We have investigated the physical and optical properties of the left-handed chiral dopant ZLI-811 mixed in a nematic liquid crystal (LC) host BL006. The solubility of ZLI-811 in BL006 at room temperature is ~24 wt%, but can be enhanced by increasing the temperature. Consequently, the photonic band gap of the cholesteric liquid crystal (CLC) mixed with more than 24 wt% chiral dopant ZLI-811 is blue shifted as the temperature increases. Based on this property, we demonstrate two applications in thermally tunable band-pass filters and dye-doped CLC lasers.
© 2006 Optical Society of America
Cholesteric liquid crystal (CLC) is a simple one-dimensional photonic crystal and has many interesting applications because of their unique properties and simple fabrication process [1–4]. A CLC is formed by rod-like molecules whose directors are self-organized in a helical structure. In the planes perpendicular to the helical axis, the LC directors are continuously rotated along the helical axis. By choosing a high birefringence LC, the periodic helical structure gives rise to a periodic modulation of the refractive index, which results in a selective reflection band. Within the band, the circularly polarized incident light with the same handedness as the cholesteric helix is reflected while the opposite handedness is transmitted. The frequency range of the reflection band is determined by the ordinary (no) and extraordinary (ne) refractive indices of the LC, and the pitch length (p) of the helical structure. The reflection band edges occur at λ1=nop and λ2 = nep, where p is the helical pitch length.
A CLC cell is typically prepared by doping some chiral agents into a nematic liquid crystal mixture. The fabrication process is quite simple. Moreover, the electromagnetic characteristics of CLC photonic band gap (PBG) can be easily controlled by adjusting the LC or chiral parameters, or by adjusting the external factors such as temperature, pressure, light irradiation, or electric field [4–10]. For example, the CLC PBG can be switched on and off by an electric field, which can be used as a bistable light shutter . The frequency range of the PBG can be varied by irradiating the CLC sample with a UV light, which has been demonstrated for tunable laser applications [7, 8]. In addition, temperature has also been widely used to modify the CLC PBG’s frequency range [9–11]. In most cases, the modification of the CLC PBG’s frequency by temperature is based on the dependency of the LC’s phase transition or the temperature-dependent birefringence [10, 11].
In this paper, we demonstrate a thermally tunable CLC PBG based on the temperature dependent solubility of the chiral dopant. As the temperature increases, the dopant’s solubility increases which, in turn, shortens the pitch length and leads to a blue shift in the reflected spectrum. Based on this property, thermally tunable band-pass filters and dye-doped CLC lasers are demonstrated. Different from prior approaches, our method is mainly based on the temperature dependent chiral solubility in the LC host, rather than the temperature dependent refractive index change [11, 12]. We find that our method is ~600X more sensitive.
2. Sample preparation
In experiment, several different CLC mixtures were prepared by doping a left-handed chiral agent ZLI-811 into BL006 and ZLI-4608 (both are Merck mixtures). The dopant concentration varies from 22 to 36 wt% by 2% interval. The refractive indices for BL006 are ne=1.816 and no=1.530 and for ZLI-4608 are ne=1.656 and no=1.499 at T=20 °C and λ=589 nm. The mixtures were stirred in isotropic phase at ~120 °C for ~4h to make the constituents uniformly mixed and then capillary filled into a 10 μm gap LC cell in the isotropic phase. The inner surfaces of the glass substrates were coated with a thin polyimide alignment layer and rubbed in anti-parallel directions. The pretilt angle is ~3°. After the temperature was gradually cooled down to room temperature, a CLC sample with left-handed (LH) helix was formed.
3. Results and discussion
First, we compared the optical properties of the CLC samples prepared in the BL006 host versus those in the LC ZLI-4608 host. The transmission spectra of the CLC samples were measured using a spectrophotometer. Here, we just take two CLC mixtures with 22 wt% ZLI-811 in BL006 and ZLI-4608 as examples to illustrate the host LC effect on the PBG. Results are plotted in Fig. 1. Although the two CLC samples contain the same concentration of ZLI-811, their PBGs occur at different spectral range and their bandwidth is also different because of the different refractive indices and birefringence of the LC hosts. Since ZLI-4608 has a smaller no and Δn than BL006, under the same chiral concentration, its CLC PBG occurs at a shorter wavelength and its bandwidth is narrower. According to the PBG transmission spectrum, we can calculate the helical pitch length (P) and the helix twist power (HTP) of ZLI-811 in the two different LC hosts using the following equations :
where λo is the central wavelength of the photonic bandgap, n = (ne + no)/2 is the average refractive index, and C is the chiral concentration. The pitch length and helix twist power of ZLI-811 are calculated to be [404.47 nm, 10.30 μm-1] and [394.39 nm, 10.56 μm-1] for the BL006 and ZLI-4608 hosts, respectively.
From the PBG transmission spectrum, we extracted the central wavelength by averaging the wavelength of the PBG at the short and long edges. Figure 2 shows the dependence of the central wavelength of the PBG on the chiral dopant concentration. The symbols are the experimental results and the solid lines are the simulation results based on the following relationship:
From Fig. 2, the experimental results agree with theory quite well for the ZLI-4608 host. As the dopant concentration increases, the central reflection wavelength decreases according to Eq. (3). However, a big discrepancy occurs for the BL006 samples as the dopant concentration exceeds 24 wt%. To understand this discrepancy, we studied the temperature effect on the PBG of the BL006-based CLC samples with more than 24 wt% chiral ZLI-811.
Figure 3 shows the temperature dependent PBG’s central wavelength for the BL006-based CLC samples with 26, 30, 32, and 34 wt% of chiral ZLI-811. As the temperature increases, the central wavelength of the CLCs’ PBG is clearly blue shifted. The blue shift of a CLC with a lower chiral dopant concentration saturates at a lower temperature and, moreover, its final PBG appears at a longer wavelength than those with a higher chiral concentration. When the blue shift of the PBG is stopped, the central wavelength of the PBG follows the chiral concentration according to Eq. (3). This indicates that at room temperature, 26 wt% of ZLI-811 is already beyond its maximum solubility in BL006. Further increasing the chiral concentration would make a portion of ZLI-811 molecules to precipitate from the BL006 host and aggregate. The aggregation might attract some chiral molecules from the LC host which, in turn, results in a lower effective chiral concentration and consequently a red shift. As a result, the PBG shifts toward a longer wavelength, as shown in Fig. 2. Since a higher temperature enhances the solubility of the chiral dopant in the LC which shortens the pitch length of the CLC’s helix, the PBG of CLCs produces blue shift as the temperature increases. A higher concentration of ZLI-811 needs a higher temperature to be totally dissolved in the BL006 LC host.
To show the phase separation and aggregation of ZLI-811 from BL006, we took the images of the CLC samples under a polarizing optical microscope. Figure 4(a) shows the microscopic photos of the CLCs doped with different chiral concentration in BL006 at room temperature (T~23 °C). It is difficult to see the phase separation when the chiral concentration is below 30 wt%. However, when the chiral concentration is above 32 wt%, the phase separation is quite distinct. For example, the 34 wt% ZLI-811 CLC sample no longer exhibits a planar cholesteric structure; instead, most part of the sample is enclosed by chain-like structures. The sample is not transparent but scatters light. The chain-like structures are induced by the phase separation and aggregation of the chiral molecules from BL006. As the temperature is increased to ~26.5 °C, the sample starts to become transparent again because more chiral molecules are dissolved in BL006. Further increasing the temperature makes the sample more and more transparent and the planar helical structure more uniform, as Fig. 4(b) shows.
4. Photonic applications
This temperature dependent CLC PBG property can be used for tuning the band pass of a filter. Here, we take the CLC sample with 34 wt% chiral dopant ZLI-811 in the BL006 host as an example to demonstrate the potential applications. Results are illustrated in Fig. 5.
Figure 5 shows the reflected color of the CLC captured by a digital camera at different temperatures. The reflected color of the CLC sample changes from red to blue as the temperature is increased from 30 °C to 50 °C. Since this CLC sample has left-handed helix, it is only useful for left circular polarization. We can obtain polarization independent bandpass filter by stacking two CLC samples with left- and right-handed helixes.
The most attractive application of the temperature dependent CLC PBG property is for tunable laser applications by doping some laser dyes into the CLC mixture. To demonstrate the thermally tunable laser application, we added 1 wt% of laser dye 4-(dicyanomethylene)-2-methyl-6-(4-dimethylaminostryl)-4H-pyran (DCM, Exciton) into the CLC mixture with 34 wt% chiral dopant ZLI-811 and then injected the well mixed dye doped CLC mixtures into an 8 μm LC cell. Figure 6 shows the normalized laser emission spectra from the dye doped CLC sample under the excitation of ~16 μJ pulse energy from a second-harmonic Nd:YAG laser at λ=532 nm with 4 ns pulse width and 1 Hz repetition rate. The lasing wavelength with ~1 nm linewidth can be tuned from 645 nm to 580 nm by merely changing the sample temperature from 26.2 °C to 28.7 °C. The lasing intensity strongly depends on the lasing wavelength, as shown in Fig. 6. The highest lasing intensity occurs at ~605 nm. For the lasing wavelengths away from 605 nm, the lasing intensity is reduced. For the same pump energy, the laser intensity is determined by the combination of the optical gain and losses in the medium. Higher laser intensity can be generated from the medium with larger optical gain and lower losses. The optical gain is determined by the fluorescence of the dye. The optical losses include the optical absorption, scattering and other facts. Although the DCM dye exhibits its maximum fluorescence at A. λ ~ 592 nm, the highest lasing intensity occurs at λ ~ 605 nm not ~592 nm due to the optical losses induced by the absorption and scattering, etc .
The temperature dependent lasing wavelengths in Fig. 6 seem inconsistent with the temperature dependent PBG of the CLC without dye as shown in Fig. 3. We have to point out that the dye used in this experiment enhances the solubility of the chiral in the mixture. From Fig. 6, as the temperature increases the lasing wavelength shifts towards a shorter wavelength due to the increase of dissolved chiral concentration. However, when the temperature is above a certain value, the slope of the shifted wavelength range over the temperature is decreased with the increased temperature, as seen in Fig. 3 and Fig. 6. The reason is that when the temperature is increased to a certain value, most of the chiral molecules are already dissolved in the LC mixture and very few chiral molecules are spared for the further temperature increase. The average change of the CLC PBG’s central wavelength reaches 26 nm/°C. In comparison, if we tune the CLC PBG using the temperature dependent refractive index, the calculated change is only 0.05 nm/°C . Our method is ~600X more sensitive.
We have investigated the physical and optical properties of the chiral agent ZLI-811 doped in the BL006 LC host. The solubility of ZLI-811 in BL006 is limited to 24 wt%. Excessive dopant would result in precipitation and aggregation which leads to light scattering. However, the solubility of ZLI-811 in BL006 can be enhanced by raising the temperature. Since a higher chiral dopant concentration can reduce the pitch length of the helix, the photonic band gap of the cholesteric liquid crystal mixed with more than 24 wt% chiral dopant ZLI-811 is blue shifted with the increase of the temperature. Its applications in thermally tunable band pass filters and mirrorless lasers have been demonstrated. Compared to the thermally tunable CLC PBG based on the temperature dependent refractive index change, our method is ~600X more sensitive.
References and links
1. C. Y. Huang, K. Y. Fu, K. Y. Lo, and M. S. Tsai, “Bistable transflective cholesteric light shutters,” Opt. Express 11, 560–565 (2003). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-11-6-560 [CrossRef] [PubMed]
2. F. Du, Y. Q. Lu, H. W. Ren, S. Gauza, and S. T. Wu, “Polymer-stabilized cholesteric liquid crystal for polarization-independent variable optical attenuator,” Jpn. J. Appl. Phys. Part 1 , 43, 7083–7086 (2004). [CrossRef]
3. B. Taheri, A. F. Munoz, P. Palffy-Muhoray, and R. Twieg, “Low threshold lasing in cholesteric liquid crystals,” Mol. Cryst. Liq. Cryst. 358, 73–81, (2001). [CrossRef]
4. M. Iwamoto, C. X. Wu, and Z. C. Ou-Yang, “Separation of chiral phases by compression: kinetic localization of the enantiomers in a monolayer of racemic amphiphiles viewed as mixing cholesteric liquid crystals,” Chem. Phys. Lett. 285, 306–312 (1998). [CrossRef]
5. N. Scaramuzza, C. Ferrero, B. V. Carbone, and C. Versace, “Dynamics of selective reflections of cholesteric liquid crystals subject to electric fields,” J. Appl. Phys. 77, 572–576 (1995). [CrossRef]
6. X. Y. Huang, D. K. Yang, and J. W. Doane, “Transient dielectric study of bistable reflective cholesteric displays and design of rapid drive scheme,” App. Phys. Lett. 67, 1211–1213 (1995). [CrossRef]
7. S. Furumi, S. Yokoyama, A. Otomo, and S. Mashiko, “Pototunable photonic bandgap in a chiral liquid crystal laser device,” Appl. Phys. Lett. 84, 2491–2493 (2004). [CrossRef]
8. A. Chanishvili, G. Chilaya, G. Petriashvili, R. Barberi, R. Bartolino, G. Cipparrone, A. Mazzulla, and L. Oriol, “Phototunable lasing in dye-doped choelsteric liquid crystals,” Appl. Phys. Lett. 83, 5353–5355 (2003). [CrossRef]
9. I. Musevic, M. Skarabot, G. Heppke, and H. T. Nguyen, “Temperature dependence of the helical period in the ferrielectric smectic phases of MHPOBC and 10OTBBB1M7,” Liq. Cryst. 29, 1565–1568 (2002). [CrossRef]
10. F. Zhang and D. K. Yang, “Temperature dependence of pitch and twist elastic constant in a cholesteric to smectic A phase transition,” Liq. Cryst. 29, 1497–1501 (2002). [CrossRef]
11. S. M. Morris, A. D. Ford, M. N. Pivnenko, and H. J. Coles, “Enhanced emission from liquid-crystal lasers,” J. Appl. Phys. 97, 023103 (2005). [CrossRef]
12. J. Li, S. Gauza, and S. T. Wu, “Temperature effect on liquid crystal refractive indices,” J. Appl. Phys. 96, 19–24 (2004). [CrossRef]
13. G. Gottarelli and G. P. Spada, “Induced cholesteric mesophases ‒ origin and applications” Mol. Cryst. Liq. Cryst. 123, 377–388 (1985). [CrossRef]
14. Y. Huang, Y. Zhou, and S. T. Wu, “Spatially tunable lasing emission in dye-doped photonic liquid crystals,” Appl. Phys. Lett. 88, 011107 (2006). [CrossRef]