Source: https://patents.google.com/patent/US20110262844A1/en
Timestamp: 2019-04-23 02:20:33+00:00

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The objective of the present invention is providing a method for fabricating high quality diffractive waveplates and their arrays that exhibit high diffraction efficiency over large area, the method being capable of inexpensive large volume production. The method uses a polarization converter for converting the polarization of generally non-monochromatic and partially coherent input light beam into a pattern of periodic spatial modulation at the output of said polarization converter. A substrate carrying a photoalignment layer is exposed to said polarization modulation pattern and is coated subsequently with a liquid crystalline material. The high quality diffractive waveplates of the present invention are obtained when the exposure time of said photoalignment layer exceeds by generally an order of magnitude the time period that would be sufficient for producing homogeneous orientation of liquid crystalline materials brought in contact with said photoalignment layer. Compared to holographic techniques, the method is robust with respect to mechanical noises, ambient conditions, and allows inexpensive production via printing while also allowing to double the spatial frequency of optical axis modulation of diffractive waveplates.
This invention was made with Government support under Contract No. W911QY-07-C-0032.
Sh. D. Kakichashvili, “Method for phase polarization recording of holograms,” Soy. J. Quantum. Electron. 4, 795-798, 1974.
T. Todorov, et al., High-sensitivity material with reversible photo-induced anisotropy, Opt. Commun., 47, 123-126, 1983.
M. Attia, et al., “Anisotropic gratings recorded from two circularly polarized coherent waves,” Opt. Commun., 47, 85-90, 1983.
G. Cipparrone, et. al, “Permanent polarization gratings in photosensitive langmuir blodget films,” Appl. Phys. Lett. 77, 2106-2108, 2000.
L. Nikolova et al., “Diffraction efficiency and selectivity of polarization holographic recording,” Optica Acta 31, 579-588, 1984.
K. Ichimura, et al., “Reversible Change in Alignment Mode of Nematic Liquid Crystals Regulated Photochemically by Command Surfaces Modified with an Azobenzene Monolayer,” Langmuir 4, 1214-1216, 1988.
W. M. Gibbons, et al., “Surface-mediated alignment of nematic liquid crystals with polarized laser light,” Nature 351, 49-50, 1991.
W. M. Gibbons, et al., “Optically controlled alignment of liquid crystals: devices and applications,” Mol. Cryst. Liquid Cryst., 251, 191-208, 1994.
W. M. Gibbons, et al., “Optically generated liquid crystal gratings,” Appl. Phys. Lett., 65, 2542-2544, 1994.
M. Schadt, et al., “Optical patterning of multi-domain liquid-crystal displays with wide viewing angles,” Nature 381, 212-215, 1996.
S. R. Nersisyan, et al., “Optical Axis Gratings in Liquid Crystals and their use for Polarization insensitive optical switching,” J. Nonlinear Opt. Phys. & Mat., 18, 1-47, 2009.
N. V. Tabiryan, et al., “The Promise of Diffractive Waveplates,” Optics and Photonics News, 21, 41-45, 2010.
H. Sarkissian et al., “Periodically Aligned Liquid Crystal: Potential application for projection displays,” Storming Media Report, A000824, 2004.
H. Sarkissian, et al., “Periodically aligned liquid crystal: potential application for projection displays and stability of LC configuration,” Optics in the Southeast 2003, Orlando, Fla., Conference Program, PSE 02.
H. Sarkissian, et al., “Potential application of periodically aligned liquid crystal cell for projection displays,” Proc. of CLEO/QELS Baltimore Md., poster JThE12, 2005.
B. Ya. Zeldovich, N. V. Tabirian, “Devices for displaying visual information,” Disclosure, School of Optics/CREOL, July 2000.
M. J. Escuti et al., “A polarization-independent liquid crystal spatial-light-modulator,” Proc. SPIE 6332, 63320M(1-8), 2006.
C. M. Titus et al., “Efficient, polarization-independent, reflective liquid crystal phase grating,” Appl. Phys. Lett., 71, 2239-2241, 1997.
J. Chen, et al., “An electro-optically controlled liquid crystal diffraction grating, Appl. Phys. Lett. 67, 2588-2590, 1995.
B. J. Kim, et al., “Unusual characteristics of diffraction gratings in a liquid crystal cell,” Adv. Materials, 14, 983-988, 2002.
R.-P. Pan, et al., “Surface topography and alignment effects in UV-modified polyimide films with micron size patterns,” Chinese J. of Physics, 41, 177-184, 2003.
A. Y.-G. Fuh, et al., “Dynamic studies of holographic gratings in dye-doped liquid-crystal films,” Opt. Lett. 26, 1767-1769, 2001.
C.-J. Yu, et al., “Polarization grating of photoaligned liquid crystals with oppositely twisted domain structures,” Mol. Cryst. Liq. Cryst., Vol. 433, pp. 175-181, 2005.
G. Crawford, et al., “Liquid-crystal diffraction gratings using polarization holography alignment techniques,” J. of Appl. Phys. 98, 123102 (1-10), 2005.
M. Schadt, et al. “Photo-Induced Alignment and Patterning of Hybrid Liquid Crystalline Polymer Films on Single Substrates,” Jpn. J. Appl. Phys. 34, L764-L767 1995.
M. Schadt, et al. “Photo-Generation of Linearly Polymerized Liquid Crystal Aligning Layers Comprising Novel, Integrated Optically Patterned Retarders and Color Filters,” Jpn. J. Appl. Phys. 34, 3240-3249, 1995.
H. Seiberle, et al., “Photo-aligned anisotropic optical thin films,” SID 03 Digest, 1162-1165, 2003.
B. Wen, et al., “Nematic liquid-crystal polarization gratings by modification of surface alignment,” Appl. Opt. 41, 1246-1250, 2002.
J. Anagnostis, D. Rowe, “Replication produces holographic optics in volumes”, Laser Focus World 36, 107-111, 2000.
M. T. Gale, “Replicated diffractive optics and micro-optics”, Optics and Photonics News, August 2003, 24-29.
S. R. Nersisyan, et al., “Characterization of optically imprinted polarization gratings,” Appl. Optics 48, 4062-4067, 2009.
H. Sarkissian, et al., “Periodically aligned liquid crystal: potential application for projection displays,” Mol. Cryst. Liquid Cryst., 451, 1-19, 2006.
V. G. Chigrinov, et al., “Photoaligning: physics and applications in liquid crystal devices”, Wiley VCH, 2008.
S. C. McEldowney et al., “Creating vortex retarders using photoaligned LC polymers,” Opt. Lett., Vol. 33, 134-136, 2008.
7,196,758 March 2007 Crawford et al.
US2008/0278675 November 2008 Escuti et al.
2010/0066929 March 2010 Shemo et al.
5,903,330 May 1999 Fünfshilling et al.
5,032,009 July 1991 Gibbons et al.
This invention relates to fabrication of one or two dimensional diffractive waveplates and their arrays, those waveplates including “cycloidal” waveplates, optical axis gratings, polarization gratings (PGs), axial waveplates, vortex waveplates, and q-plates.
Polarization recording of holograms and related “polarization gratings” were concieved in 1970's as a method for recording and reconstructing the vector field of light. A light-sensitive material that acquired birefringence under the action of polarized light was suggested in the first studies (Sh. D. Kakichashvili, “Method for phase polarization recording of holograms,” Soy. J. Quantum. Electron. 4, 795, 1974). Examples of such photoanisotropic media included colored alkaly halid crystals regarded particularly promising due to reversibilty of the recording process consisting in optically altering the orientation of anisotropic color centers in the crystal.
A grating characterized only by spatial variations in the orientation of the induced optics axis can be obtained when the photoanisotropic medium is exposed to a constant intensity, rectilinear light vibrations, with spatially varying orientation, obtained from superposition of two orthogonal circularly polarized waves propagating, in slightly different directions (M. Attia, et al., “Anisotropic gratings recorded from two circularly polarized coherent waves,” Opt. Commun. 47, 85, 1983). The use of Methyl Red azobenzene dye in a polymer layer allowed to claim that photochemical processes in such material systems would enable obtaining 100 percent diffraction efficiency even in “thin” gratings (T. Todorov, et al., “High-sensitivity material with reversible photo-induced anisotropy,” Opt. Commun. 47, 123, 1983). Highly stable polarization gratings with orthogonal circular polarized beams are obtained in thin solid crystalline Langmuir-Blodgett films composed of amphiphilic azo-dye molecules showing that “100% efficiency may be achieved for samples less than 1 μm thick” (G. Cipparrone, et al., “Permanent polarization gratings in photosensitive langmuir blodget films,” Appl. Phys. Lett. 77, 2106, 2000).
A material possesing birefringence that is not influenced by light is an alternative to the photoanisotropic materials that are typically capable of only small induced birefringence (L. Nikolova et al., “Diffraction efficiency and selectivity of polarization holographic recording,” Optica Acta 31, 579, 1984). The orientation of such a material, a liquid crystal (LC), can be controlled with the aid of “command surfaces” due to exposure of the substrate carrying the command layer to light beams (K. Ichimura, et al., “Reversible Change in Alignment Mode of Nematic Liquid Crystals Regulated Photochemically by Command Surfaces Modified with an Azobenzene Monolayer,” Langmuir 4, 1214, 1988). Further a “mechanism for liquid-crystal alignment that uses polarized laser light” was revealed (W. M. Gibbons, et al., “Surface-mediated alignment of nematic liquid crystals with polarized laser light,” Nature 351, 49, 1991; W. M. Gibbons, et al., “Optically controlled alignment of liquid crystals: devices and applications,” Mol. Cryst. Liquid Cryst., 251, 191, 1994). Due to localization of dye near the interface, the exposure can be performed in the absence of LC, and the LC is aligned with high spatial and angular resolution (potentially, submicron) after filling the cell (W. M. Gibbons, et al., “Optically generated liquid crystal gratings,” Appl. Phys. Lett. 65, 2542, 1994). Variety of photoalignment materials are developed for achieving high-resolution patterns and obtaining variation of molecular alignment within individual pixels (M. Schadt, et al., “Optical patterning of multi-domain liquid-crystal displays with wide viewing angles,” Nature 381, 212, 1996).
A critically important issue for producing LC orientation patterns at high spatial frequencies is their mechanical stability. Particularly, the cycloidal orientation of LCs obtained due to the orienting effect of boundaries is stable only when a specific condition between the material parameters, the cell thickness, and the period of LC orientation modulation is fulfilled (H. Sarkissian et al., “Periodically Aligned Liquid Crystal: Potential application for projection displays,” Storming Media Report, A000824, 2004; H. Sarkissian, et al., “Periodically aligned liquid crystal: potential application for projection displays and stability of LC configuration,” Optics in the Southeast 2003, Orlando, Fla.; Conference Program, PSE 02. and H. Sarkissian, et al., “Potential application of periodically aligned liquid crystal cell for projection displays,” Proc. of CLEO/QELS Baltimore Md., poster JThE12, 2005; B. Ya. Zeldovich, N. V. Tabirian, “Devices for displaying visual information,” Disclosure, School of Optics/CREOL, July 2000). Suggesting fabrication of cycloidal polarization gratings using the photoalignment technique with overlapping right and left circularly polarized beams, the publications by Sarkissian, Zeldovich and Tabirian cited above are credited for having theoretically proven polarization gratings can be 100% efficient and can be used as a diffractive grating for projection displays (C. Provenzano, et al., “Highly efficient liquid crystal based diffraction grating induced by polarization holograms at the aligning surfaces,” Appl. Phys. Lett., 89, 121105, 2006; M. J. Escuti et al., “A polarization-independent liquid crystal spatial-light-modulator,” Proc. SPIE 6332, 63320M, 2006).
LCs with spatially modulated orientation patterns produced using the photoalignment technqiue are known in the prior art (W. M. Gibbons, et al., “Surface-mediated alignment of nematic liquid crystals with polarized laser light,” Nature 351, 49, 1991; C. M. Titus et al., “Efficient, polarization-independent, reflective liquid crystal phase grating,” Appl. Phys. Lett. 71, 2239, 1997; J. Chen, et al., “An electro-optically controlled liquid crystal diffraction grating, Appl. Phys. Lett. 67, 2588, 1995; B. J. Kim, et al., “Unusual characteristics of diffraction gratings in a liquid crystal cell,” Adv. Materials 14, 983, 2002; R.-P. Pan, et al., “Surface topography and alignment effects in UV-modified polyimide films with micron size patterns,” Chinese J. of Physics 41, 177, 2003; A. Y.-G. Fuh, et al., “Dynamic studies of holographic gratings in dye-doped liquid-crystal films,” Opt. Lett. 26, 1767, 2001; C.-J. Yu, et al., “Polarization grating of photoaligned liquid crystals with oppositely twisted domain structures,” Mol. Cryst. Liq. Cryst. 433, 175, 2005; G. Crawford, et al., “Liquid-crystal diffraction gratings using polarization holography alignment techniques,” J. of Appl. Phys: 98, 123102, 2005; Crawford et al., U.S. Pat. No. 7,196,758).
LC polymers were widely used as well (M. Schadt, et al. “Photo-Induced Alignment and Patterning of Hybrid Liquid Crystalline Polymer Films on Single Substrates,” Jpn. J. Appl. Phys. 34, L764 1995; M. Schadt, et al. “Photo-Generation of Linearly Polymerized Liquid Crystal Aligning Layers Comprising Novel, Integrated Optically Patterned Retarders and Color Filters,” Jpn. J. Appl. Phys. 34, 3240, 1995; Escutti et al, US Patent Application US2008/0278675;). Photo-aligned anisotropic thin films can be applied to rigid or flexible substrates, which may be flat or curved and/or generate patterned retarders with continuous or periodical inplane variation of the optical axis (H. Seiberle, et al., “Photo-aligned anisotropic optical thin films,” SID 03 Digest, 1162, 2003).
The cycloidal diffractive waveplates (CDWs) wherein the optical axis of the material is periodically rotating in the plane of the waveplate along one axis of a Cartesian coordinate system are the most interesting one-dimensional structures used for applications such as displays, beam steering systems, spectroscopy etc. These are known also as cycloidal DWs (CDWs), optical axis gratings, and polarization gratings (PGs) (S. R. Nersisyan, et al., “Optical Axis Gratings in Liquid Crystals and their use for Polarization insensitive optical switching,” J. Nonlinear Opt. Phys. & Mat. 18, 1, 2009). Most interesting for applications two-dimensional orientation patterns possess with axial symmetry (N. V. Tabiryan, et al., “The Promise of Diffractive Waveplates,” Optics and Photonics News 21, 41, 2010; L. Marucci, US Patent Application 2009/0141216; Shemo et al., US Patent Application 2010/0066929).
Thus, in the prior art, optical axis modulation patterns of anisotropic material systems were demonstrated, including in LCs and LC polymers, due to modulation of boundary alignment conditions, and it was shown that such boundary conditions can be achieved by a number of ways, including using photoaligning materials, orthogonal circular polarized beams, microrubbing, and substrate rotation (Funfshilling et al., U.S. Pat. No. 5,903,330; B. Wen, et al., “Nematic liquid-crystal polarization gratings by modification of surface alignment,” Appl. Opt. 41, 1246, 2002; S. C. McEldowney et al., “Creating vortex retarders using photoaligned LC polymers,” Opt. Lett., Vol. 33, 134, 2008). LC optical components with orientation pattern created by exposure of an alignment layer to a linear polarized light through a mask, by scanning a linear polarized light beam in a pattern, or creating a pattern using an interference of coherent beams is disclosed in the U.S. Pat. No. 5,032,009 to Gibbons, et al. Also, in the prior art, “Optically controlled planar orientation of liquid crystal molecules with polarized light is used to make phase gratings in liquid crystal media” (W. M. Gibbons and S.-T. Sun, “Optically generated liquid crystal gratings,” Appl. Phys. Lett. 65, 2542, 1994).
DWs are characterized by their efficiency, optical homogeneity, scattering losses, and size. While acceptable for research and development purposes, none of the techniques known in the prior art can be used for fabricating high quality DWs and their arrays in large area, inexpensively, and in high volume production. Since DWs consist of a pattern of optical axis orientation, they can not be reproduced with conventional techniques used for gratings of surface profiles (J. Anagnostis, D. Rowe, “Replication produces holographic optics in volumes”, Laser Focus World 36, 107, 2000); M. T. Gale, “Replicated diffractive optics and micro-optics”, Optics and Photonics News, August 2003, p. 24).
It is the purpose of the present invention to provide method for the production of DWs. The printing method of the current invention does not require complex holographic setups, nor special alignment or vibration isolation as described in the publications S. R. Nersisyan, et al., “Optical Axis Gratings in Liquid Crystals and their use for Polarization insensitive optical switching,” J. Nonlinear Opt. Phys. & Mat., 18, 1, 2009; S. R. Nersisyan, et al., “Characterization of optically imprinted polarization gratings,” Appl. Optics 48, 4062, 2009 and N. V. Tabiryan, et al., “The Promise of Diffractive Waveplates,” Optics and Photonics News, 21, 41, 2010, which are incorporated herein by reference.
Energy densities required for printing DWs are essentially the same as in the case of producing a waveplate in a holographic process. This makes fabrication of diffractive waveplates much faster compared to mechanical scanning or rotating techniques. A technique for obtaining polarization modulation patterns avoiding holographic setups was discussed earlier in the U.S. Pat. No. 3,897,136 to O. Bryngdahl. It discloses a grating “formed from strips cut in different directions out of linearly dichroic polarizer sheets. The gratings were assembled so that between successive strips a constant amount of rotation of the transmittance axes occurred.” These were also essentially discontinuous structures, with the angle between the strips π/2 and π/6 at the best. The size of individual strips was as large as 2 mm. Thus, such a grating modulated polarization of the output light at macroscopic scales and could not be used for production of microscale-period gratings with diffractive properties at optical wavelengths.
Thus, the objective of the present invention is providing means for fabricating high quality DWs in large area, typically exceeding 1″ in sizes, in large quantities, with high yield, and low cost.
The second objective of the present invention is providing means for fabricating DWs with different periods of optical axis modulation.
The invention, particularly, includes converting a linear or unpolarized light, generally non-monochromatic, incoherent or partially coherent, into a light beam of a periodic pattern of polarization modulation and subjecting materials with capability of photoalignment to said pattern for time periods exceeding the times otherwise required for obtaining homogeneous orientation state.
Further objectives and advantages of this invention will be apparent from the following detailed description of presently preferred embodiment, which is illustrated schematically in the accompanying drawings.
FIG. 1A shows the schematic of printing DWs.
FIG. 1B schematically shows distribution of light polarization at the output of the linear-to-cycloidal polarization converter.
FIG. 1C schematically shows distribution of light polarization at the output of a linear-to-axial polarization converter.
FIG. 1D schematically shows distribution of light polarization at the output of a two-dimensional cycloidal polarization converter.
FIG. 2A shows the schematic of printing DWs using a cycloidal DW as a polarization converter.
FIG. 2B shows the schematic of a cycloidal DW.
FIG. 3 shows spatial frequency doubling of a cycloidal DW in the printing process. Photos are obtained under polarizing microscope with 100x magnification.
FIG. 4 shows two consecutive doubling of the order of an axially symmetric DW.
FIG. 5 shows photos of the structure of cycloidal DWs obtained under polarizing microscope for different exposure times. Photos are obtained under polarizing microscope with 40× magnification.
Before explaining the disclosed embodiment of the present invention in detail it is to be understood that the invention is not limited in its application to the details of the particular arrangement shown since the invention is capable of other embodiments. Also, the terminology used herein is for the purpose of description and not limitation.
The preferred embodiment of the present invention shown in FIG. 1A includes a light beam 101 incident upon an optical component 102 capable of converting the incident light beam 101 into a beam with spatially modulated polarization pattern 103. Of particular interest are “cycloidal” and axial modulation patterns shown schematically in FIG. 1B and FIG. 1C, correspondingly, wherein the numerals 106 indicate the linear polarization direction at each point of the plane at the output of the polarization converter (S. R. Nersisyan; et al., “Characterization of optically imprinted polarization gratings,” Appl. Optics 48, 4062, 2009). One polarization modulation period is shown in FIG. 1B, and the polarization direction is reversed 4 times for the example of the axially modulated pattern shown in FIG. 1C. Polarization modulation may have other distributions as exemplified by the two-dimensional cycloidal pattern shown in FIG. 1D.
A photoresponsive material film 104 capable of producing an internal structure aligned according to the polarization pattern 103, deposited on a substrate 105, is arranged in the area with spatially modulated polarization pattern. Examples of such materials include photoanisotropic materials such as azobenzene or azobenzene dye-doped polymers, and photoalignment materials such as azobenzene derivatives, cinnamic acid derivatives, coumarine derivatives, etc.
In case shown in FIG. 2A, a cycloidal diffractive waveplate (CDW) is used as polarization converter 102. The structure of said CDW is schematically shown in FIG. 2B wherein the numeral 109 indicates the alignment direction of the optical axis of the material. The cycloidal polarization pattern is obtained at the vicinity of the converter, near its output surface, in the overlap region of the diffracted beams 107 and 108.
The simplicity of this method, its insensitivity to vibrations, noises, air flows, as opposed to the holographic techniques makes feasible manufacturing high quality DWs with high diffraction efficiency in large areas exceeding 1″ in sizes and in large quantities with low cost. Note that adding a polarizer at the output of the DW transforms the polarization modulation pattern into a pattern of intensity modulation that could be used for printing diffractive optical elements as well.
The spatial period of the printed DW is equal to that of the DW used as a polarization converter when a circular polarized light is used. A linear polarized light, however, yields in a DW with twice shorter period of the optical axis modulation. This is evident, FIG. 3, in the photos of the structure of the DW 301 produced via printing using a linear polarized light beam as compared to the structure of the DW 302 used as a polarization converter. Photos were obtained under polarizing microscope with 100× magnification (S. R. Nersisyan, et al., “Characterization of optically imprinted polarization gratings,” Appl. Optics 48, 4062, 2009). This applies both to CDWs as well as to the diffractive waveplates with axial symmetry of optical axis orientation (ADWs) shown in FIG. 4 wherein the numeral 401 corresponds to the ADW used as a polarization converter, and 402 corresponds to the ADW obtained as a result of printing (N. V. Tabiryan, S. R. Nersisyan, D. M. Steeves and B. R. Kimball, The Promise of Diffractive Waveplates, Optics and Photonics News 21, 41, 2010). The technique of doubling the spatial frequency allows producing high degree ADWs and their arrays without using mechanical rotating setups.
Each DW in these examples was obtained by deposition of a LC polymer on the substrate carrying the photoalignment layer. This process of LC polymer deposition involves spin coating, heating to remove residual solvents, and polymerization in an unpolarized UV light. Other coating techniques (spray coating, as an example) and polymerization techniques (heating, as an example) are known and can be used for this purpose. The period of the printed CDW can be varied also by incorporating an optical system that projects the cycloidal polarization pattern onto larger or smaller area.
Another key aspect of the present invention consists in the disclosure that the photoalignment materials need to be exposed to cycloidal polarization pattern of radiation for time periods considerably exceeding the exposure time required for obtaining homogeneous aligning films at a given power density level of radiation. As an example, ROLIC Ltd. specifies 50 mJ/cm2 exposure energy density for its material ROP 103 at the wavelength 325 nm. Exposure with such an energy density yields in good homogeneous alignment, however, the structure of cycloidal DWs fabricated according to that recipe appears very poor under polarizing microscope as shown in FIG. 5. Extending the exposure time improves the structure, and practically defect-free structure is obtained for exposure energies >1 J/cm2 that is 20× exceeding the specified values for this particular material.
The quality of DWs fabricated in conventional holographic process depends on many factors: the quality of the overlapping beams; the susceptibility of the holographic setup to mechanical vibrations and air fluctuations in the path of the beam; the coherence of the beams and equality of their paths; depolarization effects due to propagation of the beams through multiple optical elements such as lenses and beam splitters; the quality of the substrate; the qualities of the photoalignment materials, their affinity with the substrate in use and the effects of spin coating and solvent evaporation process. These factors include the homogeneity of the LCs layer thickness, and their compatibility issues with the photoalignment layer. The compatibility of the LC materials with the photoalignment material is important as well. Typical thickness of these films is in the micrometer range, whereas thickness variation for as little as the wavelength of radiation, ˜0.5 μm for visible wavlengths, can dramatically affect the diffraction efficiency of those components. The absolute value of the thickness is as important due to orientation instabilities that is determined, among other things, by the ratio of the layer thickness to the modulation period (H. Sarkissian, et al., “Periodically aligned liquid crystal: potential application for projection displays,” Mol. Cryst. Liquid Cryst., 451, 1, 2006).
Among all these factors, the exposure energy, being a parameter easy to control and specified by its supplier appears to be the least suspected to affect the quality of the DW being fabricated. With all the noises, impurities, and uncertainties in many steps involved in the process, the obtained component would still show relatively small areas of good quality, good enough for a university research, but beyond the acceptable limits for practical applications. Thus, the finding that the exposure times shall considerably exceed photoaligning material specifications is critically important for fabrication of high quality DWs with homogeneous properties in a large area.
The reasons for such an effect of the exposure time lie, apparently, in the need to produce stronger forces to support a pattern of spatial modulation of the optical axis than those required for homogeneous alignment. Elastic forces against modulation of molecular orientation are strong in LC materials. Longer exposure induces stronger modulation of the microscopic orientation properties of the photoaligning materials. Anchoring energy of such materials for LCs are not comprehensively studied. The available data relate to homogeneous orientation (V. G. Chigrinov, et al., “Photoaligning: physics and applications in liquid crystal devices”, Wiley VCH, 2008).
Due to robustness of the printing method to the mechanical and other ambient noise, large area components can be fabricated by continuously translating the substrate in the region of cycloidal polarization pattern. By that, the energy of the light beam can be distributed along a long strip to produce a larger photoalignment area.
Although the present invention has been described above by way of a preferred embodiment, this embodiment can be modified at will, within the scope of the appended claims, without departing from the spirit and nature of the subject invention.
(d) exposing at least a portion of said photoresponsive material layer to the polarization modulation pattern produced by said polarization converter.
2. The method of claim 1 further comprising optical means for projecting said polarization modulation pattern of said light beam onto at least a part of the area of said photoresponsive material layer, said projection generally changing the size, shape and topography of said polarization modulation pattern obtained at the output of said polarization converter.
3. The method of claim 1 wherein said polarization converter comprises at least one diffractive waveplate that may be achromatic, and may be part of an array.
4. The method of claim 1 further comprising at least one substrate for controlling at least one of the following properties of said photoresponsive material layer: mechanical shape and stability, thermal conductivity, thickness homogeneity, radiation resistance, and resistance to adverse ambient conditions.
(d) means for exposing different areas of said photoresponsive material layer to said polarization modulation pattern.
6. The method of claim 5 wherein the means for holding and positioning the layer of said photoresponsive material include at least one of the following: a glass substrate; a polymer substrate, a drum, a translation stage, and a rotation stage.
7. The method as in claim 5 wherein the means for exposing different areas of said photoresponsive material layer to said polarization modulation pattern includes at least one of the mechanical motions, translation in the direction perpendicular to the polarization modulation axis, and rotation, said motions performed with the aid of at least one of said positioning means: the positioning means of the holder of said photoresponsive material layer, and the positioning means of said polarization modulation pattern.
(b) propagating said light beam through a diffractive waveplate, the diffractive waveplate having optical axis modulation period twice larger compared to said predetermined spatial period.
(b) exposing a photoresponsive material layer to said light beam propagated through said diffractive waveplate, the photoresponsive material having the ability of producing an anisotropy axis modulated according to the polarization of said light beam.
9. Any of the methods of claim 1, 5, or 8 further comprising at least one anisotropic material layer with ability of producing an optical axis modulation according to and under the influence of the anisotropy axis of the photoresponsive material layer.
(d) exposing said photoresponsive material layer to said polarization modulation pattern for exposure energy density exceeding at least 5 times the exposure energy density sufficient for producing waveplates with homogeneously orientation of optical axis.
(e) bringing said photoresponsive layer in contact with at least one anisotropic material layer, said anisotropic material having the ability of producing an optical axis modulation according to and under the influence of the anisotropy axis of said photoresponsive material layer.
11. The method of claim 9 or 10 wherein said optical axis modulation of at least one of said anisotropic material layers is twisted in the direction perpendicular to the modulation plane of the anisotropy axis of said photoresponsive material layer.

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