**4.1 AZ-containing amorphous polymers**

Low-molecular-weight AZ materials are superior in terms of mobility. However, it is often difficult to prepare holographic gratings with narrow fringe spacing (i.e., high resolution) and high stability because of the high mobility of AZ molecules with low molecular weight. From the application point of view, AZ-containing polymer materials might be one of the best choices for holograms because of their simple processability and high stability. On the other hand, the ordered structures or photoinduced alignment of chromophores can be easily fixed in polymer matrix.

In 1995, two groups independently reported surface-relief gratings inscribed in AZcontaining polymer materials almost at the same time (Rochon et al., 1995 ; Kim et al., 1995).

Because of easy preparation and high purity of low-molecular-weight compounds, the application of AZ materials for recording holograms began with them. Formation of holographic gratings in films of poly(vinyl alcohol) doped with low-molecular-weight AZ compounds was first reported by utilizing photoisomerization of AZs (Todorov et al., 1983, 1984, 1985). The holographic gratings recorded in the polymer-based samples were selfdeveloping and auto-erasing or re-writable since the thermally induced back isomerization of AZs could be easily obtained (Pham et al., 1997). To increase the formed birefringence |n2 n1| shown in Figure 2 and enhance the performance of recorded holograms, polymerdispersed AZ-containing low-molecular-weight LC compounds were also employed as recording media (Tondiglia et al., 1995). Due to the existence of low-molecular-weight LCs, the diffraction efficiency of the gratings could be electrically controlled (Sutherland et al., 1994). Moreover, dynamic holography was achieved in AZ-doped nematic LCs (Chen &

Although many research focused on the low-molecular-weight AZ–doped polymers, the stability of the induced anisotropy was low. To improve stability of the recorded gratings, molecular glasses fabricated with low-molecular-weight AZ compounds were developed (Shirota et al., 1998). This kind of materials can form stable amorphous and homogenous films without scattering of visible light (Nakano et al., 2002). Surface-relief gratings were successfully inscribed although the AZ derivatives were confined in the glassy sates. More interestingly, low-molecular-weight AZ crystals and co-crystals also showed capability of formation of surface-relief gratings (Nakano et al., 2005). It was believed that photoreaction

For holograms recorded in low-molecular-weight AZ materials, gain effect often occurs. It was reported that diffraction efficiency of gratings recorded in calamitic LC materials with low-molecular-weight compounds was increased sharply after annealing (Stracke et al., 1999). In recording holograms using pentaalkinylbenzene derivatives, a strong gain effect was obtained by the selective growth of crystals in the non-irradiated areas (Frese et al., 2003). For smectic trisazomelamine, the gain effect was acquired accompanied by the growth of surface modulation. At elevated temperatures, the free volume available to mesogens increased and the thermal movement led to a collective orientation along the direction given by those groups pre-aligned by the recording beams. This caused an increase of the order degree in the pre-orientated domain, which contributed to the increase of

Low-molecular-weight AZ materials are superior in terms of mobility. However, it is often difficult to prepare holographic gratings with narrow fringe spacing (i.e., high resolution) and high stability because of the high mobility of AZ molecules with low molecular weight. From the application point of view, AZ-containing polymer materials might be one of the best choices for holograms because of their simple processability and high stability. On the other hand, the ordered structures or photoinduced alignment of chromophores can be

In 1995, two groups independently reported surface-relief gratings inscribed in AZcontaining polymer materials almost at the same time (Rochon et al., 1995 ; Kim et al., 1995).

**3. Low-molecular-weight AZs** 

Brady, 1993).

only occurred in the surface.

diffraction efficiency of holograms.

**4.1 AZ-containing amorphous polymers** 

**4. AZ-containing polymers** 

easily fixed in polymer matrix.

In films of poly[4'-( 2-acryloxy)ethylamino-4-nitroazobenzene] (pDR1A, Figure 5a), surfacerelief gratings with a sinusoidal shape was recorded with an interference pattern of two light beams at 514 nm. The obtained grating structures were stable but could be erased by heating the polymer above its glass transition temperature. In addition, no permanent damage of the lm was observed. Multiple gratings can be simultaneously written and gratings can be overwritten (Rochon et al., 1995). Using an epoxy-based amorphous polymer containing AZ side groups (Figure 5b), surface-relief gratings with relatively large amplitude was successfully inscribed with two laser beams at 488 nm. Furthermore, recording perpendicular gratings on the same lm was also achieved. Such surface-relief gratings in amorphous polymer films showed uniform and controllable morphologies, like the depth of relief, the grating periodicity, and so son. Moreover, more complicated topological surfaces were tailored by superimposing several surface-relief gratings. Recently, the recorded surface-relief structures were studied for potential applications as LC alignment (Li et al., 1999), polarization discriminator, waveguide couplers (Viswanathan et al., 1999) and antireflective coatings (Natansohn & Rochon, 2002).

Fig. 5. Surface-relief gratings recorded in AZ-containing amorphous polymer materials.

Azobenzene-Containing Materials for Hologram 103

In a nematic LC polymer with AZs as side mesogens, both surface relief and refractive index modulations were recorded, as shown in Figure 7. In nematic LC phase, the obtained gratings exhibited a higher diffraction efficiency than that recorded in the glassy state even though the amplitude of surface-relief structures of the former was lower than that of the latter one (Yamamoto et al., 1999). These indicated that the contribution of refractive-index gratings to the diffraction efficiency was larger than that of surface-relief gratings. Based on the same materials, holographic image storage using a photomask as an object was

To enhance the refractive-index modulation, both cyanobiphenyl and tolane groups were used as photoinert moieties to prepare LC copolymers with AZs as photoresponsive mesogens (Yoneyama et al., 2001, 2002). However, the photoresponse was not high enough due to a low content of AZ moieties in the copolymers. To improve the photosensitivity and induce a larger birefringence for holographic applications, a concept of molecular architecture of AZ–containing LC materials was proposed in Figure 8 (Okano et al., 2005). A tolane group was directly attached onto the 4– or 4'– position of AZ molecules to prepare an azotolane mesogen, which shows far longer molecular conjugation length than one single tolane group or an AZ moiety (Okano et al., 2005). Figure 8 lists the molecular structures and LC phase behaviors of a series of azotolane nematic LC polymers synthesized based on this principle, in which three, four and five benzene rings are included in the mesogens, respectively. All the prepared azotolane-containing LCPs showed a wide nematic LC range and exhibited a phase transition temperature higher than 200 °C (Okano et al., 2006). Obviously, the photoresponse of the designed LC polymer with high birefringence was greatly enhanced because of high density of AZ mesogens, resulting in formation of holographic grating in thin films within short time under low-intensity irradiation of

Fig. 7. Holographic gratings recorded in nematic LC polymer with AZs as side mesogens.

successfully obtained (Yamamoto et al., 2000).

recording beams.

#### **4.2 AZ-containing LC polymers**

Comparing with amorphous materials, LC materials possess unique features like selforganization, fluidity with long–range order, molecular cooperative motion, formed large birefringence and anisotropy in various physical properties (optical, mechanical, electrical and magnetic), and alignment change induced by external fields at surfaces and interfaces (Ikeda, 2003; Yu & Kobayashi, 2010). Therefore, LC materials can bring about a larger change in refractive index relative to amorphous ones. An alignment change of LC materials in a periodic fashion can be easily induced upon irradiation with interference patterns by overlapping two coherent beams, resulting in a large refractive-index modulation. This can contribute to a high diffraction efficiency of recorded gratings. In films of AZ-containing LC polymers, both surface-relief and refractive-index gratings can be recorded correspondingly.

Wendorff et al. showed that holographic gratings could be inscribed in LC polymers composed of AZ moieties and photoinert mesogenic groups (Eich et al., 1987; Eich & Wendorff, 1987; Anderle & Wendorff, 1994). Hvilsted et al. achieved holographic gratings with diffraction efficiencies of about 40% in AZ-containing LC polyesters (Hvilsted et al., 1995). Recently, formation of holographic gratings in side-chain LC polymers containing AZ moieties by means of photochemical phase transition was intensively studied. Hasegawa et al. achieved dynamic holographic gratings by means of photochemical nematic-to-isotropic phase transition in LC copolymers containing an AZ moiety with strong donor-acceptor substituents in side chain (pseudostilbene-type AZs in Figure 3). As shown in Figure 6, the inscription and removal of holographic gratings with a narrow fringe spacing of 1.4 μm was obtained within 150 and 190 ms, respectively (Hasegawa et al., 1999a , 1999b). Moreover, the optical switching behaviors of the holographic diffraction were observed repeatedly by turning the writing beams on and off. Using a siloxane group as a spacer in preparation of LC polymers decreased the glass transition temperature of the designed materials. This was because of the flexibility of the siloxane unit, which resulted in an effectively photoinduced nematic-to-isotropic phase transition at room temperature and formation of real-time holographic gratings (Hasegawa et al., 1999c).

Fig. 6. Dynamic holographic gratings by means of photochemical phase transition in AZcontaining LC polymers.

Comparing with amorphous materials, LC materials possess unique features like selforganization, fluidity with long–range order, molecular cooperative motion, formed large birefringence and anisotropy in various physical properties (optical, mechanical, electrical and magnetic), and alignment change induced by external fields at surfaces and interfaces (Ikeda, 2003; Yu & Kobayashi, 2010). Therefore, LC materials can bring about a larger change in refractive index relative to amorphous ones. An alignment change of LC materials in a periodic fashion can be easily induced upon irradiation with interference patterns by overlapping two coherent beams, resulting in a large refractive-index modulation. This can contribute to a high diffraction efficiency of recorded gratings. In films of AZ-containing LC polymers, both surface-relief and refractive-index gratings can

Wendorff et al. showed that holographic gratings could be inscribed in LC polymers composed of AZ moieties and photoinert mesogenic groups (Eich et al., 1987; Eich & Wendorff, 1987; Anderle & Wendorff, 1994). Hvilsted et al. achieved holographic gratings with diffraction efficiencies of about 40% in AZ-containing LC polyesters (Hvilsted et al., 1995). Recently, formation of holographic gratings in side-chain LC polymers containing AZ moieties by means of photochemical phase transition was intensively studied. Hasegawa et al. achieved dynamic holographic gratings by means of photochemical nematic-to-isotropic phase transition in LC copolymers containing an AZ moiety with strong donor-acceptor substituents in side chain (pseudostilbene-type AZs in Figure 3). As shown in Figure 6, the inscription and removal of holographic gratings with a narrow fringe spacing of 1.4 μm was obtained within 150 and 190 ms, respectively (Hasegawa et al., 1999a , 1999b). Moreover, the optical switching behaviors of the holographic diffraction were observed repeatedly by turning the writing beams on and off. Using a siloxane group as a spacer in preparation of LC polymers decreased the glass transition temperature of the designed materials. This was because of the flexibility of the siloxane unit, which resulted in an effectively photoinduced nematic-to-isotropic phase transition at room temperature and formation of real-time

Fig. 6. Dynamic holographic gratings by means of photochemical phase transition in AZ-

**4.2 AZ-containing LC polymers** 

be recorded correspondingly.

holographic gratings (Hasegawa et al., 1999c).

containing LC polymers.

In a nematic LC polymer with AZs as side mesogens, both surface relief and refractive index modulations were recorded, as shown in Figure 7. In nematic LC phase, the obtained gratings exhibited a higher diffraction efficiency than that recorded in the glassy state even though the amplitude of surface-relief structures of the former was lower than that of the latter one (Yamamoto et al., 1999). These indicated that the contribution of refractive-index gratings to the diffraction efficiency was larger than that of surface-relief gratings. Based on the same materials, holographic image storage using a photomask as an object was successfully obtained (Yamamoto et al., 2000).

To enhance the refractive-index modulation, both cyanobiphenyl and tolane groups were used as photoinert moieties to prepare LC copolymers with AZs as photoresponsive mesogens (Yoneyama et al., 2001, 2002). However, the photoresponse was not high enough due to a low content of AZ moieties in the copolymers. To improve the photosensitivity and induce a larger birefringence for holographic applications, a concept of molecular architecture of AZ–containing LC materials was proposed in Figure 8 (Okano et al., 2005). A tolane group was directly attached onto the 4– or 4'– position of AZ molecules to prepare an azotolane mesogen, which shows far longer molecular conjugation length than one single tolane group or an AZ moiety (Okano et al., 2005). Figure 8 lists the molecular structures and LC phase behaviors of a series of azotolane nematic LC polymers synthesized based on this principle, in which three, four and five benzene rings are included in the mesogens, respectively. All the prepared azotolane-containing LCPs showed a wide nematic LC range and exhibited a phase transition temperature higher than 200 °C (Okano et al., 2006). Obviously, the photoresponse of the designed LC polymer with high birefringence was greatly enhanced because of high density of AZ mesogens, resulting in formation of holographic grating in thin films within short time under low-intensity irradiation of recording beams.

Fig. 7. Holographic gratings recorded in nematic LC polymer with AZs as side mesogens.

Azobenzene-Containing Materials for Hologram 105

Using two phase-type gratings recorded in LC cells (Figure 9), grating waveguide couplers with a at surface were fabricated as shown in Figure 9 (Bang et al., 2007). When a probe beam at 633 nm was incident to one grating, the beam propagated in the waveguide and an output beam came out from the other grating with the throughput coupling efficiency of about 5%. Upon irradiation of the lm between the two gratings with UV light to cause trans–cis photoisomerization and order-disorder transition of the AZ moiety, the intensity of the output beam was repeatedly switched upon alternating irradiation of visible light. It was found that the alternating irradiation at 366 and 436 nm induced reversible changes in the

Fig. 9. Periodically flat-structured grating waveguide couplers and photo-switching

Due to molecular cooperative motion of mesogens in LC polymers, it is difficult to record holographic gratings with a narrow periodicity in a subwavelength scale (Yu et al., 2008a). Pre-treatment with UV irradiation to induce cis-azobenzene-rich isotropic phase can illiminate such molecular cooperative effect of mesogens and enhance the photoresponse in an a lowly viscous state. These enabled us to obtain the subwavelength modulation of surface relief and refractive index with interference patterns in Figure 10 (Yu et al., 2008a). The surface relief of less than 10 nm and the refractive-index modulation were detected by atomic force microscopy in tapping and phase modes, respectively. A large phase retardation and formed birefringence were observed in the recorded subwavelength

intensity of the output beam.

behaviors.

gratings.

Fig. 8. Azotolane LC polymers with high birefringence for holograms.

Fig. 8. Azotolane LC polymers with high birefringence for holograms.

Using two phase-type gratings recorded in LC cells (Figure 9), grating waveguide couplers with a at surface were fabricated as shown in Figure 9 (Bang et al., 2007). When a probe beam at 633 nm was incident to one grating, the beam propagated in the waveguide and an output beam came out from the other grating with the throughput coupling efficiency of about 5%. Upon irradiation of the lm between the two gratings with UV light to cause trans–cis photoisomerization and order-disorder transition of the AZ moiety, the intensity of the output beam was repeatedly switched upon alternating irradiation of visible light. It was found that the alternating irradiation at 366 and 436 nm induced reversible changes in the intensity of the output beam.

Fig. 9. Periodically flat-structured grating waveguide couplers and photo-switching behaviors.

Due to molecular cooperative motion of mesogens in LC polymers, it is difficult to record holographic gratings with a narrow periodicity in a subwavelength scale (Yu et al., 2008a). Pre-treatment with UV irradiation to induce cis-azobenzene-rich isotropic phase can illiminate such molecular cooperative effect of mesogens and enhance the photoresponse in an a lowly viscous state. These enabled us to obtain the subwavelength modulation of surface relief and refractive index with interference patterns in Figure 10 (Yu et al., 2008a). The surface relief of less than 10 nm and the refractive-index modulation were detected by atomic force microscopy in tapping and phase modes, respectively. A large phase retardation and formed birefringence were observed in the recorded subwavelength gratings.

Azobenzene-Containing Materials for Hologram 107

the diffraction efficiency increased to about 9.0 %, almost two orders of magnitude larger than the diffraction efficiency before annealing. This increased diffraction efficiency might be ascribed mainly to the enhancement of surface modulation. Furthermore, multi-processes of the refractive-index gratings were successfully achieved as presented in Figure 11. The obtained grating structures were clearly observed in the polarizing optical microscopic pictures, which

Fig. 11. Holographic gratings recorded in AZ-containing LC block copolymers with well-

defined structures and enhancement of gratings upon microphase separation.

were also verified by their diffraction patterns (Yu et al., 2007a).

Fig. 10. Subwavelength modulation of surface relief and refractive index in LC polymer films.

### **4.3 AZ-containing LC block polymers with well-defined structures**

In LC block copolymers with well-defined structures, microphase separation often occurs because of the inherent immiscibility of the different blocks, resulted in diverse of nanostructures like nanospheres and nanocylinders (Yu et al., 2006a, 2006b, 2007d, 2007e, 2009b, 2011; Chen et al., 2010b). Generally, the phase-segregated nano domains are far smaller than the wavelength of the visible light (Yu et al., 2007b, 2007c), making it possible to get rid of the scattering effect. Such kinds of AZ-containing LC block polymers with nanoscale phase separation have been regarded as one of ideal materials candidates for holograms.

Generally, the diffraction efficiency is one of the most important parameters for holographic gratings. In amorphous polymer materials, a surface–relief grating contributes mainly to diffraction efficiency. Recently, microphase separation of AZ-containing LC block copolymers was used to control diffraction efficiency by enhancement of surface relief upon thermal annealing (Yu et al., 2005a, 2009a; Naka et al., 2009). As shown in Figure 11, both surface-relief and refractive–index gratings were recorded upon irradiation of an interference pattern, in which selective photoisomerization and the isotropic–to–LC phase transition were induced in the bright areas of pre-treated films. The diffraction efficiency of the gratings depended strongly on the polarization of the reading beam because of the photoalignment of mesogens in the bright area of the writing patterns. After grating formation, the surface-relief structures with a sinusoidal shape were clearly observed in the AFM images (Figure 11). The fringe spacing of the surface relief was 2.0 μm, which was identical to that of the refractive-index gratings. Then nanoscaled microphase separation was proceeded by annealing the grating sample. As a result, the surface relief was increased to about 110 nm (18.3 % of the film thickness), almost one order of magnitude larger than that before annealing. The peak-to-valley contrast became more explicit after annealing, due to the enhancement of the surface modulation. Furthermore, the sinusoidal shape of the surface profile became a little irregular, indicating that the LC alignment was disturbed upon microphase separation. Together with the enhancement of surface relief,

Fig. 10. Subwavelength modulation of surface relief and refractive index in LC polymer

In LC block copolymers with well-defined structures, microphase separation often occurs because of the inherent immiscibility of the different blocks, resulted in diverse of nanostructures like nanospheres and nanocylinders (Yu et al., 2006a, 2006b, 2007d, 2007e, 2009b, 2011; Chen et al., 2010b). Generally, the phase-segregated nano domains are far smaller than the wavelength of the visible light (Yu et al., 2007b, 2007c), making it possible to get rid of the scattering effect. Such kinds of AZ-containing LC block polymers with nanoscale phase

Generally, the diffraction efficiency is one of the most important parameters for holographic gratings. In amorphous polymer materials, a surface–relief grating contributes mainly to diffraction efficiency. Recently, microphase separation of AZ-containing LC block copolymers was used to control diffraction efficiency by enhancement of surface relief upon thermal annealing (Yu et al., 2005a, 2009a; Naka et al., 2009). As shown in Figure 11, both surface-relief and refractive–index gratings were recorded upon irradiation of an interference pattern, in which selective photoisomerization and the isotropic–to–LC phase transition were induced in the bright areas of pre-treated films. The diffraction efficiency of the gratings depended strongly on the polarization of the reading beam because of the photoalignment of mesogens in the bright area of the writing patterns. After grating formation, the surface-relief structures with a sinusoidal shape were clearly observed in the AFM images (Figure 11). The fringe spacing of the surface relief was 2.0 μm, which was identical to that of the refractive-index gratings. Then nanoscaled microphase separation was proceeded by annealing the grating sample. As a result, the surface relief was increased to about 110 nm (18.3 % of the film thickness), almost one order of magnitude larger than that before annealing. The peak-to-valley contrast became more explicit after annealing, due to the enhancement of the surface modulation. Furthermore, the sinusoidal shape of the surface profile became a little irregular, indicating that the LC alignment was disturbed upon microphase separation. Together with the enhancement of surface relief,

**4.3 AZ-containing LC block polymers with well-defined structures** 

separation have been regarded as one of ideal materials candidates for holograms.

films.

the diffraction efficiency increased to about 9.0 %, almost two orders of magnitude larger than the diffraction efficiency before annealing. This increased diffraction efficiency might be ascribed mainly to the enhancement of surface modulation. Furthermore, multi-processes of the refractive-index gratings were successfully achieved as presented in Figure 11. The obtained grating structures were clearly observed in the polarizing optical microscopic pictures, which were also verified by their diffraction patterns (Yu et al., 2007a).

Fig. 11. Holographic gratings recorded in AZ-containing LC block copolymers with welldefined structures and enhancement of gratings upon microphase separation.

Azobenzene-Containing Materials for Hologram 109

As shown in Figure 12, holographic gratings were recorded in films of two polymethyl methacrylate (PMMA)–based block copolymers containing AZ moieties (Yu et al, 2008b). One was a well–defined diblock copolymer, and the other sample was a diblock random copolymer. Here, the diblock random copolymer consisted of two blocks, in which one segment was PMMA and the other mesogenic block was statistically random distributed. After grating formation, both films showed no formation of surface-relief gratings, and only refractive-index gratings were obtained. Upon irradiation of two coherent laser beams, refractive-index gratings in the diblock copolymer containing AZs were recorded by photoalignment of AZs dispersed in phase–separated domains. In contrast, the photoalignment of the AZ moieties was amplified by the photoinert cyanobiphenyl moieties as a result of the cooperative effect in the diblock random copolymer. This led to a similar refractive–index modulation, although the AZ content was lower in the diblock random copolymer. The cooperative motion was confined within the nanoscale phase domains,

Being one of commercially available products, an ABA–type triblock copolymer, polystyrene (PS)–*b*–polybutadiene–*b*–PS, is famous for its thermoplastics. The hard block of PS with a content of 20–30 wt% forms the minority phase upon microphase separation, which acts as physical crosslinks for the majority phase of the soft block of rubbery polybutadiene (PB). Mechanical stretching can induce a large elastic deformation with recoverable properties. By applying this concept, block copolymers with thermoplastics were prepared (Bai & Zhao, 2001, 2002; Zhao et al., 2002). Upon stretching–induced elastic deformation of grating samples recorded in the thermoplastic block copolymers, fringe

Fig. 13. Mechanically tunable fringe spacing of gratings recorded in an AZ-containing block

copolymers with thermoplastics.

unlike the case of random copolymers with statistically molecular structures.

spacing or grating periodicity was successfully adjusted, as shown in Figure 13.

Comparing to other methods to control diffraction efficiency, such as gain effects, mechanical stretch, electrical switch, self–assembly, mixture with LC and cross–linking, the microphase-separation method had advantages of being simple and convenient (Yu et al., 2005a, 2009a). To precisely control diffraction efficiency of recorded gratings in the amphiphilic block copolymers, the effect of recording time on grating formation and enhancement was systematically studied. The best enhancement effect was obtained at 10 s recording upon microphase separation. By adjusting the recording time, the diffraction efficiency was finely controlled from 0.13% to about 10% (Yu et al., 2009a).

As described in section **2**, a small external stimulus can induce a large change in refractive index of the materials by the cooperative effect between photoresponsive AZ moieties and photoinert groups. These propertied have been widely used in holographic recording, which is especially useful in AZ–containing block copolymers with mesogens in the minority phase dispersed in glassy substrates (Yu et al., 2007b). It was reported that the photoinduced mass transfer was greatly prohibited due to the microphase separation in grating recording, lack of surface–relief structures was observed (Breiner et al., 2007). Thus, refractive–index modulation plays an important role in the grating formation in such well-defined block copolymers.

Fig. 12. Enhancement of surface-index modulation and prohibition of surface-relief gratings in block copolymers with photoresponsive AZ groups in the minority phase. (A, aligned, R, random).

Comparing to other methods to control diffraction efficiency, such as gain effects, mechanical stretch, electrical switch, self–assembly, mixture with LC and cross–linking, the microphase-separation method had advantages of being simple and convenient (Yu et al., 2005a, 2009a). To precisely control diffraction efficiency of recorded gratings in the amphiphilic block copolymers, the effect of recording time on grating formation and enhancement was systematically studied. The best enhancement effect was obtained at 10 s recording upon microphase separation. By adjusting the recording time, the diffraction

As described in section **2**, a small external stimulus can induce a large change in refractive index of the materials by the cooperative effect between photoresponsive AZ moieties and photoinert groups. These propertied have been widely used in holographic recording, which is especially useful in AZ–containing block copolymers with mesogens in the minority phase dispersed in glassy substrates (Yu et al., 2007b). It was reported that the photoinduced mass transfer was greatly prohibited due to the microphase separation in grating recording, lack of surface–relief structures was observed (Breiner et al., 2007). Thus, refractive–index modulation plays an important role in the grating formation in such well-defined block copolymers.

Fig. 12. Enhancement of surface-index modulation and prohibition of surface-relief gratings in block copolymers with photoresponsive AZ groups in the minority phase. (A, aligned, R,

random).

efficiency was finely controlled from 0.13% to about 10% (Yu et al., 2009a).

As shown in Figure 12, holographic gratings were recorded in films of two polymethyl methacrylate (PMMA)–based block copolymers containing AZ moieties (Yu et al, 2008b). One was a well–defined diblock copolymer, and the other sample was a diblock random copolymer. Here, the diblock random copolymer consisted of two blocks, in which one segment was PMMA and the other mesogenic block was statistically random distributed. After grating formation, both films showed no formation of surface-relief gratings, and only refractive-index gratings were obtained. Upon irradiation of two coherent laser beams, refractive-index gratings in the diblock copolymer containing AZs were recorded by photoalignment of AZs dispersed in phase–separated domains. In contrast, the photoalignment of the AZ moieties was amplified by the photoinert cyanobiphenyl moieties as a result of the cooperative effect in the diblock random copolymer. This led to a similar refractive–index modulation, although the AZ content was lower in the diblock random copolymer. The cooperative motion was confined within the nanoscale phase domains, unlike the case of random copolymers with statistically molecular structures.

Being one of commercially available products, an ABA–type triblock copolymer, polystyrene (PS)–*b*–polybutadiene–*b*–PS, is famous for its thermoplastics. The hard block of PS with a content of 20–30 wt% forms the minority phase upon microphase separation, which acts as physical crosslinks for the majority phase of the soft block of rubbery polybutadiene (PB). Mechanical stretching can induce a large elastic deformation with recoverable properties. By applying this concept, block copolymers with thermoplastics were prepared (Bai & Zhao, 2001, 2002; Zhao et al., 2002). Upon stretching–induced elastic deformation of grating samples recorded in the thermoplastic block copolymers, fringe spacing or grating periodicity was successfully adjusted, as shown in Figure 13.

Fig. 13. Mechanically tunable fringe spacing of gratings recorded in an AZ-containing block copolymers with thermoplastics.

Azobenzene-Containing Materials for Hologram 111

enhance the refractive-index modulation. AZ mesogens with a low content to the Z = about 5 mol%, which acted as photoresponsive moieties. Transparent and thick films (> 100 μm)

Fig. 14. Transparent and thick films of AZ-containing copolymers for Bragg gratings.

Upon irradiation with the writing beams, the first-order diffracted beam (+1st) appeared immediately and the intensity of the zeroth-order beam (0th) decreased (Figure 14). The maximum diffraction efficiency reached above 98 % in all the prepared films. Furthermore, the polarization-selective multiple holographic data storage could be obtained using the photoinduced anisotropy as well as rewritable holographic recording with about 100% diffraction efficiency. These materials prepared by a simple but balanced formulation would provide a new guideline for the construction of high-performance

Recent advance in AZ-containing materials has enabled one to record both Raman-Nath and Bragg holograms. Among these materials, low-molecular-weight compounds and amorphous polymers showed good capability of surface-relief grating formation. In LC polymers, refractive-index gratings are often recorded, accompanying with surface-relief modulation. Block copolymers with well-defined structures can eliminate the scattering of visible light by microphase separation and prohibit surface deformation when AZ blocks forms the minority phases. Furthermore, thick films (> 200 microns) with good optical transparency can be prepared with random copolymers or blended block copolymers,

were fabricated using a melting and pressing process.

holographic devices.

providing substrates for recording volume holograms.

**6. Conclusion** 

Generally, the fringe spacing could be decided by the pattern of the used photomask, when the grating was recorded with one writing beam. On the other hand, holographic gratings were also inscribed in block copolymer films by two coherent laser beams with an equal intensity. The recorded fringe spacing can be evaluated by Λ = λw/(2sinθ), where λw and θ are the wavelength and the incident angle of the writing laser beams, respectively. Once the writing beams are obtained, the fringe spacing is fixed. Tunable features of the fringe spacing were achieved in films of the thermoplastic block copolymers (Figure 13). When the strain direction was parallel to the grating direction, the fringe spacing was decreased. On the contrary, the fringe spacing was increased when the strain direction was perpendicular to the grating direction. By the stretching, diffraction efficiency of the gratings was adjusted accordingly (Zhao et al., 2002). Recently, mechanically tunable fringe spacing was also obtained in gratings recorded with ABA–type triblock copolymers showing properties of conventional thermoplastic elastomers, in which rubbery poly(n–butyl acrylate) was designed as middle soft block and photoresponsive polymers acted as hard block (Cui et al., 2004).

### **5. Novel AZ-containing materials**

Recent progress in chemistry and material science enables one to freely design functional materials with suitable processes to satisfy the need of advanced materials for a variety of applications. Integration of AZ materials with other functionalized materials and processing provides the designed materials for holograms with special features. For instance, graphene nanosheet grafted with AZ-containing polymer brushes was prepared via a "grafting-from" approach, which was used as dopant for an AZ-containing molecular glass in recording gratings (Wang et al., 2011). The diffraction efficiency of the inscribed gratins was enhanced due to the mass transfer of the graphene nanosheets showing a high refractive index. Chemically crosslinking of AZ-containing polymer films with surface-relief gratins could fix the obtained surface modulation, producing permanent shape change (Zettsu et al, 2008).

As shown in Figure 2, the Raman-Nath hologram recorded in a thin film exhibited a theoretically maximum diffraction efficiency of about 34%. This was far lower than the Bragg-type hologram in a thick film with a maximum diffraction efficiency of 100%. Furthermore, angular multiplicity could be easily obtained in the Bragg hologram, enabling thick films to be suitable for volume storage. To prepare thick and transparent films, amorphous and highly transparent PS blended with their block copolymers containing an AZ block as the minority phase to eliminate the scattering by utilizing the nanoscale microphase separation (Häckel et al., 2005 , 2007). Since all of the mesogens were confined in nanospheres dispersed in PS matrix, thick and optically transparent films were obtained by injection-molded method. These films showed good angle-multiplexing capability, in which 200 holograms were superimposed and reconstructed independently at the same spot and more than 1000 write/erase cycles were successfully obtained.

However, the density of photoresponsive mesogens in the block copolymer blend systems was very low, leading to a low diffraction efficiency of the recorded gratings. To induce a large change in refractive index and record Bragg gratings with high diffraction efficiency, a series of amorphous random copolymers with both AZ moieties and photoinert mesogens was prepared, as shown in Figure 14 (Saishoji et al., 2007 ; Ishiguro et al., 2007). The highly transparent PMMA was utilized as substrate, when x > 50 mol% in the materials preparation. Cyanobiphenyl and tolane groups were selected as the photoinert part to

Generally, the fringe spacing could be decided by the pattern of the used photomask, when the grating was recorded with one writing beam. On the other hand, holographic gratings were also inscribed in block copolymer films by two coherent laser beams with an equal intensity. The recorded fringe spacing can be evaluated by Λ = λw/(2sinθ), where λw and θ are the wavelength and the incident angle of the writing laser beams, respectively. Once the writing beams are obtained, the fringe spacing is fixed. Tunable features of the fringe spacing were achieved in films of the thermoplastic block copolymers (Figure 13). When the strain direction was parallel to the grating direction, the fringe spacing was decreased. On the contrary, the fringe spacing was increased when the strain direction was perpendicular to the grating direction. By the stretching, diffraction efficiency of the gratings was adjusted accordingly (Zhao et al., 2002). Recently, mechanically tunable fringe spacing was also obtained in gratings recorded with ABA–type triblock copolymers showing properties of conventional thermoplastic elastomers, in which rubbery poly(n–butyl acrylate) was designed as middle soft block and photoresponsive polymers acted as hard block (Cui et al.,

Recent progress in chemistry and material science enables one to freely design functional materials with suitable processes to satisfy the need of advanced materials for a variety of applications. Integration of AZ materials with other functionalized materials and processing provides the designed materials for holograms with special features. For instance, graphene nanosheet grafted with AZ-containing polymer brushes was prepared via a "grafting-from" approach, which was used as dopant for an AZ-containing molecular glass in recording gratings (Wang et al., 2011). The diffraction efficiency of the inscribed gratins was enhanced due to the mass transfer of the graphene nanosheets showing a high refractive index. Chemically crosslinking of AZ-containing polymer films with surface-relief gratins could fix the obtained surface modulation, producing permanent shape change (Zettsu et al, 2008). As shown in Figure 2, the Raman-Nath hologram recorded in a thin film exhibited a theoretically maximum diffraction efficiency of about 34%. This was far lower than the Bragg-type hologram in a thick film with a maximum diffraction efficiency of 100%. Furthermore, angular multiplicity could be easily obtained in the Bragg hologram, enabling thick films to be suitable for volume storage. To prepare thick and transparent films, amorphous and highly transparent PS blended with their block copolymers containing an AZ block as the minority phase to eliminate the scattering by utilizing the nanoscale microphase separation (Häckel et al., 2005 , 2007). Since all of the mesogens were confined in nanospheres dispersed in PS matrix, thick and optically transparent films were obtained by injection-molded method. These films showed good angle-multiplexing capability, in which 200 holograms were superimposed and reconstructed independently at the same spot and

However, the density of photoresponsive mesogens in the block copolymer blend systems was very low, leading to a low diffraction efficiency of the recorded gratings. To induce a large change in refractive index and record Bragg gratings with high diffraction efficiency, a series of amorphous random copolymers with both AZ moieties and photoinert mesogens was prepared, as shown in Figure 14 (Saishoji et al., 2007 ; Ishiguro et al., 2007). The highly transparent PMMA was utilized as substrate, when x > 50 mol% in the materials preparation. Cyanobiphenyl and tolane groups were selected as the photoinert part to

2004).

**5. Novel AZ-containing materials** 

more than 1000 write/erase cycles were successfully obtained.

enhance the refractive-index modulation. AZ mesogens with a low content to the Z = about 5 mol%, which acted as photoresponsive moieties. Transparent and thick films (> 100 μm) were fabricated using a melting and pressing process.

Fig. 14. Transparent and thick films of AZ-containing copolymers for Bragg gratings.

Upon irradiation with the writing beams, the first-order diffracted beam (+1st) appeared immediately and the intensity of the zeroth-order beam (0th) decreased (Figure 14). The maximum diffraction efficiency reached above 98 % in all the prepared films. Furthermore, the polarization-selective multiple holographic data storage could be obtained using the photoinduced anisotropy as well as rewritable holographic recording with about 100% diffraction efficiency. These materials prepared by a simple but balanced formulation would provide a new guideline for the construction of high-performance holographic devices.
