Study of the Experimental and Simulated Vibrational Spectra Together with Conformational Analysis of Thioether Cyanobiphenyl-Based Liquid Crystal Dimers

Abstract

Infrared spectroscopy (IR) and quantum chemistry calculations that are based on the density functional theory (DFT) have been used to study the structure and molecular interactions of the nematic and twist-bend phases of thioether-linked dimers. Infrared absorbance measurements were conducted in a polarized beam for a homogeneously aligned sample in order to obtain more details about the orientation of the vibrational transition dipole moments. The distributions to investigate the structure and conformation of the molecule dihedral angle were calculated. The calculated spectrum was compared with the experimental infrared spectra and as a result, detailed vibrational assignments are reported.

1. Introduction

Soft matter physics encompasses materials that are easily deformed by thermal fluctuations and external forces, such as, for example, liquid crystals (LC) [1]. Undoubtedly the terms “crystal” and “liquid” are mutually exclusive, but it turns out that their merge perfectly reflects the uniqueness of the material to which it refers. Liquid crystals can be broadly defined as any state of matter with some degree of positional or orientational organization intermediate between the isotropic liquid state and a crystalline solid with long-range positional and orientational order in three dimensions. They can be classified, according to the source behind the formation of the mesophases, into lyotropic and thermotropic [2]. The first group, lyotropic liquid crystals, emerges when amphiphilic mesogens, composed of a flexible hydrophobic chain and a polar head group (ionic or nonionic), are dissolved in a suitable solvent at an appropriate temperature, pressure, and concentration [3]. The second group comprises thermotropic liquid crystals, where the existence of mesophase is exclusively controlled by temperature, and the composition of the forming material is not changing with temperature. In this article, we will narrow the discussion to only thermotropic liquid crystalline phases, primarily nematic and twist-bend phases (N_TB). Without any doubt, the discovered nematic twist-bend phase is different from 3D liquids known to date because it exhibits a macroscopic chirality while formed from chemically achiral, bent-core-like molecules.

Vibrational spectroscopy has become one of the most informative tools in the study of liquid crystal materials [4,5,6,7,8,9,10,11,12,13]. An analysis of the intensity and positional changes of the vibrational bands makes it possible to identify the liquid crystal phases and to calculate the orientational order parameters. Unfortunately, for large molecules, it is virtually impossible to reliably define the vibrational fundamentals without any theoretical input; therefore, determining the vibrational frequencies using computational methods is extremely important. These methods are helpful in interpreting the experimental vibrational spectra for large molecules. They also give information about the shape of the bands and the orientation of the transition dipole moment in the molecular coordinate system.

In this research, we studied the liquid crystal dimers that are based on cyanobiphenyl mesogens. These dimers typically contain two rigid terminal groups that are chemically linked to each other by a flexible spacer with an odd number of methylene units [14,15,16]. Interest in liquid crystal dimers is high because of their extraordinary flexoelectric [17,18,19] and electro-optical properties [20,21,22,23] and their ability to form modulated nematic phases (N_TB—twist-bend, N_SB—splay-bend phase) [24,25,26,27,28,29,30,31]. This unique twist-bend phase is, in a sense, an example of the spontaneous formation of a helical structure similar to chiral helices found in DNA and proteins; twisted beta sheets form helical columns that are similar to silk and some modern synthetic analogs. The twist-bend modulated nematic phase (NTB) has a helical structure with a pitch length of several nanometers [21,25,32,33,34]. The structure of the NTB phase has primarily been studied using non-resonant (SAXS, WAXS) [35,36,37] and resonant X-ray scattering [32,33,38,39,40,41] as well as using polarized Raman [42], infrared [43,44,45,46] and nuclear magnetic resonance spectroscopy (NMR) [47,48,49,50,51]. Current experimental results show that the formation of the N_TB phase is very sensitive to changes in the shape of the molecules [52,53,54,55,56,57]; therefore, the key is to carefully define the relationship between the molecular parameters of the molecules and the occurrence of the modulated nematic phase. For this purpose, many authors have used molecular modeling methods, mainly the density functional theory (DFT) [28,29,33,34,52,58,59,60,61] or molecular dynamics simulations (MD) [62,63,64] to analyze structural and conformational changes of the dimers. However, no analysis of the conformational changes of molecules in the transition from the nematic to the twist-bend nematic phase based on a comparison of simulated and experimental vibrational spectra has been performed so far. Polarized measurements of the vibrational spectra (Raman and infrared) are extremely useful in studies of the supramolecular systems that primarily arise through intermolecular interactions such as hydrogen bonding [45,65,66,67,68,69,70] and π-π stacking [71]. The analysis of the vibrational spectra for such supramolecular systems in the first stage requires the assignment of the bands in the spectrum with regard to the individual functional groups in the molecule, which the modulated nematic phases are clearly an example of.

Here, we report on a spectroscopic and theoretical study of two groups of dimers: a symmetric one that contains the thioether-linking groups (C-S-C) and ether-linking groups (C-O-C) and an asymmetric one that contains both the ether- and thioether-linking groups. By using the polarized infrared absorbance method for a homogeneously aligned sample, it was possible to obtain information about the orientation of the transition dipole moments of a molecule. This information was compared with the theoretically calculated cartesian components of the vibrational transition dipole moment for specific vibrations and has proven to be very useful in the precise assignment of the bands in experimental spectra.

2. Results

2.1. Molecular Structures

The rotational potential barriers of the molecules were obtained using the relaxed potential energy surface scan method with the molecular geometry optimized in order to find the most probable conformations that occurred in the tested materials. In order to find the most stable conformation of a dimer, the optimization of the geometry was performed in a few steps. All of the possible conformations of the dimers that were considered were defined by the values of the dihedral angles φ₁–φ₄ (Figure 1b). In the first stage, the energy barriers to the internal rotation of the cyanobiphenyl (torsional angles φ₃ and φ₄) were determined. In a further step, the energy barriers to the rotation around the dihedral angle (φ₁, φ₂) between the cyanobiphenyl and the linker were determined. The approximate potential energy functions were calculated at intervals of ten. For the calculations, the torsional angles (φ₁–φ₄, each in turn) were fixed at arbitrarily selected values while the other geometrical parameters were optimized, after which relaxed potential energy scans were performed. This procedure enabled the values of the torsion angles for which the minimum energy was obtained to be determined. As the energy barrier to the internal rotation in the alkyl chain is very small (approx. 1 kJ/mol), no other linker/alkyl chain conformations than the all-trans were considered. In the ordered phases, in principle, the alkyl chains can take up all of the possible conformations, and therefore, adopting all of the all-trans conformations is a better representation of the average molecular shape of the dimers [72]. In the next step, taking into account the values of torsion angles that were determined, a full optimization of the geometry was performed for all of the dimers.

Dihedral Angle Distributions and Conformations

Figure 1 shows the calculated rotational potential barriers. First, the torsion angle of the cyanobiphenyl was calculated (φ₃, φ₄). The calculated value of the angle for the minimum energy was 40°, and the potential barriers to this twisted conformation were 8.71 kJ/mol for φ = 0° and 8.98 kJ/mol (for φ = 90°). The value of the φ₁/φ₂ angle is the most crucial for determining the bend angle of the molecule. There are a number of conformations for the CBSCnSCB and CBSCnOCB dimers, which are important for calculating the orientational order, primarily due to possible dihedral angle (φ₁, φ₂): C_Al-S-C_Ar-C_Ar of the sulfur bridge for CBSCnSCB and also C_Al-O-C_Ar-C_Ar (Ar—aromatic ring, Al—alkyl) of the oxygen bridge for CBSCnOCB. The conformational energies of the individual molecules were calculated with respect to those dihedral angles. Both angles were found to have a minimum energy for the “zero” angle (planar conformation) in contrast to the corresponding angle for CBCnCB: C_Al-C_Al-C_Ar-C_Ar, which was close to 90° with a potential barrier of 5.5 kJ/mol (upright conformation). The energy barrier to the rotation of the C_Al-O-C_Ar-C_Ar bridge was high enough (∆U~13.7 kJ/mol) to enable only the planar conformer to be possible. In the case of the sulfur bridge (C_Al-S-C_Ar-C_Ar), however, the barrier was much smaller (∆U~2.1 kJ/mol), and therefore, the intermolecular interactions might have influenced the molecular structure, which is in agreement with Y. Cao et al. [34]. This means that for the dimers that contain sulfur, more than one energetically stable conformation is possible. As the energy barrier to the internal rotation in the alkyl chain is very small (approx. 1 kJ/mol), no spacer other than the all-trans was considered. In the ordered phases, in principle, the alkyl chains can occupy all of the possible conformations, and, therefore, adopting all of the all-trans conformations is a better representation of the average molecular shape of the dimers [72].

Taking into account the designated torsion angles, a full optimization was performed for each conformation of the dimers. Based on the coordinates of the atoms in space and the coordinates and lengths of the vectors corresponding to the arms of the molecules, the opening angles of the molecules were estimated for all of the probable conformations of the molecules (Figure 2).

Table 1. Values of the most important torsion angles, potential energies with the root mean square (RMS) and opening angles for the optimized geometry of a dimer.

Sample	Conf.	Potential Energy RMS (kJ/mol)	Torsion Angles, φt (°)				Opening Angle (°)
			φ1	φ2	φ3	φ4
CBC9CB	Upright (U)	−3,843,952.076 0.014	92.3	86.2	−38.7	−38.5	112
CBSC7SCB	Upright (U)	−5,521,962.5193 0.0035	−92.9	−92.8	−39.0	−39.0	94
	Flat (F)	−5,521,963.9252 0.0024	5.8	5.8	−37.2	−37.2	108
CBSC7OCB	Mixed (M)	−4,673,985.9556 0.0077	−96.1	−179.1	−38.8	−37.2	120
	Flat (F)	−4,673,986.6314 0.0037	−176.3	−180.0	−37.4	−37.6	126
CBOC7OCB	Flat (F)	−3,826,009.436 0.020	−179.3	−179.2	−37.3	−37.3	144

shows the torsion angle values and opening angle values for the fully optimized geometry of all of the dimers.

The bend of a molecule is necessary for the formation of the twist-bend phase. The largest opening angle (144°) was obtained for the CBOC7OCB molecule. This caused its shape to be closer to a calamitic molecule than to a bent (banana) molecule, which means that it did not meet the conditions for the formation of the twist-bend phase, which was confirmed experimentally via the POM, DSC and FTIR measurements [46,59,73].

2.2. Molecular Vibrations

To perform an in-depth analysis of the experimental spectra, the density functional theory (DFT) was used to calculate the theoretical IR spectra for an isolated molecule. Generally, however, there are no absolute assignments of the IR frequencies, and for low symmetry molecules, the correlations of the calculated and experimental frequencies are primarily made by comparing bands that have similar frequencies, assuming that there is no rearrangement of the individual peaks in the bands.

All of the calculated vibrational frequencies are expressed as the wavenumber in cm⁻¹, while the so-called integral absorption coefficient, which is directly proportional to the sum of the components of the squares of the transition dipole moments, is represented by the formula:

$$\overline{A}=\frac{N\pi }{3c^2}\left[{\left(\frac{\partial {\mu }_x}{\partial Q}\right)}^2+{\left(\frac{\partial {\mu }_y}{\partial Q}\right)}^2+{\left(\frac{\partial {\mu }_z}{\partial Q}\right)}^2\right],$$

(1)

where N—Avogadro constant, c—speed of light and $\frac{\partial {\mu }_i}{\partial Q}$—the change in the component of the dipole moment with respect to the normal coordinates.

For a more precise analysis of the spectra, it was necessary to calculate the components of the transition dipole moment. Information about the components of the transition dipole moment for a specific vibration enables the parallel and perpendicular components of the spectral density to be calculated. The parallel component of the absorption coefficient was calculated as the square of the component of the transition dipole moment along the axis that coincided with the long axis of the dimer ${\left|{\mu }_z\right|}^2$. To determine the perpendicular component of the spectral density, the sum of the squares of the transition dipole moments along the perpendicular directions was used ${\left|{\mu }_x\right|}^2+{\left|{\mu }_y\right|}^2$. The direction of the transition dipole moment was determined according to the molecular reference system (see Figure S1 in Supplementary Materials).

In order to compare the theoretical bands with the experimental results, the discrete spectrum lines were extended using the Gaussian function with a half-width of 7 cm⁻¹. Then, the frequencies were rescaled using the scaling coefficient that was determined for the base that was used, which is 0.967 ± 0.021, according to Computational Chemistry Comparison and Benchmark Database. The intensities of the bands were divided by the intensity of the highest band in the theoretical spectrum for a given molecule (or the conformation in the case of molecules for which two stable conformers were calculated). The results of the calculations were compared with the experimental data from the nematic phase in order to identify the most important bands in the spectrum.

2.3. Vibrational Spectra and Their Assignments

It is practically impossible to obtain perfect order in an experiment, and additionally, the dichroism of the bands is influenced by many factors, mainly the intermolecular interactions. Therefore, based only on the analysis of the experimental spectra, it is difficult to say with absolute certainty which band and which of the cyanobiphenyl para axes will be characterized by the behavior of the long axis of a dimer, i.e., to independently describe the direction of the dimer arms. In the case of the theoretical spectra for symmetric dimers, for a given band of the cyanobiphenyl, two characteristic vibrations with a similar frequency but with different intensities should always be obtained. These correspond to the simultaneous vibrations in both arms, one of which is in phase and the other is out of phase. These vibrations, while coupling with each other, can ultimately cause a transition dipole moment to be along the long axis of the dimer or across it. Based on the analysis of the band dichroism for the theoretical spectra, which illustrate the theoretical, “ideal” order, it can be said that if the so-called infinite dichroism can be obtained, i.e., when one of the components is maximum and the other is close to zero, then such a band will then describe the behavior of the long axis of a dimer. On the other hand, in any other case, when the band dichroism is intermediate, there is a lack of vibration coupling for both arms and this band will describe the behavior of the para axis of the mesogens.

The experimental spectra in the entire range of wavenumbers (500–3500 cm⁻¹) for all of the studied dimers in the nematic phase are presented in Figure S2 in the Supplementary Materials.

Overall, the spectra of the cyanobiphenyl dimers can be divided into the following frequency ranges:

• 500–600 cm⁻¹ and 700–900 cm⁻¹ ranges, which cover the deformational vibrations of the carbon atoms (C-C) and hydrogen atoms (C-H) out of the benzene plane;
• 900–1650 cm⁻¹ range, which includes both the characteristic deformation vibrations in the benzene plane as well as the deformation vibrations of the methylene groups of the alkyl chain of the linker in a dimer;
• 2100–2400 cm⁻¹ range, which includes the stretching vibrations of the cyan group (C≡N) that were observed as a sharp and very intense peak in the experimental spectrum;
• 2800–2950 cm⁻¹ range, which includes the C-H stretching vibrations of the methylene groups. In this range, the vibrations were not well reproduced by the theoretical spectra because the calculations did not take into account the anharmonic effect;
• 2900–3100 cm⁻¹ range, which represents the stretching vibrations of the hydrogen atoms (C-H) in the aromatic ring. These vibrations were also not well reproduced by the theoretical frequencies. The bands in this range corresponded to the mixed vibrations, which were strongly overlapping, and the vibrations stretching the C-H hydrogen atoms, significantly disturbed by the Fermi resonance effect.

Most of the fundamentals in the range of 500–2300 cm⁻¹ were very well reproduced by the vibrations in the experimental spectra. Most of the observed changes, relative to the transition from the nematic phase to the twist-bend and with the conformational changes that were observed for the thioether dimers, were in the range from 500 to 1200 cm⁻¹.

In this section, we will present the spectra analysis for the CBS7SCB and CBS7OCB dimers in more detail. A comparison of the experimental and theoretical spectra for the dimers, CBC9CB and CBOC7OCB, is summarized in the Supplementary materials (Figures S3–S5).

2.3.1. The CBSC7SCB Dimer

The most important information in comparing the conformers is polarity of the prominent bands. The simulated spectra correspond to the perfect order. On the contrary, the experimental spectra are measured in the nematic phase, and corresponding orientational order is rather weak (S~0.5) due to the bending shape of the molecules. In order to make them comparable, we converted experimental spectra to those of the perfect order (we used the Equation (2a,2b)) [46]. Then, we analyzed differences in the theoretical spectra between the two conformations (flat and upright), with comparison to the experimental spectra in the nematic phase.

Figure 3 shows the comparison between the polarized experimental and theoretical spectra for the CBSC7SCB dimer in the region of 500–1150 cm⁻¹. In the low frequency range, two medium-intensity bands at 520 and 560 cm⁻¹, which were assigned to the deformational vibration of the carbon atoms out of the benzene plane (γCC op CB; op–out of benzene plane CB–cyanobiphenyl), and a low-intensity band on the slope of the 560 band at the wavenumber of 551 cm⁻¹, which referred to the deformational vibration of the C≡N group (δCN), were observed. In the experimental spectra, the band at the wavenumber of 520 cm⁻¹ had a perpendicular direction of the transition dipole moment. This band also involved the thioether bridge and made a significant contribution to the deformation vibration of the sulfur atom (γCC op CB + δCS). In the theoretical spectrum for the planar conformation (F), as a result of the coupling of the vibrations of both arms, a band at the wavenumber of 514 cm⁻¹ was observed with the maximum dichroism, and the transition dipole moment was perpendicular to the long axis of the dimer. In the case of the second conformation, which was called upright (U), two bands of comparable intensities were observed, one representing the vibration in the phase of both arms, which indicated the perpendicular direction of the transition dipole moment, while the antiphase vibration of both arms indicated the direction of the transition dipole moment parallel to the long axis dimer. Therefore, this band did not show dichroism for the U conformation. Additionally, for the upright conformation (U) in the theoretical spectrum, for the band at 650 cm⁻¹, we observed a splitting into two maxima, which was not observed in the experimental spectra.

In the range of 800 to 1120 cm⁻¹, the biggest differences between the conformers were associated with the out-of-plane deformation vibrations of the C-H groups (811 cm⁻¹; γCH op CB) and the deformation C-H vibrations in the benzene plane (1100 cm⁻¹). In the case of the upright conformation (U), there were two vibrations with similar wavenumbers and comparable intensities, which were similar to the 520 cm⁻¹ band. In the experimental spectra, the 811 cm⁻¹ band indicated the perpendicular direction of the transition dipole moment with a high dichroism, which corresponded to the flat conformer (F). The band at 1100 cm⁻¹ was a complexed vibration and involved a sulfide bridge and was assigned to the asymmetric stretching vibration of the C_Ar-S group (βCH ip CB + ν_as C_Ar-S; Ar–aromatic ring; as–asymmetric, ip–in the benzene plane); therefore, this band was quite sensitive to the dimer conformational changes.

Another indication that the flat conformation was more favored was the absence of a band at 1100 cm⁻¹ for the U conformer. In this range, there was also a band of low intensity at 1000 cm⁻¹, which was attributed to the breathing deformation vibration of the carbon atoms in the benzene ring (βCC).

The next spectrum range that is discussed is the 1200–1650 cm⁻¹ range, where several high-intensity bands (1460, 1594, 1600 cm⁻¹) were observed, which were assigned to the benzene ring deformations (νCC br; br–benzene ring). They corresponded to the longitudinal transition dipole, which was similar to the bands at 1000, 1100 and 2300 cm⁻¹ wavenumbers (2300 cm⁻¹–assigned to the stretching vibrations of the cyan group, νCN).

In this range, a low-intensity band with a wavenumber of about 1395 cm⁻¹ was also observed, the direction of which was the dipole transition perpendicular to the long axis of the dimer. This band was assigned to the in-plane deformation of the C-H groups (βCH ip CB). Differences between the two conformations for the benzene ring vibrations were also observed at 1600 cm⁻¹. In the experimental spectrum, this peak was split into two maxima with similar wavenumbers (1594 and 1604 cm⁻¹), for which the intensity shares changed with temperature. In the nematic phase, both peaks had a similar intensity, while in the twist-bend phase, an increase in peak intensity was observed at a lower wavenumber (1594 cm⁻¹). For the F conformer, this vibration was observed at a lower wavenumber, i.e., about 1595 cm⁻¹, while for the U conformer, it was observed at 1598 cm⁻¹ wavenumber. The above observations could lead to the conclusion that in the high temperature phases (nematic phase), the coexistence of both conformations and/or some intermediate conformers are probable, while when the temperature is lower, the planar conformation predominates, which is more preferred energetically.

In the Supplementary materials, a comparison of the unpolarized experimental and theoretical spectra for both conformations is additionally summarized in Figure S6. This comparison was intended to show that the band frequencies in the experimental spectrum are remarkably well reproduced by the theoretical ones for the flat conformation.

2.3.2. The CBSC7OCB Dimer

Figure 4 shows the comparison between the polarized experimental and theoretical spectra for the asymmetric CBSC7OCB dimer in the region of 500–1150 cm⁻¹. In the low frequency range, three medium-intensity bands were observed at 520, 530 and 560 cm⁻¹. It was observed that the band at the wavenumber 520 cm⁻¹, which characterized the vibration of the C-C groups out of plane, together with the deformation vibration of the C-S group, had a perpendicular direction of the transition dipole moment in the experimental spectrum and was split into two maxima. An additional maximum appeared at the wavenumber 530 cm⁻¹, which was not observed for the CBSC7SCB dimer. This new band was assigned to the deformation vibration of the C-C group out of the benzene plane along with the deformation vibration of the C_Ar-O-C_Al group (γCC op CB + δC_ArOC_Al; Al–alkyl chain). In the theoretical spectrum of the F conformer, a split band was also obtained and the transition dipole moment was directed perpendicular to the long axis of the dimer.

In contrast to the mixed conformation (M), only one undivided band was observed. Additionally, in the experimental spectrum, three bands were observed, which also corresponded to the transversal transition dipole moment: wavenumbers 813, 821 and 850 cm⁻¹. Compared to the CBS7SCB dimer, a new maximum appeared at 821 cm⁻¹, which was a complex band and, in addition to involving the out-of-plane deformation vibrations of the C-H group, also described the symmetrical stretching vibration of the C_Ar-O group (γCH op CB + ν_s C_ArO; s–symmetric). In the spectrum of the CBSC7OCB dimer, other new bands that were characteristic for the oxygen bridge were observed: asymmetric stretching vibrations of the C_Al-O group (ν_as C_AlO) at 1029 and 1050 cm⁻¹ and strong vibrations that were assigned to the asymmetric stretching of the C-O group (νas C_ArO) at 1249 and 1266 cm⁻¹.

In the 800–1120 cm⁻¹ range, the greatest differences between the conformers were associated with the out-of-plane vibration of the C-H group (813, 821 cm⁻¹). In the case of the mixed conformation, only one maximum of high intensity at 816 cm⁻¹ was observed. In the case of the F conformer, two maxima were observed, which was in good agreement with the experiment. Another indicator that a planar conformation is more likely was the absence of a maximum at 1100 cm⁻¹ in the spectra of M conformer, which was the same as that for the symmetric dimer.

Figure S7 in the Supplementary Materials shows a comparison of the unpolarized experimental and theoretical spectra for both conformations.

3. Discussion

The spontaneous emergence of nanoscale helices in non-chiral materials is one of the most fascinating topics in liquid crystal research with implications for soft matter research in general. An example is the nematic twist bend (N_TB) phase, where typically dimeric molecules assemble in helices of the 6–16 nm scale. The helix pitch has mainly been identified by anomalous (k-edge) scattering–a technique globally available at a very limited number of synchrotron stations. Based on the information gathered there, models for molecular assembly have been developed, essentially packing bend and twisted molecules into helices. In this contribution, we show the powerful tool of IR spectroscopy, a much more widespread and in many ways more democratic technique, as it is much cheaper and does not require access to scarce and massively oversubscribed beamlines to provide additional information on the assembly in the N_TB phase.

To clarify matters, we investigated a set of systems where the helical structure had been unambiguously identified, and we measured and analyzed the impact of different moieties using detailed polarized infrared measurements (IR) of critical groups. Additionally we employed molecular modelling methods, mainly the density functional theory (DFT) to analyze structural and conformational changes of the dimers. The analysis of the conformational changes of the molecules in the transition from the nematic to the twist-bend nematic phase based on a comparison of simulated and experimental vibrational spectra was performed for the first time for such complex systems.

In summary, it can be seen that the frequencies of the most important bands in the experimental spectra are well reproduced by the theoretical frequencies, while the differences in band intensities are due to the lack of consideration of the intermolecular interactions. The torsional barrier of the S-bridge is quite small (~2 kJ/mol). Therefore, the nearest neighbor’s molecules may significantly influence the vibration of the particular molecule. In the paper [74], we show the effect of the vibrational coupling between nearest neighbors. As a result, transition dipoles as well as absorbances of the particular vibrations significantly differ from those of a single molecule.

Table 2. Vibrational frequencies, IR intensities and assignments of the dimers.

CBC9CB		CBSC7SCB		CBSC7OCB		CBOC7OCB		Assignments
$\overline{\mathsf{\nu }}$	Ir	$\overline{\mathsf{\nu }}$	Ir	$\overline{\mathsf{\nu }}$	Ir	$\overline{\mathsf{\nu }}$	Ir
520	vvw	522	m	523	w	--	--	γCC op CB + δCS
--	--	--	--	532	w	532	w/m	γCC op CB + δCO
554	w	562	w	562	w	562	w	γCC op CB + δCN
816	vs	811	vs	813	vs	--		γCH op CB
--	--	--	--	821	s, sh	821	vs	νsCOC + γCH op CB
836 850	w	852	w	850	w	850	w	γCH op CB + νCCC sk + δasCH2 rocking
1007	w	999	w	999	w	1000	w	βCC ip CB, breathable
1026	vw	1020	vw	1013	vw	1013	vw	νCCC sk + βCH ip CB
--	--	--	--	1029 1051	w	1032	w	νasCAlO + βCH ip CB
--	--	1097	m	1095	m	--	--	νasCArS + βCH ip CB
1112	vw	--	--	--	--	1120	w	βCH ip CB
1185	m	1185	s	1180	s	1178	s	βCH ip CB
--	--	--	--	1249 1266	vs m, sh	1249 1266	vs m,sh	νasCArO + βCH ip CB
1284 1315 1360	vw	1279 1315	vw	1290 1311	vw	1290 1313	vw	γsCH2 wagging γsCH2 twisting
1397	w	1395	w	1392	w	1390	w	βCH ip CB
1460	w	1437 1462	w	1435 1472	w	1472	w	βsCH2 scissoring
-- 1493	s	1484 --	vs	1485 1494	vs	-- 1493	vs	νCC br
--	--	--	--	1522 1577	m vw	1523 1580	m w	νCC br + βsCH2 + νasCArO
-- 1605	s	1594 1604	vs	-- 1603	vs	-- 1602	vs	νCC br
2224	vs	2223	vs	2223	vs	2223	vs	νCN

Key: ip—in plane vibration; op—out of plane deformation, br—stretching and deformation vibrations of the ring (benzene ring), s—symmetrical, as—asymmetric, Al —alkyl chain, Ar—aromatic ring, sk—skeletal, ν—stretching, γ—deforming out of plane, β—deforming in plane, δ—deforming, vs—very strong, s—strong, m—medium, w—weak, vw—very weak, sh—shoulder. Ir—relative intensity of the bands.

presents a comparison of the main experimental bands and their assignments to the vibrations of the appropriate functional groups for all of the studied dimers. More-detailed and raw data on the theoretical and experimental frequencies, dichroism values, relative intensity, direction of the transition dipole moment and approximate band assignments for all of the investigated dimers are included in the Supplementary Materials (Tables S1–S4).

4. Materials and Methods

4.1. Materials

The symmetrical and asymmetrical liquid crystal dimers with the cyanobiphenyl (CB) mesogenic groups were investigated. We present three symmetric dimers, which had the general acronym CBXC7XCB (X = C or S or O), that contain nine functional groups in the chain linking the two mesogenic cores (methylene, thioether, ether); the CBC9CB that contains nine methylene groups in the linker and the CBSC7SCB and CBOC7OCB in which the alkyl chains contain seven methylene groups are connected to the cyanobiphenyls by two thioether or two ether bridges, respectively. In the asymmetric dimers with the acronym CBSCnOCB (n = 5, 7), the mesogens are linked to an alkyl chain with five or seven methylene groups on one side by a thioether bridge and on the other by an ether bridge. The details for the materials CBC9CB were reported earlier [75,76,77]. Synthesis details concerning the thioether/ether compounds were published recently [59,73]. Figure 5 shows the chemical structures of the investigated compounds.

4.2. Infrared Spectroscopy

The planarly aligned cells were prepared between two optically polished zinc selenide (ZnSe) discs. The thickness of the fabricated cells was determined to be within the range of 5.1–5.6 μm by the measurements of the interference fringes using a spectrometer that was interfaced with a PC (Avaspec-2048). The infrared spectra were acquired using a Fourier infrared spectrometer (Agilent Cary 670 FTIR). The experiment was conducted using the transmission method with a polarized IR beam. An IR-KRS5 grid polarizer was used to polarize the IR beam. The IR spectra were measured as a function of the polarizer rotation angle in the range 500–4000 cm⁻¹ of wavenumbers. The details of the sample preparation and absorbance measurement are published in Kocot et al. [46]. These measurements enabled the orientation of the transition dipole moment of the bands to be determined with respect to the long molecular axis and the temperature dependencies of the absorbance of the samples. To determine all three components of absorbance (A_x, A_y, A_z), it is necessary to measure two samples with different orientations: planar (homogeneous) and homeotropic. Unfortunately, in the case of the tested materials, i.e., for the cyanobiphenyl dimers, it was extremely difficult to obtain a good homeotropic alignment. Therefore, in order to calculate the mean absorbance of the sample and assuming that the material was uniaxial, it was assumed that A_x = A_y and, therefore, the mean absorbance was determined as A₀ = (2A_y + A_z)/3. The absorbance components were determined as the area that was bound by the contour of a given band using Bio-Rad Win-IR Pro version 2.96e. In the case of complex bands that contained more vibrations, they were separated using Origin Pro 2021 software with the Pearson VII fit.

4.3. Density Functional Theory Calculations

In this work, the calculations of the electronic structure of the molecules were performed using the Gaussian09 program (version E.01) [78]. The molecular structures, intermolecular binding energy, harmonic vibrational force constants, absolute IR intensities and components of the transition dipole moment were calculated using the density functional theory (DFT) with Becke’s three-parameter exchange functional in combination with the Lee, Yang and Parr correlation functional B3-LYP method with the basis set: 6-311(d,p) [79,80]. The results were visualized using GaussView 5.0.8.

All of the DFT optimizations were performed with the following convergence criteria, which were used with the Berny algorithm (all values in atomic units): the maximum component of the force was set to 0.00045, the root-mean square (RMS) of the forces that were calculated for the next step—smaller than 0.0003; the computed displacement for the next step—smaller than 0.0018 and the RMS of the displacement below 0.0012. These criteria restricted the dependence of the final geometry parameters on the initial starting geometry.

5. Conclusions

The extensive research on the structure of the N_TB phase, to date, permits specific conclusions to be drawn, namely, that a molecular curvature is fundamental for the formation of the phase and that the stability of this phase increases with a decrease in the molecular bending angle.

Using the DFT simulations of the electron structure of molecules, the rotational barriers were determined and the optimization of the most probable conformers that could appear in real samples was performed. Two energetically stable conformations were found for the molecules that contained sulfide bridges, and one was found for the molecules CBC9CB and CBOC7OCB. The opening angles of the tested dimers were also determined. The simulated theoretical spectra turned out to be an invaluable tool for identifying the most important bands in the experimental spectra as well as in determining the directions of the dipole transition moments of the molecules. Combined with the observations of the deflections in the normal modes of the atoms from the equilibrium positions, bands were assigned to the appropriate fragments of the molecules, and thus information about the geometry of the system was obtained.

However, due to the torsional barrier of the S-bridge that is very small (~2 kJ/mol) the nearest neighbor’s molecules may significantly influence the vibration of the particular molecule.