic phase is given in terms of the spontaneous polarization up to with the bilinear coupling term as also given previously [3] and with this free energy the system is stable. Thus, the temperature dependence of is for both meanfield models studied here. In fact the case of DOBAMBC, the relative importance of biquadratic term and term in comparison with terms involving and has been demonstrated numerically using the generalized meanfield model for the transition [3, Table III]. Thus, as explained previously [3], when relatively reliable experimental data is obtained in the temperature range studied, the biquadratic term and are not negligible as we also demonstrate in our study here (Table 2). Thus, the terms , , , and (1), and , , and (6) are required to explain the major features of the transition in C77OPDOB. We also note that from the data analysis point of view, if the term was added to the free energy of the phase (6), the fitting of the model to the experimental data would not have been a straightforward problem. This is due to the term appearing in (7) when the free energy was minimized with respect to the polarization . As a cubic polarization equation, two solutions would correspond to a local minimum of the free energy, which may then incorporate the thermal fluctuations in the meanfield model, as also pointed out previously [14].
The temperature dependence of the tilt angle was calculated here near the tricritical point () using the experimental data [9] where they obtained according to a powerlaw formula
In (10) is the tilt angle, is the amplitude, is the transition temperature, and is the critical exponent for the order parameter [26]. The experimental tiltangle data were analyzed within the temperature interval of 240 mK for mixture of 70PDOB in C7 [9]. The experimental tiltangle data were also the same as those obtained from the analyses within the temperature intervals of 103 mK , 490 mK , and 930 mK [9]. Similarly, the temperature dependence of the tilt angle can also be calculated for the transition in a mixture of 70PDOBC7 in the case of various concentrations of 70PDOB on the basis of our meanfield models given here. Since the tilt angle has been obtained from the layer spacing data as a function of for C7 and its mixture with 70PDOB for concentrations of 0 (C7), 5.15, 9.68, 15.0, and 19.4 [8], (4) and (9) can be fitted to those data to describe the transition in this mixture. Since corresponds to a firstorder transition in C7, as the concentration of 70PDOB increases towards , the transition then becomes a second order through (tricritical transition) for this mixture of 70PDOBC7. Thus, from a first order to a second order via the tricritical point (TCP) transition, as the concentration (70PDOB) increases, can be described adequately by calculating the temperature dependence of the tilt angle using the experimental data [9] on the basis of our meanfield models studied. Meanfield to tricritical crossover behaviour near the tricritical point can then be better understood for a mixture of 70PDOBC7. This work is under progress.
5. Conclusions
The tilt angle was predicted as a function of temperature for the transition of a mixture of 70PDOBC7 close to the tricritical point. The meanfield models which consider the quadratic and dipolar interactions between the tilt angle and the spontaneous polarization were used for this calculation of the tilt angle. Expressions for tilt angle which we derived from our meanfield models were fitted to the experimental data and the coefficients were determined.
Our results show that quadratic interactions seem to be dominant in the mechanism of the transition for the 70PDOBC7 mixture near the tricritical point in regard to the experimental data.
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Copyright © 2012 Mustafa Kurt and Hamit Yurtseven. 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.