JP3727643B2 - Method of manufacturing liquid crystal electro-optical device of lateral electric field drive system - Google Patents

Description

The invention disclosed in this specification relates to a method for manufacturing a liquid crystal electro-optical device having good electrical characteristics and good contrast and capable of obtaining a bright and uniform display over the entire pixel.

  A liquid crystal electro-optical device is a liquid crystal material that is generally an organic material, sandwiched between a pair of substrates, and changes the intensity of an electric field emitted from electrodes formed on the pair of substrates, thereby advancing the liquid crystal material. The light to be modulated is optically modulated.

  Therefore, if a specific electrical signal is applied to the electrode, the electrical signal can be displayed in a visually recognizable state. Furthermore, a desired image can be formed by combining a plurality of the electrodes and applying image data.

  The modulation of light in this conventionally used liquid crystal electro-optical device is performed by applying the electric field perpendicularly to the substrate and changing the electric field strength, so that the liquid crystal molecules generally have a rod shape. This is realized by changing the orientation direction of the substrate to be parallel to the substrate or perpendicular to the substrate. In this case, in general, in order to modulate light by utilizing optical anisotropy, which is one of the characteristics of the liquid crystal material, a polarizing plate is disposed in the device so that incident light becomes linearly polarized light. I was doing.

  However, a liquid crystal electro-optical device that employs such an operation method is dark and unclear when viewed from an oblique direction, even when viewing from a direction perpendicular to the display surface. There was a phenomenon of discoloration if any.

  As a method for solving such a problem of viewing angle characteristics, a method in which the direction of the electric field applied to the liquid crystal is substantially parallel to the substrate surface (hereinafter referred to as IPS mode) is disclosed in, for example, Japanese Patent Laid-Open No. 6-160878. ing. In this case, an electric field is induced between the source electrode and the common electrode formed on one substrate, and liquid crystal molecules are aligned in the direction of the electric field.

  In such an electro-optical device, since the liquid crystal molecule major axis is switched while maintaining a state parallel to the substrate, the change in the optical characteristics of the liquid crystal due to the viewing angle is small. For this reason, the light leakage due to the viewing angle, the decrease in contrast, and the like are small compared to the conventional TN and STN systems.

  In the case of the IPS mode liquid crystal electro-optical device, the active matrix method is usually used as a driving method from the viewpoint of preventing the problem of crosstalk.

  In this method, a switching element is connected to each pixel in order to control input of a video signal. When writing video data to each pixel, the switching element connected to the pixel to be input is turned on, and video data is input to the pixel (a voltage is applied to the pixel).

  At this time, the pixel can be treated as a capacitor. Therefore, in the input video data, if the switching element is turned off when the pixel is not selected, the charge (based on the video data) injected into the capacitor is held as it is. For this reason, it is possible to form an image without constantly inputting the video signal.

  However, in practice, since the capacity of the pixel alone is insufficient to hold the charge, it is a normal method to add a capacitive component (hereinafter referred to as an auxiliary capacity) to the pixel in parallel.

  The auxiliary capacitor uses a wiring for inputting a signal to a pixel or the like as one electrode, and the other electrode is arranged through an insulating film on the wiring.

  However, in general, the area occupied by the auxiliary capacitance wiring greatly reduces the aperture ratio. In particular, in the case of the IPS mode, the ratio of the pixel electrode is large, and the aperture ratio is decreased by itself. However, if the area of the auxiliary capacitance is further secured, the area of the opening is further reduced. For this reason, even if a display with a wide viewing angle was made, the screen was dark.

The present invention provides a method of manufacturing a liquid crystal electro-optical device of the lateral electric field drive system, the auxiliary capacitance is formed without decreasing the aperture ratio, a manufacturing method of a bright viewing angle wide image display capable liquid crystal electro-optical device It is to provide.

One of the inventions disclosed in this specification is:
A method of manufacturing a liquid crystal electro-optical device in which an electric field is formed in parallel with a substrate surface between a pixel electrode and a common electrode,
Forming a thin film transistor on one of the pair of substrates;
Forming a first spacer made of an electrode and a dielectric covering the electrode so as to cover the thin film transistor on the one substrate;
Forming a second spacer made of an insulator on the one substrate, spaced apart from the first spacer;
Forming the pixel electrode on a side surface of the first spacer to form a capacitor by the pixel electrode, the electrode and the dielectric, and forming the common electrode on a side surface of the second spacer;
Forming a sealing material around one of the pair of substrates;
Dropping a liquid crystal material on one substrate on which the sealing material is formed;
A step of overlapping and pressing the other of the pair of substrates on the one substrate on which the liquid crystal material is dropped.

Other aspects of the invention are:
A method of manufacturing a liquid crystal electro-optical device in which an electric field is formed in parallel with a substrate surface between a pixel electrode and a common electrode,
Forming an island-shaped silicon film, a gate electrode, and a thin film transistor having a gate insulating film between the island-shaped silicon film and the gate electrode on one of the pair of substrates;
Forming a first spacer made of an electrode and a dielectric covering the electrode so as to cover the thin film transistor on the one substrate;
Forming a second spacer made of an insulator on the one substrate, spaced apart from the first spacer;
Forming the pixel electrode on a side surface of the first spacer to form a capacitor by the pixel electrode, the electrode and the dielectric, and forming the common electrode on a side surface of the second spacer;
Forming a sealing material around one of the pair of substrates;
Dropping a liquid crystal material on one substrate on which the sealing material is formed;
A step of overlapping and pressing the other of the pair of substrates on one substrate onto which the liquid crystal material has been dropped;
And a step of attaching a polarizing plate to the outside of each of the pair of substrates.

  The liquid crystal electro-optical device disclosed in the present invention operates to rotate liquid crystal molecules in a plane parallel to the substrate in order to form an image by optical modulation using the electro-optic effect of a liquid crystal material. Therefore, the electric field applied to the liquid crystal material has a main component in a direction parallel to the substrate. As means for forming the electric field, a pair of parallel electrodes each perpendicular to the substrate is disposed on the substrate, and an electric field is formed between the electrodes. 1A and 1B are schematic views of a liquid crystal electro-optical device disclosed in the present invention. FIG. 1B shows a cross section in the A-A ′ direction in FIG.

  As shown in FIG. 1A, the liquid crystal material (103) is sandwiched between the substrates (101) and (102). If necessary, orientation means (104) and (105) are formed. Walls (106) and (107) are formed on the substrate (101). Pixel electrodes (126) and (127) are formed on both sides of the wall (106). Further, common electrodes (125) and (128) are formed on both surfaces of the wall (107).

  An electric field is formed between the pixel electrode (126) and the common electrode (125), and between the pixel electrode (127) and the common electrode (128).

  Also, as shown in FIG. 1B, video signals are input to the pixel electrodes (liquid crystal driving electrodes) (126) and (127) between the substrate (101) and the wall (106). A thin film transistor (111) to be controlled is formed.

  Furthermore, in the invention disclosed in this specification, the electrode 112 constituting one of the auxiliary capacitors is arranged in the wall 106 that supports the electrode. Specifically, as shown in FIG. 1B, the wall (106) has a configuration in which an insulator (113) is formed so as to surround the electrode (112) and the outside of the electrode (112). Yes. Using this insulator (113) as a dielectric, a capacitance is formed between the electrode (112) and the pixel electrodes (126) and (127).

  One pixel constituting the display screen is composed of a region (110) sandwiched between a pair of electrodes (125) and (128) as indicated by a dotted line in FIG. Further, since three colors of R (red), G (green), and B (blue) are necessary for a color, three areas are used, each color is assigned to each area, and these are combined to form one pixel. To do. For example, in order to perform VGA display, 640 × 480 areas are formed vertically and horizontally.

  When the liquid crystal material is driven, a voltage based on the video signal is applied to the pixel electrodes (126) and (127), and a DC voltage of 0 V or close thereto is applied to the common electrodes (125) and (128). Therefore, the voltage applied between these electrodes changes corresponding to the time change of the video signal voltage.

  On the other hand, the electrode (112) is connected to the common electrodes (125) and (128) using the periphery of the display area formed by the pixels, and is set to the same potential as the common electrode.

  Therefore, the equivalent circuit of the one pixel is as shown in FIG.

  A switching element (111) made of a thin film transistor is connected to the liquid crystal driving electrodes (126) and (127) which are pixel electrodes. Further, the liquid crystal driving electrodes (126) and (127) form a capacitor (202) (see FIG. 2) between the common electrodes (125) and (128) through the liquid crystal layer (103).

  In the invention disclosed in this specification, an inorganic material such as glass or quartz can be used as the substrate. Further, when the liquid crystal electro-optical device is intended to be lightweight, a film having a small refractive index anisotropy, such as PES, can also be used.

  As the TFT, a transistor using amorphous silicon or poly (polycrystalline) silicon as an active layer can be used. In the case of the active matrix system, the configuration of the drive element may be a known configuration performed as a stagger type or an inverted stagger type.

  In addition, when a transistor using polysilicon is used, a peripheral driver circuit for driving a liquid crystal material can be formed on a substrate on which a TFT is manufactured. The peripheral driver circuit is manufactured by the same process as that for manufacturing a TFT. It becomes possible to do. This peripheral drive circuit is formed of complementary elements combining n-ch and p-ch transistors.

  The switching element (111) is preferably a poly-Si type TFT. In particular, when poly-Si is used for the TFT active layer, the mobility of the active layer is larger than when a-Si is used for the TFT active layer, and characteristics equivalent to a-Si can be obtained in a smaller element region. Therefore, it is possible to miniaturize each element, and thus to increase the aperture ratio.

  In addition, when poly-Si having a high carrier mobility is used for the TFT active layer when applying a lateral electric field, a peripheral drive circuit for driving a liquid crystal material can be formed on the substrate, and the device is manufactured. Contributes to process reduction, yield improvement, and equipment price reduction.

  As the element electrode, the gate electrode and the source electrode are a metal made of Al, Ti, Ta, etc., a metal-containing material, a metal oxide, or a material containing Si, Si containing phosphorus, boron, etc., carbon, carbon The material etc. which contain can be utilized. When increasing the pixel density, signal delays at both the gate and source electrodes cannot be ignored, so it is desirable to use a material with a low volume resistivity. In addition to the above-mentioned various materials, ITO can also be used for the liquid crystal driving electrode and the common electrode. In particular, when a light-transmitting material such as ITO is used, the pixel aperture ratio can be improved.

Further, various interlayer insulating films, TFT protective films silicon oxide (SiO ₂ ), or silicon nitride can be used. Furthermore, it is also possible to use an organic resin made of acrylic resin, polyimide, or the like.

  A wall (106) having an auxiliary capacitance electrode is disposed after the interlayer insulating film is formed. When Al is used for the auxiliary capacitance electrode (112), an insulating film (113) made of alumina can be formed on the electrode by forming the auxiliary capacitance electrode (112) and then performing anodization using the electrode as an anode. It becomes. The anodic oxidation at this time may be a known method.

  The wall (107) is formed of a suitable insulator. The pixel electrode and the common electrode are formed after the wall 107 is formed.

  As the material constituting the wall (109), polyimide, acrylic organic resin, or an insulator such as silicon oxide, silicon nitride, or silicon oxynitride is preferable.

  The material constituting the pixel electrodes (126) and (127) and the common electrodes (125) and (128) includes metal materials such as copper, aluminum, tantalum, titanium, and chromium, and ITO (indium tin oxide). Alternatively, a light-transmitting conductive material such as tin oxide or indium oxide may be used.

  Further, the walls (106) and (107) may have trapezoidal cross sections as well as rectangles. When the trapezoidal shape is used, the wall-shaped electrode can be easily manufactured. Further, the strength of the wall-like electrode itself can be increased, and the production yield is improved.

  In the case where electrodes are formed on the side portions of the walls (106) and (107), the width from the side surface to the side surface at the bottom surface is preferably 10 μm or less, more preferably 5 μm or less. When this width is 10 μm or more, the aperture ratio of the pixel cannot be obtained sufficiently.

  Further, the distance between the pixel electrode (126) and the common electrode (125) facing each other is 4 to 20 μm, preferably 6 to 15 μm.

  Further, the height of the wall (106) or (107) on which the pixel electrode (126) or the common electrode (125) is formed on the side with respect to the substrate (101), that is, the pixel electrode (126) or the common electrode (125). ), Or the height from the bottom of the walls (106) and (107) to the apex thereof is preferably 1/8 or more of the thickness of the liquid crystal cell. If the electrode height is 1/8 or less of the liquid crystal cell thickness, it is difficult to effectively form an electric field parallel to the substrate surface.

  Next, for the second substrate (102), the same kind of material as that of the first substrate (101) can be used. A black matrix is formed on the second substrate (102).

  In addition, a metal such as Cr or a black pigment was dispersed on the first substrate (101), the second substrate (102), or both of the substrates in order to shield the portion not related to display in order to improve contrast. A black matrix is formed from a resin material or the like (not shown). Further, in the case of color display, color filters of R (red), G (green), B (blue) or C (cyan), M (magenta), and Y (yellow) are formed at positions corresponding to each pixel. . The arrangement of each color of the color filter can be a stripe arrangement or a delta arrangement.

  In addition, the surface of the substrates (101) and (102) facing the liquid crystal layer 103 is subjected to alignment treatment as necessary. The alignment treatment is performed so that the liquid crystal molecules are aligned parallel to the substrate and uniaxially. As the alignment treatment, rubbing treatment or oblique vapor deposition is effective.

  For example, when a liquid crystal material having a positive dielectric anisotropy is used, the direction is 45 ° with respect to a direction perpendicular to the electrode surface, or an angle closer to that direction.

  Furthermore, in the case of a material having a negative dielectric anisotropy, the orientation is 45 ° with respect to the direction parallel to the electrode surface, 45 ° with respect to the direction perpendicular to the direction, or an angle closer to the direction parallel with the electrode surface. The direction.

  3A and 3B schematically show the alignment state of the liquid crystal material of the liquid crystal electro-optical device of the present invention. Here, as an example, a case where a material having a positive dielectric anisotropy is used is shown. 3A shows the alignment state when no electric field is applied, and FIG. 3B shows the alignment state when the electric field is applied. In this figure, as a schematic diagram, only the pixel electrodes (126) and (127), the common electrodes (125) and (128), and the polarizing plates (301) and (302) as the components on the pair of substrates are shown. The other elements, wiring, etc. are omitted.

  Since the liquid crystal electro-optical device performs display using the birefringence of the liquid crystal material, a pair of polarizing plates (301) and (302) are arranged so that their optical axes (303) and (304) are orthogonal to each other. A liquid crystal cell is sandwiched between the pair of polarizing plates. At this time, the orientation direction of the liquid crystal material (108) is parallel to the optical axis (304) of the polarizing plate (302) when the light source is on the polarizing plate (302) side in FIG.

  When no electric field is applied, as shown in FIG. 3A, the liquid crystal molecules (103) are uniaxially aligned with the major axis parallel to the substrate and parallel to the optical axis (304) of the polarizing plate (302).

  Next, when an electric field is applied from the pixel electrodes (126) and (127) (when an electric field is applied), as shown in FIG. 3B, liquid crystal molecules (108) in the vicinity of the alignment film interface having a strong alignment regulating force. Maintains the direction parallel to the optical axis (304) of the polarizing plate (302), and the liquid crystal molecules (109) in the vicinity of the center of the liquid crystal layer having a weak alignment regulating force change the optical axis by an electric field. When a liquid crystal material having a positive dielectric anisotropy is used, the major axis of the liquid crystal molecules (108) is oriented in parallel to the electric field direction.

  For this reason, for the light transmitted through the liquid crystal electro-optical device, the orientation of the liquid crystal material (108) is parallel to the optical axis (304) of the analyzer (302) in the cell when no electric field is applied. 301) cannot be transmitted, and the amount of transmitted light at this time is zero. On the other hand, when the electric field is applied, the direction of the optical axis of the liquid crystal material (301) changes, so that the incident light becomes elliptically polarized light and passes through the polarizer (301).

  In addition, although it was set as the structure which used two polarizing plates for the above, if the reflecting plate which consists of a metal etc. is formed in any one of said pair of board | substrates (101) and (102), one polarizing plate will be used. However, it is possible to manufacture a liquid crystal electro-optical device without using it, and a bright display can be realized. Further, the metallic reflector can also serve as an electrode for a pixel or the like.

  When the configuration of the present invention is adopted, a large-capacity auxiliary capacitor can be arranged without causing a decrease in the aperture ratio.

  By utilizing the invention disclosed in this specification, in a liquid crystal electro-optical device of a lateral electric field drive system, an auxiliary capacitor can be formed without reducing the aperture ratio, and a liquid crystal display that can display a bright image with a wide viewing angle. An optical device can be obtained.

  In this embodiment, an example of a method for manufacturing the liquid crystal electro-optical device of FIG. 1 is shown.

  First, a silicon oxide film is formed as a base film on a glass substrate (101) such as Corning 1737 by thermal CVD.

  Next, an amorphous silicon film is formed in a thickness of 300 to 2000, for example, 500 by plasma CVD.

  Next, crystallization was performed by thermal annealing at a temperature of 600 ° C. or lower, preferably 550 ° C. or lower. After the thermal annealing, annealing may be performed with laser light or strong light equivalent thereto to improve crystallinity.

  In particular, during thermal crystallization, a small amount of a catalyst element that promotes crystallization, such as nickel, is added to the amorphous silicon film, so that crystallization is promoted and a polysilicon film having high crystallinity on an inexpensive glass substrate. Can be formed. Details are disclosed in JP-A-6-244103.

  The silicon film thus obtained is etched to form an island-shaped silicon film (117). Next, a silicon oxide film as a gate insulating film (118) is formed in a thickness of 500 to 200, for example, 1000 by plasma CVD using TEOS.

  Thereafter, aluminum is formed to a thickness of 2000 to 6000 mm by sputtering, and this is patterned to obtain a gate electrode and a scan line (114).

  The gate electrode and scan line (114) made of aluminum may be anodized using a weak acid solution as a chemical conversion solution on the surface thereof to form a dense anodic oxide film (not shown) having a thickness of about several thousand. As a result, when forming the source and drain regions of the thin film transistor, after implanting impurity ions using the gate electrode as a mask, an offset region is formed between the channel region and the source / drain region, thereby reducing the OFF current of the thin film transistor. Contribute to. In addition, it is possible to prevent a short circuit between wirings provided in a stacked manner.

  Next, by ion doping, impurity ions are implanted into the island-like silicon region (117) in a self-aligning manner using the gate electrode (114) as a mask to give n-type or p-type conductivity.

  Note that it is effective to use a so-called monolithic type in which a peripheral driving circuit (not shown) is provided around the outer side of the active matrix region by using a thin film transistor made of polysilicon. In that case, complementary structures can be obtained by providing p-channel and n-channel thin film transistors.

  A silicon nitride film having a thickness of 3000 to 6000 mm, for example 4000 mm, is formed thereon by plasma CVD to form a first interlayer insulating film (119). This may be a silicon oxide film or a multilayer film of a silicon oxide film and a silicon nitride film.

  Next, a contact hole is formed by etching in the first interlayer insulating film (119) on the source region of the thin film transistor. A source film and a data line (115) are formed thereon by depositing and patterning an aluminum film having a thickness of 2000 to 000 mm, for example, 3000 mm, or a multilayer film of titanium and aluminum by sputtering.

  A polyimide or acrylic light-transmitting organic resin film is formed on this film at 4000 to 10000, for example, 5000 to form a second interlayer insulating film (120). Then, after providing a contact hole on the drain region of the thin film transistor 111, a conductive material, for example, a film of aluminum, copper, chromium, titanium, ITO or the like is formed and patterned by a known method such as sputtering, and the pixel electrode Line (116) is formed.

  Next, a silicon oxide film is formed as an insulating film (121) to a thickness of 1000 mm by plasma CVD.

  Next, an aluminum film having a thickness of 2000 mm is formed by sputtering and patterned to form patterns (122), (123), and (124) made of an aluminum film. Note that (122) and (124) are common lines.

  A resist mask (not shown) is disposed above the patterns (122) and (124), and an aluminum film is formed to a thickness of 6 μm by vapor deposition. Further, this is patterned to form a rectangular wall made of aluminum having a width of 3 μm and a height of 6 μm.

  The aluminum wall (112) is then anodized. Here, L-tartaric acid as an electric field solution is diluted with ethylene glycol at a concentration of 5%, and the pH is adjusted to 7.0 ± 0.2 using ammonia. The substrate is immersed in the solution, the + side of the low current source is connected, the platinum electrode is connected to the-side, a voltage is applied in a low current state of 20 mA, and a voltage of 150 mA is applied in a low voltage state to 0.1 mA. Continue oxidation until: In this way, an anodic oxide film (113) is formed to a thickness of 2000 mm.

  Next, photosensitive polyimide is applied to the entire surface of the substrate and pre-baked, and then patterned by photolithography. Thereafter, post-baking is performed to form a polyimide wall (107). Here, as shown in FIG. 7A, the cross-sectional shape is substantially rectangular, the width is about 3 μm, and the height is about 6 μm.

  It is also possible to make the cross-sectional shape of the wall (105) trapezoidal by appropriately controlling the intensity of ultraviolet rays and the mask pattern when polyimide is exposed.

  In the subsequent process, when a conductor to be a pixel electrode or a common electrode is formed, if the cross-sectional shape of the wall (107) is rectangular, adhesion of the conductor to the side surface becomes insufficient, leading to poor contact. There is. In such a case, it is particularly preferable that the cross-sectional shape of the wall (107) is a trapezoid.

  It is desirable to perform sufficient cleaning so that no polyimide is present around the bottom of the wall (107). If unnecessary polyimide is present, it is necessary to pay attention because the electrical connection between the pixel electrode or common electrode to be formed later and the pixel electrode line or common line becomes insufficient.

  Next, a contact hole is formed at the bottom in contact with the side surface of the wall (106) and in the vicinity of the side surface. Then, a common or different kind of conductor such as the common lines (122) and (124) and the pixel electrode line (116), for example, an aluminum thin film is formed by a known method such as sputtering. Further, this thin film is patterned to form pixel electrodes (126) and (127), and further common electrodes (125) and (128).

  Here, the pixel electrodes (126) and (125) form a pair, and an electric field parallel to the substrate is formed between the electrodes. Further, the pixel electrodes (127) and (128) form a pair, and an electric field parallel to the substrate is formed between the electrodes.

  In this step, auxiliary capacitors are formed between the aluminum wall (112) and the pixel electrode (126) and between the aluminum wall (112) and the pixel electrode (127).

  In the figure, the pixel electrodes (126) and (127) are shown as being separated on both sides of the wall, but a configuration across the wall is also possible.

Next, alignment films (104) and (105) made of polyimide are formed on the surfaces of the substrates (101) and (102), and rubbing is performed. Regarding the rubbing direction, when a liquid crystal material having a positive dielectric anisotropy is used, the direction is a direction that is not parallel to the electric field and forms an angle of 45 ° or less with respect to the direction parallel to the electric field. When a liquid crystal material having a negative dielectric anisotropy is used, the direction is a direction that is not perpendicular to the electric field and that forms an angle of 45 ° or smaller with respect to the direction perpendicular to the electric field. The rubbing treatment on the counter substrate (102) side is performed so as to be parallel or antiparallel to the rubbing direction on the substrate (101) side.

  Next, a sealing material (not shown) is formed around one substrate with an epoxy resin, and the substrates (101) and (102) are bonded to form a cell.

  In this embodiment, the walls (106) and (107) can also serve as a substrate interval maintaining function as a spacer. In that case, the spacer spraying step can be omitted. Of course, spacers may be dispersed as in a normal liquid crystal display device to maintain the substrate interval.

  Thereafter, a liquid crystal material is injected between the substrates through a liquid crystal injection port provided in a part of the sealing material by a vacuum injection method or the like, and then sealed.

  When it is difficult to inject the liquid crystal material due to the presence of the walls (106) and (107), the liquid crystal material is injected by dropping the liquid crystal material on one substrate and pressing the other substrate on top of each other. May be performed. Thereafter, a polarizing plate is attached to the outside of both substrates to complete the liquid crystal electro-optical device.

  In this embodiment, an operation mode of the liquid crystal electro-optical device shown in FIG. 1 will be described with reference to FIG.

  In the liquid crystal electro-optical device shown in FIG. 1, pixel electrodes (126) and (127) for applying an electric field to the liquid crystal, and two common electrodes (125) arranged corresponding to the two pixel electrodes ( 128) constitutes one pixel of the liquid crystal panel.

  In the liquid crystal electro-optical device of the present invention, as shown in Embodiment 1, the pixel electrode (126) and the common electrode (125), and the pixel electrode (127) and the common electrode (128) are substantially perpendicular to the substrate. And they are arranged substantially parallel to each other. Thereby, a uniform parallel electric field can be applied to the liquid crystal molecules (108) in the cell thickness direction (304).

  If a liquid crystal material having positive dielectric anisotropy is used here, the liquid crystal molecules (103) are polarized in the major axis direction. When an electric field is applied to the liquid crystal molecules (108), the liquid crystal molecules (108) rotate so that the major axis direction is aligned with the electric field direction.

  In the liquid crystal panel, light is transmitted and blocked by a combination of the electro-optical characteristics of the liquid crystal molecules (103) and the polarization axes of the two polarizing plates (301) and (302) sandwiching the panel.

  Here, the orientation vector orientation of the liquid crystal molecules (108) in the absence of an electric field is parallel to the polarization axis of the polarizing plate (302) as shown in FIG. 3 (a), and each of the electrodes (125) to (128). The homogeneous orientation is such that the major axis direction of the liquid crystal molecules is 45 degrees with respect to the electrode surface and parallel to the substrate surface. The alignment of liquid crystal molecules may be performed while applying a magnetic field or an electric field at the time of liquid crystal injection, or rubbing treatment may be used before liquid crystal injection.

  In this case, the polarizing axis of the polarizing plate (301) is arranged so as to be orthogonal to the polarizing plate (302). Thereby, when there is no electric field, incident light from the external light source becomes linearly polarized light through the polarizing plate 302 used as a polarizer. The linearly polarized light is incident so that the vibration direction coincides with the alignment vector of the liquid crystal. For this reason, the light whose polarization direction does not change reaches the polarizing plate (301) used as the analyzer through the liquid crystal layer. Since the vibration direction of the linearly polarized light and the polarization axis of the polarizing plate (301) are shifted by 90 degrees, this light cannot pass through the polarizing plate (301) and is in a dark state.

  Next, as shown in FIG. 3B, a parallel electric field is applied between the pixel electrode (126) and the common electrode (125) shown in FIG. 1, and between the pixel electrode (127) and the common electrode (128).

  In this case, the liquid crystal molecules (108) rotate in the electric field direction according to the strength of the electric field. When viewed in the vicinity of the substrate where the alignment force is strong, it is hardly affected by this electric field, but in a macroscopic manner, the alignment vector of the liquid crystal is aligned with the electric field direction.

  In this case, the orientation of the orientation vector of the liquid crystal molecules changes from 0 ° to a maximum angle of 45 ° with respect to the vibration direction of the incident linearly polarized light depending on the strength of the electric field. At this time, the light reaching the polarizing plate (301) changes from linearly polarized light to elliptically polarized light and becomes circularly polarized light. This light is brought into a bright state through the polarizing plate (301). When the orientation vector is 45 ° with respect to the vibration direction of the incident linear light, the light transmittance is maximized. Gray scale display is realized by the angle of this orientation vector.

  As the liquid crystal material, a liquid crystal material having negative dielectric anisotropy may be used. In this case, since the minor axis direction is aligned with the electric field direction when an electric field is applied to the liquid crystal, the orientation direction of the liquid crystal molecules with respect to the electrode and the polarization axis of the polarizing plate are set with respect to the direction when a liquid crystal material having positive dielectric anisotropy is used. The direction needs to be rotated 90 degrees.

  Since the liquid crystal electro-optical device of the present invention shown in FIG. 1 can apply a uniform electric field to the liquid crystal molecules in the cell thickness direction, the liquid crystal molecules on the side close to the counter substrate (102) can also be applied to the substrate (101). The liquid crystal molecules on the near side can be operated in substantially the same manner.

  Therefore, most liquid crystal molecules in the cell thickness direction can change the orientation vector orientation in response sufficiently to the electric field strength.

  Therefore, compared with the conventional structure in which the thin film electrode is formed on the substrate (101) side, the contrast is improved, and the rise of the display and the response characteristics can be made faster. Furthermore, color rubbing can be reduced.

1 is a schematic diagram of a liquid crystal electro-optical device of an example. FIG. The figure which shows the equivalent circuit of 1 pixel of an Example. The figure which shows the orientation state of the liquid-crystal material of the liquid-crystal electro-optical apparatus of an Example.

Explanation of symbols

101 Substrate 117 Thin film semiconductor (active layer)
111 Thin film transistor 115 Source electrode (source line)
116 Contact wiring 126 to pixel electrode electrode 127, 127 Pixel electrode 125, 128 Common electrode 107 Wall 112 made of insulator 112 Aluminum electrode (capacitance electrode)
113 Anodized film

Claims (7)

A method of manufacturing a liquid crystal electro-optical device in which an electric field is formed in parallel with a substrate surface between a pixel electrode and a common electrode,
Forming a thin film transistor on one of the pair of substrates;
Forming a first spacer made of an electrode and a dielectric covering the electrode so as to cover the thin film transistor on the one substrate;
Forming a second spacer made of an insulator on the one substrate, spaced apart from the first spacer;
Forming the pixel electrode on a side surface of the first spacer to form a capacitor by the pixel electrode, the electrode and the dielectric, and forming the common electrode on a side surface of the second spacer;
Forming a sealing material around one of the pair of substrates;
Dropping a liquid crystal material on one substrate on which the sealing material is formed;
A method of manufacturing a liquid crystal electro-optical device of a lateral electric field driving method, comprising a step of overlapping and pressing the other of the pair of substrates on one substrate onto which the liquid crystal material is dropped. A method of manufacturing a liquid crystal electro-optical device in which an electric field is formed in parallel with a substrate surface between a pixel electrode and a common electrode,
Forming an island-shaped silicon film, a gate electrode, and a thin film transistor having a gate insulating film between the island-shaped silicon film and the gate electrode on one of the pair of substrates;
Forming a first spacer made of an electrode and a dielectric covering the electrode so as to cover the thin film transistor on the one substrate;
Forming a second spacer made of an insulator on the one substrate, spaced apart from the first spacer;
Forming the pixel electrode on a side surface of the first spacer to form a capacitor by the pixel electrode, the electrode and the dielectric, and forming the common electrode on a side surface of the second spacer;
Forming a sealing material around one of the pair of substrates;
Dropping a liquid crystal material on one substrate on which the sealing material is formed;
A step of overlapping and pressing the other of the pair of substrates on one substrate onto which the liquid crystal material has been dropped;
A method of manufacturing a liquid crystal electro-optical device of a lateral electric field drive method, comprising a step of attaching a polarizing plate to the outside of each of the pair of substrates.   3. The method of manufacturing a liquid crystal electro-optical device according to claim 1, wherein the thin film transistor is formed to be an inverted stagger type. Oite to claim 2, wherein the gate insulating film manufacturing method of the liquid crystal electro-optical device of the lateral electric field drive system which is formed by a plasma CVD method using TEOS. 5. The method of manufacturing a liquid crystal electro-optical device of a lateral electric field drive method according to claim 1, wherein the pixel electrode and the common electrode are formed using a metal material or a light-transmitting conductive material. In any one of claims 1 to 5, wherein the electrode manufacturing method of the liquid crystal electro-optical device of the lateral electric field drive system which is formed by patterning the aluminum film. In any one of claims 1 to 6, wherein the first spacer and the second spacer, the cross section is transverse electric field drive system which is formed to be rectangular or trapezoidal shape of the liquid crystal electro-optical device Production method.

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