# 액정올리고머에 있는 카보닐그룹들의 동적순서에 대한 2차원 라만상관분광법 연구

• Jung, Kab-Sang (Department of Chemistry, Kunsan National University) ;
• Yu, Soo-Chang (Department of Chemistry, Kunsan National University) ;
• Han Yu, Keon-Ok (Department of Chemistry, Kunsan National University)
• 정갑상 (군산대학교 자연과학대학 화학과) ;
• 유수창 (군산대학교 자연과학대학 화학과) ;
• 한건옥 (군산대학교 자연과학대학 화학과)
• Published : 2004.06.20
• 100 25

#### Abstract

We investigated the order of local movement of functional groups (-C(=O)O) in a liquid crystalline (LC) oligomer (12-4) using 2D Raman correlation spectroscopy. The results suggest that the free carbonyl near the ethyl terminal group moved first, followed by the hydrogen-bonded group. The free carbonyl group between the biphenyl groups rarely moved. Interestingly, 2D sample-to-sample correlation spectroscopy (2D STSCS) revealed that some of the carbonyl modes started to move at far below (50$^{\circ}C$) the LC temperature (135$^{\circ}C$), countering conventional beliefs.

#### Keywords

2D Raman Correlation Spectroscopy;Liquid Crystalline Oligomer;Dynamics;Carbonyl Group

# INTRODUCTION

Liquid crystalline polymers (LCPs) containing an ester functional group in a mesogenic unit have long been the subject of studies of intermolecular interactions. Many theoretical and experimental works have examined the planarity of the benzene rings and adjacent carbonyl groups, and the site of bond rotation near the phase transition (solid-to-liquid crystal) temperature.1-3 We recently characterized an LC oligomer with a biphenyl ester moiety using Raman spectroscopy to better understand the mechanism of the conformational change that accompanies modification of the intermolecular interactions.4,5

In order to understand the mechanism of the conformational changes during the phase transition, we compared the spectral evolution of the combination mode of the aromatic C-C(=O)O and C(=O)O stretching vibrations at 1274 cm−1 with those of analogous molecules as a function of temperature, and found that bond rotation occurs around the aromatic C and the C(=O)O near the ethyl terminal. This bond rotation is thought to be facilitated mainly by cleavage of the hydrogen bond between the carbonyl oxygen near the ethyl terminal and one of the hydrogen atoms in the poly(ethylene oxide) (PEO) chain. Analysis of the C=O stretching mode allowed us to locate the carbonyl group that participated in the hydrogen bonding. Although the mechanism of the conformational changes was revealed, the local dynamics has not been analyzed fully.

Two-dimensional (2D) correlation spectroscopy is a very useful technique for analyzing the dynamics of molecules under various perturbations, such as temperature, time, and concentration.6-9 In brief, there are two components in 2D spectroscopy, one of which is called synchronous v (designated Φ (v1, v2)) and the other asynchronous (designated Ψ [v1, v2]). The synchronous spectrum represents simultaneous or coincidental changes at variables v1 and v2, while the asynchronous spectrum provides information about the order or priority of the modes of the variables. This technique simplifies complex spectra with many overlapping peaks and enhances the spectral resolution by spreading the peaks over a second dimension, identifying various inter- and intramolecular interactions from the selective correlation peaks.

We sought insights into the dynamics of LC oligomer 12-4 (Fig. 1) near the transition temperature using 2D Raman correlation spectroscopy. We investigated the order of local movement of functional groups (-C(=O)O), which determines the LC phase transition temperature.

Fig. 1.The chemical structure of 12-4.

# EXPERIMENTAL

The details of the synthesis and characterization of 12-4 were reported previously.4 The crystallineto-LC phase transition temperature (heating at a rate of 10 ℃ min-1) was observed at 135.2 ℃, using a Perkin Elmer DSC-7 differential scanning calorimeter (DSC) equipped with a 1020 thermal analysis controller.

The Raman spectra were obtained using a Renishaw Raman microsystem 2000 with excitation at the 632.8-nm line of a HeNe laser. The laser power at the sample was ca. 5 mW and the resolution of the spectra was ±2 cm−1. After the samples were put on glass slides, data were acquired using a Linkam heating and freezing stage (THMSE 600) with a controller (TMS 92), and then calibrated to the silicon band at 521 cm−1.

Prof. Yukihiro Ozaki at Kwansei Gakuin University in Japan kindly provided the analysis software for 2D correlation spectroscopy. The program was written using MATLAB 5.3 following the algorithm developed by I. Noda.

# RESULTS AND DISCUSSION

Information on the dynamics of carbonyl groups is critical for understanding the conformational changes in a LC oligomer at the crystal-to-LC temperature. In order to understand this, various LC polymers have been studied.4,5,10 In 12-4, one of the carbonyl modes forms hydrogen bonds with a hydrogen in the poly(ethylene oxide) group in the neighboring molecule.4,5 When hydrogen bonding occurs, a new band appears at 1725 cm−1 giving three bands (1717, 1725, 1734 cm−1). As the temperature increases, the hydrogen bond breaks up gradually, giving two bands. The changes in the intermolecular interaction with increasing temperature were deduced by monitoring three complementary Raman modes, i.e., the C=O, C=C, and aromatic C-H vibrational modes. However, we could not obtain information on local movement of a specific functional group using one-dimensional (1D) Raman spectroscopy. Therefore, it was necessary to explore the dynamics using 2D correlation spectroscopy.

Two-dimensional Raman correlation spectra in the carbonyl region were obtained from 1D Raman spectra5 and are shown in Fig. 2(a) and (b). They show three carbonyl modes, at 1711, 1724, and 1736 cm-1, which are assigned to the free carbonyl between biphenyl moieties, the hydrogen bonded carbonyl, and the free carbonyl next to the ethyl terminal group, respectively, based on the 1D Raman spectrum.5

Fig. 2.The 2D Raman correlation spectra in the carbonyl region, (a) synchronous and (b) asynchronous spectrum.

Peaks with positive and negative signs are represented by white and shaded contours, respectively. Referring to the 2D correlation rules, a positive sign indicates that the intensities of the corresponding bands in the one-dimensional spectra are either increasing or decreasing together, while a negative sign indicates that one is increasing and the other is decreasing. Negative cross peaks appearing at (1736, 1724) are seen in the synchronous spectrum in Fig. 2(a) and suggest that the two modes behave in opposite directions, as already observed in 1D Raman spectra. The cross peaks at (1736, 1711) and (1724, 1711) in the asynchronous spectrum are not seen in the synchronous spectrum. Referring to the 1D Raman spectra, the mode at 1724 cm−1 decreased with increasing temperature, while the intensity of the mode at 1711 cm−1 remained constant. This indicates that the intensity at 1711 cm−1 increased relatively. Likewise, the relative intensity at 1736 cm−1 increased, while the mode at 1711 cm−1 decreased.

In the asynchronous spectrum (Fig. 2(b)), we are concerned with the cross peaks at (1736, 1711), (1736, 1724), and (1724, 1711). The asynchronous correlation peak Ψ[v1, v2] provides information about the sequential order of the changes in the variables v1 and v2. A positive cross peak in an asynchronous spectrum indicates that v1 occurs predominantly before v2, while a negative cross peak indicates that v2 occurs first. This rule is reversed when the sign of the corresponding cross peak in the synchronous spectrum is negative. We used this relationship to determine the sequential order of the intensity change between the two bands in the asynchronous spectrum.

The positive peaks positioned at (1736, 1711) in Fig. 2(b) indicate that the mode at 1736 cm-1 changed before movement of the mode at 1711 cm-1 occurred. The negative sign at (1736, 1724) indicates that the mode at 1724 cm-1 moves before that at 1736 cm-1. However, the sign of the synchronous spectrum at (1736, 1724) is negative, indicating that the movement of the mode at 1736 cm-1 occurs predominantly before that at 1724 cm-1. The negative sign of the peaks at (1724, 1711) represents the priority of the movement of the mode at 1711 cm-1. However, the priority is reversed based on deductions from the 1D spectra explained above.

Therefore, the order of the movement is 1736 cm-1 ＞ 1724 cm-1 ＞ 1711 cm-1. The carbonyl group next to the ethyl terminal (at 1736 cm-1) moves first, followed by the hydrogen-bonded one (at 1724 cm-1). Finally, the carbonyl group between the biphenyl groups moves (at 1711 cm-1). This makes sense, because the free carbonyl groups next to the ethyl terminal are the most flexible. Then, the movement of the free carbonyl group perturbs the hydrogenbonded carbonyl group in turn, cleaving the hydrogen bond. The carbonyl between the biphenyl groups is very stiff compared with the free carbonyl next to the ethyl terminal or the hydrogen bonded one. This suggests that the movement of the carbonyl group between the biphenyl groups needs more thermal energy than the other two. These results are in good agreement with our previous results, which found that the carbonyl group at the ethyl terminal rotates at the crystalline-to-LC phase transition temperature, whereas the carbonyl group between the biphenyl groups rarely rotates.4

Mesogenic conformational changes are mostly responsible for the differences between the adjacent crystalline polymorphs in liquid crystalline molecules.11,12 Therefore, mesogenic Raman bands reflecting mesogenic conformational changes with environmental changes, such as temperature changes, are of particular interest. Since the LC temperature of 12-4 is ca. 135 ℃, the movement of the carbonyl modes should reflect this temperature. Therefore, we monitored the movement of the carbonyl modes with increasing temperature, because they belong to the mesogenic part, which determines the LC temperature, using 2D sample-to-sample correlation spectroscopy (2D STSCS), which is explained elsewhere.13

Two-dimensional STSCS is a powerful technique for monitoring slight changes in the intensity of a certain mode and we applied it to our system. For comparison, we plotted 2D STSCS for the entire spectral region (360~3150 cm-1) as well as for the carbonyl region (1697~1755 cm-1) by obtaining spectra at temperatures from 20 to 180 ℃ at increments of 10 ℃. As Fig. 3 shows, an apparent change in the spectral pattern of the entire region occurred at around 130 ℃, which is in relatively good agreement with the LC temperature. However, the spectral change in the carbonyl region was quite different, indicating that the local movement of the carbonyl mode does not occur at the LC temperature. A marked change was observed at 50 ℃, indicating that some of the carbonyl groups start to move at far below the LC temperature of 130 ℃. Generally, the PEO chain moves freely at lower temperatures than the mesogenic moieties do because of its flexible character. Therefore, the PEO chain mainly reflects the Tg temperature. Our result is quite different from this conventional concept. The carbonyl group in the mesogenic unit moved along with the PEO coil in a concerted way.

Fig. 3.The 2D sample-to-sample correlation spectrum (a) in the whole region (360 ~3150 cm-1) and (b) the carbonyl region (1697~1755 cm-1). First indicates the lowest temperature while the last represents the highest temperature.

# CONCLUSIONS

We used 2D Raman correlation spectroscopy to study the dynamics of 12-4 during the LC process. The analysis of complementary synchronous and asynchronous spectra showed that the free carbonyl group near the ethyl terminal moved first, followed by the hydrogen-bonded one. The free carbonyl group between the biphenyl groups rarely moved. The results obtained from 2D STSCS also revealed the interesting fact that some of the carbonyl modes started to move at far below (50 ℃) the LC temperature (135 ℃), countering accepted belief.

#### References

1. Yu, S.-C.; Choi, Y.; Yu, K. H.; Yu, J.; Choi, H.; Kim, D.H.; Lee, M. Macromolecules 2000, 33, 6527. https://doi.org/10.1021/ma991933m
2. Nakano, T.; Shimada, S.; Saitoh, R.; Noda, I. Appl. Spectrosc.1993, 47(9), 1337. https://doi.org/10.1366/0003702934067595
3. Hummel, J. P.; Flory, P. J. Macromolecules 1996, 13,479.
4. Birner, P.; Kugler, S.; Simon K.; Naray-Szabo. Mol.Cryst. Liq. Cryst. 1982. 80, 11. https://doi.org/10.1080/00268948208071018
5. Yu, K. H.; Rhee, J. M.; Lim, J.-H.; Yu, S.-C. Bull.Korean Chem. Soc. 2002, 23, 633. https://doi.org/10.5012/bkcs.2002.23.4.633
6. Ellis, G.; Marco, C.; del Pino, J.; Lorente, J.; Gomez, M.A.; Fatou, J. G. Vibr. Spectrosc. 1995, 9, 49. https://doi.org/10.1016/0924-2031(94)00070-W
7. del Pino, J; Gomez, M. A; Ellis, G; Marco, C.; Fatou,J. G. Macromol. Chem. Phys. 1994, 195, 2049. https://doi.org/10.1002/macp.1994.021950614
8. Bahadur, B. Liquid Crystals: Applications and Uses;World Scientific Publishing Co.: Singapore, 1990.
9. del Pino, J.; Gomez, M. A.; Marco, C.; Ellis, G.; Fatou,J. G. Macromolecules 1992, 25, 4642. https://doi.org/10.1021/ma00044a027
10. Lachenal, G.; Buchet, R.; Ren, Y.; Ozki, Y. In Twodimensional Correlation Spectroscopy; Ozaki, Y.; Noda, I., Eds.; American Institute of Physics: Melville, New York, 1999.
11. Sasic′, S.; Muszynski, A.; Ozaki, Y. J. Phys. Chem. A2000, 104, 6380. https://doi.org/10.1021/jp000510f
12. Ren, T.; Murakami, T.; Nishioka, K.; Noda, I.; Ozki, Y.Macromolecules 1999. 32(19), 6307. https://doi.org/10.1021/ma990072e
13. Noda, I. Apple, Spectrosc, 1993, 47(9), 1329.

#### Cited by

1. Progress in two-dimensional (2D) correlation spectroscopy vol.799, pp.1-3, 2006, https://doi.org/10.1016/j.molstruc.2006.03.053
2. Two-dimensional hetero-spectral correlation fluorescence-Raman spectroscopy for a thermotropic liquid-crystalline oligomer vol.51, pp.1, 2009, https://doi.org/10.1016/j.vibspec.2008.09.005