Bistable nematic liquid crystal device

专利摘要:
The liquid crystal device of the invention comprises a layer 2 of nematic liquid crystal material contained between the electrode structures 6, 7 and the two cell walls 3, 4 supporting the alignment surfaces 20, 21, respectively. . The alignment layers 20, 21 on one or both cell walls are formed of a plurality of small (<15 μm) surface features, each of which can individually provide a bistable preliminary slope and alignment direction and collectively layer Larger changes in molecular orientation across (2) can be caused. The device can be switched between a light transmission state and a light transmission state. The small surface features may be regions of the grating 21, protrusion 25 or blind hole 26, separated by monostable flat surfaces Fm coated with a vertical alignment layer. The grating provides a bistable switching operation between low surface slope and high surface slope, and the low slope alignment direction suitably varies between adjacent grating regions.
公开号:KR20020095165A
申请号:KR1020027006859
申请日:2000-11-23
公开日:2002-12-20
发明作者:조네스존클리포드
申请人:키네티큐 리미티드；
IPC主号:

专利说明:

Bistable nematic liquid crystal device
[2] Liquid crystal devices typically comprise a thin layer of liquid crystal material received between cell walls, at least one of which is light transmissive. The walls are typically coated with a transparent conductive layer on the inner surface so that an external electric field can be applied. The electrodes are often formed as column or line electrodes on one wall and as a series of strips that form rows on the other wall. The intersection of columns and rows provides an xy matrix of elements or pixels that can be addressed. Other devices may be used including segmented or rθ displays.
[3] In addition, some liquid crystal devices include regions of the semiconductor alongside electrodes designed to form nonlinear elements such as thin film transistors (TFTs). Other layers, including color filters, flat and barrier layers, and absorbing or reflecting layers, may be housed inside the device.
[4] Typically, the innermost surface of each pixel includes an alignment layer that provides the required orientation of the liquid crystal director. Typically, the alignment layer is a polymer layer, such as polyimide, for example, buffed with a cloth to give the surface a predetermined direction. This provides a suitable alignment and surface slope for the liquid crystal molecules. If the polymer is not buffed, liquid crystal molecules represented by unit vectors, generally referred to as directors, provide a planar orientation parallel to the local surface of the polymer. In addition, grating surfaces formed on layers of photoresists are described, for example, in British Patents 2,312,523, 2,290,629, International Applications WO98 / 59275, WO97 / 39382, and US Pat. Nos. 5,808,717, 4,247,174. As disclosed in the arc, it is used for alignment and surface slope. Photoresist materials typically result in planar alignment of the director, and suitable alignment directions and preliminary tilts are generated by elastic distortions close to the surface generated by the grooves of the diffraction grating surface.
[5] For example, different types of alignment are often achieved using low surface energy provided by surfactants. In this case, the director is locally perpendicular to the surface and is called homeotropic. In all cases, the molecules of the liquid crystal material adjacent the substrate surface transmit the alignment direction suitable for the bulk of the sample through the elastic force of the liquid crystal.
[6] Applying an electric field across the liquid crystal device can have any of a number of effects. Many devices rely on the intrinsic dielectric anisotropy of the liquid crystal (Δε = ε∥-ε⊥, where ∥ and 지칭 refer to directions parallel and perpendicular to the director). If Δε is positive, the electrostatic energy of the liquid crystal is minimal when the director is parallel to the applied electric field, whereas if Δε is negative, the director tends to be positioned perpendicular to the applied electric field. These effects are related to the RMS value of the field and are independent of the polarity of the electric field. Most materials are positive or negative over the operating frequency range of the device, but some materials are designed to exhibit "two frequency" behavior within the operating electrical frequency range where Δε is positive at low frequencies and negative at high frequencies. Recently, several devices have been disclosed that use flexo-electric effects that occur in multiple liquid crystals (R.B. Meyer 1969, Phys Rev Lett. V22, p918). This effect is caused by the polar alignment of the liquid crystal molecules induced by some elastic distortion of the liquid crystal director field. The strength of this effect is related to the DC field and depends on the polarity of the applied electric field.
[7] In conventional twisted nematic devices, electro-optic modulation is due to the effect of Δε. By applying the appropriate voltage, the liquid crystal molecules are rotated from the twisted state (rotating the plane of plane polarized light) approximately parallel to the layer thickness to the non-rotating state approximately perpendicular to the layer (switching state). The twist and bit twist states can be identified by observing the cell when it is between polarizers, which may be arranged in an orthogonal state or some other suitable arrangement, depending on the design of the liquid crystal cell.
[8] Alternatively, optical contrast can be achieved by modulating the scattering degree of incident light. Dynamic scattering nematics (Heilmeier et al. 1968, Appl. Phys Lett v13 p46); Dynamic scattering smetics (eg, Crossland et al. 1979, US Pat. No. 4,139,273); Thermally and electrically addressed scattering Schematic A devices (eg, Coates, IN Bahadur, "Liquid Crystals: Applications and Uses, Volume 1, World Scientific, 1990, p275) micro-encapsulated and polymer dispersed liquid crystals (eg For example, Fergason et al. 1984, US Pat. No. 4,435,047, SEIKO, EP 0 749 031 A1, Doane et al., Appl. Phys, Lett., 1986 v48 p269 and Coates et al. US Pat. No. 5,604,612; , 1976 British Patent No. 1 442 360); electric field induction of a diffraction grating of refractive index in nematic liquid crystals (Huignard et al., 1987, US Pat. No. 4,630,091, Canon US Pat. No. 4,878,742); ferroelectric liquid crystals with patterned electrodes Many devices, including (O'Callaghan, Handschy, 1990, US Pat. No. 5,182,665) use this effect.
[9] Other liquid crystal devices operate on the principle of optical absorption anisotropy to identify different states. The performance of this type of device is usually greatly enhanced by adding polychromatic dyes to the liquid crystal material. One example of this type of device is a guest host mode cholesteric (Taylor, White 3,833,287, 1974).
[10] Recently, novel grating surfaces have been disclosed in which one or more stability directions of nematic directors exist. Bigrating structures that lead to bistable surfaces with different azimuthal orientations (ie, directors in the plane of the cell or different orientations of the average direction of the liquid crystal molecules) are described in British Patent No. 2,286,467-A and US Pat. 5,796,459. The local director is planar to the surface and the two surface orientations are stabilized by precise control of the grating pitches, amplitude and degree of brightness.
[11] Novel surfaces are disclosed in British Patent Application No. 9521106.6 and International Application WO97 / 14990 and British Patent No. 2,318,422, wherein a single lattice surface having a vertically oriented local director has two different angles of inclination in the same plane. Causes a stable state. The surface is used to form a Zenithal Bistable Device (ZBD). The device has significantly improved switching characteristics compared to the azimuthal bistable device of British Patent No. 2,286,467-A, since the torque applied by an electric field applied perpendicular to the substrate acts on the same plane as the two steady state directors. to be. Due to the initial bistable surface, there is at least one state that includes a defect or disclination of the director field, and one state called a continuous state that does not include the defects. For example, British Patent No. 2,318, 422 describes a defect state that causes a low pretilt of a nematic director spaced a predetermined distance away from the grating surface (typically corresponding to the grating pitch), and a continuous state that causes a high preliminary tilt. Existing bistable surfaces present are disclosed. It should be noted that pre-tilt is used herein to mean the angle of the director with respect to the cell plane.
[12] Common problems with many conventional liquid crystal display devices include narrow viewing angles, lack of contrast and reflectivity, poor switching performance, inefficiency in power usage, and difficulty in manufacturing large areas. Moreover, liquid crystal devices are frequently used for light control in other applications, including privacy windows. Often, a problem in these applications is the need for continuous power application.
[1] TECHNICAL FIELD The present invention relates to liquid crystal devices, and more particularly, to a modulation device operating with or without a single polarizer, wherein modulation is generated by diffraction, scattering or absorption of incident light.
[37] 1 is a plan view of a matrix multiplex address type liquid crystal display.
[38] 2 is a cross-sectional view of the display of FIG.
[39] 3A and 3B illustrate the use of a mask and the conventional direction of illumination onto the photoresist used to form the grating structure.
[40] 4 is a cross-sectional view of an asymmetrical grating plane suitable for providing initial bistable alignment.
[41] 5A, 5B, and 5C are plan views and two side views of one cell wall capable of modulating light in a single direction, in an embodiment of the invention.
[42] 6A and 6B schematically illustrate an electrically converting molecular arrangement for a cell having the alignment of FIG. 5.
[43] 7A, 7B and 7C show, in schematic form, a top view and two side views of the gratings on the cell wall;
[44] FIG. 8 shows a two-dimensional plot of the grating profile for modulating light polarized in two orthogonal directions as used in FIG. 7.
[45] 9A, 9B and 9C are similar to FIG. 8 but include square regions having a flat surface between the grating regions.
[46] 10A, 10B, and 10C are similar to FIG. 8 but include flat surface spaces between each grating region.
[47] 11A, 11B and 11C are similar to FIG. 10 but with asymmetric inversion between neighboring grating regions.
[48] FIG. 12 shows a two-dimensional plot of another embodiment of a grating formed by dipoles. FIG.
[49] FIG. 13 shows one cell wall with regular shaped grating regions varying in regions with different grating alignment directions and profiles. FIG.
[50] FIG. 14 shows one cell wall with irregularly shaped grating areas varying in areas with different grid alignment directions and profiles. FIG.
[51] FIG. 15 shows one cell wall with irregularly shaped grating regions where the grating is bilattice, with grating alignment directions and bistable profiles varying within different regions. FIG.
[52] FIG. 16 shows one cell wall with different shaped grating regions where the grating alignment direction changes within each grating region. FIG.
[53] FIG. 17 illustrates a grating region formed by a plurality of protrusions whose width, height and spacing dimensions may provide bistable alignment.
[54] FIG. 18 is a schematic side view of the cell with the alignment of FIG. 17 in two transition states; FIG.
[55] FIG. 19 illustrates a grid region formed by a plurality of blind holes whose width, height and spacing dimensions can provide bistable alignment.
[56] 20 is a side view of the cell wall with the arrangement of FIG. 19 in two transition states;
[57] 21 shows a metal mask for manufacturing the gratings of FIGS. 7 and 8.
[58] 22, 23 and 24 are micrographs of bistable cells converted to their two states, prepared using the mask of FIG. 21, showing latching.
[59] 25, 26 and 27 show the resulting diffraction patterns for a cell resulting from the devices of FIGS. 22, 23 and 24.
[60] FIG. 28 shows graphical output of a two-dimensional fragment from a three-dimensional numerical simulation of a director profile in a continuous state surrounding a single cylindrical protrusion having the same height and diameter.
[61] Figures 29A and 29B show 40 times the texture of the cell between the cross polarizers, with one inner surface having the vertically oriented dilatation of Figure 12, in which the cell is shown in two states: a) defective and b) continuous. Magnified micrograph.
[62] FIG. 30 shows a plot of transmission versus time for the cell of FIG. 29 when driven by alternating 30V, 2ms dipole pulses with a duty ratio of 1000: 1.
[63] FIG. 31 illustrates the light transmission of the cell of FIG. 29 as a function of the orientation of the cell when viewed between crossed polarizers using an a × 10 objective lens.
[64] FIG. 32 shows the contrast ratio as a function of the orientation of the cell of FIG. 29 when viewed between crossed polarizers using an a × 10 objective lens. FIG.
[65] FIG. 33 illustrates response time versus pulse amplitude to achieve latching between both states for the cells of FIGS. 29 and 35.
[66] FIG. 34 is a photograph of a laser beam incident on a screen after passing through the shallow dilatent cell of FIG. 29 after latching in a) defective (scattered) and b) continuous (non-scattered) states.
[67] FIG. 35 is a micrograph of a second cell similar to that used in FIG. 29 but showing deeper dilatation, showing two states: a) defective and b) continuous.
[68] FIG. 36 shows the optical response of the cell of FIG. 35 to an alternating polarity pulse (pulse peak amplitude is 40V with a duration of 500 Hz).
[69] FIG. 37 is an enlarged view of FIG. 36 showing a slow transition from a continuous (less scattering, diffraction or absorption) state with a transition time of 80 ms to a defect (more scattering, diffraction or absorption) state.
[70] FIG. 38 is an enlarged view of FIG. 36 showing rapid defect to continuous state transition with a transition time of 4 ms. FIG.
[71] FIG. 39 is a photograph of a laser beam incident on a screen after passing through the deep dilatation cell of FIG. 35 already latched in a) a defective (scattered) state and b) a continuous (nonscattered) state.
[72] FIG. 40 is a schematic diagram of another embodiment of the present invention in which both inner surfaces of the liquid crystal device are fabricated to form initial bistable regions of different orientation, with regions of monostable vertical alignment.
[73] 41, 42 and 43 are sectional views of another embodiment of the present invention.
[13] According to the invention, the problems are a liquid crystal cell which can be switched between two bistable states of high light scattering (or absorption) state and very low light scattering (or absorption) state, for example a transmission state. Is reduced. Scattering states are obtained by small surface features on one or both cell walls that cause local deviations in molecular orientation. Suitably the surface features are provided by a lattice structure or suitably arranged surface relief structure.
[14] According to the present invention, there is provided a liquid crystal device comprising a layer of nematic liquid crystal material received between an electrode structure and two cell walls each having an alignment surface,
[15] An alignment layer having a primary modulation and a secondary modulation is provided in at least one cell wall,
[16] The primary modulation is formed by a plurality of small (<15 μm) alignment regions each having a profiled surface and a vertically oriented surface that provide a bistable pre-slope alignment and an alignment direction for liquid crystal molecules,
[17] The secondary modulation is formed by the spacing and / or surface alignment direction of the small alignment region,
[18] The device is characterized in that it can be switched between a light transmission state and a light transmission state.
[19] According to another aspect of the invention, there is provided a liquid crystal device comprising a layer of nematic liquid crystal material received between two cell walls each having an electrode structure and an alignment surface, the liquid crystal device comprising:
[20] An alignment layer is provided on the at least one cell wall, the alignment layer individually generating a small local deviation of molecular orientation, and collectively a plurality which can cause large variations in molecular orientation across the layer. Small surface features, wherein the local surface alignment of the liquid crystal molecules in the surface features is vertical alignment, and the device can be switched between a light transmissive or reflective state and a light nontransmissive or reflective state. It is done.
[21] For example, a small alignment area (surface features) of size <15 μm may be formed of a plurality of lattice areas, protrusions, or blind holes, separated by an area of monostable alignment, which is usually a vertical alignment. Can be. Suitably, the alignment in the lattice regions or the like provides a bistable switchable state to the liquid crystal material in which the bistable states have different values of preliminary slopes. Alignment features can be changed in adjacent areas. Lattice regions and the like can have a uniform or non-uniform size, shape, and alignment direction. If the grid areas are of uniform size as in a display application, the deviation in the alignment direction may be the same for each or multiple areas so that the entire display is formed. Within each region, a gradient variation can be provided to provide a grayscale effect by depending on the amplitude of the applied voltage.
[22] The liquid crystal material may be nematic, long pitch cholesteric, (or chiral nematic), or smectic.
[23] The present invention further provides that, on one or both interior surfaces, an alignment direction resulting from a grating of either low energy states or low energy states is further modulated in one or more directions in the surface plane relative to the surface of British Patent No. 2 318 422. In addition to the requirements, the prior art US Pat. No. 5,796,459 and UK Pat. No. 2,318,422 have to be local vertically oriented dipole structures arranged to provide two states with different preliminary inclinations. Use alignment grids similar to those disclosed in the call. The initial bistable of British Patent No. 2 318 422, with two bistable states having different preliminary inclinations, is more suitable than the asymmetric bistable of US Pat. No. 5,796,459 because it allows for optimal electro-optic performance, as described below. It is a form used in various embodiments.
[24] Simple devices can be constructed that provide a monostable alignment and cause a reduction in refractive index variation when the liquid crystal director is redirected in response to an electric field to which electro-optic modulation is applied.
[25] However, significantly improved operation is possible by ensuring that the surface causes initial bistable in certain areas of the cell. In such devices, one of the two states is high diffraction, high scattering or superabsorbent, and the other state is low diffraction, low scattering or low absorption. The two states can be selected using electrical pulses of appropriate voltage, polarity, period and shape.
[26] Many properties can be changed to maximize scattering to provide good brightness (and contrast) of the scattering device. This is particularly true of reflective mode devices that use backscattered light to provide a bright state. First, backscattering is maximized when refractive index modulation occurs over a length scale shorter than the incident wavelength (typically [lambda] / 5). Of these fine features in the initial bistable grating that induce high backscattering of the optical wavelength Although manufacturing is difficult in practice, it has been found that satisfactory results are possible by using surface features of 0.2 μm to 2 μm pitch. This is because stabilized binding cores at surface features such as peaks and troughs provide additional centers of scattering. Moreover, it has been found that the extent to which the defect core increases the backscattering degree is related to the orientation regulation energy of the surface, and the elastic modulus of the liquid crystal.
[27] These properties also affect the adjacent surface director profile in the continuous state (and therefore scattering and contrast ratio in the small scattering state) and the electrical switching properties. However, it has been found that the defect structure itself plays a secondary role in scattering, and the grating structure itself is a significant factor in controlling light scattering. This results in a refractive index variation associated with defects and the like concentrated very close to the grating surface, and the elastic distortion is sharply weakened to a uniform director profile within 1 micron or very far from the surface. Changing its alignment from one part of the surface to the next ensures a very high degree of scattering, which is done by second order modulations of the grating profile.
[28] Another important factor for maximizing both forward and back scattering is the birefringence [Delta] n and thickness of the liquid crystal layer, ie the cell gap d. The birefringence should be as high as possible, but due to material limitations (such as having appropriate phase transition temperature, chemical stability, low viscosity, etc.), Δn is usually in the range of 0.18 to 0.25 at the optical wavelength. Similarly, cell gap is limited by other conditions including switching voltage and contrast ratio. It has been found that good brightness and contrast are obtained in typical cell gaps in the range of approximately 10 μm ≦ d ≦ 50 μm for use in optical systems.
[29] However, for devices that rely on flexo-electric effects to latch between bistable states, the use of such high cell spacings that compromise the device's performance makes the electric field threshold higher. Because of this, cell gaps in the range of 3 μm ≦ d ≦ 6 μm are also used. Alternatively, the two-frequency effect of identifying between the states can be used to switch cells at higher intervals since the dielectric switching is an RMS voltage effect and independent of d. The surface pretilt at which the grating is provided to the liquid crystal director at predetermined intervals within the cell depends on the degree of asymmetry of the grating shape.
[30] To ensure maximum scattering, the device is designed close to the symmetrical grating shape such that the preliminary slope is close to zero. This means that at proper polarization, the two bistable states have a maximum difference in refractive index (ie, nearly complete Δn) from one scattering center to the next scattering center.
[31] Improved contrast can also be achieved by matching the normal light refractive index of the liquid crystal to the normal light refractive index of the grating material (eg, photoresist). This helps to provide a better "dark" state by reducing scattering in the continuous state. Thus, careful optimization of the liquid crystal composition, surface layer composition and surface profile are respective important factors for improving device performance.
[32] Alternatively, the devices of the present invention can be operated using the principle of absorption rather than scattering. For example, a suitable dye is mixed into the liquid crystal at a concentration typically in the range of 0.5% to 5% by weight, usually 3% by weight before the device is charged. Considering this liquid crystal, Δn plays a smaller role, and the optical contrast and brightness are dictated by factors such as dye order anisotropy and dye absorption anisotropy in the liquid crystal host.
[33] The most important factor and basic principle of the invention is the design of the grating surface, in particular in the form of secondary modulation. Many different structures are possible and the selection is frequently defined by the field of application. Common to each of the structures described above is that the grating surface is modulated with two or more length scales, and / or two orthogonal dimensions parallel to the plane of the substrate.
[34] In one embodiment of the invention, a homeotropic mono grating structure as used in GB 2 318 422 is configured in a single groove direction, but has two or more modulation amplitudes of different pitch (or pitches). The first modulation is a lattice structure that results in good bistable states that differentiate the pretilt of the liquid crystal director, and the second modulation of higher pitch than the first modulation causes the regions to have one of the different values of the pretilt, or the liquid crystal director To provide a single mono-stable orientation of. In this form, the cell may be latched into two or more steady states where there is a modulation of cell delay or absorption in the direction of the surface modulations.
[35] In a preferred embodiment of the invention, the grating is modulated in such a way that it is in two directions (or more directions) within the surface plane. These secondary modulations can have a predetermined pitch from the same as that of the first modulation used to align the liquid crystal molecules to many times this distance. As an example, the modulation used to obtain the bistable alignment may have periodicity L1 for the device operating at optical wavelengths, and the secondary modulation may have periodicity L2 = 10L1. It may be appropriate to use L2> 10L1 for longer wavelengths (eg IR). Therefore, the surface is arranged to provide an alignment of nematic liquid crystal molecules, which changes in the direction crossing the surface on the length scale of the same order as the magnitude of the wavelength of the incident light to be modulated (ie, between λ / 10 to 10λ). . These wavelengths may be near infrared to ultraviolet wavelengths (eg, 200 nm to 12 μm).
[36] The cell wall is typically a glass material, but can be made of a rigid or flexible plastic material. For large devices, spacers may be included in the liquid crystal material, or gratings may include internal spacers. The grating may be complemented by internal metal or other reflectors, color filters, polymer walls or dot spacers, absorbers, collimator diffuser sheets, and the like.
[74] The display of FIGS. 1 and 2 comprises a liquid crystal cell 1 formed of a layer 2 of nematic or long pitch cholesteric liquid crystal material received between glass walls 3, 4. The spacer ring 5 keeps the walls typically arranged 1-50 μm apart. For some embodiments, a layer thickness of 1-6 μm is used, and for others the 10-50 μm spacing is used. In addition, multiple beads of the same dimension can be dispersed in the liquid crystal to maintain accurate wall spacing. By way of example, strip-shaped column electrodes 6 made of SnO ₂ or ITO (indium tin oxide) are formed on one wall 3, and a similar row electrode 7 is formed on the other wall 4. In m-column and n-row electrodes, this forms an m × n matrix of addressable elements or pixels. Each pixel is formed by superposition of column and row electrodes.
[75] The column driver 8 supplies a voltage to each column electrode 6. Similarly, the row driver 9 supplies a voltage to each row electrode 7. The control of the applied voltage is from the control logic 10, which receives power from the voltage source 11 and receives timing from the clock 12.
[76] On one or both sides of the cell 1 there are polarizers 13, 13 ′. In addition, as an example, an optical compensation layer 17 made of stretched polymer can be added adjacent the liquid crystal layer 2 between the cell wall and the polarizer. A partially reflective mirror or absorbing layer 16 may be arranged behind the cell 1 with the light source 15. These allow the display to be seen in reflections, and also to allow the faint ambient light to be illuminated from the back. In the transmissive device, the mirror or absorber 16 may be omitted. Other embodiments may use two polarizers 13, 13 ′ as described below.
[77] Prior to assembly, one or more cell walls 3 and 4 are treated with alignment features such as surface relief gratings to provide the necessary alignment, ie monostable or bistable alignment with or without preliminary inclination. The other surface may be a plane (i.e., a few degrees of preliminary slope with alignment direction or zero) or a vertically oriented monostable surface, or a few degrees of preliminary slope with no degenerating plane surface (i.e. no good alignment direction in the plane of the cell) Level or 0).
[78] This arrangement allows each pixel to be addressed independently in both visually different states. Collectively, different states in each pixel provide the display of the necessary information. The waveforms from the addressing of each pixel may be conventional. By way of example, in a bistable grating, the waveform is WO / 005271-A1; It may be as described in GB patent application 99 / 04704.5, filed March 3, 1999.
[79] The structure of the cell shown in FIG. 2 may be modified, for example, to provide a shutter that provides an opposing privacy screen. In this case, the sheet electrodes are replaced with strip electrodes, and the entire cell is switched between those two states, for example transmission and non-transmission or diffusion.
[80] The alignment grating may be formed as shown in FIGS. 3A and 3B. A piece of indium tin oxide (ITO) coated glass to form the cell walls 3 and 4 is washed with acetone and isopropanol, and then spin coated at 3000 rpm for 30 seconds with photoresist 20 (Shipley 1805). A coating thickness of about 0.55 μm is provided. Thereafter, softbaking is performed at 90 ° C. for 30 minutes. Exposure is performed with non-vertical incidence, in this case a 60 ° angle is used. The coated cell walls 3 and 4 are exposed to light from a mercury lamp (Osram Hg / 100) of intensity 0.8 mW / cm ² for a period of about 40 to 180 seconds. The mask 19 orientation is such that the groove direction is substantially perpendicular to the plane of incidence as shown in FIGS. 3A and 3B.
[81] Exposure of the present geometry results in an asymmetric intensity distribution, thus resulting in an asymmetric grating profile as shown in FIG. 4. In the case where light is incident perpendicularly to the mask, the grating profile is symmetrical (not shown). The mask 19 is then removed, the grating is developed for 10 seconds in Shipley MF319, and then rinsed in deionized water. The photoresist 20 is then exposed to deep UV radiation (245 nm), followed by baking for 45 minutes at 160 ° using an etchant that removes the area depending on the degree of illumination received. Cures. The final shape of the photoresist surface is a grating 21 as shown by way of example in FIG. 4. As will be described below, the entire photoresist layer 20 may be formed of one or more grating regions, or only a portion of the grating 21 is left, and the remainder remains the flat surface 22.
[82] The surfaces 21 and 22 are then covered with a low energy surfactant or a polymer such as lecithin, so that the liquid crystal molecules tend to be placed locally perpendicular to the surface, i.e., in a vertical orientation interface. This shape of the surface (and therefore some of its properties) depends on several factors, which factors the depth of the grating (relative to the exposure duration), its pitch (given by the pitch of the chrome mask) and the angle of incidence of the light (Eg, the degree of asymmetry or blaze).
[83] Other fabrication techniques can be used to fabricate such surfaces (see, for example, MC Hutley, 1982, "Diffraction Grating" Academic Press pp 71-128), which are scoring, embossing, printing, lithographic, laser cutting and interfero. Includes graphics skills. A cross-sectional SEM of a typical grating used to achieve initial bistable is shown in FIG. 4. Indeed, there are some variations in these properties that are allowed while maintaining the bistable stability of the surface. By way of example, bistable may be formed for a grating having a depth of about 0.3 μm to 2.0 μm.
[84] 5 and 6 illustrate one of the simplest embodiments of the invention.
[85] As shown in Figures 5A, 5B and 5C. The cell wall 4 carries the electrode 6 and the grating layer 21. Grating 21 has an area of primary grating Gb, each of which has a profile similar to that of FIGS. 3A and 3B to provide initial bistable. That is, liquid crystal molecules can be switched between vertical alignment and planar alignment or close to alignment. These primary lattice regions Gb are interspersed with the flat regions Fm of substantially the same width as the primary regions. The grating Gb has, for example, dimensions of 0.3 μm high and 0.6 μm pitch L1. The modulation of the grating Gb and the flat surface Fm has a pitch L2, which is typically between 2 and 10 times larger than L1 (dimensions of about L2 ≒ 6 μm are illustrated). A vertically oriented coating such as lecithin is applied over both the primary grating region (Gb) and the flat surface (Fm). In this form, the liquid crystal material surface alignment is varied from the bistable lattice region Gb and the monostable vertical alignment region Fm, where the bistable lattice region is vertical alignment (vertical alignment) or by way of example of applied DC voltage. According to the sign it may be aligned parallel to the average plane of the surface, the monostable vertically oriented area is always perpendicular to the wall (4).
[86] 6A and 6B show a cell 1 formed by the wall 4 of FIG. 5 opposite the wall 3 with the electrode 7 coated with the vertical alignment layer 22 without any grating. To show. The cell 1 receives plane polarized light through the polarizer 13. In this arrangement, the region of the cell affected by the bistable primary lattice (Gb) can be either high inclination (continuous) or low inclination (defective), and the planar region (Fm) molecules are high inclination (conventionally). The primary lattice region Gb of the cell 1 is switched between two bistable states by positive and negative isostatic voltage pulses of appropriate length applied to the electrodes 6, 7. .
[87] FIG. 6A shows a nonscattering (or diffraction) or weakly scattering (or diffraction) state in which the bistable primary lattice region G and interspersed monostable flat region Fm are in a vertical (vertical alignment) alignment state.
[88] FIG. 6B shows the strong scattering (or diffraction state) in which the bistable lattice region Gb is in a low slope state. On the flat region Fm, the molecules remain in a vertical alignment. The cause of this diffraction is due to the regular phase grating formed by the liquid crystal. Light polarized in the plane of the figure (as shown) experiences strips of index of refraction that are approximately equal to the normal index of the liquid crystal material n _o interspersed with strips of near abnormal refractive index n _e . Thus, the cells form what can be called a phase grating for incident light. Bragg's well known diffraction law gives 2 (L2) sinθ = nλ, where n is an integer. When L2 is about 12 μm, the structure of FIG. 6 results in first order diffraction spots of red light (lambda = 600 nm) at an angle (setter) of ± 1.4 ° and an angle of ± 9.6 ° near infrared (IR). (Setter) results in a wavelength of lambda = 4 mu m.
[89] If the incident polarization is parallel to the grating groove in this embodiment (ie, outside of the paper plane of Figs. 6A and 6B), there is no modulation or diffraction of the refractive index. Also, if the polarization is in the plane of the paper but the light is incident at an angle away from the vertical direction, then a reduced exponential modulation is observed corresponding to the weaker diffraction.
[90] 7A, 7B and 7C show another embodiment of the cell wall 4, where the grating 21 is modulated in two orthogonal directions as shown in the two-dimensional plot of FIG. 8. FIG. 7 is a schematic diagram showing small rectangular regions each having a bistable grating profile and groove directions orthogonal in the region adjacent the wall surface. In the embodiment of FIG. 7, there are no monostable alignment regions. This schematic diagram is used in various parts of the present specification, and as in FIG. 5, the lattice period in each small square is L1, and the period in the different alignment direction is L2. The grating 21 can be formed by photolithographic techniques as shown in FIGS. 3A and 3B, which are accompanied by two steps of using a single mask specifically designed in a good pattern or accompanied by a 90 ° rotation of the mask. Can be formed by photolithographic techniques as shown in FIGS. 3A and 3B. The entire cell wall 4 is coated with a surfactant.
[91] A cell with a wall as in FIG. 7 is used with the wall 3 in FIG. 6. The cells can be switched by positive and negative dc voltage pulses to be applied either in the vertical alignment (nonscattering) of FIG. 6A or in a scattering state similar to that of FIG. 6B.
[92] In the embodiment of FIG. 7, the diffraction state has refractive index modulation for incident light polarized in both the paper plane and the direction perpendicular thereto. For example, if L1 is selected to 0.3 μm (having a lattice depth of about 0.15 μm to provide bistable alignment) and L2 is selected to 2.5 μm, then four agents for red light having an angle of 7 ° from vertical are selected. First order diffraction spots exist.
[93] 9, 10 and 11 show three additional embodiments in which variations on the wall 4 of FIG. 7 exist and there are two or more modulations in both dimensions. In these cases, the small squares of the bistable alignment grating alternately repeat the modulation directions, and the grating region is interspersed with flat regions of monostable vertical alignment. It has the effect of increasing the refractive index mismatch between adjacent areas irrespective of the incident angle of the incident light.
[94] 9B and 9C, it should be noted that the direction of the preliminary inclination on alternating grating regions is the same direction and the same in FIG. 10. In contrast, in FIG. 11, the direction of asymmetry is reversed between adjacent regions, thereby improving the angular characteristics of the device. This asymmetry is shown in the direction of arrow 23 in FIGS. 11B and 11C when the material is in its low surface oblique switching state.
[95] FIG. 12 shows a limited case in which L1 = L2 (also L1 _x = L1 _y ), that is, a initial bistable dipole is formed for the orthogonal grids. Such dilatants are already used, for example, in US Pat. No. 5,796,459 to provide bistable surface states. In this device, the dilatation results in a bistable alignment direction (ie, asymmetric bistable) with components at different angles in the substrate plane. The dilattice structure results in orthogonal sets of two grooves in the surface plane that can cause liquid crystal alignment. Although the conditions for bistableness depend on the relative shape of the two overlapping gratings, the alignment along one groove or the remainder is insensitive to the structure of each grating shape (eg, pitch and amplitude). In the present invention, the dilatometer has the additional constraint that the surface must be overcoated with a low energy treatment or formed of a low energy material, so that the local liquid crystal orientation at the surface should tend to be perpendicular along the local surface. Along with this, the second constraint is that the amplitude-to-pitch ratio, empirically generally a / L1 ≒ 0.9, in which both gratings forming the dilatation are in the range 0.1 <a / L1 <2, preferably 0.25 <a / L1 <1 (a / L1). These are the conditions that result in the initial bistable as described in UK patent application 9521106.6, patent number GB-2,318,422.
[96] In FIG. 12, the " gol " and " hill " formed by the vertically oriented dilatation may contain defect loops that result in either a net high or low inclination of the director in that region. Alternatively, the director field may be continuous for each feature and cause a uniform high slope of the director in the vicinity of the feature. This is superior to previous embodiments (eg FIGS. 7-11) that the modulation distance is shorter and therefore suitable for scattering applications where the modulation length scales are on the same order as the light wavelength.
[97] 13, 14, and 15 illustrate three embodiments that use these principles to provide scattering rather than diffraction. In previous embodiments, the grating region is regular with respect to both the alignment grating and the longer modulation length scales. Such devices are particularly useful for diffractive optical applications when used in absorption mode. Devices as shown in FIG. 7 flow when used in an absorption mode.
[98] For scatter based display applications, it is preferred that the grating regions are more irregular, as shown in the examples of FIGS. 13, 14, and 15. The grid regions of FIGS. 13 and 14 consist of different sizes, spacing and alignment directions. Between the grid regions there are flat regions coated with a surfactant to provide monostable alignment. Initial bistable single lattice (FIGS. 13 and 14) or bilattices (FIG. 15) may be used. In most grating manufacturing techniques, there is significant freedom in the possible shapes, and therefore the exact structure of the pattern used varies. However, a good scattering state is formed in the simplest form, as shown in Fig. 14, in which each provided region (or scattering center) is kept small (i.e., <10 lambda). The devices may have repetition for this irregular or random pattern over larger length scales, so that, for example, all pixels across a large area display may have a uniform degree of scattering in a defect state.
[99] 16 shows another embodiment in the form of a grating structure causing scattering. Again, the pattern is pseudo random and is designed to provide good scattering or backscattering conditions, but in contrast to the previous embodiments, the initial bistable lattice itself (ie, having the smallest period L1). Changes in the direction in the plane of the wall 4. This has the advantage that very fine features can be formed, in particular, in the center of the curvature of the grooves. Areas without lattice are flat and coated with a surfactant.
[100] FIG. 17 shows a variant of the type of FIG. 12 of the scattering surface taken for this limitation, with protrusions 25 arranged pseudorandomly on the cell wall 4. Each protrusion 25 is similar to that produced by the dilatation of FIG. The initial bistable ensures that the surface of each protrusion is coated with a suitable low energy material or formed of a suitable low energy material to induce a vertical alignment, and that each protrusion (in areas where bistable is needed) is It is brought about by ensuring that it is of the correct shape and properly spaced from its neighbors. By way of example, small cylindrical bumps spaced between 0.5D and 2D, similar in diameter and height (h ≒ D), typically cause initial bistable (these figures are known from protrusions of regular grating structures). ). In order to provide bistable, the area of the walls between the areas where the protrusions 25 are properly spaced has a local monostable vertical alignment, thereby helping to provide improved scattering. The best performance is found from a cluster of these protrusions 25 with gaps arranged to provide different degrees of scattering. In addition, feature size may vary across the cell wall 4 to improve optical performance. Typically, the protrusions are from 0.1 μm to 2 μm in height, from 0.1 μm to 2 μm in diameter, and the spacing between the protrusions is from 0.1 μm to 2 μm, and each of these surfaces is required to exhibit initial stability. It is suitable to lie between 0.5 and 1.0 μm for the regions of. The protrusions can be symmetrical or asymmetrical in profile.
[101] FIG. 18 shows a side view of the cell wall 4 having the lattice layer and the electrodes 6 with the protrusions 25 as in FIG. 17. The protrusions 25 are shaped (height, sharp in diameter and shaped) and spaced apart to have substantially equal energies to provide bistable operation in which bistable plane and vertical orientation states can be electrically switched. When the area adjacent to the protrusion 25 is in the planar state (C1 to D1 and E1 to F1), this area serves as a scattering center. When the areas proximate to the protrusion 25 are in their switched vertical orientation (as in A1 to B1), very little scattering exists. Scattering can be further reduced by matching the diffraction index of the cell wall 4 with the conventional diffraction index of the liquid crystal material 2. In areas where the surface is monostable and perpendicular (B1 to C1 and D1 to E1), there is little scattering.
[102] 18 is similar to the previous embodiment shown in FIG. 6, where L2 = (3L1) / 2 in the bistable region. This allows for easier fabrication and improved scattering, since the scattering centers have a higher density and have feature sizes that can be more easily produced for the wavelength of the incident light. As in FIG. 12, the defect states of FIG. 18 in two dimensions are complex, but may have defect loops wound around the features both in the gap grooves and around the tops of the features. Domain walls generally extend from one surface to another surface, although they sometimes intersect on the same surface from one region to another, as indicated by C1, D1 and E1.
[103] FIG. 19 shows an area of the cell wall that is the initial bistable surface with the approximately opposite relief profile of FIG. 18. Here, the scattering centers are formed with blind holes 26 in the photoresist layer 20 on the cell wall 4. Again, the initial stability depends on the relative diameter, depth and spacing of the holes 26 and the vertically aligned coating alignment. This type of structure has a number of advantages over the structure of FIG. 18. First, although the arrangement of the holes is still an important factor for determining the optical scattering profile, bistable itself is less sensitive to the position of neighboring holes. In addition, bistable may, in principle, be achieved for features of about one third of the size that is possible to use structures such as those of FIG. 18. Typically, the pore diameter varies between 0.1 and 2 μm, the depth varies between 0.1 and 2 μm, and the spacing between the holes varies between 0.1 and 2 μm. This hole 26 may be symmetrical or asymmetrical in the detective.
[104] 20 schematically illustrates two electrically switched bistable states of the device. Again, domain walls from one surface to the other are marked C2, D2, E2 and F2. Between A2 and B2, the liquid crystal material is switched to a high tilt state that provides less scattering. From C2 to D2 and E2 to F2, the material is switched to its planar state and there is scattering from C2 to F2.
[105] In another embodiment, not shown, the cell wall may have a mixture of holes 26 and protrusions 25 that are present in different areas of the larger display or mixed with each other.
[106] FIG. 21 shows a picture of a chrome mask, which can be used to produce a grating structure of the type used in the embodiments of FIGS. 7 and 8. The mask is divided into a 10 μm grid, in each of which there is a series of 1 μm wide chrome strips of the type shown in FIGS. 3A and 3B.
[107] 22, 23 and 24 are micrographs of the initial bistable device manufactured according to the first embodiment of the present invention. 22 and 23 are micrographs (× 100) of the cell between the cross polarizers and when the electrical pulses of the appropriate energy are followed to latch into high and low inclination states, respectively. In both cases, the cell was imaged between cross polarizers in the vertical and horizontal directions (the groove direction is ± 45 ° relative to the polarizers). The higher transmission in FIG. 22 allows the cell domains to fully latch from high slope to low slope after removal of the electric field. The addition of the quarterwave plate (45 ° to the polarizers) indicates that the alignment directions in neighboring domains are orthogonal as shown in the micrograph of FIG. 24.
[108] 25, 26 and 27 show images of diffraction patterns generated by this device when illuminated using a HeNe laser (632.8 nm at normal incidence). The image of FIG. 25 was formed by a device in a diffractive (low slope) state and corresponds to what was observed between the cross polarizers of FIG. In this case, the laser polarization direction is horizontal, and the domain grid extends in the vertical direction and the horizontal direction. Many higher diffraction orders are clearly seen in this image. The polarization direction is now vertical, where an image was obtained with identical primary features (FIG. 26). Therefore, scattering is mainly independent of polarization. Finally, if the cell is switched to the non-diffraction state (high slope), then only zero order beams are observed (Figure 27).
[109] FIG. 28 shows the results of a simulation of a nematic liquid crystal proximate to a single protrusion as used to form the initial bistable according to FIG. 18. The simulation was done in three dimensions, but only a single two-dimensional sheet is shown for clarity. In this example, the top face is also vertically oriented, but the directors at the vertical edges are free, so a single protrusion was modeled. The result is that there is a significant deterioration of the director profile near the protrusion, but it is shown to rapidly decay in all directions from the protrusion that is uniformly vertical. This is equivalent to the continuous or non-defective state described in patent GB 2 318 422. Attempts have been made to simulate this defect condition. This was done by providing periodic boundary conditions at the edges of the simulation. As expected for a bistable system, one of two visual scenarios resulted. Either the same structure (i.e., continuous state) occurs as shown in Figure 28, or the simulation formed a number of defects and could not reach a satisfactory solution.
[110] FIG. 29 shows micrographs of a device constructed from a shallow vertical orientation dipole (described below in the sixth embodiment) after latching into a defect state (FIG. 29A) and a continuous state (FIG. 29B). In both cases, when the cross polarizers were observed at a magnification of 40 times using an optical microscope, the cell was observed to be transmissive. The picture was taken at the edge of the grid area, which corresponds to the dark part of the field of view at the bottom of both pictures. This is dark between the cross polarizers for all orientations of the cell, indicating that it is a vertical alignment region. This is expected because it corresponds to a flat monostable region. The two states were latched using alternating polarity bipolar pulses with appropriate voltage and duration. The optical response to this pulse sequence was monitored using a photodiode (with visual response filter), using the resulting transmission response shown in the oscilloscope trace of FIG.
[111] After switching to both states, permeability was monitored as the cell was rotated between the cross polarizers and the results are shown in FIG. 31. In the continuous state (lower trace), there is a small change in the measured transmission, confirming that the liquid crystal molecules are now evenly orthogonal in the volume of the sample. When latched to another, defect state (upper trace), it confirms that there is a higher level of transmission and that the liquid crystal director now contains high components in the plane of the cell. In other words, the preliminary slope of this state is lower than that of the previous continuous state. When the cell in a defective state is rotated, the texture of FIG. 29A is obviously changed, since different regions with different director orientations in the cell plane provide different transmittance depending on their respective orientations to the cross polarizer. In addition, the angle dependence, shown in FIG. 31 (upper trace), clearly indicates that the orientation of these domains is arbitrary. Although this is based around the defect structures in the grooves between the dipole projections and around the protrusion vertices, the domain walls do not form a completely regular pattern, but the defects of each other and adjacent structures to form a random structure. To interact with them. This results in worse performance of the device if the defect is regulated to follow a regular pattern of dilatations.
[112] FIG. 32 shows the contrast ratio calculated from the ratio of the results of FIG. 31. When such a device is used between cross polarizers, the average contrast is about 20. It should be appreciated that the measured contrast ratio is highly dependent on the magnification of the sample, and that the lower available magnification (five times) provides an approximate average contrast regardless of cell orientation.
[113] The amplitude and duration of the trailing pulse required for latching between the two states are shown in FIG. 33. The results are compared with the later embodiment (seventh embodiment), and both cells were found to have similar electro-optic responses to those of the prior art bistable liquid crystal devices.
[114] The cells of the sixth example were placed in the path of the HeNe laser (wavelength 628 nm) and the resulting transmission was observed on the screen. 34A and 34B show the resulting pattern for defect (scattered) and continuous (non-scattered) states, respectively.
[115] FIG. 35 shows the texture of the deeper vertically oriented dilatometer of the seventh embodiment in defect (FIG. 53A) and continuous (FIG. 35B) states using the same experimental apparatus as described in FIG. 29 described above. Comparison with FIG. 29 shows that the permeability is significantly improved and the domain size is significantly smaller.
[116] The electro-optical response for the cell of FIG. 35 is shown in FIGS. 36, 37, and 38. This indicates that bistable stability is improved over that of the shallow bilattice shown in FIG. 30. FIG. 36 shows the optical response of the cell of FIG. 35 to an alternating dipole pulse (pulse peak amplitude is 40V with a duration of 500 Hz). The slow transition from continuity to defect (FIG. 37) and the faster response return for the continuity state (FIG. 38) are also consistent with the prior art for the initial bistable device.
[117] 39A and 39B show the deviation of laser light scattering for the cell of the seventh embodiment in two states. Comparison with that of the shallow grating (FIG. 34) shows that the degree of scattering of the defect state (FIG. 39A) is significantly improved, while very weak scattering of the continuous state (FIG. 39B) is maintained.
[118] 40A and 40B show an apparatus similar to that of FIG. 6 in which like components are given like reference numerals. The apparatus has walls 3, 4 for receiving liquid crystal material 2 and a initial bistable lattice structure 21 on the inner surface of both walls 3, 4 having a vertical alignment on the walls between the gratings. . The electrode is not shown but is the same as in FIG. The back plate 30 may be present behind the cell 1. The plate 30 may be absorbent, and may be made of one or more colors, and may be uniform or different for each pixel having a different amount of absorption or reflection or different colors in each pixel. The liquid crystal material may be nematic, cholesteric, long pitch cholesteric with or without dichroic dye additives.
[119] The figure illustrates areas of the grating and flat vertical alignment areas on both surfaces where the lattice orientation is defined to the plane of the page. More generally, the grating changes in all directions parallel to the plane of the device. In addition, when both surfaces are in a defective state, there is no registration of the top and bottom surfaces so that the amount of defects in the bulk of the cell increases. 40A shows the state when both surfaces are in a high preliminary inclination state. This provides a uniform vertical alignment throughout the cell and no scattering is observed. 40B shows a possible director profile when both surfaces are in a low slope, defective state. This may provide a significantly higher degree of scattering than previous embodiments of the present invention.
[120] It is important to understand that the cell designed according to FIG. 40 is not latched between the two states shown when switched by DC fields such as monopole and dipole pulses used in all previous embodiments given in the present invention. This is because an electric field is applied across the cell, so that a DC pulse of a given polarity results in opposing field directions at both surfaces. Therefore, the device is latched by the DC electric field between one surface of the low slope and the other surface of the high slope. This problem is eliminated by using a two-frequency nematic liquid crystal such as TX2A obtained from Merck. Instead of coupling to the intrinsic flexoelectric effect in the jaws, this uses the fact that at low frequencies, the material has a positive dielectric anisotropy, and that the applied RMS results in a high slope on both surfaces (FIG. 40A). This is because the lowest electrostatic energy state during application of the low frequency field has a director parallel to the field direction that is substantially perpendicular along the surface. At sufficient voltage, the applied field latches the director close to the grating surface in a continuous state, which has the highest component of the director parallel to the field direction.
[121] Alternatively, the high frequency (typically 50 kHz or higher for TX2A having a crossover frequency of 6 kHz at 25 ° C.) latches into a low slope state on both surfaces and forms the state shown in FIG. 40B. This is because it has a director perpendicular to the electric field to which the lowest electrostatic energy is applied, thereby latching the director structure with the lowest slope when the voltage is high enough.
[122] 41, 42 and 43 show cross-sectional views of another embodiment. The simplest form of arrangement is a simple switchable scattering or diffusion device, where different degrees of scattering are maintained after the application of the switching voltage is terminated, ie when the device is bistable.
[123] 41A and 41B show an apparatus similar to that of FIG. 6, wherein like components are given like reference numerals. The device comprises a liquid crystal material 2, a vertical alignment on the inner surface of the wall 3, and a lattice structure 21 on the inner surface of the wall 4. The electrodes are not shown but are the same as in FIG. 6. Behind the cell 1 is the back plate 30. The plate 30 may be absorbent and may be made of one or more colors and may be uniform or different in color or in an amount of absorbency or reflectivity in each pixel on a pixel-by-pixel basis. The liquid crystal material may be nematic, cholesteric, long pitch cholesteric with or without dichroic dye additives.
[124] 41A shows one switching state in which the liquid crystal molecules are in a high tilt switching state. 41B shows another switching state in which selected regions are in a planar state. The device can be switched between the scattering device (FIG. 41B) and the reflecting device (FIG. 41A), and when switched to the reflecting device, the device has the same color as the backplate 30.
[125] Alternatively, the liquid crystal material 2 comprises a dye and the back plate 30 comprises a reflector. In this case, the uniform high surface tilt state of FIG. 41A has a high reflectance, and the variable planar state of FIG. 41B absorbs incident light, thereby providing optical contrast.
[126] 42A and 42B are similar to FIGS. 41A and 41B with the addition of the micro prism sheet 31. This enhances backscattering in a form similar to that described by Kenemoto et al., Page 183-186, in the International Display Conference Bulletin, Monterey, California, USA, October 13, 1994. The device is switched between non-scattering (FIG. 42A) and scattering (FIG. 42B) states. In this scattered state, some light incident on the device close to the vertical is backscattered, but most is forward scattered. This results in very poor contrast of the display. However, incorporating one or more prism sheets as shown increases the effective angle of light transmitted through the prism array combination and device. In the zero or weak scattering state, this only results in a slight loss of device resolution, but in the stronger scattering state, the transmitted angle is significantly increased to cause total internal reflection at the rear surface of the prism array. In this way, the degree of backscattering is enhanced to lose device resolution. Additional reinforcement is possible by using crossed second prism arrays with respect to the first prism array.
[127] 43 illustrates another embodiment that includes a conventional twisted nematic device cell 33 having electrodes 34, 35 arranged to provide a pixelated display and a reflective (or semi-reflective) backplate 36. Illustrated. Above the cell 30 there is a device 1 of the invention which is somewhat similar to that of FIG. 40 with the walls 3, 4 and the gratings 21 on both walls 3, 4. The area of bistable grating 21 on one wall is partially opposed to the planar area of the other wall.
[128] The conventional cell 33 has low parallax operation and high resolution in reflection or transflective mode. However, when viewed from a directional (non-diffusing) light source, the display has the disadvantages of very specular reflection and the resulting critical toxicity. The use of a diffuser fixed in front of the device is a conventional solution. In the present invention, the device 1 acts as a variable diffuser, so that the combined optical properties can be adjusted very easily with no significant increase in output loss by the complete display. The device 1 may be a single shutter covering the entire area of the display or may be selectively switched in different areas.
[129] One known switchable diffuser is described in US Pat. No. 5,831,698.
[130] Details of additional fabrication of the grating and cells are described below.
[131] First embodiment
[132] Conventional contact photoresist techniques (such as those shown in FIGS. 3A and 3B) can be used to make gratings such as those of FIGS. 5, 7, 8, 9, 10, 11 and 12. In the case of two orthogonal directions, each with a preliminary slope of the defect state resulting from the degree of brilliance or asymmetry for the grating, the light is at a predetermined angle with respect to the vertical of the surface and with respect to the direction of both gratings. It must be incident at an azimuth angle. As shown in Fig. 11, the case where the preliminary inclination direction changes over the grating is more difficult to manufacture by this method, and more easily manufactured by using the multi-beam interferographic method. Structures such as those of FIGS. 13, 14, 15, 16, 17, 18, 19 and 20 can also be fabricated using contact lithography, but zero preliminary inclination (vertical incidence of light used for crosslinking of photoresist is used). Case) or a preliminary slope that changes with the lattice direction, which results in a variable switching threshold that may be undesirable for some applications.
[133] In a first embodiment, a grating structure similar to that shown in FIGS. 7 and 8 is fabricated using a standard contact lithography process. A piece of 1.1 mm thick ITO coated glass is spin coated with a photoresist (Shipley 1805) for 30 seconds at a speed of 3000 rpm. This gives a film of 0.55 μm thickness. The surface is then soft baked at 90 ° C. for 30 minutes to remove excess solvent. The chrome mask produced using the e-beam method (see FIG. 10) is then fixed in close contact with the photoresist surface. The mask is composed of 0.5 μm chrome lines spaced by 0.5 μm, as shown in FIG. 10. The sample is exposed for 530 seconds using an unfiltered mercury lamp (0.3 mW / cm ² ). The exposure is performed at an angle of 60 degrees to the surface normal, and at components in the substrate plane at an angle of 45 degrees to both grating directions in the mask.
[134] This process results in a defect state pretilt for each part of the grid grid of 45 ° (ie, the initial bistable states are pretilts between 45 ° and 90 °). Thereafter, spin development is performed at 800 rpm for 10 seconds using Shipley MF 319, followed by cleaning in deionized water. This resulted in the formation of a grid grid surface with a 1.0 μm pitch. The photoresist was then cured by exposure to deep UV (254 nm) followed by baking at 180 ° C. for 2 hours. Finally, the surface is treated with a vertical alignment polymer (JALS 688), spun at 3000 rpm, and baked at 180 ° C. for 30 seconds to exhibit vertical alignment. Thereafter, a 4 μm liquid crystal cell is produced by placing this initial bistable grid surface on a flat vertically oriented surface using the same JALS 688 process described above. This opposing surface is formed in a similar manner to the grating surface, but by making a thinner Shipley 1805 layer (0.2 μm) without performing grating exposure. The cell is formed using an edge sealing adhesive comprising 20 μm glass bead spacers from one grating surface and one flat surface. The cell is filled with a commercial nematic liquid crystal (MLC6602; available from E. Merck, Germany) with a high Δn value to provide maximum diffraction effects, with positive dielectric anisotropy throughout the range of possible frequencies and temperatures. . Charging is carried out by capillary action of the isotropic phase followed by slow cooling to the nematic phase.
[135] Following the structure as described above, electrical contacts are made to the ITO of each substrate, and alternating switching pulses are applied at a duty cycle of 100: 1. This signal consists of rectangular pulses with a typical duration of 0.1 to 100 ms and sizes ranging from 20 to 100V. Duty ratios between 50: 1 and 500: 1 are used, with AC waveforms of frequency 1 kHz to 100 kHz and magnitude Vrms (0 V to 10 V) superimposed. Other electrical signals may be used, such as the multiplexing signal used for 9521106.6. The resulting change in texture when viewed using a light microscope between cross polarizers is shown in FIGS. 22, 23 and 24.
[136] This cell is illuminated by a helium neon laser light source and the resulting diffraction pattern is projected onto the screen. Bistable latching is obtained between diffraction and non-diffraction states, and the results are shown in FIGS. 25, 26 and 27. In addition, the cell is illuminated with a tungsten white light source and observed using pulses of appropriate polarity and appropriate duration and magnitude so that each state is electrically selected to be transparent in a state different from weak scattering in one state.
[137] Second embodiment
[138] A cell similar to that of the second embodiment is produced this time using a zinc-sulfide substrate rather than a conventional glass. This cell is then tested for use in IR by warm object imaging using an IR camera that senses a wavelength in the range of 3 to 5 μm. The contrast between the scattering and non-scattering states was found to be significantly higher than that observed at the optical wavelengths, so that clearly identifiable images within the non-scattering phase were clarified by the cell after latching into the scattering state.
[139] Third embodiment
[140] A third cell is prepared with the same procedure as in the previous embodiments, but with the cell filled with liquid crystal E7 in which 2% by weight of black dichroic dye is mixed (see for example Bahadur liquid crystal; Bahadur Liquid Crystals: Applications and Uses, Volume 3, Chapter 11, World Scientific Press). In this case, a contrast ratio of about 2: 1 was observed between the two latched states with respect to the normal incident light due to the deviation of the optical absorption between the two states. This is further improved by operating the cell in a reflective mode in which the flat surface on one side of the cell is coated with a reflective aluminum layer.
[141] Fourth embodiment
[142] In the previous embodiment, scattering is very weak and did not attract attention to the display device. This is because the magnitude of the change in alignment direction in the substrate plane is present on the length scale significantly higher than the wavelength of the incident light. In order to ensure a higher level of scattering for optical wavelengths, the substrate is manufactured using a mask having a design similar to that of FIG. 6B, where the grating pitch is 0.15 μm and the features in the constant groove direction are about 0.6 μm. Has an average width. Smaller feature sizes are achieved using an argon ion laser (see eg Hutley ibid p99 at 257 nm) used to develop deep UV photoresist (PMGI). In this embodiment, the substrate is irradiated at normal incidence. After development, the surface is coated with a fluorinated chromium complex vertically aligning surfactant and is spaced 20 탆 away from the second flat vertically oriented surface. The cell is charged with BLO36 as in the first embodiment and used for switching between the transmissive and scattering states. The device has also been found to provide moderate backscattering. This is used for display structures in which the device has no polarizers mounted in front of a dark (or colored) background. This provided a contrast ratio of about 4: 1 for vertical incident light suitable for some display applications where low power bistable and mechanical durability were the primary requirements.
[143] An additional improvement on the brightness of the backscattered state was achieved using a holographic reflector as described in US 3 910 681. This collects the incident light and partially reflects off the outgoing light, thereby providing multiple paths through the scattering device.
[144] Fifth Embodiment
[145] In addition, the method of the fourth embodiment was applied to form a surface having randomly spaced micro voids as shown in Fig. 9, wherein each hole is about 0.2 탆 deep and 0.35 탆 in diameter. This gave better scattering and non-scattering conditions than the previous examples.
[146] Sixth embodiment
[147] A pre-coated, properly etched glass substrate with ITO is spin coated with photoresist layer SU8 for 30 seconds at a spin of 3000 rpm. The sample is then soft baked at 100 ° C. for 10 minutes, then exposed to UV light for 3 minutes, and baked at 160 ° C. for 30 minutes. This layer was used to form a barrier layer over the ITO electrode. Thereafter, it was overcoated with the grating formed using the following process. The photoresist (Shipley 1813) is spun down at 3000 rpm for 30 seconds and then baked at 115 ° C. for 60 seconds to form a layer 1.55 μm thick. A single lattice mask (such as shown in FIGS. 3A and 3B) with a 1.2 μm pitch is pressed against this surface, which uses a strong UV source (1 kW OAI mercury xenon arc lamp generating 30 mW / cm ² intensity). Exposure for 6 seconds. The mask was then reoriented 90 ° and exposed again for a period of 6 seconds.
[148] Thereafter, the dilatation was developed by Shipley 319 spin coating at 800 rpm for 10 seconds, and then washed in double ion removal water. This twin lattice was then cured in strong UV and baked at 180 ° C. for 2 hours. The dilattice surface was then spun at 3000 rpm with a vertically aligned alignment polymer (JALS 688; manufactured by Japan Synthetic Rubber Company) and baked at 180 ° C. for 60 seconds. A 4.5 μm cell was constructed using a flat substrate coated with JALS 688 as with this dilatometric surface.
[149] The cell was then filled with liquid crystal material (MLC 6204) from Merck, Germany. The cell was initially cooled from the isotropic phase, forming a defect condition over the entire active area. These virgin defects are of a larger size than either of FIG. 29 or FIG. 35 and exhibit negligible scattering of the laser light. This cell was then connected to any waveform generator to supply the appropriate electrical signal. The signal used during the entire experiment is a single pulse of polarity + V and duration τ followed immediately by a pulse of -V and duration τ, followed by a period of 0V 1000τ, followed by a second dipole pulse, where This second dipole pulse is of opposite polarity (-V followed by + V).
[150] Means are provided to allow the pulse train to be stopped, with no signal applied except a cell in any of the zero field states. When a pulse train of 40 V amplitude and 3 ms slot duration was applied, the cell was observed to latch between the bright and dark states. Permeability was detected using a photodiode (and visual response filter), and temporal changes were monitored using a storage oscilloscope. The temporal response shown in FIG. 30 clearly shows the difference between the two states observed (see FIGS. 31 and 32). In the sixth embodiment, because the defects were initially incorporated, there is a decline in the optical response in the bright (defective) state. This is considered to be because the lattice is shallow.
[151] Seventh embodiment
[152] A second dipole cell was fabricated, followed by the same procedure as used in the sixth embodiment, but with a photoresist Shipley 1818 (providing a photoresist thickness of 2.18 μm) and orthogonal single gratings for a duration of 9 seconds. Each is exposed. This process results in deeper dilatation structures in an attempt to improve bistability. Both the virgin state and the latched defect state of this sample have domains smaller than those of the sixth embodiment, and the continuous state is darker even among the cross polarizers. This means that nearly double permeability is measured in the defect state and a contrast of 70: 1 is achieved. The change in bright state permeability and contrast in the sal orientation is also lower than that in the sixth embodiment. This is due in part to the absence of loss of optical state transmissivity immediately after the trailing pulse of the applied field (see FIG. 36). In addition, the seventh embodiment provides a good optical appearance when used as a device with a higher level of laser scattering.
[153] An alternative manufacturing method for random initial bistable surfaces is as follows.
[154] The initial bistable surfaces may be manufactured using techniques that are not commonly used to make gratings. The novel method used in the present invention is via mixed alignment. This method is described in Harada et al., EP 0 732 610 A2, in which two or more polymers of different solubility are mixed in a solvent and spin-coated onto a suitable substrate to act as the microdrop surface energy of the substrate to control the droplet size and shape. Described in the heading. In a fifth embodiment of this patent, polymer (PAS) and poly 4 vinylbiphenyl are mixed in N-methyl pyrrolidone (NMP) solvent to provide a concentration of 3% by weight in a ratio of 10: 1. Thereafter, spin coating and baking for 1 hour at 200 ° C. resulted in a 50 nm thick tomb with irregularly spaced surface protrusions about 30 nm high and 50 nm in diameter. In the present invention, this surface is then coated with a low energy surfactant such as a fluorinate chromium complex or silane (eg, ZLI 3334) orthogonal agent. Although some areas remain monostable when in a defective state, the contrast is poor due to relatively high scattering levels in other states, but the high density of very small scattering centers causes very high scattering conditions. This is a common problem for many non-lattice methods because it makes it difficult to achieve a certain level of surface control. However, adding surfactants in the polymer solution to help control the microdroplet size has been found to allow some improvement. Other examples may also include the use of two immiscible alignment alignment polymers, and the use of one polymer with different solubility in two immiscible solvents and the like.
[155] Similar techniques can also be used to produce microporous surfaces, where the alignment layer is formed in the same form as PDLC (ie, "Liquid", for example, "liquid crystal" in Bahadur, "Liquid"). Crystals ": the use of optical, thermal or solvent induced phase separation (PIPS, TIPS or SIPS) methods reviewed in Applications and Uses, Volume 1, World Scientific, 1990, P361). This monomer containing solvent (sometimes used in conjunction with a suitable optical initiator, when a PIPS process is employed) is spun down to provide a surface film having a precisely controlled thickness.
[156] Surfaces of the type shown in FIGS. 17, 18, 19 and 20 are possible through careful control of solution concentration, temperature and humidification properties of the lower surface. Alternatively, fine aerosol sprays of monomer droplets can be used and cured (thermally and / or optically) to coat the vertically oriented surface and coated with the vertically oriented surfactant, if desired. In this example, the initial surfactant coating functions as an alignment agent for the liquid crystal, and also humidifies to ensure well formed, beveled features of accurate formation to increase the contact angle of the droplets before curing to provide initial bistable. Function as zero.

权利要求:
Claims (30)
[1" claim-type="Currently amended] In a liquid crystal device comprising a layer 2 of nematic liquid crystal material received between the electrode structures 6, 7 and the two cell walls 3, 4 respectively supporting the alignment surface 21.
With alignment layers 21, 22 on at least one cell wall 4, having both primary and secondary modulation,
The primary modulation is formed by a plurality of small (<15 μm) alignment regions each having a profiled surface and a vertically oriented surface that provide a bistable pre-slope alignment and an alignment direction for liquid crystal molecules,
The secondary modulation is formed by the spacing and / or surface alignment direction of the small alignment region (FIGS. 5-20),
Thereby, the device can be switched between a light transmission state and a light transmission state.
[2" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein the plurality of small alignment regions are formed by a plurality of lattice regions (21).
[3" claim-type="Currently amended] 3. The liquid crystal device of claim 2, wherein the lattice regions comprise a single lattice structure (FIGS. 5, 7, 9, 10, 11) and / or a dilatent structure (FIG. 12).
[4" claim-type="Currently amended] 2. A liquid crystal device according to claim 1, wherein each small alignment region is formed by a plurality of protrusions (25).
[5" claim-type="Currently amended] 2. A liquid crystal device according to claim 1, wherein each small alignment region is formed by a plurality of blind holes (26).
[6" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein the secondary modulation is formed by distinguishing a plurality of small alignment regions having regions of vertically aligned surface alignment (FIGS. 5, 7, 9, and 11).
[7" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein said secondary modulation is formed by changing the alignment direction of adjacent small alignment regions (FIG. 7).
[8" claim-type="Currently amended] The liquid crystal device of claim 1, wherein the plurality of small surface features are arranged to provide alignment in a plurality of different directions.
[9" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein said plurality of small alignment regions have a regular shape (FIGS. 5 to 11).
[10" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein the plurality of small alignment regions have an irregular shape (FIGS. 14, 15, and 16).
[11" claim-type="Currently amended] The liquid crystal device of claim 1, wherein the plurality of small alignment regions are continuous in one or more directions.
[12" claim-type="Currently amended] The liquid crystal device of claim 2, wherein the gratings are a series of symmetrical or asymmetrical grooves.
[13" claim-type="Currently amended] 3. The liquid crystal device according to claim 2, wherein the gratings are a series of symmetrical or asymmetrical grooves in which the direction of the groove changes in at least some of the alignment regions.
[14" claim-type="Currently amended] 3. The liquid crystal device according to claim 2, wherein the periodicity in the lattice regions is L1, and the period is uniform in each alignment region (Figs. 13, 14, 15).
[15" claim-type="Currently amended] 3. The liquid crystal device according to claim 2, wherein the periodicity in the lattice regions is L1, and the period is variable in each alignment region.
[16" claim-type="Currently amended] The method of claim 2, wherein the grating regions are separated by regions having a vertically aligned surface alignment,
The combination of the lattice regions and the regions of the vertical alignment is a liquid crystal device in which L2 is periodic.
[17" claim-type="Currently amended] 2. Liquid crystal device according to claim 1, wherein one cell wall (3) has a vertically aligned surface treatment.
[18" claim-type="Currently amended] 17. The liquid crystal device according to claim 16, wherein the periodicity L2 varies from a value equal to the periodicity L1 (Fig. 12) to 10L1 in the lattice regions.
[19" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein said liquid crystal material contains a predetermined amount of dichroic dye.
[20" claim-type="Currently amended] 2. Liquid crystal device according to claim 1, wherein the device comprises at least one polarizer (13, 13 ').
[21" claim-type="Currently amended] 4. The liquid crystal device according to claim 3, wherein the grating has a groove having an amplitude of a and a period of L1, wherein 01 <a / L1 <0.75.
[22" claim-type="Currently amended] The liquid crystal device of claim 1, wherein the nematic layer thickness is between 1 µm and 50 µm.
[23" claim-type="Currently amended] 2. Liquid crystal device according to claim 1, wherein the electrode structures (6, 7) are formed of column electrodes on one cell wall and row electrodes on another cell wall to form an xy matrix of addressable pixels or display elements.
[24" claim-type="Currently amended] 24. The liquid crystal device of claim 23, wherein the primary and secondary variations are constant within each pixel.
[25" claim-type="Currently amended] The method of claim 23, wherein the primary and secondary modulations vary within each pixel,
A liquid crystal device in which at least a plurality of pixels have the same change.
[26" claim-type="Currently amended] 2. Liquid crystal device according to claim 1, wherein the electrode structures (6, 7) are sheet electrodes, whereby the entire cell can be switched between two different levels of light transmission states.
[27" claim-type="Currently amended] The liquid crystal device according to claim 1, wherein the liquid crystal material (2) is a chiral nematic or smear material.
[28" claim-type="Currently amended] 2. Liquid crystal device according to claim 1, wherein the device is sandwiched between crossed polarizers (13, 13 ').
[29" claim-type="Currently amended] In a liquid crystal device comprising a layer 2 of nematic liquid crystal material received between electrode structures 6, 7 and two cell walls 3, 4 respectively supporting the alignment surfaces 21, 22.
One or more cell walls, formed by a plurality of small (<15 μm) lattice regions each providing bistable alignment to liquid crystal molecules having a plurality of lattice regions providing a plurality of alignment directions (FIGS. 7-16) With the alignment layer 21 on (4),
The grating region is separated by regions having a monostable high surface tilt alignment,
Thereby, the device can be switched between a light transmission state and a light transmission state.
[30" claim-type="Currently amended] In a liquid crystal device comprising a layer 2 of nematic liquid crystal material received between an electrode structure 6, 7 and two cell walls 3, 4 supporting the alignment surface 21, respectively.
With an alignment layer 21 on one or more cell walls 4,
The alignment layer is formed of a plurality of small (<15 μm) surface features,
Each of the small surface features can independently cause small local changes in molecular orientation, and can collectively cause a larger change in molecular orientation across the layer 2, whereby the device is in a light transmissive state. And a liquid crystal device capable of switching between a light nontransmissive state.

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同族专利:

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公开号 | 公开日

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JP2003515788A|2003-05-07|

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AU1532701A|2001-06-12|

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EP1234207B1|2005-07-20|

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US20090002617A1|2009-01-01|

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GB9928126D0|2000-01-26|

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AT300058T|2005-08-15|

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US8384872B2|2013-02-26|

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EP1234207A1|2002-08-28|

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DE60021416D1|2005-08-25|

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DE60021416T2|2006-05-24|

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TW550422B|2003-09-01|

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WO2001040853A1|2001-06-07|

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CA2392452A1|2001-06-07|

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US7471362B1|2008-12-30|

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CN1433529A|2003-07-30|

引用文献:

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公开号 | 申请日 | 公开日 | 申请人 | 专利标题

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法律状态:
1999-11-30|Priority to GB9928126.3

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1999-11-30|Priority to GBGB9928126.3A

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2000-11-23|Application filed by 키네티큐 리미티드

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2000-11-23|Priority to PCT/GB2000/004447

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2002-12-20|Publication of KR20020095165A

优先权:

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申请号 | 申请日 | 专利标题

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GB9928126.3|1999-11-30|

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GBGB9928126.3A|GB9928126D0|1999-11-30|1999-11-30|Bistable nematic liquid crystal device|

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PCT/GB2000/004447|WO2001040853A1|1999-11-30|2000-11-23|Bistable nematic liquid crystal device|