FMCp - 6 Cellulose Ether Polymers as Optical Compensation Films for LCDs High Birefringence and Tunable Optics Zhuo Wang, Jason Folkenroth*, Weijun Zhou**, Yongwen Zhang, Xiuqin Shi Dow Chemical, No. 936, Zhangheng Road, Pudong District, Shanghai 201203, China *Dow Wolff Cellulosics, 1691 N. Swede Road, Larkin Laboratory, Midland, MI 48674, U.S. **Dow Materials Science, Core R&D, 2301 N. Brazosport Blvd., Freeport, TX 77541, U.S. Keywords: LCD, Compensation Film, Ethyl Cellulose, Silicone, Birefringence ABSTRACT ETHOCEL ethylcellulose polymers from Dow Chemical provide an alternative material to tri-acetyl cellulose (TAC) for LCD retardation films to increase viewing angle and contrast through its unique birefringence optics, excellent optical transparency, and low haze. Moreover, a new ETHOCEL-based polymer system has recently been developed with new optical properties such as tunable birefringence and flat wavelength dispersion. molecular liquid crystals with rod-like or disk-like orientation to achieve out of plane birefringence. Similar with plasticizer, long-term stability is a big concern for these additives. Recently, high molecular weight polymers were blended with cellulose ester or cellulose ether. For example, ethyl cellulose (EC) was blended with CAP (cellulose acetate propionate), and a copolymer of SMA (styrene maleic anhydrate copolymer) [5-7] was blended with ethyl cellulose. However, the miscibility is a big concern for these blending systems and the haze is difficult to reduce to below 1%. 1. INTRODUCTION The dominant LCD markets have different optical property requirements for retardation films based on LCD [1] modes . As shown in Table 1, there are three general types of LCDs, TN, VA and IPS modes, dominating the LCD products such as TVs, PCs, monitors, tablet PCs, phones, and others. The high-end products such as large size TVs, tablet PCs, smart phones usually have more demanding requirements for viewing angle and contrast, as a result, require special in-plane (Ro) and out-of-plane (Rth) retardation for optical films, as shown in Table 1: In this report, ethyl cellulose (EC) and its polymer blends are introduced with high and tunable retardation values, respectively. Table 1 LCD retardation film Ro/Rth requirements Applications Large size TVs (>32”) LCD modes VA mode IPS mode PCs, laptops TN mode High ending Tablet PCs, smart phones VA mode IPS mode Ro needs Rth needs 50 nm 0 nm (<10 nm) 125~570 nm 50 nm 0 nm (<10 nm) 130 nm 0 nm (<10 nm) No needs 130 nm 0 nm (<10 nm) To meet the current application targets, blending and coating are effective ways to tune the optical properties. For example, retardation adjusting additives and coating [2-4] technologies are widely used. 2. EXPERIMENTAL Raw materials: ethylcellulose is from The Dow TM Chemical Company with the brand name of ETHOCEL STD 100. Tri-acetyl cellulose is from ACROS, di-acetyl cellulose L-50 is from Daicel, cellulose acetate propionate CAP-381-0.5 and cellulose acetate butyrate CAB-482-0.5 are from Eastman. Silicone solid flakes are from Dow Corning Corporation. Film preparation: ethylcellulose powders and silicone flakes are first dissolved in a toluene/ethanol solvent mixture with total solid content of 10 % by weight for film preparation. The film was prepared by casting the dope on a glass substrate by using an automatic casting machine. After drying at room temperature for 15 hours, the films were peeled off the substrate for performance testing and structure characterization. The film thickness was controlled for 90 micrometers. Performance testing: Optical transparency and haze properties were tested under ASTM 1003 by using Transmittance & Haze meter (BYK 4727). Film birefringence properties were collected by using Kobra Automatic Birefringence Analyzer. Most of these retardation additives are based on small ISSN-L 1883-2490/19/0499 © 2012 ITE and SID IDW/AD ’12 499 3.1 Rth comparison As shown in Fig. 1, the pure ethyl cellulose film shows much higher Rth than cellulose ester films prepared similarly, including cellulose acetate polymers of higher substitution degree (TAC) and lower substitution degree (di-acetyl cellulose, DAC), blends of acetate and propionate/butyrate (CAP, CAB). So, high Rth is a characteristic property for ethyl cellulose polymer. The high Rth of ethyl cellulose makes it a promising ultra-thin film material toward the trend of light and thin portable devices. 500 470 4 400 3 300 200 148 1 0.5 0.6 45 0.3 0.9 100 0.648 0 DAC TAC CAP CAB Fig. 1 Ro, Rth of cellulose polymers At the same time, adjustable Rth for ethyl cellulose based films was also developed for existing technologies to meet the various Rth needs in VA/IPS/TN mode LCDs. As shown in Fig. 2, by addition of silicone additives with ethyl cellulose, Rth of as-prepared films decreased from 470 nm to 1 nm. Rth can be easily controlled by the ratio of ethyl cellulose to silicone. Rth-hypothetical 400 300 200 y = -4.7x + 470 y = -10.133x + 481.48 R² = 0.9958 100 0 0 20 40 60 80 100 Silicone ratio in total solid, % Fig. 3 Linear relationship of Rth and additive dosages This interaction is also helpful for the good miscibility of ethyl cellulose and silicone polymers. The miscibility could also be indirectly observed by transparency and haze testing. As shown in Figure 4, EC/silicone blend films exhibit very high transparency and ultra low haze. Across the wide blending ratio 5% to 70%, all blend films show transparency higher than 92% and haze lower than 0.5%, which also supports the excellent miscibility of ethyl cellulose and silicone polymers. EC/Silicone: Transparency & Haze Transparency, % EC/Silicone: Rth 600 500 Rth(60um), nm Rth-exp 500 9 0 EC EC/Silicone: Rth 600 400 300 100 5.0 80 4.0 60 3.0 40 2.0 20 1.0 0 0.0 0 200 Haze, % 2 Rth(60um), nm Ro(60um), nm 5 silicone polymer. By comparison of the experimental data with the ideal physical blending hypothesis for Rth, the actual Rth decreases much faster than hypothetic data. This fast decrease of Rth might be caused by the strong interaction between the blending polymers, which weakens the orientation of ethyl cellulose to an isotropic status. Rth(60um), nm 3. RESULTS AND DISCUSSION 5 10 20 30 40 50 70 Silicone ratio in total solid, % 100 R² = 0.9995 0 0 20 40 60 Fig. 4 Film transparency and haze 80 Silicone ratio in total solid, % Fig. 2 Rth of EC films with additives Although Rth doesn’t decrease linearly with silicone ratio across the whole range from 0% to 70%, it was found that Rth first decreases linearly with the increase of the blending ratio of silicone from 0% to 40%, as shown in Figure 3. The linear relationship between Rth and blending ratio reflects the good miscibility of ethyl cellulose and 500 IDW/AD ’12 Refractive index is a critical parameter to high transparency and low reflection of films. As shown in Figure 5, the refractive index of EC/Silicone films is very similar to pure ethyl cellulose film and only slightly increases with blending ratio of silicones. The similar refractive index of ethyl cellulose and silicone resin and continuous variation with the blending ratio further supports the excellent miscibility of ethyl cellulose and silicone resins. In Plane Retardation: Ro 1.520 1.510 1.500 1.490 1.480 1.470 1.460 Ro, nm (60um thickness) Refractive Index EC/Silicone: Refraction Index R² = 0.9896 0 20 40 60 80 500 400 300 200 100 0 0 20 100 R² =60 0.9885 80 40 100 Stretching ratio, % Silicone blending ratio, % Fig. 7 Stretching on Ro properties Fig. 5 Film refraction index Ro needs to be lower than 10 nm in IPS mode LCD retardation films, so EC/Silicone blend film can meet Ro/Rth requirements in IPS mode LCD very well. However, in VA mode and TN mode LCD retardation films need a larger Ro such as 50nm, 125 nm, or higher. Usually, the large Ro comes from in-plane refractive index difference which is achieved by thermal stretching of TAC, PC, and COP films. In this study, film thermal stretching was also tried to confirm the Ro adjustment capability for ethyl cellulose films. In LCD displays, three colors of light with different wavelength will pass through retardation films and other films associated with the polarizer. So, flat wavelength dispersion is preferred for retardation film to avoid color shifting. As shown in Figure 8, the EC/Silicone blend film shows flat wavelength dispersion, which is similar to the COP film and much smaller than PC and TAC retardation films. The VA TAC reference film shows reverse wavelength dispersion, which might be induced by additives. As shown in Figure 6, stretched films become white in cross section polarizing light, while the unstretched part at each edge of the film is still black, which means the stretching is effective to increase Ro of EC/Silicone films. Ro/Ro(590) Wavelength dispersion 1.1 1.08 1.06 1.04 1.02 1 0.98 0.96 0.94 EC/Silicone VA TAC 1/4ʄPC 1/4ʄCKP 400 500 600 700 800 Wavelength, nm Fig. 8 Wavelength Dispersion Fig. 6 Stretched film under cross polarizing light Ro is tested by using Kobra birefringence analyzer. As shown in Figure 7, Ro of the films increase linearly with the stretching ratio from 0% to 100%. An Ro of 50 nm for VA mode LCDs will be achieved at stretching ratio of 10% and 125 nm Ro for TN mode 3D LCDs will be achieved at stretching ratio of 26%. Higher Ro can be achieved via higher stretching ratio for various TN mode LCD applications. 4. CONCLUSION In this study, ethyl cellulose based optical films are reported for their high out-of-plane retardation and tunable optics including Ro and Rth. The out-of-plane retardation of blend films, based on a normal 60 μm thickness, is tunable from 470 nm to 1 nm. The EC blend films are also capable of increasing Ro from 0 nm to more than 400 nm via mechanical stretching technology. The tunable optics of EC blends make it a viable compensation film for various LCD modes including VA mode, IPS mode, and TN/STN mode as well as a conventional polarizer protection film. Moreover, ethyl cellulose based films show flat wavelength dispersion properties which are helpful to reduce the color shift. Furthermore, the high transparency and low haze IDW/AD ’12 501 properties provide ethyl cellulose based films huge potential in high-end optical film applications. REFERENCES [1] S. Nimura, et. al, US20070184212, Fujifilm Corporation, 2007 [2] H. Takeuchi, et.al, EP1369713A1, FUJI PHOTO FILM CO LTD, 2003 [3] S. Yoshikawa, et. al, JP2006113500A, FUJI PHOTO FILM CO LTD, 2006 [4] Y. Kaneko, et. al, JP2009122172A, KONICA 502 IDW/AD ’12 MINOLTA OPTO INC, 2007 [5] M. Tsukamotot, et. al, JP 2009251530, Kaneka Corporation, 2011 [6] S. Fujii, JP2003096207, Kanegafuchi Chemical Ind, 2011 [7] J. M. Choi, KR2012015612, LG, 2012
© Copyright 2026 Paperzz