Enhancement of Spontaneous Polarization and Acid Vapor-Induced Polymerization in the Thin-Film States of Phenylterthiophene Derivative Bearing a Cyclotetrasiloxane Ring

: We have achieved the measurement of spontaneous polarization of spin-coated thin ﬁlms of a ferroelectric liquid crystal based on a phenylterthiophene skeleton. Uniaxially aligned spin-coated ﬁlms with a thickness of 100 nm were prepared by the friction transfer method. The spontaneous polarization of the spin-coated ﬁlms was measured by the Sawyer–Tower method and polarization inversion current technique under the application of triangular-wave bias. These measurements revealed the spontaneous polarization of 50 nC cm − 2 in the thin-ﬁlm state which is 1.5 times larger than the value of 35 nC cm − 2 in the bulk state. This result should be attributed to the strong anchoring of the liquid-crystalline molecules on the substrate surface and the inhibition of polarization relaxation caused by the formation of the helical structure. Moreover, insolubilization of the thin ﬁlms was carried out by an in situ ring-opening polymerization induced by acid vapors. The molecular alignment in the thin ﬁlms of the ferroelectric liquid crystal was retained during the polymerization process.


Introduction
Ferroelectric liquid crystals (FLCs) can be regarded as materials which are responsive to electric fields. FLCs have been extensively studied for the development of high-speed liquid crystal (LC) displays [1]. The strong interaction between the spontaneous polarization and the external electric field results in a short response time in the order of 1 µs, and the memory effect leads to low electrical power consumption [1]. For the display application, FLCs are used as fluidic materials pinched between two glass substrates and the thickness of the FLC materials is usually more than 2 µm which is limited by the flatness of the substrates. Thus, optical and electrical properties of FLCs have been characterized in LC cells consisting of two glass plates coated with indium tin oxide (ITO), whose thickness is generally more than 2 µm [2][3][4]. Studies on optical and physical properties of FLCs in thin-film states with thicknesses less than 1 µm have been very limited.
The significance of preparation of LC thin films has been recognized for the applications of LC semiconductors comprised of extended π-conjugated units to thin-film electronic devices [5]. For applications to field-effect transistors and light-emitting diodes, the thickness of the LC thin films Crystals 2020, 10 was less than 100 nm [6][7][8]. For FLCs bearing extended π-conjugated moieties, a few research groups have recently reported interesting phenomena based on the coupling of electronic charge transport with spontaneous polarization. The diodes with switchable polarity based on pyrene derivatives bearing hydrogen-bonding amide moieties [9], photorefractive effects of chiral terthiophene-based dye-doped LCs [10], linearly polarized electroluminescence with a rotatable polarized plane [11], and photovoltaic effects based on the built-in potential produced by spontaneous polarization instead of a p-n junction have been reported [12][13][14][15][16]. In the application of FLCs to diodes and photovoltaic devices as well as memories [17] and actuators [18], the preparation of thin films is essential. However, it has been difficult to produce thin films for FLCs with a thickness less than 1 µm by a solution process. Most FLCs are low-molecular weight materials and crystallize at room temperature. By the spin-coating method, polycrystalline inhomogeneous films with a high defect density are produced. Except for polymers bearing ferroelectric mesogens in their side chains [19,20], spin-coated thin films of low-molecular weight FLCs have been quite limited and their polarization inversion currents or hysteresis loops characteristic of the ferroelectricity have not been confirmed in the thin-film states of FLCs.
Regarding external stimuli other than electric fields, a few research groups have provided acid vapor-responsive organic liquids which change their colors by the reaction between the basic compounds with acid vapors [21]. We have already reported LC perylene bisimide derivatives bearing cyclotetrasiloxane rings which polymerize in thin-film states by exposure to acid vapors [22]. The stabilization and insolubilization of thin films are necessary for device fabrication. Only a few photopolymerizable FLCs have been reported; however, other in situ polymerization methods have been limited [23].
In this study, we synthesized an FLC consisting of a phenylterthiophene unit and a cyclotetrasiloxane ring. FLC thin films with a thickness around 100 nm were deposited on glass substrates coated with ITO by a spin-coating method. The aluminum (Al) electrode was vacuum-deposited on the LC layer to prepare a sandwich-type sample. The spontaneous polarization of the thin films was determined by polarization inversion current measurements and the Sawyer-Tower method. These measurements revealed that the spontaneous polarization in the thin-film state was 1.5 times larger than that in the bulk state. In addition, the insolubilization of the thin films was carried out by an in situ ring-opening polymerization induced by acid vapors. The molecular alignment in the as-deposited LC thin films was retained during the polymerization process.

Synthesis and Mesomorphic Behaviors of FLCs
In general, it is not always easy to produce homogeneous thin films of LC compounds by the spin-coating method. Most LC materials crystallize at room temperature and inhomogeneous crystallization occurs during the solvent evaporation in the spin-coating process [24]. We have studied the preparation of the thin films of LC semiconductors by the spin-coating method [25][26][27][28]. When we use LC semiconductors which exhibit ordered smectic phases or columnar phases at room temperature, homogeneous thin films of the LC states can be produced by the spin-coating method at room temperature. From the self-healing effect in the LC phases, homogeneous thin films with low defect densities could be obtained by a thermal annealing. High-quality LC thin films were applied to field-effect transistors [25][26][27]29], organic light-emitting diodes [30], and bulk heterojunction solar cells [31].
For this purpose, we synthesized the phenylterthiophene derivative (S)−1 bearing a chiral side chain and a cyclotetrasiloxane unit at the terminal position of alkyl linker ( Figure 1). The synthetic procedure, spectral data, differential scanning calorimetric thermograms, X-ray diffraction patterns and polarizing optical microscopic textures are indicated in the supplementary file (S-1, Scheme S1; S-2, Figures S1−S4). An analogous compound (S)−2 bearing an alkenyl side chain (Figure 1) was Crystals 2020, 10, 983 3 of 10 also synthesized according to the literature reported previously [14]. Compared to alkenyl analog (S)−2, the bulky cyclotetrasiloxanering inhibits crystallization; however, it promotes nanosegregation between the π-conjugated units and the oligosiloxane moieties, resulting in the formation of layer structures [12,13,32]. These compounds exhibit an ordered smectic phase at room temperature and ferroelectric chiral smectic C (SmC*) phase at an elevated temperature. These LC phases are enantiotropic. The mesomorphic properties of chiral LC fluorophenylterthiophene derivatives (S)−1 and (S)−2 are summarized in Table 1. Recrystallization of compound (S)−1 from n-hexane provides waxy precipitates in the chiral smectic G (SmG*) phase while a crystalline solid is obtained in the recrystallization of compound (S)−2 from n-hexane. Compound (S)−1 exhibits higher solubility in various organic solvents as compared with (S)−2. The characterization of their mesophases was supported by studies of polarizing optical microscopy (POM), X-ray diffraction and differential scanning calorimetry [12][13][14]. structures [12,13,32]. These compounds exhibit an ordered smectic phase at room temperature and ferroelectric chiral smectic C (SmC*) phase at an elevated temperature. These LC phases are enantiotropic. The mesomorphic properties of chiral LC fluorophenylterthiophene derivatives (S)−1 and (S)−2 are summarized in Table 1. Recrystallization of compound (S)−1 from n-hexane provides waxy precipitates in the chiral smectic G (SmG*) phase while a crystalline solid is obtained in the recrystallization of compound (S)−2 from n-hexane. Compound (S)−1 exhibits higher solubility in various organic solvents as compared with (S)−2. The characterization of their mesophases was supported by studies of polarizing optical microscopy (POM), X-ray diffraction and differential scanning calorimetry [12][13][14].   (a) The abbreviations SmG*, SmC*, and Iso denote chiral smectic G, chiral smectic C, and isotropic liquid phases, respectively. The phase transition temperatures were taken at the peak onset of DSC charts. (b) Ref. [14].

Characterization of Ferroelectricty
Their ferroelectric properties of the bulk state in the SmC* phases were evaluated by the Sawyer-Tower method [33]. Samples in the isotropic liquid state were filled by capillary action into ITO sandwich empty cells with a cell gap of 2 μm (EHC. Co., Ltd., Tokyo, Japan, KSSO-02/A307P1NSS05). The area of electrodes was 4 × 4 mm. The temperature of the sample was controlled by a hot stage with a proportional-integral-differential (PID) thermo-controller. Triangular-wave bias (±25 kV/cm, 100 Hz) was applied to the sample cells using a function generator (NF Co., Ltd., Yokohama, Japan, WF1973) and a power amplifier (NF Co., Ltd., Yokohama, Japan, HSA 4011). A current induced by electrical polarization was recorded on a digital oscilloscope (Tektronix, Inc., Salem, MA, USA, TDS 3034C) as the voltage drop across a reference capacitor placed in series with the sample. The capacitance of the reference capacitor is 33 nF.
The spontaneous polarization in the bulk and thin-film states was also determined by the polarization inversion method [4], using the same oscilloscope, the same function generator and the same type of samples. Triangular-wave bias was applied to the sample cells. The polarization inversion current was detected by the oscilloscope as a voltage drop through a serial resistor with the resistance of 1 kΩ. Compared to the Sawyer-Tower method, the polarization inversion method is effective for the measurements of FLCs which exhibit a larger leakage current. The detailed estimation of spontaneous polarization values is described in the supplementary files (S-3, S1) For the measurement in the thin-film states, we used sandwich-type samples produced by vacuum-deposition of the Al electrode on the spin-coated thin films of compound (S)−1 with a thickness of around 100 nm deposited on ITO-coated glass substrates. For the measurement of the spontaneous polarization, the planar alignment of the LC molecules is requisite because the dipole  a The abbreviations SmG*, SmC*, and Iso denote chiral smectic G, chiral smectic C, and isotropic liquid phases, respectively. The phase transition temperatures were taken at the peak onset of DSC charts. b Ref. [14].

Characterization of Ferroelectricty
Their ferroelectric properties of the bulk state in the SmC* phases were evaluated by the Sawyer-Tower method [33]. Samples in the isotropic liquid state were filled by capillary action into ITO sandwich empty cells with a cell gap of 2 µm (EHC. Co., Ltd., Tokyo, Japan, KSSO-02/A307P1NSS05). The area of electrodes was 4 × 4 mm. The temperature of the sample was controlled by a hot stage with a proportional-integral-differential (PID) thermo-controller. Triangular-wave bias (±25 kV/cm, 100 Hz) was applied to the sample cells using a function generator (NF Co., Ltd., Yokohama, Japan, WF1973) and a power amplifier (NF Co., Ltd., Yokohama, Japan, HSA 4011). A current induced by electrical polarization was recorded on a digital oscilloscope (Tektronix, Inc., Salem, MA, USA, TDS 3034C) as the voltage drop across a reference capacitor placed in series with the sample. The capacitance of the reference capacitor is 33 nF.
The spontaneous polarization in the bulk and thin-film states was also determined by the polarization inversion method [4], using the same oscilloscope, the same function generator and the same type of samples. Triangular-wave bias was applied to the sample cells. The polarization inversion current was detected by the oscilloscope as a voltage drop through a serial resistor with the resistance of 1 kΩ. Compared to the Sawyer-Tower method, the polarization inversion method is effective for the measurements of FLCs which exhibit a larger leakage current. The detailed estimation of spontaneous polarization values is described in the supplementary files (S-3, S1). For the measurement in the thin-film states, we used sandwich-type samples produced by vacuum-deposition of the Al electrode on the spin-coated thin films of compound (S)−1 with a thickness of around 100 nm deposited on ITO-coated glass substrates. For the measurement of the spontaneous polarization, the planar alignment of the LC molecules is requisite because the dipole moment of the LC molecules is perpendicular to the molecular axis. The planar alignment was confirmed by POM observations.

Preparation of Thin Films of FLCs
Thin films of compounds (S)−1 and (S)−2 were deposited on glass substrates by a spin-coating method. The spin-coated thin films were prepared on ITO-coated glass plates under the following conditions (rotational speed: 2000 rpm, rotation time: 120 s, concentration of solutions: 20 g L −1 in acetone). The surface of the ITO-coated glass plates was hydrophilized by a UV/O 3 method or treated by a friction transfer (FT) technique [34,35]. In the FT technique, the substrate was heated to over 200 • C, and the heated surface of the substrate was rubbed with a polytetrafluoroethylene (PTFE) block. PTFE nanofibers adhered on the substrate, aligning parallel to the rubbing direction. The average thickness of prepared LC thin films was around 100 nm.
In situ polymerization of the spin-coated thin films was carried out by the exposure of the thin films on vapors of trifluoromethanesulfonic acid at 70 • C. A spin-coated thin film and a glass container including a few drops of trifluoromethanesulfonic acid were placed in a glass petri dish and it was left at 70 • C for 30 min. The ring-opening polymerization did not occur below 50 • C, indicating that this in situ polymerization process should require the thermal motion of the cyclotetrasiloxane moieties.

Ferroelectricity in the Bulk State of Compound (S)−1
In the POM observation for the ITO-sandwiched LC cell of (S)−1, broken fan-like textures with stripes originated from helical structures were observed in the SmC* phase (see the supplementary files; Figure S3a) [35]. The broken fan-like textures indicated that the LC molecules exhibited planar alignment between two ITO electrodes. The helical pitch of 1~2 µm was estimated from the width of stripe patterns in the POM image. On the surface of the bare glass substrate, schlieren textures were observed in the SmC* phase of (S)−1. Because the schlieren textures can be observed in a nematic phase as well as SmC/SmC* phases with homeotropic alignments, LC molecules of (S)−1 aligned perpendicular to the glass surface [36]. However, this area did not contribute to the electrical measurements. For compound (S)−1, ferroelectric hysteresis loops were observed in their SmC* phases ( Figure 2a). Their spontaneous polarization values were estimated by extrapolation of these polarization curves to zero bias. The spontaneous polarization in the SmC* phase of (S)−1 was 35 nC cm −2 at 100 • C, which is smaller than the value of 68 nC cm −2 determined by the Sawyer-Tower method for (S)−2 [14]. A comparable spontaneous polarization, 31 nC cm −2 , was obtained by the polarization inversion current measurement, as shown in Figure 2b. The bulky cyclotetrasiloxane unit of (S)−1 should inhibit the molecular aggregation in the SmC* phase, resulting in a more disordered structure.

Deposition of Thin LC Film
LC molecules generally align perpendicular to the surface of the substrate in spin-coated films of LC compounds exhibiting smectic phases because the surface energy at the interface between the LC layer and air should strongly influence the molecular alignment [25][26][27]. Therefore, conventional techniques, such as an alignment layer method using rubbed polyimide thin films could not produce the uniaxially aligned films of LC spin-coated films. We adopted the FT method [33,34] aligning the LC molecules parallel to the surface of the substrate. The interaction of the LC molecules and adhered PTFE nanofibers on the substrates resulted in uniaxial alignment of the LC molecules. This method has been used to align π-conjugated polymers [37].
Crystals 2020, 10, 983 5 of 10 polarization curves to zero bias. The spontaneous polarization in the SmC* phase of (S)−1 was 35 nC cm −2 at 100 °C, which is smaller than the value of 68 nC cm −2 determined by the Sawyer-Tower method for (S)−2 [14]. A comparable spontaneous polarization, 31 nC cm −2 , was obtained by the polarization inversion current measurement, as shown in Figure 2b. The bulky cyclotetrasiloxane unit of (S)−1 should inhibit the molecular aggregation in the SmC* phase, resulting in a more disordered structure.   Figure 3a, inhomogeneous crystalline films consisting of sub-micron sized crystallites were obtained. The thin films contained many defects and pin holes and the sample for electrical measurements could not be prepared. Because the solubility of compound (S)−2 in organic solvents was not so high as that of compound (S)−1, the choice of the solvent was limited in the spin-coating of compound (S)−2. In contrast to compound (S)−2, homogeneous and continuous thin films could be produced by the spin-coating method for compound (S)−1. It should be noted that the spin-coated thin films of compound (S)−1 were in the SmG* phase at room temperature because compound (S)−1 did not crystallize during the evaporation process of the solvent. In the case of thin films deposited on the UV/O 3 -treated ITO surface, polydomain optical textures which consisted of several ten micron-sized birefringent and homeotropic domains were observed in the as-deposited films, as shown in Figure 3b. The molecular orientation in each domain would be random. The LC molecules tended to orient vertical to the substrate surface in the spin-coated films while the LC molecules were aligned parallel to the electrode surfaces (homogeneous alignment) in the 2 µm-thick LC cell. By the classical rubbing method for an ultrathin polyimide layer deposited on the ITO electrode, homogeneous alignment could not be achieved.

Deposition of Thin LC Film
LC molecules generally align perpendicular to the surface of the substrate in spin-coated films of LC compounds exhibiting smectic phases because the surface energy at the interface between the LC layer and air should strongly influence the molecular alignment [25][26][27]. Therefore, conventional techniques, such as an alignment layer method using rubbed polyimide thin films could not produce the uniaxially aligned films of LC spin-coated films. We adopted the FT method [33,34] aligning the LC molecules parallel to the surface of the substrate. The interaction of the LC molecules and adhered PTFE nanofibers on the substrates resulted in uniaxial alignment of the LC molecules. This method has been used to align π-conjugated polymers [37]. Figure 3 displays polarizing optical micrographs of the spin-coated thin films of compounds (S)−1 and (S)−2. For compound (S)−2, homogeneous thin films were not obtained by the spin-coating method. As shown in Figure 3a, inhomogeneous crystalline films consisting of sub-micron sized crystallites were obtained. The thin films contained many defects and pin holes and the sample for electrical measurements could not be prepared. Because the solubility of compound (S)−2 in organic solvents was not so high as that of compound (S)−1, the choice of the solvent was limited in the spincoating of compound (S)−2. In contrast to compound (S)−2, homogeneous and continuous thin films could be produced by the spin-coating method for compound (S)−1. It should be noted that the spincoated thin films of compound (S)−1 were in the SmG* phase at room temperature because compound (S)−1 did not crystallize during the evaporation process of the solvent. In the case of thin films deposited on the UV/O3-treated ITO surface, polydomain optical textures which consisted of several ten micron-sized birefringent and homeotropic domains were observed in the as-deposited films, as shown in Figure 3b. The molecular orientation in each domain would be random. The LC molecules tended to orient vertical to the substrate surface in the spin-coated films while the LC molecules were aligned parallel to the electrode surfaces (homogeneous alignment) in the 2 μm-thick LC cell. By the classical rubbing method for an ultrathin polyimide layer deposited on the ITO electrode, homogeneous alignment could not be achieved. On the other hand, uniaxially oriented LC films were obtained using the friction-transferred ITO substrates as shown in Figure 3c. The optical contrast was changed by every 45-degree rotation of samples. The uniaxially extended PTFE fibers adhering on the substrate should strongly restrict the orientation of the LC molecules in the thin films. These optical textures were retained when the sample heated to the temperature range of the SmC* phase. In the temperature range of the SmC* phase, POM observations revealed only dark field and clear optical textures could not be obtained for both films deposited on UV/O3-treated and FT-treated substrates because of the small birefringence of the thin films with thicknesses around 100 nm. On the other hand, uniaxially oriented LC films were obtained using the friction-transferred ITO substrates as shown in Figure 3c. The optical contrast was changed by every 45-degree rotation of samples. The uniaxially extended PTFE fibers adhering on the substrate should strongly restrict the orientation of the LC molecules in the thin films. These optical textures were retained when the sample heated to the temperature range of the SmC* phase. In the temperature range of the SmC* phase, Crystals 2020, 10, 983 6 of 10 POM observations revealed only dark field and clear optical textures could not be obtained for both films deposited on UV/O 3 -treated and FT-treated substrates because of the small birefringence of the thin films with thicknesses around 100 nm.

Ferroelectricity of Thin-film States
Top Al electrodes were vacuum-deposited on spin-coated films. Ferroelectric polarization of the spin-coated films of compound (S)−1 was evaluated by the Sawyer-Tower method (Al/ LC/ ITO, ±500 kV cm −1 , 100 Hz). Figure 4a shows hysteresis loops of the spin-coated thin films of (S)−1. The polarization versus electric field curve of the thin film deposited on the UV/O 3 -treated ITO surface showed dielectric-like behavior, in which hysteresis was not remarkable, despite the bulk ferroelectricity of compound (S)−1. In contrast, the thin film prepared on the FT-treated substrate showed ferroelectric hysteresis behavior. The coercive electric field was shifted to around 80 kV cm −1 as compared with 2 µm-thick LC cell. The shift of coercive electric field could be caused by molecular orientation on the surface and inside of the thin film. The upfield shift could be explained by the surface stabilization effect of FLC molecules. In addition, molecular orientation at the interface between the LC layer and electrodes can also affect the upfield shift. The estimated spontaneous polarization reached around 75 nC cm −2 . 500 kV cm −1 , 100 Hz). Figure 4a shows hysteresis loops of the spin-coated thin films of (S)−1. The polarization versus electric field curve of the thin film deposited on the UV/O3-treated ITO surface showed dielectric-like behavior, in which hysteresis was not remarkable, despite the bulk ferroelectricity of compound (S)−1. In contrast, the thin film prepared on the FT-treated substrate showed ferroelectric hysteresis behavior. The coercive electric field was shifted to around 80 kV cm −1 as compared with 2 μm-thick LC cell. The shift of coercive electric field could be caused by molecular orientation on the surface and inside of the thin film. The upfield shift could be explained by the surface stabilization effect of FLC molecules. In addition, molecular orientation at the interface between the LC layer and electrodes can also affect the upfield shift. The estimated spontaneous polarization reached around 75 nC cm −2 .
In the samples exhibiting high leakage currents, the polarization values obtained by the Sawyer-Tower method may be overestimated by distortion of hysteresis loops. Therefore, the spontaneous polarizations of the thin films were also measured by the polarization inversion method. Figure 4b exhibits the polarization inversion current for the thin films of compound (S)−1 in the SmC* phase at 100 °C. The measurements revealed the spontaneous polarization of 27 nC cm −2 for a thin film deposited on UV/O3-treated substrate. For the uniaxially aligned thin film formed by the frictiontransfer method, the spontaneous polarization increased to 50 nC cm −2 . This value was 1.5 times greater than that in the bulk state of compound (S)−1.
Small spontaneous polarization and an ambiguous hysteresis loop in the thin films deposited on UV/O3-treated substrates should originate from the presence of the domains in which the LC molecules were aligned perpendicular to the electrode surface. In the molecules of compound (S)−1, the permanent dipole moments, which contributed mainly to the ferroelectricity, were almost perpendicular to the molecular axis, while the induced dipole moment derived from the polarization of the π-conjugated unit was parallel to the molecular axis.  Compared to the spontaneous polarization in the 2 μm-thick cells, those in the thin-film states on the FT-treated substrates were 1.5 times greater. In past studies on spontaneous polarization measurements of FLC cells with thicknesses larger than 2 μm, the spontaneous polarization decreased with the decrease in the sample thickness [38][39][40]. That results have been explained by the confinement of the LC molecules on the substrate surface. In the spin-coated films deposited on FTtreated substrates, the LC molecules are more strongly adsorbed on the electrode surface and the molecular ordering on the electrode surface should induce more ordered structure over the whole thin film. The influence from the molecular orientation on the electrode surface should be more remarkable in the thin-film states in LC cells. In the samples exhibiting high leakage currents, the polarization values obtained by the Sawyer-Tower method may be overestimated by distortion of hysteresis loops. Therefore, the spontaneous polarizations of the thin films were also measured by the polarization inversion method. Figure 4b exhibits the polarization inversion current for the thin films of compound (S)−1 in the SmC* phase at 100 • C. The measurements revealed the spontaneous polarization of 27 nC cm −2 for a thin film deposited on UV/O 3 -treated substrate. For the uniaxially aligned thin film formed by the friction-transfer method, the spontaneous polarization increased to 50 nC cm −2 . This value was 1.5 times greater than that in the bulk state of compound (S)−1.
Small spontaneous polarization and an ambiguous hysteresis loop in the thin films deposited on UV/O 3 -treated substrates should originate from the presence of the domains in which the LC molecules were aligned perpendicular to the electrode surface. In the molecules of compound (S)−1, the permanent dipole moments, which contributed mainly to the ferroelectricity, were almost perpendicular to the molecular axis, while the induced dipole moment derived from the polarization of the π-conjugated unit was parallel to the molecular axis.
Compared to the spontaneous polarization in the 2 µm-thick cells, those in the thin-film states on the FT-treated substrates were 1.5 times greater. In past studies on spontaneous polarization measurements of FLC cells with thicknesses larger than 2 µm, the spontaneous polarization decreased with the decrease in the sample thickness [38][39][40]. That results have been explained by the confinement of the LC molecules on the substrate surface. In the spin-coated films deposited on FT-treated substrates, the LC molecules are more strongly adsorbed on the electrode surface and the molecular ordering on the electrode surface should induce more ordered structure over the whole thin film. The influence from the molecular orientation on the electrode surface should be more remarkable in the thin-film states in LC cells.

In-Situ Polymerization of Thin Films of Compound (S)−1
Thin films deposited on UV/O 3 -and FT-treated substrates were polymerized by the ring-opening polymerization induced by the vapors of trifluoromethanesulfonic acid. Figure 5 exhibits polarizing optical micrographs of the uniaxially aligned thin films of compound (S)−1 deposited on UV/O 3 -treated substrates before and after the ring-opening polymerization. Birefringent domains with a size of several millimeters were observed, indicating a planar alignment in each domain. There were a few dark domains, although homeotropic alignment could not be confirmed in the domains because of the small size of the domains and low contrast. The sizes and birefringence of LC domains were retained during the ring-opening polymerization induced by the acid vapors. As-deposited thin films were soluble in organic solvents except for alcohol. Polymerized thin films were insoluble in acetone and dichloromethane.

In-Situ Polymerization of Thin Films of Compound (S)−1
Thin films deposited on UV/O3-and FT-treated substrates were polymerized by the ringopening polymerization induced by the vapors of trifluoromethanesulfonic acid. Figure 5 exhibits polarizing optical micrographs of the uniaxially aligned thin films of compound (S)−1 deposited on UV/O3-treated substrates before and after the ring-opening polymerization. Birefringent domains with a size of several millimeters were observed, indicating a planar alignment in each domain. There were a few dark domains, although homeotropic alignment could not be confirmed in the domains because of the small size of the domains and low contrast. The sizes and birefringence of LC domains were retained during the ring-opening polymerization induced by the acid vapors. As-deposited thin films were soluble in organic solvents except for alcohol. Polymerized thin films were insoluble in acetone and dichloromethane.  Figure 6 exhibits polarizing optical micrographs of the uniaxially aligned thin films of compound (S)−1 deposited on FT-treated substrates after the ring-opening polymerization. By the polymerization, the thin film was insolubilized in acetone and dichloromethane. As shown in Figure  6, the transmittance of the thin film under a cross-Nicol observation was changed by every 45-degree the rotation of samples, indicating the uniaxial planar alignment before and after polymerization. The uniaxial alignment of the thin film was retained during the polymerization process. In the polymerized thin films, supramolecular aggregation structures should be immobilized and the micrographic textures did not change when the temperatures of thin films were elevated to 100 °C.  Figure 6 exhibits polarizing optical micrographs of the uniaxially aligned thin films of compound (S)−1 deposited on FT-treated substrates after the ring-opening polymerization. By the polymerization, the thin film was insolubilized in acetone and dichloromethane. As shown in Figure 6, the transmittance of the thin film under a cross-Nicol observation was changed by every 45-degree the rotation of samples, indicating the uniaxial planar alignment before and after polymerization. The uniaxial alignment of the thin film was retained during the polymerization process. In the polymerized thin films, supramolecular aggregation structures should be immobilized and the micrographic textures did not change when the temperatures of thin films were elevated to 100 • C. polymerization, the thin film was insolubilized in acetone and dichloromethane. As shown in Figure  6, the transmittance of the thin film under a cross-Nicol observation was changed by every 45-degree the rotation of samples, indicating the uniaxial planar alignment before and after polymerization. The uniaxial alignment of the thin film was retained during the polymerization process. In the polymerized thin films, supramolecular aggregation structures should be immobilized and the micrographic textures did not change when the temperatures of thin films were elevated to 100 °C.

Conclusions
In conclusion, uniaxially aligned spin-coated thin films of π-conjugated FLC compound (S)−1 bearing a cyclotetrasiloxane moiety were prepared. Compound (S)−1 exhibited SmC* and SmG* phases. In the 2 µm-thick LC cells, the spontaneous polarization value of compound (S)−1 was 35 nC cm −2 . Compound (S)−1 showed good solubility in acetone (> 20 g L −1 ) and other organic solvents, in contrast to the aliphatic analog (S)−2. The spin-coated thin films were prepared on UV-O 3 -treated and FT-treated ITO-glass substrates. The uniaxially aligned thin films with a thickness of 100 nm were deposited on the ITO substrates. The spontaneous polarization was enhanced in the uniaxially aligned thin film and reached 50 nC cm −2 . The coercive electric field was upfield shifted due to the surface stabilization of the LC thin layer.
The spin-coated thin films of compound (S)−1 were insolubilized by the ring-opening polymerization induced by the acid vapors. The molecular alignment of the thin films was retained during the polymerization process. Uniaxially aligned thin films of compound (S)−1 could also be polymerized, retaining the uniaxial alignment by this method.
Supplementary Materials: The following are available online at http://www.mdpi.com/2073-4352/10/11/983/s1, Section S-1: Synthetic procedure and spectral data (Scheme S1: Synthetic route of compound (S)-1), Section S-2: Characterization of mesomorphism of (S)-1 ( Figure S1: DSC thermogram of compound (S)-1 at the scanning rates of 10 K/min, Figure S2: X-ray diffraction patterns of compound (S)-1 in the (a) SmC* phase at 110 • C, and (b) SmG* phase at 90 • C, Figure S3: Polarizing optical micrographs of compound (S)-1 in the (a) SmC* phase at 110 • C, and (b) SmG* phase at 90 • C. The LC samples were filled in an ITO sandwich cell with the gap of 2 µm, Figure S4: Polarizing optical micrographs of compound (S)-1 in the SmC* phase at 110 • C under the application of DC bias. The DC voltage was applied (a) to backward direction (+10 V) and (b) to forward direction (−10 V). The LC samples were filled in an ITO sandwich cell with the gap of 2 µm), Section S-3: Evaluation of ferroelectric properties of (S)-1 (Equation. S1: Determination of spontaneous polarization in the polarization inversion current method for (S)-1).