# Temperature Dependence of the Electroclinic Effect in the Twist-Bend Nematic Phase

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## Abstract

**:**

_{TB}) phase of bent-shaped molecules has recently attracted much attention due to the spontaneous bend of its director field and the doubly-degenerate chirality of its heliconical structure. Despite intensive experimental and theoretical investigation worldwide, the main structural characteristics (pitch and conical angle) and elastic properties of the phase are still barely understood. This is mainly due to the difficulty in growing large single domains of the N

_{TB}phase, which prevents the application of the powerful electro-optical techniques developed for the nematic (N) phase. Moreover, the twist and bend distortions of the optic axis are forbidden by the pseudo-layered structure of the N

_{TB}phase, which makes its response to the field smectic-like instead of nematic-like. Therefore, the only macroscopic electric effect that can be observed deep in the N

_{TB}phase is the smectic-like “electroclinic” effect (ECE

_{NTB}). Here, we achieve large monochiral N

_{TB}domains which remain uniform over a wide temperature range (20–60 °C) in thin (1.5 µm) planar cells, thus avoiding the so-called stripe- and rope-like textural instabilities. This allowed us to experimentally determine, using electro-optical measurements, the temperature dependence of the ECE

_{NTB}response in four different N

_{TB}materials: namely the dimers CB7CB, CB9CB, CB6OCB, and BNA76. For all compounds, the thermal dependences of conical angle and pitch in the vicinity of the N-N

_{TB}transition follow the theoretically predicted power law behaviour. However, the agreement between the measured and predicted power law exponents remains only qualitative, which calls for improvement of the theoretical models.

## 1. Introduction

**n**. In the ground state, the director is uniform but, under external constraints, it can be distorted, which gives rise to elastic distortion energy [1]:

_{11}, K

_{22}, and K

_{33}are the elastic moduli for the three eigenmodes of the director distortion: splay $n(\nabla \cdot n)$, twist $n\cdot (\nabla \times n)$, and bend $n\times (\nabla \times n)$, respectively.

**h**, such that

**h**⊥

**n**.

_{b}. Another long-standing theoretical prediction [3,4,5,6] was that bent-shaped molecules can form nematic phases with a spontaneously bent director, namely the splay-bend nematic, N

_{SB}, and twist-bend nematic, N

_{TB}, phases. Two distinct origins of the spontaneous bend have been proposed: either the coupling of a flexoelectric polarization with a transverse ferroelectric polarization of the nematic [3,4] or an elastic instability of the phase due to the natural tendency of the bent-shaped molecules to orient parallel to a curved director [5,6]. For a long time, neither of these arguments attracted much attention, until the N

_{TB}phase was experimentally identified in the bent-shaped mesogenic dimer CB7CB [7]. As predicted, the molecules in the N

_{TB}phase form a conical helix, with helix axis

**h**, pitch p, and long molecular axis L parallel to the local director

**n**, that is tilted at an angle θ, with respect, to

**h**(see Figure 1). Moreover, the structure is locally biaxial, the curvature of the bent-shaped molecule matching the curvature of the director field and thus, the bend vector, $b=n\times (\nabla \times n)$ (

**b**⊥

**n**), is a secondary director of the nematic order tensor. Due to its heliconical structure, the N

_{TB}phase is chiral, even when it is formed by achiral molecules. The chiral symmetry of the phase is spontaneously broken [5] and two different structures are possible, with left or right-handedness of the conical helix. These chiral structures can coexist in the sample forming large monochiral domains suitable for optical and electro-optical observations [8,9,10].

_{TB}phase generated great interest and stimulated further chemical and physical studies. Hundreds of new bent-shaped mesogenic dimers presenting this phase have been synthesized (see [11,12] for recent reviews) and the N

_{TB}heliconical structure was confirmed [7,9,13,14,15,16,17,18,19,20] using a large number of techniques. X-ray scattering studies confirmed that the phase is indeed nematic, with no long-range positional order [7,14,21,22,23,24]. The early indirect prediction [9,25] of the extremely small pitch of the helix, p < 10 nm, was then quickly confirmed by direct freeze-fracture transmission electron microscopy studies [13,14] and later by resonant X-ray scattering experiments [18,19,26]. The values of p reported for different N

_{TB}-forming compounds are always of the order of 10 nm and slowly decrease with decreasing temperature.

_{TB}transition, θ < 10° for CB7CB, and even close to zero when the phase transition is very weak first order. As theoretically expected, θ increases up to 30–40° far below the transition temperature.

_{TB}phase behaves in several aspects as a smectic (Sm) phase. It shows typical smectic textures, such as focal-conics, fan-shaped textures, and stripe- and rope-textures [7], both in sandwich cells and as free drops. In biphasic coexistence with the conventional nematic phase, the N

_{TB}phase forms structures almost identical to the “bâtonnets” observed during the growth of the smectic A (SmA) phase from an isotropic melt [28]. The macroscopic elastic properties of the N

_{TB}phase and its response to external fields are also smectic-like [7,9,29,30,31]. This prevents applying to it the efficient and accurate electric and electro-optical techniques developed for the conventional nematic phase, thus limiting the choice of tools available to investigate its physical properties.

_{TB}phase [29,31]. The periodic mass-density wave of the smectic phase, which gives rise to the smectic layers, is absent in the N

_{TB}phase, but instead, a periodic distortion wave takes place because the planes perpendicular to the helix axis, which correspond to the same azimuthal orientation of the director, form a set of equidistant “pseudo-layers”. This pseudo-layered structure, which is quite similar to the well-known pseudo-layered structure of the cholesteric phase [29], is responsible for the smectic-like elastic properties at a large length scale (>>p).

_{TB}phase is periodic in one dimension (due to the pseudo-layering), uniaxial (due to the D

_{∞}global symmetry of the helix axis), and chiral (due to the helix handedness). This symmetry is the same as that of the chiral smectic A (SmA*) phase, which allowed for the coarse-grained (CG) description of the N-N

_{TB}phase transition [31,32], by analogy with the de Gennes theory [33] of the N-SmA phase transition. This CG approach provides the description of all the macroscopic properties of the twist-bend nematic [31,32], for example, the smectic-like elasticity, response to external fields, and surface anchoring. Moreover, after choosing one of the available microscopic models [5,34] of the N-N

_{TB}phase transition, the CG model allows one to calculate all the macroscopically relevant parameters and their temperature dependences in the N

_{TB}phase from the microscopic properties of the N-phase.

_{TB}-SmA* analogy, some of the electro-optic effects of the SmA*, such as the electro-clinic effect (ECE) [35], can be expected to have N

_{TB}analogues, such as the ECE

_{NTB}in the N

_{TB}phase [9]. Although the physical origin differs in the two cases, (ferroelectricity in SmA* instead of flexoelectricity in N

_{TB}), the result is the same: under a strong field, the distortion of the periodic structure results in a fast rotation of the optical axis, with respect to the normal (pseudo) layers. Despite the small amplitude of the effect, it can be measured precisely over a large temperature range [9] in the N

_{TB}phase, giving valuable (although semi-quantitative) information about the phase structure. However, due to some experimental issues (mainly the difficulty of obtaining large monochiral domains and to keep them uniform, deep in the N

_{TB}phase), a precise study of the ECE

_{NTB}has only been reported so far for CB7CB, even though it has qualitatively been described for a few other compounds [22,36,37].

_{NTB}response in four different N

_{TB}materials, the dimers CB7CB [7,20,38], CB9CB [15], CB6OCB [16], and BNA76 [39]. In thin planar cells, we achieve large monochiral domains which remain uniform over a wide temperature range. We measure the temperature dependencies of the amplitude and the characteristic time of the ECE

_{NTB}response in all four compounds and compare them with their theoretically predicted behaviour. The agreement of the experimental results with the theory remains only qualitative, suggesting the need to further improve the theoretical models.

## 2. Theoretical Background

_{NTB}and its coarse-grained description that have been reported in detail elsewhere [5,31,34,37,40].

#### 2.1. N_{TB}-SmA* Analogy and CG Description of the N_{TB} Phase

_{TB}phase is similar to that of the SmA*. The unperturbed SmA* state is uniaxial, with D

_{∞}symmetry axis along the director

**n**

_{0}, which is also the optic axis of the phase, and the mass density ρ is modulated along ${n}_{0}$, with wave vector ${q}_{0}={q}_{0}{n}_{0}$, where ${q}_{0}=2\pi /d$ and d is the layer thickness (see Figure 2a). When the SmA* phase is distorted, the director

**n**(

**r**) and the positions of the layers vary slowly in space, and this distortion costs some elastic energy. To describe the structure of the SmA phase and its elastic properties, de Gennes [33] introduced a complex order parameter $\psi =\left|\psi \right|\mathrm{exp}(i\varphi )$, where $\left|\psi \right|$ is the amplitude of the mass-density wave and ϕ is the phase which describes the local layer displacement, $u=d\varphi /2\pi $, and varies slowly in space.

**n**along the helix axis

**h**in the N

_{TB}phase is analogous to the density wave in the smectic. Accordingly, the N

_{TB}phase can be considered as a stack of pseudo-layers, perpendicular to

**h**, with a very small period, p ~10 nm. At a much larger, macroscopic, scale, the phase is uniaxial with a symmetry axis defined by the optic axis

**N**– a unit vector pointing along the average orientation of the director

**n**over one heliconical period, i.e., along the axis of the helical cone (see Figure 2b). By analogy with the SmA* phase, the structure of the N

_{TB}and its elastic properties can be described by a complex order parameter, $\sigma (r)=\mathrm{sin}\theta (r)\mathrm{exp}(i\phi (r))$ [31]. When $\theta (r)$ and $q(r)=\nabla \phi (r)$ are close to their equilibrium values and vary slowly with

**r**, the macroscopic elastic energy of the N

_{TB}is formally the same [31] as that of the SmA* [33]. It contains smectic-like terms, e.g., the pseudo-layer compression term, ${\scriptscriptstyle \frac{1}{2}}B{(1-p/{p}_{0})}^{2}$ which also takes into account the increase in the energy density when the pitch, p, deviates from its equilibrium value, p

_{0}. Another important smectic-like term, ${\scriptscriptstyle \frac{1}{2}}{K}_{\delta N}{\mathrm{sin}}^{2}\alpha $, includes the energy cost for the tilt of the optic axis

**N**by a small angle α, with respect to the helix axis,

**h**(

**N**is parallel to

**h**in the ground state but can deviate from

**h**under external constraints). Additionally, the energy contains three nematic-like terms,

**N**are forbidden because they are incompatible with the pseudo-layered structure of the phase. Moreover, the splay distortion of

**N**is coupled with a splay of the helix axis, which requires a reorganization of the layers and is strongly hindered in confined samples.

_{TB}–SmA* analogy provides the general expression for the macroscopic elastic energy of the distorted N

_{TB}phase but not the values of the elastic moduli. However, these moduli can be obtained by coarse-graining a microscopic model of the N–N

_{TB}phase transition [5,34]. For this purpose, one should consider a large-wavelength distortion of the phase having a small amplitude. The energy cost of the distortion is calculated using the microscopic model and the result is averaged over one pitch length, thus removing all of the periodic terms. The comparison of this microscopic result with the macroscopic elastic energy then provides the values of the elastic moduli.

_{TB}phase transition [5]. The basic assumption of this model is that the elastic constant K

_{33}of the nematic formed by bent-shaped molecules decreases with decreasing temperature T and becomes negative at some T = T*. Therefore, for T < T*, the ground state of the nematic is no longer uniform but it is spontaneously bent. However, as explained earlier, the bend distortion must be coupled to another distortion mode which is the twist mode in the case of the N

_{TB}phase. Introducing a fourth-order bend elastic modulus, C > 0, and assuming that K

_{33}varies linearly with temperature in the vicinity of T*, ${K}_{33}=a(T-{T}^{*})$, with $a>0$, and that all of the other nematic moduli remain approximately constant, one obtains [5], after minimization of the energy, that the ground-state structure of the phase is heliconical, with $n(z)=(\mathrm{sin}{\theta}_{0}\mathrm{cos}{q}_{0}z,\mathrm{sin}{\theta}_{0}\mathrm{sin}{q}_{0}z,\mathrm{cos}{\theta}_{0})$, where

**z**║

**h**. Under these assumptions, the system undergoes a second-order phase transition at T = T* and, close to T*, the equilibrium tilt angle and wave vector of the helix are given by:

_{TB}phase transition was proposed by Shamid et al. [34]. In that model, the transition is driven by the strong flexoelectric polarization expected in a nematic formed by bent-shaped molecules. Due to the strong flexoelectric fluctuations in the pretransitional nematic range, the effective bend modulus, ${K}_{33}^{eff}$, renormalized by the flexoelectric effect, decreases with decreasing temperature and changes sign at the N-N

_{TB}transition. Therefore, despite the different physical origins of the transition, that model also predicts a second-order phase transition at T = T* and, close to T*, the behaviour of the tilt angle and wave vector follow power laws:

_{TB}transition.

_{TB}phase [40]. It again predicts a second-order N-N

_{TB}transition at some temperature T*, but with a more complex temperature dependence of ${\theta}_{0}$ and ${q}_{0}$. This dependence shows a crossover of the power law exponents for ${\theta}_{0}$ and ${q}_{0}$ at some temperature T* − δT, where δT was found to be very small for the N

_{TB}-forming mixture studied in [40]. Indeed, for T* > T > T* − δT, the exponents are the same as in Equation (4), ${\beta}_{\theta}={\beta}_{q}=$1/2, while for T < T* − δT they become ${\beta}_{\theta}={\beta}_{q}=$1/4.

#### 2.2. Behaviour under External Fields

_{TB}phase to strong external fields, e.g., when an electric field, E, is applied, is expected to be different on the microscopic (<p) and macroscopic (>>p) scale. Microscopically, the response is nematic-like, with a local director,

**n**, reorientation inside the heliconical period, resulting in variation of the pitch and tilt angle [9,30,41], distortion of the helix from circular to elliptic [9,30], or field-induced transition to the nematic [30,41] or splay-bend nematic [42] phases. Due to the small pitch, the N

_{TB}phase is expected to be very stiff and these effects are very small for realistically strong fields. Indeed, no experimental evidence has been provided so far for this microscopic effect of the field, except for the N

_{TB}to N

_{SB}transition under a strong topological constraint [10] or strong electric field [42], E ~8 V/µm.

**n**, the torque integrated over a large volume of the N

_{TB}phase acts on the optic axis

**N**and can drive its reorientation. This macroscopic response may (or may not) be coupled with a reorientation of the helix axis. Indeed, the pseudo-layered structure of the phase forbids the bend and twist of

**N**in a defect-free N

_{TB}domain. The splay of

**N**under a field, although not forbidden, is also hindered in most sample geometries because it requires the reorientation and displacement of the pseudo-layers (large splay distortion leads also to layer dilation, which is energetically prohibitively costly). Consequently, smooth, continuous, and defect-less textural changes similar to the Fréedericksz transition in nematics are impossible in the N

_{TB}phase. Instead, in sufficiently strong fields, a large macroscopic N

_{TB}domain can reorient by coupled rotation of

**N**and

**h**, giving rise to the nucleation of many defects, located either in the bulk or at the grain boundaries separating the reoriented domain from the adjacent regions. This kind of irreversible, defect-mediated, effect was reported experimentally under moderate electric fields [7,43].

**E**, applied parallel to the SmA* layers, the director

**n**tilts at an angle α, with respect to the normal

**k**to the layers, in a plane perpendicular to

**E**(see Figure 3a). This effect can be understood as a field-induced SmA*-SmC* phase transition: in the SmC*, under field, the director

**n**is tilted, with respect to

**k**and the phase is ferroelectric, with the polarization ${P}_{fer}$ proportional to $n\times k$. In the SmA*, due to $n\parallel k$, ${P}_{fer}$ vanishes, but when the field is applied, it induces a director tilt and a ferroelectric polarization, ${P}_{fer}\ne 0$, with resulting energy gain $-E\cdot {P}_{fer}$(i.e., ECE is an inverse ferroelectric effect). The smectic elasticity, however, disfavors the tilt, and the energy minimization giving $\mathrm{sin}\alpha ={c}_{\alpha}E$, where ${c}_{\alpha}$ is the electroclinic coefficient. Typically, due to the stiff SmA elasticity, α is very small (α << 1°) even in strong fields, but much higher amplitudes have been reported in the vicinity of a SmA*-SmC* phase transition. For symmetry reasons, the smectic C ferroelectricity and the ECE are forbidden in an achiral medium. Indeed, the polarization ${P}_{fer}$ is a true vector, while $n\times k$ is a pseudo-vector, so their proportionality coefficient should be a pseudo-scalar, which cannot exist in an achiral system. Moreover, because the ECE response is linear in the field, the sign of α should change with the sign of E, as well as with the chirality handedness.

_{TB}phase, a fast linear electro-optic effect was observed in it [36] and has been reported as an analogue of the flexo-electric effect seen for cholesterics [44]. A detailed theoretical analysis [9] later showed that this effect is the N

_{TB}counterpart, ECE

_{NTB}, of the ECE in the SmA* phase. As in the SmA*, when a dc electric field

**E**is applied parallel to the pseudo-layers of an N

_{TB}monochiral domain (see Figure 3b), the optic axis

**N**tilts away from the helix axis

**h**at an angle α proportional to the field amplitude. Although ECE

_{NTB}and ECE have the same geometry, their physical origins differ in that the former is due to flexoelectricity whereas the latter is due to ferroelectricity. Indeed, as in usual nematics, the director distortion in the N

_{TB}phase results in a flexoelectric polarization, ${P}_{fl}={e}_{1}\hspace{0.17em}n(\nabla \cdot n)-{e}_{3}\hspace{0.17em}n\times (\nabla \times n)$, where ${e}_{1}$ and ${e}_{3}$ are Meyer’s splay and bend flexoelectric coefficients [45]. In the ground state of the N

_{TB}phase, the splay is negligible but the bend is strong, giving rise to a large polarization perpendicular to both

**h**and

**n**, and forming an orthogonal helix. Due to this heli-electric organization, the total flexo-polarization of the phase averages zero. However, it has been shown that a uniform tilt of the optic axis leads to excess average flexoelectric polarization, $\langle {P}_{fl}\rangle \propto \hspace{0.17em}N\times h$, which results, under an applied field

**E**, in an energy density gain $\langle {f}_{fl}\rangle =-\langle {P}_{fl}\rangle \cdot E$. The straightforward CG calculation and minimization of the energy give the amplitude of the ECE

_{NTB}tilt angle [9]:

_{TB}wavenumber (with its sign depending on the handedness of the domain). The values and the temperature dependences of the constants ${e}_{1}-{e}_{3}$, ${K}_{11}$, and ${K}_{22}$ in the N

_{TB}phase are unknown, but as a reasonable approximation, it may be assumed that they are continuous at the N-N

_{TB}transition and that their thermal variation is negligible compared to the fast variation of ${K}_{33}$ and ${q}_{0}$. Therefore, the electroclinic coefficient ${c}_{\alpha}$ is expected theoretically to vary as ${c}_{\alpha}\propto {(T*-T)}^{-{\beta}_{\alpha}}$, where the critical exponent is either ${\beta}_{\alpha}=$1/2 [9,31] or shows a cross-over from 1/2 to 1/4 at $T={T}^{*}-\delta T$ [40].

_{TB}transition and to follow an Arrhenius law on cooling. In the vicinity of the transition, for both microscopic models of the N-N

_{TB}transition, a power law behaviour of the response time is expected, $\tau \propto {({T}^{*}-T)}^{-{\beta}_{\tau}}$, where the critical exponent is either ${\beta}_{\tau}=$2 [9,31] or shows a cross-over from 2 to 1 at $T={T}^{*}-\delta T$ [40].

_{NTB}measurements have been reported only for CB7CB, showing a very fast effect ($\tau $ < 1 µs), with a small amplitude ($\alpha <$ 1° for E = 10 V/µm) [9]. Qualitatively, these results confirmed several important features predicted by Equations (5) and (6): the tilt angle increases linearly with E and changes sign with that of the field and with the handedness of the studied monochiral domain; the time-dependence of the tilt angle is exponential and shows the same response time for both the rise and fall. Estimating the values of ${e}_{1}-{e}_{3}$, ${K}_{11}$, ${K}_{22}$, and ${\gamma}_{1}$ from their usual nematic values, it was inferred that, close to the N-N

_{TB}transition, the pitch is extremely small, $p\approx $ 7 nm [9,25], a value that was later confirmed by more direct techniques [13,14,19].

_{TB}phase is interesting for two main reasons. On one side, its fast, sub-microsecond, response times are very attractive for practical applications, despite the disappointingly small tilt angle. Therefore, it is important to study a larger number of compounds showing the N

_{TB}phase to check whether these values are typical and whether they can be optimized. From a more fundamental point of view, the ECE technique is one of the few that can be applied, without hysteresis and reversibility issues, to test some basic structural parameters of the N

_{TB}phase over a large temperature range, thus providing an opportunity to discriminate between the available theoretical models. Moreover, we demonstrate here that the experimental difficulties (related to the small values of $\alpha $ and $\tau $, especially, to the realization of the required large, uniform, monochiral domains) that have so far hampered the investigation of the ECE, can be easily overcome to gather useful information about the N

_{TB}phase.

## 3. Materials and Methods

#### 3.1. N_{TB}-Forming Mesogenic Dimers

_{TB}phases, that were chosen according to three criteria: (i) a wide temperature range of the N

_{TB}phase to avoid crystallization of the samples during the experiments; (ii) the ability to obtain uniform monochiral domains sufficiently large for the ECE measurements; (iii) selection of different dielectric anisotropy (positive or negative) and different strength of the weakly first order N-N

_{TB}phase transition (to test the influence of these parameters on the ECE amplitude and the temperature dependences of $\alpha $ and $\tau $).

_{TB}phase. Table 1 also presents the phase transition temperatures observed in our electro-optical experiments upon cooling for each compound. Note that they differ in some cases by as much as 2 °C from those measured by DSC. This difference is mainly due to two factors: (i) the very different cooling rates in the two cases (≥5 °C/min for DSC and ≤0.1 °C/min in our experiments); (ii) the different surface/volume ratios in the two experiments. This ratio is much larger in our thin sandwich cells, leading to some diffusion in the sample of impurities from the alignment layers and sealing walls of the cell (this contamination leads to a shift in the transition temperatures but does not significantly influence our ECE experiments).

#### 3.1.1. CB7CB

_{TB}-forming compound. Indeed, the N

_{TB}phase was discovered with this material [7]. It was also the first compound (or at least one of the first) for which the structural and physical properties of the N

_{TB}phase were characterized, e.g., pitch [9,13,14], conical tilt angle [9,10,14], and dielectric constant [7]. CB7CB was also the compound used in the first detailed ECE study [9] (note that we repeat here the ECE experiment with CB7CB over a larger temperature range and with a significantly improved time resolution).

_{TB}-N) = 376 K and T (N-I) = 389 K, respectively. These phase transitions were found to be first order [46]; the entropies of transition, ΔS/R, are 0.34 and 0.31, respectively [38].

_{TB}phase close to the transition [7]. As for the other materials presenting ∆ε > 0, in the ECE experiments, we limit the duration of the applied high-field electric pulses to < 100 µs to avoid textural changes under the strong dielectric torque.

#### 3.1.2. CB9CB

_{TB}phase over a large (>20 °C) temperature range. However, due to the similar chemical structures of these homologues, their physical properties are also similar, and in particular, ∆ε~2 in the vicinity of the N-N

_{TB}transition. The entropies of the I-N and N-N

_{TB}transitions, ΔS/R, are 0.33 and 0.08, respectively [15], indicating that the N-N

_{TB}transition is much more weakly first-order in character than seen for CB7CB.

#### 3.1.3. CB6OCB

_{2})

_{6}O spacer. The synthesis and characterisation of this dimer have been described in detail elsewhere [15,16]. Due to the ether link on one side of the spacer, which results in a smaller bend-angle of the molecule, both nematic phases of CB6OCB, N and N

_{TB}, are enantiotropic and show significantly wider temperature ranges than for CB7CB. The entropy of the N-N

_{TB}transition is extremely small, ΔS/R = 0.01 [15], which indicates that the transition is much more weakly first-order in character than seen for CB7CB. Due to the similar chemical structures of these dimers, their physical properties are similar, in particular, ∆ε ~ 2 in the vicinity of the N-N

_{TB}transition.

#### 3.1.4. BNA76

_{b}). The entropy of the N-N

_{TB}transition is small [39], ΔS/R = 0.05, which indicates a weak first-order transition, as expected [16,46] because of the wide temperature range of the N-phase. Due to the absence of large longitudinal dipoles in the mesogenic units, BNA76 shows a negative dielectric anisotropy, ∆ε < 0, and therefore no textural changes are observed in the N and N

_{TB}phases in our planar cells, even under strong fields (E ~ 20 V/µm). This allows us to apply arbitrarily long dc voltage pulses (or ac voltage bursts) in our ECE experiments without textural change issues. (Note that the cell behaviour is different in the SmA

_{b}phase: because of the phase biaxiality, textural transitions [8] are observed in voltages of under ~4 V. However, the SmA

_{b}phase is achiral and, therefore, as expected, it does not show any electroclinic response.)

#### 3.2. Measurement Technique

_{TB}phase transition, we observed the growth of uniform monochiral N

_{TB}domains separated by domain walls. The typical size of these domains varied from tens to hundreds of micrometers, depending on the compound and cooling rate. On further N

_{TB}-N-N

_{TB}cycling, the domain pattern changed randomly without visible memory of the domain handedness.

_{TB}-N-N

_{TB}cycles, the domains were sufficiently large to allow for ECE measurements in monochiral regions of at least 50 × 50 µm

^{2}in size. Usually, a few tenths of a degree below the transition, the domains were reasonably uniform but, upon further cooling, in most cases, the well-known stripe- and (at a lower temperature) rope instabilities [7] were observed. To avoid these instabilities, which can disturb the electro-optical response to the field, the temperature of the N

_{TB}phase was slowly decreased while superposing weak temperature oscillations (with typical amplitude~1 °C and frequency ~0.01 Hz). During this process, an ac voltage (f = 10 kHz, U < 6 V) was switched on- and off- at about 0.1 Hz. This treatment progressively weakened the instabilities and was repeated until they no longer significantly disturbed the ECE measurements, or until they completely vanished (in the best case). The best results of this treatment were obtained for CB7CB which showed a uniform texture of the monodomains over a temperature range of more than 50 °C below the N-N

_{TB}transition, and the worst results were for CB6OCB, with only a 20 °C range.

_{TB}optical axis,

**N**

_{0}, is parallel to the polarizer P (Figure 4). When the field

**E**is applied, the optical axis rotates in the plane of the cell by a small angle α to a new orientation,

**N**. With the analyzer, A, set at 45°, with respect to P, the transmitted light intensity, I, is approximately a linear function of α [9]:

_{0}is the intensity of the incident light. The sensitivity of the measurement is optimal for $\Delta L\approx (m+1/2)\lambda $ with m an integer. For our cell gap, d = 1.5 µm, $\Delta L$ varies with temperature in the 150–250 nm range, resulting in a reasonably large slope for I(α). To calibrate the measurements of α, without additional birefringence measurements, we measured directly, at each temperature, the slope of I(α) by rotating the cell to a known fixed angle α

_{0}= ± 4° (at fixed I

_{0}and U = 0).

^{2}) in the image plane. To minimize the response time of the detection system, the current signal from the PMT is sent directly to a small resistive load, R

_{L}= 1 kΩ. The voltage drop on the charge is sent to a digital oscilloscope (DSO-X 2004A, Agilent), where it is accumulated up to 64,000 times to improve the signal-to-noise ratio. The typical error in α is estimated to be less than 0.01° and the response time, τ

_{exp}, of the experimental setup, measured with a LED light source driven by short rectangular pulses, is about 160 ns. The main effect of the instrumental response time on the measured signal is an additional delay (~τ

_{exp}) of the ECE response without a change in the slope of the ECE curve. Using a suitable fitting procedure, taking into account this effect, the error in the measured ECE response times can be reduced to only around 30 ns.

_{TB}helix under the strong dielectric torque. For BNA76, however, ∆ε < 0, the dielectric torque stabilized the planar alignment of the helix in our cells, and arbitrarily long pulses could be applied without destroying the uniform N

_{TB}texture.

## 4. Results

_{TB}phase.

_{NTB}effect). The change of the response sign with the sign of the field is also direct evidence that the macroscopic structure of the phase is chiral.

#### 4.1. CB7CB

_{TB}phase was first confirmed experimentally [7], remains the most studied N

_{TB}compound to date. In particular, it was the dimer for which the first detailed ECE experiment was reported [9]. However, this study presents a more recent experiment with better time resolution, a wider temperature range, and a larger number of temperature data points. Although the present data are in excellent agreement with previous results, they provide better precision on the values of the fit parameters. The experimental results for ${c}_{\alpha}(T)$ and $\tau (T)$, over the whole temperature range of the N

_{TB}phase, are shown in Figure 7. The value ${c}_{\alpha}(T)$ is already small at the transition and it decreases further throughout the N

_{TB}phase. At low temperature, it approaches a limiting value. Magnifying the ${c}_{\alpha}(T)$ curve in the vicinity of the N-N

_{TB}phase transition (see inset) reveals a relatively large temperature range (99.5–100.2 °C) of biphasic coexistence, in good agreement with previous reports [7,9,10]. In the following discussion, we define the median temperature of this biphasic range, T

_{c}= 99.85 °C, as the experimentally observed N-N

_{TB}transition temperature (the same approach is used for the other compounds). The ECE response time is very short at the transition, τ ≈ 0.7 µs. Upon cooling, it decreases even further over a few °C and then levels off at a value of about 0.23 µs over the next 20 °C. Upon further cooling, $\tau (T)$ grows exponentially, due to the Arrhenius temperature dependence of the rotational viscosity to which it is proportional (see Equation (6) and the discussion section).

_{TB}transition (Figure 8), where the slow temperature variation of all the nematic parameters, except K

_{33}, can be neglected. Moreover, ${c}_{\alpha}(T)$ follows a power law dependence over the entire available temperature range whereas $\tau (T)$ deviates from this, but only far from the transition. However, the critical temperatures T* derived from these two fits are not the same and, in disagreement with the theoretical models, they differ from the experimental value of T

_{c}by small but significant values, $\Delta {T}_{\alpha}={{T}_{\alpha}}^{*}-{T}_{c}=0.20$ °C and $\Delta {T}_{\tau}={{T}_{\tau}}^{*}-{T}_{c}=0.35$ °C.

#### 4.2. CB9CB

_{TB}phase, and approaches a limiting value at low temperature. The N-N

_{TB}phase transition is very sharp, almost without any biphasic coexistence, and takes place at T

_{c}= 107.00 °C. At the transition, the ECE response time, τ ≈ 2.2 µs, is slower than in CB7CB but it remains of the same order of magnitude. Upon cooling, it decreases further over a few °C, then levels off at about 0.36 µs and grows exponentially upon further cooling. However, even at T = 50 °C, the response time remains rather fast, τ ≈ 1.1 µs.

_{TB}transition (Figure 10). As for CB7CB, the ${c}_{\alpha}(T)$ curve is fitted well by the power law over the entire available temperature range whereas $\tau (T)$ deviates from this far from the transition. The critical temperatures T*, derived from the two fits, are again different and also differ from the experimental value of T

_{c}, with $\Delta {T}_{\alpha}={{T}_{\alpha}}^{*}-{T}_{c}=0.45$ °C and $\Delta {T}_{\tau}={{T}_{\tau}}^{*}-{T}_{c}=0.14$ °C.

#### 4.3. CB6OCB

_{TB}phase transition is almost second-order, whereas that of CB7CB is weakly first-order. The experimental results for ${c}_{\alpha}(T)$ and $\tau (T)$ in the whole temperature range of the N

_{TB}phase are shown in Figure 11. Note that, for this compound, the texture instabilities could not be completely suppressed below 95 °C, which reduced the quality of the data. The value ${c}_{\alpha}(T)$ is small at the transition, decreases throughout the N

_{TB}phase, and approaches a limiting value at low temperature. The N-N

_{TB}phase transition is sharp and takes place at T

_{c}= 108.08 °C, with a small biphasic coexistence range (108.05–108.10 °C). At the transition, the ECE response time, τ ≈ 7 µs, is about one order of magnitude slower than in CB7CB. Upon cooling, it decreases sharply over a few °C and levels off to about 0.8 µs.

_{TB}transition, ${c}_{\alpha}(T)$ and $\tau (T)$ follow power laws, like the previous compounds (Figure 12). Both curves fit well by power laws over 10 °C below the phase transition. The critical temperatures T* determined from the two fits are quite different and also differ from the experimental value of ${T}_{c}$, with $\Delta {T}_{\alpha}={{T}_{\alpha}}^{*}-{T}_{c}=1.70$ °C and $\Delta {T}_{\tau}={{T}_{\tau}}^{*}-{T}_{c}=0.36$ °C.

#### 4.4. BNA76

_{TB}phase transition that takes place at T

_{c}= 120.00 °C. As for the other compounds, ${c}_{\alpha}(T)$ is small at the transition and decrease throughout the N

_{TB}phase (Figure 13). The ECE response time is similar to that of CB9CB; decreasing from τ ≈ 7.2 µs at the transition to τ ≈ 1.0 µs at 95 °C.

_{c}, with $\Delta {T}_{\alpha}={{T}_{\alpha}}^{*}-{T}_{c}=1.17$ °C and $\Delta {T}_{\tau}={{T}_{\tau}}^{*}-{T}_{c}=0.50$ °C.

## 5. Discussion

_{NTB}features that are expected theoretically are based on the macroscopic symmetry of the N

_{TB}phase and its analogy with the chiral smectic A phase. Indeed, the geometry of the effect, with a torque, applied to the optic axis

**N**and proportional to the pseudo-vector $h\times E$, is only possible in a chiral system. Therefore, the mere existence of the electroclinic effect is direct proof of the chiral structure of the N

_{TB}phase and its layered or pseudo-layered organization. Similarly, the alternation of the sign of the ECE

_{NTB}response from one monochiral domain to the next is direct evidence of the doubly-degenerate chirality of the phase. Moreover, the fact that the response is linear in the field reveals that the effect is not dielectric but flexo- or ferroelectric.

_{NTB}experiments using CB7CB [9], giving an early confirmation of the heliconical (and helielectric) structure of the N

_{TB}phase. Here, we show that this behaviour is typical for twist-bend nematics as is observed for all of the four compounds under study. Indeed, for all compounds, close to the N-N

_{TB}transition temperature, we find that the amplitude of the electroclinic tilt of

**N**is small of the order of 0.5–1° for 10 V/µm (or ${c}_{\alpha}<0.1$ °V/µm). On cooling, ${c}_{\alpha}$ decreases further, by a factor of 2 to 5, depending on the compound. The CG theory of the N

_{TB}phase relates the value ${c}_{\alpha}$ close to the transition with the material constants in the nematic phase to the pitch p of the N

_{TB}phase (see Equation (5)). With the typical values of the constants available for the nematics, it has been deduced previously [9,25], from the small value of ${c}_{\alpha}$ for CB7CB, that the pitch is about 7 nm. This surprisingly small value was later confirmed by direct measurements [13,14,19] and is now accepted to be typical.

_{TB}phase. However, the agreement between the decrease (≈50%) of $p(T)$ in the 10 °C range below T

_{c,}deduced from Figure 7 and that reported in [19] (<20 %), is not quantitative. This disagreement may be due to the assumptions of the theoretical model, for example: neglecting the temperature dependence of the nematic constants in the vicinity of T

_{c}, and the approximation that the nematic order tensor is continuous at the N-N

_{TB}transition remaining uniaxial in the N

_{TB}phase [5,31], despite the biaxial local symmetry of the phase. The resonant X-ray scattering experiments provide a direct measurement of $p(T)$, but their temperature dependence shows some hysteresis, which is due to the polydomain structure of the samples, and the defect pinning that hinders the relaxation of the pitch to its equilibrium value after a temperature variation. Our ECE

_{NTB}measurements do not suffer from this problem as no hysteresis of ${c}_{\alpha}(T)$ is observed with our thin and well-aligned monodomain samples. Moreover, the smooth variation of ${c}_{\alpha}(T)$, observed on heating/cooling at a rate of 1 °C/min, indicates that the pitch follows the temperature variation adiabatically.

_{NTB}response times of the four dimers show the same behaviour as that reported in previous experiments using CB7CB. The on- and off- response times are the same, as expected from Equation (6), and they are very close to the N-N

_{TB}phase transition for all the compounds ($\tau $ < 10 µs). However, the initial value was found to vary by one order of magnitude, from ~0.7 µs for CB7CB up to ~7 µs for BNA76. We attribute this variation to the different material constants in Equation (6) for the different dimers, in particular to the rotational viscosity ${\gamma}_{1}$, which varies significantly between the different nematogenic compounds. Indeed, ${\gamma}_{1}$ is relatively small for the nematic compound 5CB [47], which is very close to the monomer unit of CB7CB and CB9CB. This correlates well with the faster ECE responses that we report for these compounds.

_{c}, $\tau $ decreases rapidly in the first 5–10 °C; then, it saturates to a ~20 °C wide plateau, for which the ECE response is the fastest ($\tau $ < 1 µs); finally, on further cooling, $\tau (T)$ grows exponentially, clearly due to the usual Arrhenius-law increase of the rotational viscosity.

_{TB}heliconical parameters; and the final increase of $\tau (T)$, which is absent for ${c}_{\alpha}(T)$, would be explained by the exponential growth of ${\gamma}_{1}$ at low temperature. Moreover, as expected theoretically, ${c}_{\alpha}(T)$ and $\tau (T)$ follow a power law for at least 5 °C below the N-N

_{TB}transition. In fact, the power law fit is excellent for ${c}_{\alpha}(T)$ over a much larger temperature range, see for example, Figs. 8 and 10, which confirms that the nematic constants, apart from ${\gamma}_{1}$, vary only weakly with the temperature.

_{TB}phase transition. The main parameters derived from the power law fit of ${c}_{\alpha}(T)$ and $\tau (T)$ are compared to the predictions of the theoretical models [31,40] in Table 2. Both models predict a second-order N-N

_{TB}transition and, therefore, that the critical temperature, T*, of the power laws should be identical to the measured transition temperature, T

_{c}[31,40]. Theoretically, for a 2

^{nd}order transition, there is no biphasic coexistence, but it is observed experimentally for CB7CB and, although quite small, ~0.05 °C, for CB6OCB, indicates that the transition for these compounds is in fact first-order. For the other two compounds, the biphasic coexistence is essentially zero, which shows that the transition is much closer to being second-order, as indicated by the DSC data [15,38,39]. Nevertheless, for each compound, the critical temperature T* obtained from the power law fits of our data, differs from the transition temperature T

_{c}. This result disagrees with the two Landau-like theoretical models of the N-N

_{TB}transition considered here [31,40], and with the second-order transition predicted by other theoretical models, based on a Landau-like [48] or a generalized Maier-Saupe [49] description of the N

_{TB}phase. Moreover, according to the models described in [31,40], the critical temperatures obtained from the fits of ${c}_{\alpha}(T)$ and $\tau (T)$ should be identical for each compound, which again disagrees with our measurements. Indeed, different critical temperatures were systematically obtained from the two fits, ${{T}_{\alpha}}^{*}\ne {{T}_{\alpha}}^{*}>{T}_{c}$, which can be up to ~2 °C higher than ${T}_{c}$ (see Table 2). Quite surprisingly, at least for the case of ${{T}_{\alpha}}^{*}$, the difference with ${T}_{c}$ is larger for the compounds CB6OCB and BNA76 that present an N-N

_{TB}transition almost second-order in nature and are therefore expected to be a better match to the theoretical prediction ${{T}_{\alpha}}^{*}={{T}_{\tau}}^{*}={T}_{c}$.

_{TB}transition and the corresponding results for ${\beta}_{\tau}$.

_{NTB}effect (linear response to the field, opposite signs of the electroclinic tilt in monochiral domains with opposite handedness, geometry of the effect with deviation of the optic axis under field $\delta N\parallel \hspace{0.17em}E\times N$) are in the CG approach, only based, on the macroscopic symmetry of the N

_{TB}phase and its analogy with the symmetry of the SmA* phase [31]. These main features are indeed observed for all the compounds studied, confirming once more the now well-established heliconical structure of the phase. Moreover, the small amplitude of the electroclinic tilt (α < 1°) and its extremely fast response time (τ < 10 µs) reveal qualitatively that the heliconical pitch is very small, in the order of 10 nm. (This conclusion follows directly from the analogy with the flexoelectric effect in the cholesteric phase [44] and the order of magnitude of the nematic constants involved.)

_{TB}transition. Any one of the two analytical Landau-like models considered here [31,40] leads to the simple expressions in Equations (5) and (6), which involve the nematic constants ${e}_{1}-{e}_{3}$, ${K}_{11}+{K}_{22}$, and ${\gamma}_{1}$. Unfortunately, most of these constants have not been measured for any N

_{TB}-forming compound, even in its nematic phase, and their behaviour in the N

_{TB}phase and across the N-N

_{TB}transition remains unknown. Therefore, to compare our measurements with theory, additional approximations must be made, namely that the nematic constants remain continuous at the transition, and vary slowly with temperature in the N

_{TB}phase (compared to the fast temperature dependency on the pitch and heliconical angle in the vicinity of the transition). However, this approximation, which is inspired by the prediction of the Landau-like models that the N-N

_{TB}transition is second-order, is questionable and its failure may explain to some extent the disagreement between the experimental results and the theoretical predictions.

_{TB}transition. This assumption, leading to a second-order phase transition, denies the experimentally reported weakly first-order character of the transition [15,38,39], and the observed jump of the scalar order parameter S for CB7CB [10]. Further development of the models, taking into account the coupling between S and the structural N

_{TB}parameters, ${\theta}_{0}$ and $p$, may lead to a first-order transition and, therefore, to finite values of ${\theta}_{0}$ and $p$ at the transition. This should also alter the power laws expected for these parameters and, consequently, for ${c}_{\alpha}(T)$ and $\tau (T)$, leading hopefully to better agreement with the experiments.

_{TB}phase transition that also takes account of the jump of the nematic order parameter tensor,

**Q**, at the N-N

_{TB}transition, and the coupling of

**Q**with the N

_{TB}order parameter $\mathrm{sin}{\theta}_{0}$. This model predicts a first-order N-N

_{TB}transition, with strength decreasing with the thermal range of stability of the nematic phase above the N

_{TB}phase. This prediction is in excellent agreement with the experimental observations for a large number of N

_{TB}-forming compounds and with the calorimetric data for several mesogenic dimers and mixtures [46], including CB6OCB [16]. We expect that a future CG theory of the ECE

_{NTB}, based on this improved Landau model, will provide a better agreement with our present experimental results.

**Q**, in the N

_{TB}phase. Indeed, even in the N phase, the bend distortion breaks the revolution symmetry of the nematic phase and

**Q**becomes slightly biaxial. Due to the strong spontaneous bend of the N

_{TB}phase, the resulting biaxiality of

**Q**(which is again the primary order parameter of the phase) might become important, as it was recently reported to lead to important changes in the phase behaviour under an applied field [42]. Because the bend distortion, and therefore the biaxiality of the order tensor

**Q**, depends strongly on the temperature, taking this dependence into account could lead to significant changes in the theoretically predicted behaviour for ${c}_{\alpha}(T)$ and $\tau (T)$, in better agreement with the experimental results.

## 6. Conclusions

_{TB}phase of four mesogenic dimers. The ECE

_{NTB}response is observed over the whole N

_{TB}temperature range of the compounds (more than 60 °C wide for CB9CB). The amplitude of the effect is very small at the phase transition (α~1° for E = 10 V/µm) and decreases further on cooling. As reported previously for CB7CB [9], the on- and off- ECE response times are equal and very short, typically in the microsecond range. This feature is very attractive for fast applications but has not yet been exploited because of the small amplitude of the electroclinic tilt. Qualitatively, our results are similar for all four compounds, despite their different physical properties including, for example, different signs of the dielectric anisotropy, and different strengths of the weakly first-order phase transition. The amplitude and the response time are largely related to the value of the heliconical pitch. Therefore, any practical application of the ECE

_{NTB}might only be expected if compounds with larger N

_{TB}pitches (~30–50 nm) are discovered.

_{TB}heliconical structure and the biaxiality of the nematic order parameter tensor in the N

_{TB}phase.

## Author Contributions

## Funding

## Data Availability Statement

## Conflicts of Interest

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**Figure 1.**Heliconical structure of the N

_{TB}phase. The long axes, L, of the bent-shaped molecules are on average oriented parallel to the nematic director,

**n**. Along the helix axis,

**h**, the director rotates and follows a conical helix with pitch p. The bend vector,

**b**, is organized on a right-angle helix. (The heliconical structure is doubly degenerate but only the right-handedness is shown here for simplicity.).

**Figure 2.**The analogy between the layered structure of the SmA* phase (

**a**) and the pseudo-layered structure of the N

_{TB}phase (

**b**).

**Figure 3.**Electroclinic effect in the SmA* (

**a**) and N

_{TB}(

**b**) phases. When the field is applied in the plane of the SmA* layers, the director

**n**rotates in a plane perpendicular to

**E**and tilts at an angle α with respect to the normal layers. Similarly, when an electric field is applied in a direction parallel to the N

_{TB}pseudo-layers, the optic axis,

**N**, tilts away at an angle α from the helix axis,

**h**, in a plane perpendicular to

**E**. The whole director cone (the shaded region) tilts by the same angle α, without much distortion.

**Figure 5.**ECE

_{NTB}response (black open symbols) to a square dc pulse (15 V/µm, 20 µs) measured in a BNA76 monochiral domain. The solid lines are the best fit of the data with an exponential law for the rise (red) and the fall (blue) of the response. The inset shows two large monochiral uniform domains of opposite chirality observed with slightly uncrossed polarizers.

**Figure 6.**CB6OCB at T = 108.05 °C: Time-evolution of the electroclinic tilt angle α (blue open symbols, right axis) subject to a triangular voltage pulse (black line, left axis).

**Figure 7.**Temperature dependence of the ECE parameters, ${c}_{\alpha}(T)$ and $\tau (T)$, measured in the N

_{TB}phase of the dimer CB7CB. The inset shows a magnification of the relatively large N-N

_{TB}biphasic coexistence range.

**Figure 8.**Best fits (red solid lines) of ${c}_{\alpha}(T)$ and $\tau (T)$ with power laws for CB7CB: (

**a**) For ${c}_{\alpha}(T)$, the fit ${c}_{\alpha}(T)\propto {({{T}_{\alpha}}^{*}-T)}^{-{\beta}_{\alpha}}$ is good over the entire (60 °C) range under study, with ${{T}_{\alpha}}^{*}$ = 100.05 °C and ${\beta}_{\alpha}$ = 0.23; (

**b**) For the response time, the law $\tau (T)\propto {({{T}_{\tau}}^{*}-T)}^{-{\beta}_{\tau}}$, with ${{T}_{\tau}}^{*}$ = 100.20 °C and ${\beta}_{\tau}$ = 0.42 fits the curve well only in a range of about 6 °C. At low temperature, the curve is well-fitted by an exponential growth law (blue dashed curve).

**Figure 9.**Temperature dependence of the ECE parameters, ${c}_{\alpha}(T)$ and $\tau (T)$, measured in the N

_{TB}phase of the bent-shaped dimer CB9CB. For this compound, the N-N

_{TB}biphasic coexistence temperature range is very narrow and almost undetectable.

**Figure 10.**Best fits (red solid lines) of ${c}_{\alpha}(T)$ and $\tau (T)$ with power laws for CB9CB: (

**a**) For ${c}_{\alpha}(T)$, the fit ${c}_{\alpha}(T)\propto {({{T}_{\alpha}}^{*}-T)}^{-{\beta}_{\alpha}}$ is good over the entire (>60 °C) range under study, with ${{T}_{\alpha}}^{*}$ = 107.45 °C and ${\beta}_{\alpha}$ = 0.33; (

**b**) The power law $\tau (T)\propto {({{T}_{\tau}}^{*}-T)}^{-{\beta}_{\tau}}$, with ${{T}_{\tau}}^{*}$ = 100.14 °C and ${\beta}_{\tau}$ = 0.45 fits the curve well only in a range of about 5 °C. As for CB7CB, at low temperature, the curve is well-fitted by an exponential growth law (blue dashed curve).

**Figure 11.**Temperature dependences of the ECE parameters, ${c}_{\alpha}(T)$ and $\tau (T)$, measured in the N

_{TB}phase of the bent-shaped dimer CB6OCB. The inset shows a magnification of the N-N

_{TB}biphasic coexistence range.

**Figure 12.**Best fits (solid red lines) of ${c}_{\alpha}(T)$ and $\tau (T)$ with power laws for CB6OCB: (

**a**) For ${c}_{\alpha}(T)$, the fit ${c}_{\alpha}(T)\propto {({{T}_{\alpha}}^{*}-T)}^{-{\beta}_{\alpha}}$ provides ${{T}_{\alpha}}^{*}$ = 109.78 °C and ${\beta}_{\alpha}$ = 0.31; (

**b**) The power law for the response time, $\tau (T)\propto {({{T}_{\tau}}^{*}-T)}^{-{\beta}_{\tau}}$, gives ${{T}_{\tau}}^{*}$ = 108.44 °C and ${\beta}_{\tau}$ = 0.64.

**Figure 13.**Temperature dependences of the ECE parameters, ${c}_{\alpha}(T)$ and $\tau (T)$, measured in the N

_{TB}phase of the dimer BNA76. The N-N

_{TB}phase transition takes place at T

_{c}= 120.00 °C and the N-N

_{TB}biphasic coexistence temperature range is very narrow, almost undetectable.

**Figure 14.**Best fits (solid red lines) of ${c}_{\alpha}(T)$ and $\tau (T)$ with power laws for BNA76: (

**a**) For ${c}_{\alpha}(T)$, the fit ${c}_{\alpha}(T)\propto {({{T}_{\alpha}}^{*}-T)}^{-{\beta}_{\alpha}}$ is very good over the entire 25 °C range under study, with ${{T}_{\alpha}}^{*}$ = 121.17 °C and ${\beta}_{\alpha}$ = 0.23; (

**b**) The power law $\tau (T)\propto {({{T}_{\tau}}^{*}-T)}^{-{\beta}_{\tau}}$, with ${{T}_{\tau}}^{*}$ = 120.50 °C and ${\beta}_{\tau}$ = 0.78, fits the curve well only in a range of about 6 °C.

**Table 1.**Molecular structure and phase transition temperatures of the mesogenic dimers. The temperatures are measured on cooling in our thin sandwich cells. The biphasic coexistence range and its median temperature, T

_{c}, are shown for the N-N

_{TB}phase transition. Also shown, in brackets, are the melting points of the crystal/solid which gives the N

_{TB}phase for the three cyanobiphenyl dimers [15] and that containing two naphthalene groups [39]. These are included to show that thermodynamically the twist-bend nematic range can be extremely short; however this range can be significantly extended as early studies, especially for CB7CB, have shown [7].

Compound | Molecular Structure and Phase Transition Temperatures |
---|---|

CB7CB | Iso—114.8 °C-N—99.85 ± 0.35 °C-N _{TB}—37 °C-Cr (Cr—102 °C-N_{TB}) |

CB9CB | Iso—124.1 °C-N—107.00 ± 0.0 °C-N _{TB}—41 °C-Cr (Cr—86 °C-N_{TB}) |

CB6OCB | Iso—156.6 °C-N—108.08 ± 0.03 °C-N _{TB}—80 °C-Cr (Cr—99 °C-N_{TB}) |

BNA76 | Iso—153.1 °C-N—120.00 ± 0.0 °C-N _{TB}—89 °C-SmA_{b} (Cr—121 °C-N_{TB}) |

**Table 2.**Comparison of the ECE

_{NTB}parameters obtained from the power law fits of the experimental results with the predictions of the theoretical models.

Compound | ECE Experiment | Theory [9,31] | Theory [40] | |||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|

$\mathbf{\Delta}{\mathit{T}}_{\mathit{\alpha}}$ (°C) | $\mathbf{\Delta}{\mathit{T}}_{\mathit{\tau}}$ (°C) | ${\mathit{\beta}}_{\mathit{\alpha}}$ | ${\mathit{\beta}}_{\mathit{\tau}}$ | $\mathbf{\Delta}\mathit{T}$ (°C) | ${\mathit{\beta}}_{\mathit{\alpha}}$ | ${\mathit{\beta}}_{\mathit{\tau}}$ | $\mathbf{\Delta}{\mathit{T}}_{}$ (°C) | $\mathit{T}\mathbf{>}\mathit{T}\mathbf{*}\mathbf{-}\mathit{\delta}\mathit{T}$ | $\mathit{T}\mathbf{<}\mathit{T}\mathbf{*}\mathit{-}\mathit{\delta}\mathit{T}$ | |||

${\mathit{\beta}}_{\mathit{\alpha}}$ | ${\mathit{\beta}}_{\mathit{\tau}}$ | ${\mathit{\beta}}_{\mathit{\alpha}}$ | ${\mathit{\beta}}_{\mathit{\tau}}$ | |||||||||

CB7CB | 0.20 | 0.35 | 0.23 | 0.42 | 0 | 0.5 | 2.0 | 0 | 0.5 | 2.0 | 0.25 | 1.0 |

CB9CB | 0.45 | 0.14 | 0.33 | 0.45 | 0 | 0.5 | 2.0 | 0 | 0.5 | 2.0 | 0.25 | 1.0 |

CB6OCB | 1.70 | 0.36 | 0.31 | 0.64 | 0 | 0.5 | 2.0 | 0 | 0.5 | 2.0 | 0.25 | 1.0 |

BNA76 | 1.17 | 0.50 | 0.23 | 0.78 | 0 | 0.5 | 2.0 | 0 | 0.5 | 2.0 | 0.25 | 1.0 |

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**MDPI and ACS Style**

Meyer, C.; Davidson, P.; Luckhurst, G.R.; Dokli, I.; Knežević, A.; Lesac, A.; Paterson, D.A.; Walker, R.; Storey, J.M.D.; Imrie, C.T.;
et al. Temperature Dependence of the Electroclinic Effect in the Twist-Bend Nematic Phase. *Crystals* **2023**, *13*, 465.
https://doi.org/10.3390/cryst13030465

**AMA Style**

Meyer C, Davidson P, Luckhurst GR, Dokli I, Knežević A, Lesac A, Paterson DA, Walker R, Storey JMD, Imrie CT,
et al. Temperature Dependence of the Electroclinic Effect in the Twist-Bend Nematic Phase. *Crystals*. 2023; 13(3):465.
https://doi.org/10.3390/cryst13030465

**Chicago/Turabian Style**

Meyer, Claire, Patrick Davidson, Geoffrey R. Luckhurst, Irena Dokli, Anamarija Knežević, Andreja Lesac, Daniel A. Paterson, Rebecca Walker, John M. D. Storey, Corrie T. Imrie,
and et al. 2023. "Temperature Dependence of the Electroclinic Effect in the Twist-Bend Nematic Phase" *Crystals* 13, no. 3: 465.
https://doi.org/10.3390/cryst13030465