JP2004348163A - Liquid crystal display - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a liquid crystal display having the characteristics of a wide viewing angle and high display quality. <P>SOLUTION: The display has a plurality of pixel regions each defined by a first electrode formed on the liquid crystal layer side of a first substrate and by a second electrode formed on a second substrate and opposing to the first electrode via the liquid crystal layer. In each pixel region, the first electrode has a plurality of openings and filled parts. The liquid crystal layer produces a vertical alignment state when no voltage is applied between the first electrode and the second electrode: when a voltage is applied between the first electrode and the second electrode, the liquid crystal layer produces a plurality of liquid crystal domains having a radial graded alignment state in each of the plurality of openings and filled parts, and display is performed when alignment status of two or more liquid crystal domains changes according to applied voltage, corresponding to liquid crystal domain is also contribute to display in opening by oblique electric fields generating in the edges of the openings of the first electrode. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

  The present invention relates to a liquid crystal display device, and more particularly to a liquid crystal display device having a wide viewing angle characteristic and performing high-quality display.

  2. Description of the Related Art In recent years, a thin and lightweight liquid crystal display device has been used as a display device used for a display of a personal computer or a display unit of a portable information terminal device. However, the conventional twisted nematic (TN) and super twisted nematic (STN) liquid crystal display devices have a drawback of a narrow viewing angle, and various technical developments have been made to solve them. ing.

As a typical technique for improving the viewing angle characteristics of a TN type or STN type liquid crystal display device, there is a method of adding an optical compensator. As another method, there is a lateral electric field method in which an electric field in a direction horizontal to the surface of the substrate is applied to the liquid crystal layer. This horizontal electric field type liquid crystal display device has been mass-produced in recent years and has been receiving attention. Further, as another technique, a nematic liquid crystal material having a negative dielectric anisotropy is used as a liquid crystal material, and a vertical alignment film is used as an alignment film.
mation of vertical aligned phase). This is one of voltage controlled birefringence (ECB: electrically controlled birefringence) systems in which the transmittance is controlled using the birefringence of liquid crystal molecules.

  However, although the in-plane switching method is one of the methods effective as a technique for widening the viewing angle, the production margin in the manufacturing process is significantly narrower than that of a normal TN type, so that stable production is difficult. is there. This is because unevenness in the gap between the substrates and deviation in the direction of the transmission axis (polarization axis) of the polarizing plate with respect to the alignment axis of the liquid crystal molecules greatly affects the display brightness and the contrast ratio. In order to achieve stable production, further technological development is required.

  Further, in order to perform uniform display without display unevenness in a DAP type liquid crystal display device, it is necessary to control the alignment. As a method of controlling the alignment, there is a method of performing an alignment treatment by rubbing the surface of the alignment film. However, when a rubbing treatment is performed on the vertical alignment film, rubbing streaks are easily generated in a display image, and thus the method is not suitable for mass production.

  On the other hand, as a method of controlling alignment without performing a rubbing process, a method of generating an oblique electric field by forming a slit (opening) in an electrode and controlling the orientation direction of liquid crystal molecules by the oblique electric field has been devised. (For example, JP-A-6-301036 and JP-A-2000-47217). However, as a result of the study by the present inventor, in the method disclosed in the above publication, the alignment state of the region of the liquid crystal layer corresponding to the opening of the electrode is not defined, and the continuity of the alignment of the liquid crystal molecules is not sufficient. However, it is difficult to obtain a stable alignment state over the entire picture element, resulting in a rough display.

  The present invention has been made to solve the above problem, and has as its object to provide a liquid crystal display device having a wide viewing angle characteristic and high display quality.

  A liquid crystal display device according to the present invention includes a first substrate, a second substrate, and a liquid crystal layer provided between the first substrate and the second substrate, wherein the first substrate has a liquid crystal layer side. A plurality of picture element regions each defined by a first electrode provided on the second substrate and a second electrode provided on the second substrate and facing the first electrode via the liquid crystal layer, In each of a plurality of picture element regions, the first electrode has a plurality of openings and a solid portion, and a voltage is applied to the liquid crystal layer between the first electrode and the second electrode. It takes a vertical alignment state when not, and is generated at edges of the plurality of openings of the first electrode when a voltage is applied between the first electrode and the second electrode. Due to the oblique electric field, each of the plurality of openings and the solid portion takes a radially inclined orientation state. Forming a liquid crystal domain having, in response to the applied voltage is configured to perform display by the alignment state of the plurality of liquid crystal domains is changed, the object is met.

  At least some of the plurality of openings have substantially the same shape and the same size, and are configured to form at least one unit cell arranged to have rotational symmetry. Is preferred.

  The shape of each of the at least some of the plurality of openings preferably has rotational symmetry.

  Each of the at least some of the plurality of openings may be substantially circular.

  Each of the regions of the solid part (unit solid part) surrounded by the at least one opening may be substantially circular.

  Each of the solid portion regions (unit solid portions) surrounded by the at least some of the openings may have a configuration in which a corner portion is a substantially rectangular shape having a substantially circular arc shape.

  Preferably, in each of the plurality of picture element regions, the total area of the plurality of openings of the first electrode is configured to be smaller than the area of the solid portion of the first electrode.

  A projection is further provided inside each of the plurality of openings, and a cross-sectional shape of the projection in an in-plane direction of the substrate is the same as a shape of the plurality of openings, and a side surface of the projection is The liquid crystal layer of the liquid crystal layer may have an alignment regulating force in the same direction as the alignment regulating direction by the oblique electric field.

  Preferably, the plurality of liquid crystal domains are configured to assume a spiral radially inclined alignment state.

  The liquid crystal device further includes a pair of polarizing plates provided outside the first substrate and the second substrate and arranged so that polarization axes thereof are substantially orthogonal to each other. One of the pair of polarizing plates, wherein θ is an angle formed between liquid crystal molecules and the center of each of the plurality of liquid crystal domains in the display surface at 12 o'clock with respect to the display surface at 12 o'clock. Is more than 0 ° and less than 2θ with respect to the 12 o'clock direction of the display surface in the same direction as the direction in which the liquid crystal molecules located in the 12 o'clock direction of the display surface are inclined with respect to the 12 o'clock direction of the display surface. It is preferable that they are inclined at an angle of.

  More preferably, the one polarization axis of the pair of polarizing plates is inclined at an angle of more than 0 ° and θ or less, and the one polarization axis of the pair of polarizing plates is substantially the same as θ / 2. May be configured to be inclined at an angle θ, or may be configured to be inclined at substantially the same angle as θ.

  The solid portion includes a plurality of islands arranged in a matrix of m rows and n columns, and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands to one another. And the plurality of branches may be configured such that the number of branches is less than (2mn−mn).

  The first substrate further includes an active element provided corresponding to each of the plurality of picture element areas, and the first electrode is provided for each of the plurality of picture element areas, and is switched by the active element. The second electrode may be at least one counter electrode facing the plurality of pixel electrodes. The counter electrode is typically formed as a single electrode over the entire display area.

  Another liquid crystal display device according to the present invention includes a first substrate, a second substrate, and a liquid crystal layer provided between the first substrate and the second substrate. A plurality of picture element regions each defined by a first electrode provided on the layer side and a second electrode provided on the second substrate and facing the first electrode via the liquid crystal layer; In each of the plurality of picture element regions, the liquid crystal layer takes a vertical alignment state when no voltage is applied between the first electrode and the second electrode, and the first electrode is Each of the plurality of picture element regions is configured to have a plurality of openings arranged at at least corners and a solid portion, thereby achieving the above object.

  It is preferable that the shape of the region of the solid portion surrounded by at least a part of the plurality of openings has a rotational symmetry.

  A region of the solid portion surrounded by at least a part of the plurality of openings may be substantially circular.

  The region of the solid portion surrounded by at least a part of the plurality of openings may have a configuration in which a corner is a substantially rectangular shape having a substantially circular arc shape.

  The solid portion includes a plurality of islands arranged in a matrix of m rows and n columns, and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands to one another. And the plurality of branches may be configured such that the number of branches is less than (2mn−mn).

  Hereinafter, the operation will be described.

  In the liquid crystal display device of the present invention, one of a pair of electrodes for applying a voltage to the liquid crystal layer in the picture element region has a plurality of openings (portions in the electrodes where no conductive film exists) and a solid portion (electrodes). (A part other than the opening, and a part where the conductive film is present). The solid portion is typically formed from a continuous conductive film. The liquid crystal layer assumes a vertical alignment state when no voltage is applied, and forms a plurality of liquid crystal domains that assume a radially inclined alignment state due to an oblique electric field generated at an edge of the opening of the electrode when a voltage is applied. . Typically, the liquid crystal layer is made of a liquid crystal material having negative dielectric anisotropy, and the alignment is regulated by vertical alignment films provided on both sides thereof.

  The liquid crystal domains formed by the oblique electric field are formed in regions corresponding to the openings and solid portions of the electrodes, and display is performed by changing the alignment state of these liquid crystal domains according to the voltage. Since each of the liquid crystal domains has an axially symmetric orientation, the viewing angle dependence of display quality is small and the liquid crystal domain has wide viewing angle characteristics.

  Further, since the liquid crystal domains formed in the opening and the liquid crystal domains formed in the solid portion are formed by an oblique electric field generated at the edge of the opening, they are alternately formed adjacent to each other, In addition, the alignment of liquid crystal molecules between adjacent liquid crystal domains is essentially continuous. Therefore, no disclination lines are generated between the liquid crystal domains formed in the openings and the liquid crystal domains formed in the solid portions, and the display quality is not degraded, and the alignment stability of the liquid crystal molecules is maintained. Is also expensive.

  In the liquid crystal display device of the present invention, the liquid crystal molecules take a radially inclined alignment not only in the region corresponding to the solid portion of the electrode but also in the region corresponding to the opening, and therefore, compared to the above-described conventional liquid crystal display device. In addition, the continuity of alignment of liquid crystal molecules is high, a stable alignment state is realized, and a uniform display without roughness can be obtained. In particular, in order to achieve good response characteristics (fast response speed), it is necessary to apply an oblique electric field for controlling the orientation of liquid crystal molecules to many liquid crystal molecules. Need to be formed more. In the liquid crystal display device of the present invention, a liquid crystal domain having a stable radial tilt alignment is formed corresponding to the opening, so that even if a large number of openings are formed to improve the response characteristics, the display quality associated therewith is increased. (Generation of roughness) can be suppressed.

  At least a part of the plurality of openings has substantially the same shape and the same size, and is configured to form at least one unit cell arranged so as to have rotational symmetry. Since a plurality of liquid crystal domains can be arranged with high symmetry using a unit lattice as a unit, the viewing angle dependence of display quality can be improved. Further, by dividing the entire picture element region into unit cells, the orientation of the liquid crystal layer can be stabilized over the entire picture element region. For example, the openings are arranged such that the center of each opening forms a square lattice. If one picture element region is divided by an opaque component such as an auxiliary capacitance line, a unit lattice may be arranged for each region contributing to display.

  By making each of at least a part of the plurality of openings (typically, an opening forming a unit cell) into a shape having rotational symmetry, the radial shape of the liquid crystal domains formed in the openings is improved. The stability of the tilt alignment can be improved. For example, the shape of each opening (the shape when viewed from the normal direction of the substrate) is a circle or a regular polygon (for example, a square). In addition, according to the shape (aspect ratio) of the picture element or the like, a shape having no rotational symmetry (for example, an ellipse) may be used. In addition, since the shape of the region of the solid portion substantially surrounded by the opening (the “unit solid portion” described later) has rotational symmetry, the radially inclined alignment of the liquid crystal domain formed in the solid portion is achieved. Stability can be improved. For example, when the openings are arranged in a square lattice, the openings may have a substantially star shape or a cross shape, and the solid portions may have a substantially circular shape or a substantially square shape. Of course, the shape of the opening and the solid portion substantially surrounded by the opening may be substantially square.

  In order to stabilize the radially inclined alignment of the liquid crystal domains formed in the openings of the electrodes, the liquid crystal domains formed in the openings are preferably substantially circular. Conversely, the shape of the opening may be designed so that the liquid crystal domains formed in the opening are substantially circular.

  Of course, in order to stabilize the radially inclined alignment of the liquid crystal domains formed in the solid portion of the electrode, it is preferable that the region of the solid portion substantially surrounded by the opening is substantially circular. One liquid crystal domain formed in a solid portion formed from a continuous conductive film is formed corresponding to a solid portion region (unit solid portion) substantially surrounded by a plurality of openings. Is done. Therefore, the shape and arrangement of the openings may be determined so that the shape of the solid region (unit solid portion) is substantially circular.

  In any case described above, it is preferable that the total area of the openings formed in the electrodes in each of the picture element regions is smaller than the area of the solid portion. The larger the area of the solid portion, the larger the area of the liquid crystal layer (defined in the plane when viewed from the normal direction of the substrate) directly affected by the electric field generated by the electrodes, The optical characteristics (for example, transmittance) with respect to the voltage are improved.

  Whether to adopt a configuration in which the opening is substantially circular or a configuration in which the unit solid portion is substantially circular is preferably determined depending on which configuration can increase the area of the solid portion. Which configuration is preferable is appropriately selected depending on the pitch of the picture elements. Typically, when the pitch exceeds about 25 μm, it is preferable to form the opening so that the solid part is substantially circular, and when the pitch is about 25 μm or less, it is preferable to form the opening substantially circular. .

  Further, when the solid region substantially surrounded by the opening has a configuration in which the corners are substantially rectangular with a substantially circular arc shape, the radially inclined orientation is stabilized and the transmittance (effective aperture ratio) is increased. ) Is improved.

  Since the alignment regulating force generated by the oblique electric field generated at the edge of the opening formed in the electrode described above acts only when a voltage is applied, when no voltage is applied or when a relatively low voltage is applied, For example, when an external force is applied to the liquid crystal panel, the liquid crystal domain may not be able to maintain the radially inclined alignment. In order to solve this problem, a liquid crystal display device according to an embodiment of the present invention includes a side surface having an alignment control force in the same direction as the alignment control direction by the above-described oblique electric field with respect to liquid crystal molecules of a liquid crystal layer. A protrusion is provided inside the opening of the electrode. The cross-sectional shape of the convex portion in the in-plane direction of the substrate is the same as the shape of the opening, and preferably has rotational symmetry similarly to the shape of the opening described above.

  By adopting a configuration in which a plurality of liquid crystal domains take a spiral radially inclined alignment state, the alignment is further stabilized, a uniform display without roughness is realized, and the response speed is improved. The spiral radially inclined alignment state is realized, for example, by using a material obtained by adding a chiral agent to a nematic liquid crystal material having negative dielectric anisotropy. Whether it forms a clockwise spiral or a counterclockwise spiral depends on the type of chiral agent used.

  When having such a configuration and further including a pair of polarizing plates provided outside the first substrate and the second substrate and arranged so that the polarization axes are substantially orthogonal to each other, the following configuration is adopted. This makes it possible to further improve the display quality.

  Specifically, when the angle formed by the liquid crystal molecules positioned at 12 o'clock with respect to the center of the liquid crystal domain with respect to the 12 o'clock direction of the display surface is θ, the polarization axis of the polarizing plate (a pair of polarizing plates) One of the polarization axes) is inclined at an angle of more than 0 ° and less than 2θ with respect to the display surface 12 o'clock direction in the same direction as the direction in which the liquid crystal molecules are inclined with respect to the display surface 12 o'clock direction. When the polarizing plate is arranged as described above, the transmittance of light when the liquid crystal domains take a spiral radially inclined alignment state is improved, and a bright display is realized. In particular, when the polarizing plate is arranged so that the polarizing axis of the polarizing plate is inclined at substantially the same angle as θ, the light transmittance is further improved, and a brighter display is realized. When the polarizing plate is arranged so that the polarizing axis of the polarizing plate is inclined at an angle of more than 0 ° and not more than θ, a bright display is realized, and a tailing phenomenon (white tailing phenomenon and black tailing phenomenon) occurs. Is suppressed, and high-quality display is realized. In particular, when the polarizing plate is arranged such that the polarizing axis of the polarizing plate is inclined at substantially the same angle as θ / 2, the occurrence of the white tailing phenomenon and the black tailing phenomenon is substantially prevented, and higher quality is achieved. The display is realized.

  The solid portion of the electrode includes, for example, a plurality of islands and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands. Since the branches existing between the islands reduce the alignment control effect due to the oblique electric field, the narrower the width of the branches or the smaller the number of branches, the more the decrease in the alignment control effect is suppressed, and the response characteristics are improved. Is improved.

  In a case where a plurality of islands are arranged in a matrix of m rows and n columns, if branches are provided between all adjacent islands, the number of branches is (2mn-mn). By configuring the plurality of branches to be smaller than (2mn-mn) branches, a decrease in the alignment control effect is suppressed, and the response characteristics are improved.

  The liquid crystal display device according to the present invention is, for example, an active matrix type liquid crystal display device including a switching element such as a TFT for each picture element region, wherein the electrode having the above-mentioned opening is a picture element electrode connected to the switching element. And the other electrode is at least one counter electrode facing the plurality of pixel electrodes. Thus, stable radial tilt alignment can be realized only by providing an opening in one of a pair of electrodes provided to face each other with a liquid crystal layer interposed therebetween. That is, according to the known manufacturing method, when the conductive film is patterned into the shape of the pixel electrode, the photomask is simply modified so that the openings having the desired shape are formed in the desired arrangement. A liquid crystal display device can be manufactured. Of course, a plurality of openings may be formed in the counter electrode.

  In another liquid crystal display device according to the present invention, one of a pair of electrodes for applying a voltage to a liquid crystal layer in a pixel region has a plurality of openings arranged at least at corners of the pixel region, and a solid portion. When a voltage is applied between the pair of electrodes, an oblique electric field is formed at the edge of the opening of the electrode. Therefore, due to the oblique electric field generated at least at the edges of the plurality of openings arranged at the corners, the liquid crystal layer forms a liquid crystal domain that assumes a radially inclined alignment state in a voltage applied state, and thus has a wide field of view. An angular characteristic is obtained.

  A unit solid portion (a region of a solid portion substantially surrounded by an opening) existing in a certain pixel region may be a plurality of unit solid portions or an opening arranged at a corner. May be one unit solid part surrounded by. When the unit solid part existing in a certain pixel region is one unit solid part, the opening surrounding the unit solid part may be a plurality of openings arranged at the corners, A plurality of openings arranged at the corners may be continuous, substantially one opening.

  Since the region of the solid portion substantially surrounded by the opening (unit solid portion) has rotational symmetry, it is possible to enhance the stability of the radially inclined alignment of the liquid crystal domains formed in the solid portion. it can. For example, the shape of the unit solid portion may be substantially circular, substantially square, or substantially rectangular.

  When the shape of the unit solid portion is substantially circular, the radially inclined alignment of the liquid crystal domains formed in the solid portion of the electrode can be stabilized. One liquid crystal domain formed in a solid portion formed from a continuous conductive film is formed corresponding to the unit solid portion, so that the opening of the unit solid portion becomes substantially circular. What is necessary is just to determine the shape of a part and its arrangement.

  Further, when the shape of the unit solid portion is a substantially rectangular shape having a substantially arc-shaped corner portion, the stability of the radially inclined orientation and the transmittance (effective aperture ratio) can be increased.

  The solid portion of the electrode includes, for example, a plurality of islands and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands. Since the branches existing between the islands reduce the alignment control effect due to the oblique electric field, the narrower the width of the branches or the smaller the number of branches, the more the decrease in the alignment control effect is suppressed, and the response characteristics are improved. Is improved.

  In a case where a plurality of islands are arranged in a matrix of m rows and n columns, if branches are provided between all adjacent islands, the number of branches is (2mn-mn). By configuring the plurality of branches to be smaller than (2mn-mn) branches, a decrease in the alignment control effect is suppressed, and the response characteristics are improved.

  According to the present invention, a liquid crystal domain having a radially inclined orientation, which is formed corresponding to an opening formed in a picture element electrode, also contributes to display, so that the display quality of a conventional liquid crystal display device having a wide viewing angle characteristic is improved. It can be further improved.

  In addition, by providing a convex portion inside the opening of the pixel electrode, the stability of the radial tilt orientation is improved, and even if the radial tilt orientation collapses when an external force is applied, the radial tilt orientation is easily restored. And a highly reliable liquid crystal display device that can be used.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings.

(Embodiment 1)
First, the electrode structure of the liquid crystal display device of the present invention and its operation will be described. Since the liquid crystal display device according to the present invention has excellent display characteristics, it is suitably used for an active matrix type liquid crystal display device. Hereinafter, an embodiment of the present invention will be described for an active matrix liquid crystal display device using a thin film transistor (TFT). The present invention is not limited to this, and can be applied to an active matrix type liquid crystal display device using MIM or a simple matrix type liquid crystal display device. Hereinafter, embodiments of the present invention will be described with reference to a transmissive liquid crystal display device, but the present invention is not limited thereto. Can be applied.

  In the specification of the present application, a region of the liquid crystal display device corresponding to a "picture element" which is a minimum unit of display is referred to as a "picture element region". In the color liquid crystal display device, “picture elements” of R, G, and B correspond to one “pixel”. In an active matrix type liquid crystal display device, a picture element region defines a picture element region by a picture element electrode and a counter electrode facing the picture element electrode. In a simple matrix type liquid crystal display device, each region where a column electrode provided in a stripe shape and a row electrode provided orthogonal to the column electrode intersects each other defines a picture element region. Note that, in the configuration in which the black matrix is provided, strictly speaking, of the regions to which the voltage is applied according to the state to be displayed, the region corresponding to the opening of the black matrix corresponds to the pixel region. .

  The structure of one picture element region of the liquid crystal display device 100 according to the first embodiment of the present invention will be described with reference to FIGS. Hereinafter, a color filter and a black matrix are omitted for simplicity of description. In the following drawings, components having substantially the same functions as those of the liquid crystal display device 100 are denoted by the same reference numerals, and the description thereof is omitted. FIG. 1A is a top view as viewed from the normal direction of the substrate, and FIG. 1B is a cross-sectional view taken along line 1B-1B 'in FIG. 1A. FIG. 1B shows a state where no voltage is applied to the liquid crystal layer.

  The liquid crystal display device 100 is provided between an active matrix substrate (hereinafter, referred to as “TFT substrate”) 100a, a counter substrate (also referred to as “color filter substrate”) 100b, and the TFT substrate 100a and the counter substrate 100b. And a liquid crystal layer 30. The liquid crystal molecules 30a of the liquid crystal layer 30 have a negative dielectric anisotropy, and are formed by a vertical alignment layer (not shown) provided on the surface of the TFT substrate 100a and the counter substrate 100b on the liquid crystal layer 30 side. When no voltage is applied to the vertical alignment film, as shown in FIG. At this time, the liquid crystal layer 30 is said to be in a vertical alignment state. However, the liquid crystal molecules 30a of the liquid crystal layer 30 in the vertical alignment state may be slightly inclined from the normal of the surface of the vertical alignment film (the surface of the substrate) depending on the type of the vertical alignment film and the type of the liquid crystal material. In general, a state in which a liquid crystal molecular axis (also referred to as “axial direction”) is oriented at an angle of about 85 ° or more with respect to the surface of a vertical alignment film is called a vertical alignment state.

  The TFT substrate 100a of the liquid crystal display device 100 has a transparent substrate (for example, a glass substrate) 11 and picture element electrodes 14 formed on the surface thereof. The counter substrate 100b has a transparent substrate (for example, a glass substrate) 21 and a counter electrode 22 formed on the surface thereof. The alignment state of the liquid crystal layer 30 for each picture element region changes according to the voltage applied to the picture element electrode 14 and the counter electrode 22 arranged to face each other with the liquid crystal layer 30 interposed therebetween. Display is performed using a phenomenon in which the polarization state and amount of light transmitted through the liquid crystal layer 30 change with the change in the alignment state of the liquid crystal layer 30.

  The pixel electrode 14 included in the liquid crystal display device 100 has a plurality of openings 14a and a solid portion 14b. The opening 14a indicates a portion of the pixel electrode 14 formed of a conductive film (for example, an ITO film) where the conductive film is removed, and the solid portion 14b indicates a portion where the conductive film is present (other than the opening 14a). Part). The plurality of openings 14a are formed for each pixel electrode, but the solid portions 14b are basically formed of a single continuous conductive film.

  The plurality of openings 14a are arranged such that their centers form a square lattice, and are substantially surrounded by four openings 14a whose centers are located on four lattice points forming one unit lattice. The solid portion (referred to as a "unit solid portion") 14b 'has a substantially circular shape. Each of the openings 14a has a substantially star-shaped shape having four quarter-arc-shaped sides (edges) and having a rotation axis at its center four times. In order to stabilize the orientation over the entire pixel region, it is preferable to form a unit lattice up to the end of the pixel electrode 14. Therefore, as shown in the figure, the end of the pixel electrode corresponds to about one-half of the opening 14a (the area corresponding to the side) and about one-fourth of the opening 14a (the area corresponding to the corner). It is preferable that it is patterned in the shape which does.

  The openings 14a located at the center of the picture element region have substantially the same shape and the same size. The unit solid portions 14b 'located in the unit lattice formed by the openings 14a are substantially circular, have substantially the same shape and the same size. The unit solid portions 14b 'adjacent to each other are connected to each other, and constitute a solid portion 14b which functions substantially as a single conductive film.

  When a voltage is applied between the pixel electrode 14 and the counter electrode 22 having the above-described configuration, a plurality of liquid crystal domains each having a radially tilted orientation are formed by an oblique electric field generated at the edge of the opening 14a. It is formed. One liquid crystal domain is formed in each of the regions corresponding to the openings 14a and the regions corresponding to the solid portions 14b 'in the unit cell.

  Here, the square pixel electrode 14 is illustrated, but the shape of the pixel electrode 14 is not limited to this. Since the general shape of the pixel electrode 14 is approximated to a rectangle (including a square and a rectangle), the openings 14a can be regularly arranged in a square lattice. Even if the pixel electrode 14 has a shape other than a rectangle, the openings 14a are regularly (for example, in a square lattice shape as illustrated) so that liquid crystal domains are formed in all the regions in the pixel region. If it arrange | positions, the effect of this invention can be acquired.

  The mechanism by which a liquid crystal domain is formed by the above-described oblique electric field will be described with reference to FIGS. 2 (a) and 2 (b). FIGS. 2A and 2B show states in which a voltage is applied to the liquid crystal layer 30 shown in FIG. 1B, respectively. FIG. FIG. 2B schematically shows a state in which the orientation of the liquid crystal molecules 30a has begun to change (ON initial state). FIG. 2B shows that the orientation of the liquid crystal molecules 30a changed in accordance with the applied voltage is steady. The state where the state has been reached is schematically shown. Curves EQ in FIGS. 2A and 2B show equipotential lines EQ.

  When the pixel electrode 14 and the counter electrode 22 are at the same potential (when no voltage is applied to the liquid crystal layer 30), as shown in FIG. 1A, the liquid crystal molecules 30a in the pixel region are Are oriented perpendicular to the surfaces of both substrates 11 and 21.

  When a voltage is applied to the liquid crystal layer 30, a potential gradient represented by an equipotential line EQ (perpendicular to the electric force lines) EQ shown in FIG. 2A is formed. This equipotential line EQ is parallel to the surface of the solid portion 14b and the counter electrode 22 in the liquid crystal layer 30 located between the solid portion 14b of the picture element electrode 14 and the counter electrode 22. The liquid crystal layer 30 falls on a region corresponding to the opening 14a of the elementary electrode 14 and is inclined in the liquid crystal layer 30 on the edge portion of the opening 14a (around the inside of the opening 14a including the boundary (extension) of the opening 14a). An oblique electric field represented by the equipotential line EQ is formed.

  A torque acts on the liquid crystal molecules 30a having a negative dielectric anisotropy so as to orient the axis direction of the liquid crystal molecules 30a parallel to the equipotential line EQ (perpendicular to the lines of electric force). Therefore, the liquid crystal molecules 30a on the edge portion EG are clockwise in the right edge portion EG in the drawing and counterclockwise in the left edge portion EG in the drawing, as indicated by arrows in FIG. In the directions, they incline (rotate), and are oriented parallel to the equipotential lines EQ.

  Here, the change in the alignment of the liquid crystal molecules 30a will be described in detail with reference to FIG.

  When an electric field is generated in the liquid crystal layer 30, a torque acts on the liquid crystal molecules 30a having negative dielectric anisotropy so as to orient the axis of the liquid crystal molecules 30a in parallel with the equipotential line EQ. As shown in FIG. 3A, when an electric field represented by an equipotential line EQ perpendicular to the axis direction of the liquid crystal molecules 30a is generated, the liquid crystal molecules 30a are tilted clockwise or counterclockwise. Acts with equal probability of torque. Therefore, the liquid crystal molecules 30a receiving the clockwise torque and the liquid crystal molecules 30a receiving the counterclockwise torque are mixed in the liquid crystal layer 30 between the electrodes of the parallel plate type opposed to each other. As a result, the change to the alignment state according to the voltage applied to the liquid crystal layer 30 may not occur smoothly.

  As shown in FIG. 2A, at the edge EG of the opening 14a of the liquid crystal display device 100 according to the present invention, an electric field (oblique) represented by an equipotential line EQ inclined with respect to the axial direction of the liquid crystal molecules 30a. When an electric field is generated, as shown in FIG. 3B, the liquid crystal molecules 30a are inclined in a direction in which the amount of inclination for becoming parallel to the equipotential line EQ is small (counterclockwise in the illustrated example). Further, the liquid crystal molecules 30a located in a region where an electric field is generated by an equipotential line EQ perpendicular to the axial direction of the liquid crystal molecules 30a, as shown in FIG. The liquid crystal molecules 30a are tilted in the same direction as the liquid crystal molecules 30a positioned on the tilted equipotential lines EQ so that the alignment with the liquid crystal molecules 30a positioned on the line EQ is continuous (matched). As shown in FIG. 3D, when an electric field that forms a continuous uneven shape with the equipotential lines EQ is applied, the alignment regulated by the liquid crystal molecules 30a located on the respective inclined equipotential lines EQ. The liquid crystal molecules 30a positioned on the flat equipotential lines EQ are aligned so as to match the direction. Here, “located on the equipotential line EQ” means “located in the electric field represented by the equipotential line EQ”.

  As described above, the change in the alignment starting from the liquid crystal molecules 30a located on the inclined equipotential line EQ progresses, and when the liquid crystal molecules reach a steady state, the alignment state is schematically shown in FIG. 2B. Since the liquid crystal molecules 30a located near the center of the opening 14a are almost equally affected by the orientation of the liquid crystal molecules 30a at the opposite edge portions EG of the opening 14a, the liquid crystal molecules 30a are perpendicular to the equipotential lines EQ. The liquid crystal molecules 30a in a region away from the center of the opening 14a maintain the alignment state, and are inclined under the influence of the alignment of the liquid crystal molecules 30a at the near edge EG, and are symmetric with respect to the center SA of the opening 14a. Form a tilted orientation. This alignment state is such that, when viewed from a direction perpendicular to the display surface of the liquid crystal display device 100 (a direction perpendicular to the surfaces of the substrates 11 and 21), the axial orientation of the liquid crystal molecules 30a is radially aligned with respect to the center of the opening 14a. (Not shown). Therefore, in the specification of the present application, such an orientation state is referred to as “radially inclined orientation”. Further, a region of the liquid crystal layer having a radially inclined alignment with respect to one center is referred to as a liquid crystal domain.

  In regions corresponding to the unit solid portions 14b 'substantially surrounded by the openings 14a, liquid crystal domains in which the liquid crystal molecules 30a take a radially inclined alignment are also formed. The liquid crystal molecules 30a in the region corresponding to the unit solid portion 14b 'are affected by the orientation of the liquid crystal molecules 30a at the edge EG of the opening 14a, and the center SA of the unit solid portion 14b' (formed by the opening 14a). (Corresponding to the center of the unit cell).

  The radial tilt alignment in the liquid crystal domain formed in the unit solid portion 14b 'and the radial tilt alignment formed in the opening 14a are continuous, and both match the alignment of the liquid crystal molecules 30a at the edge EG of the opening 14a. Orientation. The liquid crystal molecules 30a in the liquid crystal domain formed in the opening 14a are oriented in a cone shape with the upper side (substrate 100b side) open, and the liquid crystal molecules 30a in the liquid crystal domain formed in the unit solid part 14b 'are positioned lower. The side (substrate 100a side) is oriented in an open cone shape. As described above, the liquid crystal domains formed in the openings 14a and the radially inclined alignments formed in the liquid crystal domains formed in the unit solid portions 14b 'are continuous with each other. No alignment defect) is formed, and therefore, display quality is not degraded due to generation of disclination lines.

  In order to improve the viewing angle dependency of the display quality of the liquid crystal display device in all directions, the existence probability of the liquid crystal molecules oriented along each of the azimuthal directions in each picture element region has a rotational symmetry. Preferably, and more preferably, have axial symmetry. That is, it is preferable that the liquid crystal domains formed over the entire picture element region are arranged so as to have rotational symmetry and further have axial symmetry. However, it is not always necessary to have rotational symmetry over the entire picture element region, and liquid crystal domains (for example, a plurality of liquid crystal domains arranged in a square lattice shape) arranged to have rotational symmetry (or axial symmetry) are not necessarily required. The liquid crystal layer in the picture element region may be formed as an aggregate of (liquid crystal domains). Therefore, the arrangement of the plurality of openings 14a formed in the picture element region does not necessarily have to have rotational symmetry throughout the picture element region, and is arranged so as to have rotational symmetry (or axial symmetry). The opening may be represented as a set of openings (for example, a plurality of openings arranged in a square lattice). Of course, the arrangement of the solid unit 14b 'substantially surrounded by the plurality of openings 14a is the same. In addition, since the shape of each liquid crystal domain also preferably has rotational symmetry and further has axial symmetry, the shape of each opening 14a and unit solid portion 14b 'also has rotational symmetry and further has axial symmetry. Is preferred.

  Note that a sufficient voltage may not be applied to the liquid crystal layer 30 near the center of the opening 14a, and the liquid crystal layer 30 near the center of the opening 14a may not contribute to display. That is, even if the radially inclined orientation of the liquid crystal layer 30 near the center of the opening 14a is slightly disturbed (for example, the center axis is shifted from the center of the opening 14a), the display quality may not be reduced. Therefore, it is sufficient that the liquid crystal domains formed corresponding to at least the unit solid portions 14b 'are arranged so as to have rotational symmetry and further axial symmetry.

  As described with reference to FIGS. 2A and 2B, the pixel electrode 14 of the liquid crystal display device 100 according to the present invention has a plurality of openings 14a, and the liquid crystal layer 30 in the pixel region. Inside, an electric field represented by an equipotential line EQ having an inclined region is formed. The liquid crystal molecules 30a having a negative dielectric anisotropy in the liquid crystal layer 30 in the vertical alignment state when no voltage is applied change their alignment directions by using the change in the alignment of the liquid crystal molecules 30a located on the inclined equipotential line EQ as a trigger. Then, a liquid crystal domain having a stable radially inclined alignment is formed in the opening 14a and the solid portion 14b. The display is performed by changing the orientation of the liquid crystal molecules in the liquid crystal domain according to the voltage applied to the liquid crystal layer.

  The shape (the shape viewed from the normal direction of the substrate) of the opening 14a of the picture element electrode 14 included in the liquid crystal display device 100 of the present embodiment and the arrangement thereof will be described.

  The display characteristics of a liquid crystal display device show azimuth dependence depending on the alignment state (optical anisotropy) of liquid crystal molecules. In order to reduce the azimuth angle dependency of the display characteristics, it is preferable that the liquid crystal molecules are aligned with equal probability for all azimuth angles. Further, it is more preferable that the liquid crystal molecules in each picture element region are oriented with equal probability for all azimuth angles. Therefore, it is preferable that the opening 14a has a shape that forms a liquid crystal domain such that the liquid crystal molecules 30a in each picture element region are oriented with equal probability at all azimuth angles. . Specifically, the shape of the opening 14a preferably has rotational symmetry (preferably symmetry of two or more rotational axes) with the center (normal direction) as the axis of symmetry. It is preferable that the openings 14a are arranged so as to have rotational symmetry. Also, the shape of the unit solid portion 14b 'substantially surrounded by these openings preferably has rotational symmetry, and the unit solid portion 14b is also preferably arranged to have rotational symmetry. .

  However, the openings 14a and the unit solid portions 14b do not necessarily need to be arranged so as to have rotational symmetry over the entire picture element region. For example, as shown in FIG. (Symmetry having a rotation axis) is the minimum unit, and if a picture element region is constituted by a combination of them, the liquid crystal molecules over the entire picture element region have substantially the same probability at all azimuth angles. It can be oriented.

  FIG. 4A shows an alignment state of the liquid crystal molecules 30a in a case where the substantially star-shaped openings 14a and the substantially circular unit solid portions 14b having the rotational symmetry are arranged in a square lattice shape, as shown in FIG. This will be described with reference to FIGS.

  4A to 4C schematically show the alignment state of the liquid crystal molecules 30a as viewed from the normal direction of the substrate. In FIGS. 4B and 4C, which show the alignment state of the liquid crystal molecules 30a as viewed from the normal direction of the substrate, the ends of the liquid crystal molecules 30a drawn in an elliptical shape are indicated by black dots. This shows that the liquid crystal molecules 30a are inclined such that the end is closer to the substrate side where the picture element electrode 14 having the opening 14a is provided than the other end. The same applies to the following drawings. Here, one unit lattice (formed by four openings 14a) in the picture element region shown in FIG. 1A will be described. Cross sections along diagonal lines in FIGS. 4A to 4C correspond to FIGS. 1B, 2A, and 2B, respectively, and will be described with reference to these drawings. I do.

  When the pixel electrode 14 and the counter electrode 22 are at the same potential, that is, when no voltage is applied to the liquid crystal layer 30, the vertical alignment layer (provided on the liquid crystal layer 30 side surfaces of the TFT substrate 100 a and the counter substrate 100 b) The liquid crystal molecules 30a whose alignment direction is regulated by (not shown) take a vertical alignment state as shown in FIG.

  When an electric field is applied to the liquid crystal layer 30 and an electric field represented by the equipotential line EQ shown in FIG. 2A is generated, the liquid crystal molecules 30a having a negative dielectric anisotropy have an axial orientation of equipotential. A torque is generated so as to be parallel to the line EQ. As described with reference to FIGS. 3A and 3B, the liquid crystal molecules 30a under an electric field represented by an equipotential line EQ perpendicular to the molecular axis of the liquid crystal molecules 30a have tilted liquid crystal molecules 30a. Since the direction of (rotation) is not uniquely determined (FIG. 3 (a)), the change of the orientation (tilt or rotation) does not easily occur, whereas the orientation of the liquid crystal molecule 30a is inclined. Since the tilt (rotation) direction of the liquid crystal molecules 30a placed below the potential line EQ is uniquely determined, the alignment easily changes. Therefore, as shown in FIG. 4B, the liquid crystal molecules 30a start to tilt from the edge of the opening 14a where the molecular axis of the liquid crystal molecules 30a is tilted with respect to the equipotential line EQ. Then, as described with reference to FIG. 3C, the surrounding liquid crystal molecules 30a are also tilted so as to match the orientation of the tilted liquid crystal molecules 30a at the edges of the openings 14a. In the state shown in (1), the axis direction of the liquid crystal molecules 30a is stabilized (radial tilt alignment).

  As described above, when the opening 14a has a shape having rotational symmetry, the liquid crystal molecules 30a in the picture element region move from the edge of the opening 14a toward the center of the opening 14a when a voltage is applied. Are tilted, the liquid crystal molecules 30a near the center of the opening 14a where the alignment control force of the liquid crystal molecules 30a from the edge balances maintain a state of being aligned perpendicular to the substrate surface, and the surrounding liquid crystal molecules 30a A state in which the liquid crystal molecules 30a are continuously inclined radially around the liquid crystal molecules 30a near the center of the opening 14a is obtained.

  In addition, the liquid crystal molecules 30a in a region corresponding to the substantially circular unit solid portion 14b ′ surrounded by the four substantially star-shaped openings 14a arranged in a square lattice are also generated at the edge of the opening 14a. The liquid crystal molecules 30a are tilted so as to match the alignment of the liquid crystal molecules 30a tilted by the oblique electric field. The liquid crystal molecules 30a near the center of the unit solid portion 14b 'where the alignment control force of the liquid crystal molecules 30a from the edge portion is balanced maintain a state of being oriented perpendicular to the substrate surface, and the surrounding liquid crystal molecules 30a are A state in which the liquid crystal molecules 30a are continuously tilted radially around the liquid crystal molecules 30a near the center of the real part 14b 'is obtained.

  As described above, when the liquid crystal domains in which the liquid crystal molecules 30a take a radially inclined alignment are arranged in a square lattice pattern over the entire pixel region, the existence probability of the liquid crystal molecules 30a in each axis direction has a rotational symmetry. That is, it is possible to realize a high-quality display without roughness in all viewing angle directions. In order to reduce the viewing angle dependence of the liquid crystal domain having the radially inclined alignment, the liquid crystal domain preferably has high rotational symmetry (preferably two or more rotation axes, more preferably four or more rotation axes). Further, in order to reduce the viewing angle dependence of the entire picture element region, a plurality of liquid crystal domains formed in the picture element region have high rotational symmetry (preferably two or more rotation axes, preferably four or more rotation axes). It is preferable to form an array (for example, a square lattice) represented by a combination of units (for example, a unit lattice) having (preferably).

  It should be noted that the radial tilt alignment of the liquid crystal molecules 30a is more counterclockwise or clockwise as shown in FIGS. 5B and 5C than the simple radial tilt alignment as shown in FIG. The spiral radial oblique orientation is more stable. In the spiral alignment, the alignment direction of the liquid crystal molecules 30a does not change spirally along the thickness direction of the liquid crystal layer 30 as in a normal twist alignment, but the alignment direction of the liquid crystal molecules 30a is viewed in a minute region. And almost no change along the thickness direction of the liquid crystal layer 30. In other words, the cross section at any position in the thickness direction of the liquid crystal layer 30 (the cross section in a plane parallel to the layer surface) is in the same alignment state as that shown in FIG. There is almost no twist deformation along the vertical direction. However, a certain amount of twist deformation occurs in the entire liquid crystal domain.

  When a material in which a chiral agent is added to a nematic liquid crystal material having a negative dielectric anisotropy is used, the liquid crystal molecules 30a are centered on the opening 14a and the unit solid portion 14b 'when a voltage is applied, as shown in FIG. And (c) a counterclockwise or clockwise spiral radially inclined orientation. Whether clockwise or counterclockwise depends on the type of chiral agent used. Therefore, the liquid crystal layer 30 in the opening 14a is spirally and radially inclined when voltage is applied, so that the liquid crystal molecules 30a that are radially inclined are wound around the liquid crystal molecules 30a that stand perpendicular to the substrate surface. Since the direction can be made constant in all the liquid crystal domains, uniform display without roughness can be achieved. Further, since the direction of winding around the liquid crystal molecules 30a standing perpendicular to the substrate surface is determined, the response speed when a voltage is applied to the liquid crystal layer 30 is also improved.

  When the chiral agent is added, the orientation of the liquid crystal molecules 30a changes spirally along the thickness direction of the liquid crystal layer 30, as in a normal twist orientation. In an alignment state in which the alignment of the liquid crystal molecules 30a does not spirally change along the thickness direction of the liquid crystal layer 30, the liquid crystal molecules 30a that are aligned in a direction perpendicular or parallel to the polarization axis of the polarizer are incident light. The incident light that passes through the region in such an alignment state so as not to give a phase difference does not contribute to the transmittance. On the other hand, in the alignment state in which the alignment of the liquid crystal molecules 30a changes spirally along the thickness direction of the liquid crystal layer 30, the liquid crystal molecules 30a that are aligned in a direction perpendicular or parallel to the polarization axis of the polarizing plate are also changed. In addition to giving a phase difference to the incident light, the optical rotation of the light can be used. Accordingly, the incident light passing through the region in such an alignment state also contributes to the transmittance, so that a liquid crystal display device capable of bright display can be obtained.

  FIG. 1A illustrates an example in which the opening 14a has a substantially star shape, the unit solid portion 14b ′ has a substantially circular shape, and these are arranged in a square lattice. The shape of the unit solid portion 14b 'and the arrangement thereof are not limited to the above example.

  FIGS. 6A and 6B show top views of the pixel electrodes 14A and 14B having the opening 14a and the unit solid portion 14b 'having different shapes, respectively.

  The opening portions 14a and the unit solid portions 14b 'of the pixel electrodes 14A and 14B shown in FIGS. 6A and 6B respectively correspond to the opening portions 14a and the unit solid portions of the pixel electrodes shown in FIG. The real part 14b 'has a slightly distorted shape. The opening portions 14a and the unit solid portions 14b 'of the pixel electrodes 14A and 14B have two rotation axes (no four rotation axes) and are regularly arranged so as to form a rectangular unit lattice. ing. Each of the openings 14a has a distorted star shape, and each of the unit solid portions 14b 'has a substantially elliptical shape (distorted circle). Even when the pixel electrodes 14A and 14B are used, a liquid crystal display device having high display quality and excellent viewing angle characteristics can be obtained.

  Further, picture element electrodes 14C and 14D as shown in FIGS. 7A and 7B, respectively, can be used.

  The pixel electrodes 14C and 14D have substantially cross-shaped openings 14a arranged in a square lattice so that the unit solid portions 14b 'are substantially square. Of course, these may be distorted and arranged so as to form a rectangular unit cell. As described above, even if the unit solid portions 14b 'of a substantially rectangular shape (rectangles include a square and a rectangle) are regularly arranged, a liquid crystal display device with high display quality and excellent viewing angle characteristics can be obtained. .

  However, the shape of the opening 14a and / or the unit solid portion 14b 'is preferably a circle or an ellipse rather than a rectangle because the radially inclined orientation can be stabilized. This is presumably because the sides of the opening 14a change continuously (smoothly), so that the alignment direction of the liquid crystal molecules 30a also changes continuously (smoothly).

  From the viewpoint of the continuity of the alignment direction of the liquid crystal molecules 30a described above, the pixel electrodes 14E and 14F shown in FIGS. 8A and 8B are also conceivable. The picture element electrode 14E shown in FIG. 8A is a modified example of the picture element electrode 14 shown in FIG. 1A, and has an opening 14a consisting of only four arcs. The picture element electrode 14F shown in FIG. 8B is a modified example of the picture element electrode 14D shown in FIG. 7B, and the unit solid portion 14b 'side of the opening 14a is formed in an arc. . Each of the opening portions 14a and the unit solid portions 14b 'of the pixel electrodes 14E and 14F has four rotation axes and is arranged in a square lattice (having four rotation axes). However, as shown in FIGS. 6A and 6B, the shape of the unit solid portion 14 b ′ of the opening 14 a is distorted to have a shape having two rotation axes, and a rectangular lattice (two rotation axes) is used. ).

  In the above example, the substantially star-shaped or substantially cross-shaped opening 14a is formed, and the shape of the unit solid portion 14b 'is substantially circular, substantially elliptical, substantially square (rectangular), and substantially rectangular with corners. The configuration has been described. On the other hand, the relationship between the opening 14a and the unit solid portion 14b 'may be reversed from negative to positive. For example, FIG. 9 shows a picture element electrode 14G having a pattern in which the opening 14a and the unit solid part 14b of the picture element electrode 14 shown in FIG. As described above, the pixel electrode 14G having the pattern of the negative-positive inversion has substantially the same function as the pixel electrode 14 shown in FIG. When the opening 14a and the unit solid portion 14b 'are substantially square as in the pixel electrodes 14H and 14I shown in FIGS. 10A and 10B, respectively, the negative-positive inversion is performed. In some cases, the pattern becomes the same as the original pattern.

  Like the pattern shown in FIG. 9, even when the pattern shown in FIG. 1A is inverted from the negative to the positive, the edge of the pixel electrode 14 has a unit solid portion 14 b ′ having rotational symmetry. It is preferable to form a part (about one-half or about one-fourth) of the opening 14a so that is formed. By adopting such a pattern, the effect of the oblique electric field can be obtained at the edge of the pixel region as well as at the center of the pixel region, and a stable radially inclined orientation can be obtained over the entire pixel region. Can be realized.

  Next, the picture element electrode shown in FIG. 9 having a pattern obtained by inverting the pattern of the picture element electrode 14 of FIG. 1A, the opening 14a of the picture element electrode 14 and the unit solid part 14b 'from negative to positive. Using 14G as an example, which of the negative-positive patterns should be used will be described.

  Regardless of which negative-positive pattern is employed, the length of the side of the opening 14a is the same in both patterns. Therefore, there is no difference between these patterns in the function of generating an oblique electric field. However, the area ratio of the unit solid portion 14b '(the ratio to the total area of the pixel electrodes 14) may be different between the two. That is, the area of the solid portion 16 (the portion where the conductive film actually exists) that generates the electric field used for the liquid crystal molecules of the liquid crystal layer may be different.

  Since the voltage applied to the liquid crystal domain formed in the opening 14a is lower than the voltage applied to the liquid crystal domain formed in the solid portion 14b, for example, when displaying in a normally black mode, The liquid crystal domains formed in the portion 14a become dark. That is, as the area ratio of the opening 14a increases, the display luminance tends to decrease. Therefore, it is preferable that the area ratio of the solid portion 14b is high.

  Which of the pattern in FIG. 1A and the pattern in FIG. 9 has a higher area ratio of the solid portion 14b depends on the pitch (size) of the unit cell.

  FIG. 11A shows a unit lattice of the pattern shown in FIG. 1A, and FIG. 11B shows a unit lattice of the pattern shown in FIG. 9 (however, centering on the opening 14a). Is showing. Note that, in FIG. 11A, a portion that plays a role of connecting the unit solid portions 14b 'in FIG. 1 (a branch extending from a circular portion to four sides) is omitted. The length (pitch) of one side of the square unit lattice is p, and the length of the gap (one side space) between the opening 14a or the unit solid part 14b 'and the unit lattice is s.

  Various pixel electrodes 14 having different values of the pitch p and the space s on one side were formed, and the stability of the radially inclined orientation was examined. As a result, first, an oblique electric field necessary for obtaining a radially inclined orientation is generated using the pixel electrode 14 having the pattern shown in FIG. 11A (hereinafter, referred to as a “positive pattern”). For this purpose, it has been found that the space s on one side is required to be about 2.75 μm or more. On the other hand, with respect to the picture element electrode 14 having the pattern shown in FIG. 11B (hereinafter referred to as “negative pattern”), in order to generate an oblique electric field for obtaining a radial oblique orientation, one side space s is It was found that about 2.25 μm or more was required. Using the one-sided space s as the lower limit, the area ratio of the solid portion 14b when the value of the pitch p was changed was examined. The results are shown in Table 1 and FIG.

  As can be seen from Table 1 and FIG. 11 (c), when the pitch p is about 25 μm or more, the positive (FIG. 11 (a)) pattern has a higher area ratio of the solid portion 14b and is shorter than about 25 μm. Then, the negative type (FIG. 11B) has a larger area ratio of the solid portion 14b. Therefore, from the viewpoint of the display luminance and the stability of the orientation, the pattern to be adopted changes when the pitch p is about 25 μm. For example, when three or less unit lattices are provided in the width direction of the pixel electrode 14 having a width of 75 μm, the positive pattern shown in FIG. 11A is preferable, and when four or more unit lattices are provided. Is preferably a negative pattern shown in FIG. In the case other than the exemplified pattern, either the positive type or the negative type may be selected so that the area ratio of the solid portion 14b is increased.

  The number of unit cells is obtained as follows. The size of the unit cell is calculated such that one or more integer number of unit cells are arranged with respect to the width (horizontal or vertical) of the pixel electrode 14, and the solid part is calculated for each unit cell size. Calculate the area ratio and select the unit cell size that maximizes the solid area ratio. However, when the diameter of the unit solid portion 14b ′ is less than 15 μm in the case of the positive pattern and the diameter of the opening 14a is less than 15 μm in the case of the negative pattern, the alignment regulating force due to the oblique electric field decreases, and It becomes difficult to obtain a radially inclined alignment. The lower limit of these diameters is when the thickness of the liquid crystal layer 30 is about 3 μm. If the thickness of the liquid crystal layer 30 is smaller than this, the diameters of the unit solid portion 14b ′ and the opening 14a are Even if the liquid crystal layer 30 is thicker than this lower limit, a stable radial tilt alignment can be obtained even if it is smaller than the lower limit, and the unit solid portions 14b 'and The lower limit of the diameter of the opening 14a is larger than the above lower limit.

  In addition, as described later in the second embodiment, by forming a convex portion inside the opening 14a, the stability of the radially inclined orientation can be increased. Each of the above conditions is for the case where no convex portion is formed.

  In the case where the positive pattern as shown in FIG. 11A is employed, various picture element electrodes 14 having different shapes of the unit solid portion 14b 'and the value of the space s on one side are formed, and the radially inclined orientation is stabilized. Properties and transmittance values were examined. In addition, the alignment stability when the cell thickness (the thickness of the liquid crystal layer 30) was changed was also examined. In the following study, a normally black mode liquid crystal display device equipped with an 18.1-inch SXGA panel was used.

  First, for the pixel electrode 14 having the unit solid portions 14b 'having the shapes as shown in FIGS. 12A to 12D, the pitch p is 42.5 μm, and the space s on one side is 4.25 μm, 3.5 μm. The alignment stability was evaluated when the cell thickness was changed to 2.75 μm and the cell thickness was changed to 3.70 μm and 4.15 μm. In the 18.1-inch SXGA panel, when the pitch p is 42.5 μm, the unit lattice can be arranged most efficiently (without waste in the picture element region).

  FIG. 12A is a diagram schematically showing a unit lattice of the picture element electrode 14 having the unit solid portion 14b ′ formed in a substantially circular shape, and FIGS. FIG. 12D is a diagram schematically illustrating a unit lattice of the pixel electrode 14 having a unit solid portion 14b ′ in which a corner is formed in a substantially arc-shaped substantially square shape. FIG. It is a figure which shows typically the unit lattice of the pixel electrode 14 which has a unit solid part 14b '. The unit solid part shown in FIGS. 12B and 12C has a ratio of a radius of curvature r that approximately represents the shape of a substantially arc-shaped corner to a length L of one side of the unit solid part. They differ from each other in that they are 1: 3 and 1: 4, respectively. 12 (a) to 12 (d), the portions (the branches extending from the circular portion to the four sides from the circular portion) of the unit solid portions 14b 'in FIG.

  The strength of the alignment stability can be evaluated, for example, by checking the presence or absence of an afterimage when displaying a moving image. When displaying an image in which a black square (box) moves in the background of the halftone display state, the difference in the strength of the alignment stability is likely to be reflected, and if the alignment stability is relatively weak, a white tail image is generated. Sometimes. This white tail image may occur when a nematic liquid crystal material to which a chiral agent is added is used as the liquid crystal material. The cause of the occurrence of the white trailing image will be described later, and the description thereof is omitted here.

  Table 2 shows the results of visual evaluation of the degree of occurrence of this white tailing afterimage while changing various parameters as described above. In Table 2, the shapes of the unit solid portions 14b 'shown in FIGS. 12A to 12D are shown as a circle, a barrel A, a barrel B, and a square. In Table 2, ◎ indicates that no trailing image was observed, ○ indicates that almost no trailing image was observed, and Δ indicates that a trailing image was observed.

  As shown in Table 2, with respect to the shape of the unit solid portion 14b ', orientation stability is high in the order of circle, barrel A, barrel B, and square. This is because the continuity of the alignment direction of the liquid crystal molecules 30a in the radially inclined alignment state is higher as the shape of the unit solid portion 14b 'is closer to a circle. Further, as shown in Table 2, the larger the value of the space s on one side, the higher the orientation stability. This is because the larger the value of the one-sided space s, the greater the effect of the alignment control by the oblique electric field. Further, the thinner the cell thickness, the higher the alignment stability. This is because the smaller the cell thickness, the greater the effect of the alignment control by the oblique electric field.

  In order to evaluate the alignment stability, the degree of unevenness due to pressing (after-pressing image) was also evaluated. As a result, it was confirmed that the thinner the cell thickness, the higher the alignment stability. The evaluation of the afterimage of the pressing was evaluated by examining the degree to which the alignment disorder generated when a stress was applied to the panel surface of the liquid crystal display device remained as display unevenness when the stress was removed.

  Next, the transmittance was evaluated by changing various parameters in the same manner as in the evaluation of the orientation stability. Table 3 shows the results of transmittance measurement of a liquid crystal display device having a cell thickness of 3.70 μm during white display (here, when a voltage of 6.0 V is applied to the liquid crystal layer). In Table 3, the transmittance of the liquid crystal display device using the pixel electrode 14 in which the unit solid portion 14b 'has a barrel shape B and the space s on one side is 4.25 μm is 1, and the transmittance is 1. The ratio is shown. Numerical values in parentheses in Table 3 indicate measured transmittance values (front transmittance values when the light intensity of the backlight light source during white display is 100).

  As shown in Table 3, the transmittance of the unit solid portion 14b 'is higher in the order of square, barrel B, barrel A, and circle. This is because when the value of the one-sided space s is the same, the area ratio of the solid portion 14b is higher as the shape of the unit solid portion 14b 'is closer to a square, so that the influence of the electric field generated by the electrode is reduced. This is because the area of the liquid crystal layer directly received (defined in a plane when viewed from the normal direction of the substrate) increases, and the effective aperture ratio increases. Further, as shown in Table 3, the smaller the value of the space s on one side, the higher the transmittance. This is because the smaller the value of the one-side space s, the higher the area ratio of the solid portion 14b, and thus the higher the effective aperture ratio.

  As described above, the orientation stability is higher as the shape of the unit solid portion 14b 'is closer to a circle, and the orientation stability is higher as the value of the one-sided space s is larger. In addition, the smaller the cell thickness, the higher the alignment stability.

  Further, the higher the area ratio of the solid portion 14b, the higher the effective aperture ratio. Therefore, the closer the shape of the unit solid portion 14b 'is to a square (or a rectangle), the higher the transmittance and the value of the one-sided space s becomes. The smaller the value, the higher the transmittance.

  Therefore, the shape of the unit solid portion 14b ', the value of the space s on one side, and the cell thickness may be determined in consideration of desired alignment stability and transmittance.

  As shown in FIGS. 12 (b) and 12 (c), when the unit solid portion 14b ′ has a substantially arc-shaped substantially square corner, both the alignment stability and the transmittance are relatively high. Can be. Of course, the above-described effect can be obtained even if the unit solid portion 14b 'is a substantially rectangular shape having a substantially arc-shaped corner. Strictly speaking, the corners of the unit solid portion 14b ′ formed from the conductive film are not arc-shaped, but obtuse-angled polygons (a plurality of corners exceeding 90 °) due to restrictions in the manufacturing process. (A structured shape), not only a quarter-arc shape or a regular polygonal shape (for example, a part of a regular polygon), but also a slightly distorted arc shape (a part of an ellipse) or distorted shape It may be a simple polygonal shape. Further, the shape may be formed by a combination of a curve and an obtuse angle. In the present specification, the shape including the above-mentioned shape is referred to as a substantially arc shape. For a similar reason in the manufacturing process, the substantially solid unit solid portion 14b 'as shown in FIG. 12A is not a strict circle but a polygonal shape or a slightly distorted shape. Sometimes.

  In the liquid crystal display device whose alignment stability and transmittance are shown in Tables 2 and 3, for example, by using the pixel electrode 14 in which the shape of the unit solid portion is the barrel shape B and the space s on one side is 4.25 μm. , Both the alignment stability and the transmittance can be relatively high.

  The configuration of the liquid crystal display device of Embodiment 1 described above can adopt the same configuration as a known vertical alignment type liquid crystal display device, except that the pixel electrode 14 is an electrode having an opening 14a. It can be manufactured by a manufacturing method.

  Typically, a vertical alignment layer (not shown) is formed on the surface of the pixel electrode 14 and the counter electrode 22 on the liquid crystal layer 30 side in order to vertically align liquid crystal molecules having negative dielectric anisotropy. ing.

  As the liquid crystal material, a nematic liquid crystal material having negative dielectric anisotropy is used. A guest-host mode liquid crystal display device can also be obtained by adding a dichroic dye to a nematic liquid crystal material having negative dielectric anisotropy. The guest-host mode liquid crystal display device does not require a polarizing plate.

(Embodiment 2)
The structure of one picture element region of the liquid crystal display device 200 according to the second embodiment of the present invention will be described with reference to FIGS. In the following drawings, components having substantially the same functions as the components of the liquid crystal display device 100 are denoted by the same reference numerals, and description thereof will be omitted. FIG. 13A is a top view as seen from the normal direction of the substrate, and FIG. 13B is a cross-sectional view taken along line 13B-13B ′ in FIG. 1A. FIG. 13B shows a state where no voltage is applied to the liquid crystal layer.

  As shown in FIGS. 13A and 13B, the liquid crystal display device 200 is different from the liquid crystal display device 200 in that the TFT substrate 200a has a projection 40 inside the opening 14a of the picture element electrode 14 as shown in FIG. And (b) are different from the liquid crystal display device 100 of the first embodiment. A vertical alignment film (not shown) is provided on the surface of the protrusion 40.

  The cross-sectional shape of the projection 40 in the in-plane direction of the substrate 11 is the same as the shape of the opening 14a, as shown in FIG. However, the adjacent convex portions 40 are connected to each other, and are formed so as to completely surround the unit solid portion 14b 'in a substantially circular shape. The cross-sectional shape of the projection 40 in an in-plane direction perpendicular to the substrate 11 is trapezoidal as shown in FIG. That is, it has a top surface 40t parallel to the substrate surface and a side surface 40s inclined at a taper angle θ (<90 °) with respect to the substrate surface. Since the vertical alignment film (not shown) is formed so as to cover the convex portion 40, the side surface 40s of the convex portion 40 has the same direction as the alignment control direction due to the oblique electric field with respect to the liquid crystal molecules 30a of the liquid crystal layer 30. It has an alignment regulating force and acts to stabilize the radially inclined alignment.

  The operation of the projection 40 will be described with reference to FIGS. 14 (a) to 14 (d) and FIGS. 15 (a) and 15 (b).

  First, the relationship between the alignment of the liquid crystal molecules 30a and the shape of the surface having vertical alignment will be described with reference to FIGS.

  As shown in FIG. 14A, the liquid crystal molecules 30a on the horizontal surface are perpendicular to the surface due to the alignment regulating force of the surface having vertical alignment (typically, the surface of the vertical alignment film). Orientation. When an electric field represented by an equipotential line EQ perpendicular to the axis direction of the liquid crystal molecules 30a is applied to the liquid crystal molecules 30a in the vertical alignment state, a clockwise or counterclockwise direction is applied to the liquid crystal molecules 30a. Act with equal probability. Therefore, the liquid crystal molecules 30a receiving the clockwise torque and the liquid crystal molecules 30a receiving the counterclockwise torque are mixed in the liquid crystal layer 30 between the electrodes of the parallel plate type opposed to each other. As a result, the change to the alignment state according to the voltage applied to the liquid crystal layer 30 may not occur smoothly.

  As shown in FIG. 14 (b), when an electric field represented by horizontal equipotential lines EQ is applied to the liquid crystal molecules 30a oriented vertically to the inclined surface, the liquid crystal molecules 30a Is inclined in a direction in which the amount of inclination for becoming parallel to the equipotential line EQ is small (clockwise in the illustrated example). Further, as shown in FIG. 14C, the liquid crystal molecules 30a oriented vertically to the horizontal surface are continuous with the liquid crystal molecules 30a oriented perpendicular to the inclined surface. The liquid crystal molecules 30a are tilted in the same direction (clockwise) as the liquid crystal molecules 30a located on the tilted surface so as to be aligned (matched).

  As shown in FIG. 14 (d), the top surface of the continuous uneven surface having a trapezoidal cross section is aligned with the alignment direction regulated by the liquid crystal molecules 30a on each inclined surface. And the liquid crystal molecules 30a on the bottom face are aligned.

  The liquid crystal display device of the present embodiment stabilizes the radially inclined alignment by matching the direction of the alignment control force by such a surface shape (convex portion) with the alignment control direction by the oblique electric field.

  FIGS. 15A and 15B show states in which a voltage is applied to the liquid crystal layer 30 shown in FIG. 13B, respectively. FIG. FIG. 15B schematically shows a state in which the orientation of the liquid crystal molecules 30a has begun to change (the initial ON state). FIG. 15B shows that the orientation of the liquid crystal molecules 30a changed in accordance with the applied voltage is steady. The state where the state has been reached is schematically shown. Curves EQ in FIGS. 15A and 15B show equipotential lines EQ.

  When the pixel electrode 14 and the counter electrode 22 have the same potential (state in which no voltage is applied to the liquid crystal layer 30), as shown in FIG. 13B, the liquid crystal molecules 30a in the pixel region Are oriented perpendicular to the surfaces of both substrates 11 and 21. At this time, the liquid crystal molecules 30a in contact with the vertical alignment film (not shown) on the side surface 40s of the protrusion 40 are aligned perpendicularly to the side surface 40s, and the liquid crystal molecules 30a near the side surface 40s are in contact with the peripheral liquid crystal molecules 30a. (Property as an elastic body), as shown in FIG.

  When a voltage is applied to the liquid crystal layer 30, a potential gradient represented by the equipotential line EQ shown in FIG. This equipotential line EQ is parallel to the surface of the solid portion 14b and the counter electrode 22 in the liquid crystal layer 30 located between the solid portion 14b of the picture element electrode 14 and the counter electrode 22. The liquid crystal layer 30 falls on a region corresponding to the opening 14a of the elementary electrode 14 and is inclined in the liquid crystal layer 30 on the edge portion of the opening 14a (around the inside of the opening 14a including the boundary (extension) of the opening 14a). An oblique electric field represented by the equipotential line EQ is formed.

  Due to this oblique electric field, as described above, the liquid crystal molecules 30a on the edge portion EG move clockwise in the right edge portion EG in the drawing, as shown by the arrow in FIG. At the left edge portion EG, each of them inclines (rotates) in the counterclockwise direction and is oriented parallel to the equipotential line EQ. The alignment control direction by the oblique electric field is the same as the alignment control direction by the side surface 40s located at each edge portion EG.

  As described above, the change in the alignment starting from the liquid crystal molecules 30a located on the inclined equipotential line EQ progresses, and when the liquid crystal molecules reach a steady state, the alignment state is schematically shown in FIG. 15B. The liquid crystal molecules 30a located near the center of the opening 14a, that is, near the center of the top surface 40t of the projection 40 have substantially the same influence of the alignment of the liquid crystal molecules 30a on the opposite edge portions EG of the opening 14a. Therefore, the liquid crystal molecules 30a in a region away from the center of the opening 14a (the top surface 40t of the convex portion 40) maintain the alignment state perpendicular to the equipotential line EQ, It tilts under the influence of the orientation of the liquid crystal molecules 30a, and forms a tilted orientation that is symmetric with respect to the center SA of the opening 14a (the top surface 40t of the projection 40). In addition, also in a region corresponding to the unit solid portion 14b 'substantially surrounded by the opening 14a and the convex portion 40, an inclined orientation symmetric with respect to the center SA of the unit solid portion 14b' is formed.

  Thus, in the liquid crystal display device 200 of the second embodiment, similarly to the liquid crystal display device 100 of the first embodiment, the liquid crystal domains having the radially inclined alignment are formed corresponding to the openings 14a and the unit solid portions 14b '. Is done. Since the convex portion 40 is formed so as to completely surround the unit solid portion 14 b ′ in a substantially circular shape, the liquid crystal domain is formed corresponding to the substantially circular region surrounded by the convex portion 40. Further, the side surface of the convex portion 40 provided inside the opening 14a acts so as to tilt the liquid crystal molecules 30a near the edge EG of the opening 14a in the same direction as the alignment direction by the oblique electric field. Stabilizes the tilt orientation.

  Naturally, the alignment regulating force due to the oblique electric field acts only when a voltage is applied, and its strength depends on the strength of the electric field (the magnitude of the applied voltage). Therefore, when the electric field strength is weak (that is, when the applied voltage is low), the alignment regulating force by the oblique electric field is weak, and when an external force is applied to the liquid crystal panel, the radially inclined alignment may be broken by the flow of the liquid crystal material. Once the radial tilt orientation has collapsed, the radial tilt orientation is not restored unless a voltage sufficient to generate an oblique electric field exhibiting a sufficiently strong alignment regulating force is applied. On the other hand, the alignment regulating force by the side surface 40s of the convex portion 40 acts regardless of the applied voltage, and is very strong as known as the anchoring effect of the alignment film. Therefore, even if the liquid crystal material flows and the radial tilt alignment is once broken, the liquid crystal molecules 30a near the side surface 40s of the convex portion 40 maintain the same alignment direction as in the radial tilt alignment. Therefore, as long as the flow of the liquid crystal material stops, the radially inclined alignment can be easily restored.

  As described above, the liquid crystal display device 200 according to the second embodiment has a characteristic that the liquid crystal display device 100 according to the first embodiment is strong against external force, in addition to the characteristics of the liquid crystal display device 100 according to the first embodiment. Therefore, the liquid crystal display device 200 is suitably used for a PC or PDA that is likely to be applied with external force and that is frequently used in a portable manner.

  When the projection 40 is formed using a highly transparent dielectric, there is an advantage that the contribution of the liquid crystal domain formed corresponding to the opening 14a to the display is improved. On the other hand, when the convex portion 40 is formed using an opaque dielectric, there is an advantage that light leakage due to the retardation of the liquid crystal molecules 30a that are obliquely aligned by the side surface 340s of the convex portion 40 can be prevented. Which one to employ may be determined according to the application of the liquid crystal display device and the like. In any case, the use of the photosensitive resin has an advantage that the patterning process corresponding to the opening 14a can be simplified. In order to obtain a sufficient alignment control force, it is preferable that the height of the projections 40 be in the range of about 0.5 μm to about 2 μm when the thickness of the liquid crystal layer 30 is about 3 μm. In general, it is preferable that the height of the protrusion 40 be in the range of about 1/6 to about 2/3 of the thickness of the liquid crystal layer 30.

  As described above, the liquid crystal display device 200 has the convex portion 40 inside the opening 14 a of the pixel electrode 14, and the side surface 40 s of the convex portion 40 has an oblique electric field with respect to the liquid crystal molecules 30 a of the liquid crystal layer 30. Has an alignment regulating force in the same direction as the alignment regulating direction. Preferred conditions for the side surface 40s to have the alignment control force in the same direction as the alignment control direction by the oblique electric field will be described with reference to FIGS. 16 (a) to 16 (c).

  16A to 16C schematically show cross-sectional views of the liquid crystal display devices 200A, 200B, and 200C, respectively, and correspond to FIG. Each of the liquid crystal display devices 200A, 200B, and 200C has a convex portion inside the opening 40, but the arrangement relationship between the entire convex portion 40 as one structure and the opening 40 is different from that of the liquid crystal display device 200. I have.

  In the above-described liquid crystal display device 200, as shown in FIG. 15A, the entirety of the projection 40 as a structure is formed inside the opening 40a, and the bottom of the projection 40 has an opening. It is smaller than the part 40a. In the liquid crystal display device 200A shown in FIG. 16A, the bottom surface of the projection 40A coincides with the opening 14a, and in the liquid crystal display device 200B shown in FIG. 16B, the projection 40B has an opening. It has a bottom surface larger than the portion 14a and is formed so as to cover a solid portion (conductive film) 14b around the opening 14a. The solid portion 14b is not formed on the side surface 40s of any of these convex portions 40, 40A and 40B. As a result, as shown in each figure, the equipotential line EQ is substantially flat on the solid portion 14b, and drops at the opening 14a as it is. Therefore, the side surfaces 40s of the convex portions 40A and 40B of the liquid crystal display devices 200A and 200B exhibit the same alignment regulating force as that of the oblique electric field, similarly to the convex portion 40 of the liquid crystal display device 200 described above. Stabilizes radial tilt orientation.

  On the other hand, the bottom surface of the protrusion 40C of the liquid crystal display device 200C shown in FIG. 16C is larger than the opening 14a, and the solid portion 14b around the opening 14a is formed on the side surface 40s of the protrusion 40C. Have been. A mountain is formed on the equipotential line EQ under the influence of the solid portion 14b formed on the side surface 40s. The peak of the equipotential line EQ has an inclination opposite to that of the equipotential line EQ falling at the opening 14a, which generates an oblique electric field that is opposite to the oblique electric field that causes the liquid crystal molecules 30a to be radially inclined. It indicates that. Therefore, in order for the side surface 40s to have the alignment control force in the same direction as the alignment control direction by the oblique electric field, it is preferable that the solid portion (conductive film) 14b is not formed on the side surface 40s.

  Next, the cross-sectional structure of the protrusion 40 shown in FIG. 13A along the line 17A-17A 'will be described with reference to FIG.

  As described above, since the convex portion 40 shown in FIG. 13A is formed so as to completely surround the unit solid portion 14b ′ in a substantially circular shape, the adjacent unit solid portion 14b ′ The portion that plays the role of connecting to (a branch from the circular portion to the four sides) is formed on the convex portion 40 as shown in FIG. Therefore, in the step of depositing the conductive film forming the solid portion 14b of the pixel electrode 14, there is a high risk that disconnection may occur on the projection 40 or separation may occur in a later step of the manufacturing process.

  Therefore, as shown in the liquid crystal display device 200D shown in FIGS. 18A and 18B, when the opening portions 14a are formed so as to completely include the independent convex portions 40D, the solid portions 14b are formed. Since the conductive film is formed on the flat surface of the substrate 11, there is no danger of disconnection or peeling. Although the convex portion 40D is not formed so as to completely surround the unit solid portion 14b 'in a substantially circular shape, a substantially circular liquid crystal domain corresponding to the unit solid portion 14b' is formed. As in the example, the radial tilt orientation is stabilized.

  By forming the protrusions 40 in the openings 14a, the effect of stabilizing the radially inclined orientation is not limited to the openings 14a of the illustrated patterns, but may be applied to the openings 14a of all the patterns described in the first embodiment. And the same effect can be obtained. In order to sufficiently exhibit the effect of stabilizing the alignment with respect to the external force due to the protrusions 40, the pattern of the protrusions 40 (the pattern when viewed from the normal direction of the substrate) surrounds the liquid crystal layer 30 in an area as large as possible. Preferably, it is shaped. Therefore, for example, a positive pattern having a circular unit solid portion 14b 'has a larger effect of stabilizing the alignment by the convex portions 40 than a negative pattern having a circular opening 14a.

(Arrangement of polarizer and retarder)
A so-called vertical alignment type liquid crystal display device including a liquid crystal layer in which liquid crystal molecules having negative dielectric anisotropy are vertically aligned when no voltage is applied can perform display in various display modes. For example, in addition to the birefringence mode in which display is performed by controlling the birefringence of the liquid crystal layer by an electric field, an optical rotation mode or a combination of the optical rotation mode and the birefringence mode is applied to the display mode. By providing a pair of polarizing plates outside (a side opposite to the liquid crystal layer 30) of a pair of substrates (for example, a TFT substrate and a counter substrate) of all the liquid crystal display devices described in the first and second embodiments, birefringence is provided. A mode liquid crystal display device can be obtained. Further, if necessary, a phase difference compensating element (typically, a phase difference plate) may be provided. Further, a bright liquid crystal display device can be obtained even when substantially circularly polarized light is used.

  As shown in FIGS. 5B and 5C, in a liquid crystal display device having a configuration in which the liquid crystal domains adopt a spiral radially inclined alignment state, the display quality is improved by optimizing the arrangement of the polarizing plates. It is possible to further improve. Hereinafter, a preferred arrangement of the polarizing plate will be described. Here, a liquid crystal display having a pair of polarizing plates provided outside a pair of substrates (for example, a TFT substrate and a counter substrate) and arranged so that polarization axes thereof are substantially orthogonal to each other, and performing display in a normally black mode. The apparatus will be described as an example. The spiral radially inclined alignment state is realized, for example, by using a material obtained by adding a chiral agent to a nematic liquid crystal material having negative dielectric anisotropy. In the following description, the “spiral radially inclined orientation” is also simply referred to as the “spiral orientation”.

  First, an alignment state of liquid crystal molecules when a liquid crystal domain assumes a spiral alignment state will be described with reference to FIGS. FIG. 19A is a diagram schematically showing the alignment state of liquid crystal molecules immediately after a voltage is applied to the liquid crystal layer, and FIGS. 19B and 19C show the liquid crystal when alignment is stable (steady state). It is a figure which shows the orientation state of a molecule typically.

  Immediately after a voltage is applied to the liquid crystal layer, in a plurality of liquid crystal domains, the liquid crystal molecules 30a take a simple radial tilt alignment as shown in FIG. Thereafter, when the alignment further proceeds, the liquid crystal molecules 30a incline in a predetermined direction in the in-plane direction of the liquid crystal layer, and when the alignment is stable (steady state), as shown in FIG. The liquid crystal molecules 30a assume a clockwise or counterclockwise spiral alignment state.

  At this time, when the liquid crystal molecules 30a are tilted counterclockwise (counterclockwise), the liquid crystal domains are in a clockwise spiral alignment state as shown in FIG. 19B, and the liquid crystal molecules 30a are tilted clockwise (clockwise). Then, as shown in FIG. 19C, a left-handed spiral orientation state is set. Whether clockwise or counterclockwise is determined, for example, by the type of chiral agent to be added.

  As shown in FIG. 19B and FIG. 19C, the degree of tilt of the liquid crystal molecules 30a in the in-plane direction is, as shown in FIGS. The direction is defined by the angle θ formed by the liquid crystal molecules 30a ′ positioned in the direction (the upward direction of the display surface, hereinafter also simply referred to as the 12:00 direction). The center of the liquid crystal domain typically coincides substantially with the center of the opening or the center of the solid part.

  Actually, some of the liquid crystal molecules 30a 'existing at the above-mentioned positions are inclined at an angle different from [theta]. In the present specification, when the existence probability of each liquid crystal molecule 30a 'with respect to the angle (tilt angle) between the display surface 12 o'clock direction and the above-described liquid crystal molecule 30a' is examined, the liquid crystal molecule 30a having the highest existence probability is obtained. Is defined as θ. Typically, the angle between the liquid crystal molecules 30a 'near the center in the thickness direction of the liquid crystal layer and the 12 o'clock direction substantially matches θ. Note that the angle formed by the liquid crystal molecules 30a 'with respect to the 12 o'clock direction is strictly the angle formed between the azimuthal direction of the alignment direction of the liquid crystal molecules 30a' and the 12 o'clock direction.

  As described above, in a liquid crystal display device having a configuration in which liquid crystal domains take a spiral alignment state, one polarization axis of a pair of polarizing plates is oriented in the same direction as the direction in which the liquid crystal molecules are inclined. By arranging the polarizing plate so as to be inclined at an angle of more than 0 ° and less than 2θ with respect to the 12 o'clock direction, it is possible to improve the transmittance of light when the liquid crystal domain takes a spiral alignment state, A bright display is realized. Hereinafter, this will be described in more detail by way of example.

  First, referring to FIG. 20, in a white display state, that is, in a state where a predetermined voltage is applied to the liquid crystal layer and the liquid crystal domain is in a spiral radially inclined alignment state, the pair of polarizing plates are placed in a crossed Nicol state. The change in transmittance when the polarization axis is rotated with respect to the 12 o'clock direction while rotating with respect to the liquid crystal panel while maintaining the transmittance will be described. FIG. 20 shows the transmittance in the white display state of a liquid crystal display device provided with a liquid crystal layer (thickness: 3.8 μm) made of a liquid crystal material having a chiral pitch of 16 μm on the vertical axis. 4 is a graph showing the angle formed by the vertical axis. Here, the transmittance when the angle between the polarization axis and the 12:00 direction is 0 ° is set to 100%. The liquid crystal molecules of the liquid crystal layer included in the liquid crystal display device take a clockwise spiral alignment as shown in FIG. 19B when the alignment is stabilized, and the liquid crystal molecules located at 12 o'clock are in the 12 o'clock direction. On the other hand, it is inclined approximately 13 ° counterclockwise (that is, θ ≒ 13 °). In the following drawings, unless otherwise specified, the liquid crystal display device described above (the liquid crystal molecules take a clockwise spiral alignment when the alignment is stabilized, and the liquid crystal molecules located at the 12 o'clock direction are shifted leftward with respect to the 12 o'clock direction. (A liquid crystal display device having a configuration inclined about 13 ° around the liquid crystal display device).

  As shown in FIG. 20, as the polarization axis is inclined counterclockwise with respect to the 12 o'clock direction, the transmittance increases, and the angle formed by the polarization axis with respect to the 12 o'clock direction is about 13 ° (that is, θ). Sometimes the transmittance is at a maximum. When the polarization axis is further inclined, the transmittance decreases, and when the angle formed by the polarization axis with respect to the 12:00 direction is about 26 ° (that is, 2θ), the transmittance becomes the same as when the angle is 0 °. When the angle exceeds 0 °, the transmittance is lower than when the angle is 0 °.

  The reason why the light transmittance changes as described above is that the area of the light shielding region in the liquid crystal domain changes according to the inclination angle of the polarization axis with respect to the 12 o'clock direction. The light-shielding region is a region defined by liquid crystal molecules oriented in a direction perpendicular or parallel to the polarization axis, and the liquid crystal layer in this region hardly gives a phase difference to incident light. Therefore, the incident light passing through this region hardly contributes to the transmittance. Therefore, the transmittance when the liquid crystal domain takes a spiral alignment state depends on the area of the light-shielding region. The transmittance is lower as the area of the light-shielding region is larger, and the transmittance is higher as the area of the light-shielding region is smaller.

  The change of the light shielding area according to the tilt angle of the polarization axis will be described with reference to FIGS. 21 (a) and (b) and FIGS. 22 (a) and (b). FIGS. 21A and 21B are diagrams schematically showing the light-shielding region SR in the liquid crystal domain when the polarization axis is provided in parallel to the 12 o'clock direction, and FIGS. (b) is a diagram schematically showing the light-shielding region SR in the liquid crystal domain when the polarization axis is provided at an angle of about 13 ° with respect to the 12:00 direction.

  As shown in FIG. 21A, when the polarization axis is provided in parallel with the 12 o'clock direction, the light-shielding region SR is positioned at a distance from the center of the liquid crystal domain as shown in FIG. At 12:00, 3 o'clock, 6 o'clock, and 9 o'clock directions. On the other hand, as shown in FIG. 22A, when the polarization axis is provided at an angle of about 13 ° with respect to the 12:00 direction, as shown in FIG. The light-shielding region SR is observed at 12:00, 3 o'clock, 6 o'clock, and 9 o'clock with respect to the center of the liquid crystal domain.

  When the polarization axis is provided in parallel to the 12 o'clock direction as shown in FIG. 21B, the area of the light shielding region SR is S1, and as shown in FIG. Assuming that the area of the light-shielding region SR is S2 when the light-shielding region SR is provided at an angle of about 13 ° (that is, θ) with respect to the time direction, S1 is larger than S2 (S1> S2). This is because when the polarization axis is provided at an angle of about 13 ° with respect to the 12 o'clock direction, it is more polarized than when the polarization axis is provided parallel to the 12 o'clock direction. This is because the existence probability of liquid crystal molecules oriented in a direction perpendicular or parallel to the axis is low.

  As described above, when the angle formed by the liquid crystal molecules positioned at 12 o'clock with respect to the center of the liquid crystal domain with respect to the 12 o'clock direction is θ, the polarization axis of the polarizing plate (one of the pair of polarizing plates). However, when the polarizing plate is arranged so that the liquid crystal molecules are inclined at an angle of more than 0 ° and less than 2θ with respect to the 12 o'clock direction in the same direction as the direction in which the liquid crystal molecules are inclined with respect to the 12 o'clock direction. The existence probability of liquid crystal molecules oriented in a direction perpendicular or parallel to the polarization axis is lower than when the polarization axis is provided in parallel with the 12 o'clock direction. Therefore, by arranging the polarizing plates as described above, the transmittance of light when the liquid crystal domains take a spiral radially inclined alignment state is improved, and a bright display is realized.

  Further, as shown in FIG. 22A, when the polarizing plate is arranged so that the polarization axis of the polarizing plate is inclined at substantially the same angle as θ, the light is blocked as shown in FIG. 22B. The region SR is located at 12 o'clock, 3 o'clock, 6 o'clock, and 9 o'clock with respect to the center of the liquid crystal domain, and the existence probability of liquid crystal molecules oriented in a direction perpendicular or parallel to the polarization axis is high. Lowest. Therefore, by disposing the polarizing plate in this manner, the light transmittance is further improved, and a brighter display is realized.

  In the above description, the preferred arrangement of the polarizing plate has been described from the viewpoint of improving the transmittance, but one polarization axis of the pair of polarizing plates is in the same direction as the direction in which the liquid crystal molecules are inclined, By arranging the polarizing plate so as to be inclined at an angle of more than 0 ° and not more than θ with respect to the 12 o'clock direction, a bright display is realized and a white tailing phenomenon (white tailing afterimage is observed). Phenomena) and black tailing (a phenomenon in which black tailing afterimages are observed) are suppressed, and high-quality display is realized.

  The white tailing phenomenon may occur, for example, when an image in which a black square (box) moves in the background of the halftone display state is displayed on the liquid crystal display device. FIG. 23 is a diagram schematically showing the white tailing phenomenon. As shown in FIG. 23, when displaying an image in which a black square (box) moves from left to right in the halftone background, an area having a higher luminance than the halftone exists on the left side of the black square, It may be observed as a trailing image.

  The above-described white tailing phenomenon is relatively likely to occur, for example, when the polarization axis of the polarizing plate is provided parallel to the 12:00 direction. On the other hand, for example, in a liquid crystal display device whose transmittance change is shown in FIG. 20, the polarization axis is arranged so as to be inclined at an angle of about 13 ° with respect to the 12:00 direction. As shown in FIG. 24, occurrence of a white tail phenomenon when displaying an image in which a black square (box) moves from left to right in the figure in the halftone background is prevented.

  The reason will be described with reference to FIGS. 25 (a) to (c) and FIGS. 26 (a) to (c). FIGS. 25A to 25C are diagrams schematically showing the light-shielding region SR in the liquid crystal domain when the polarization axis of the polarizing plate is provided in parallel to the 12 o'clock direction. ) Shows the polarization axis of the polarizing plate at this time, FIG. 25B shows the light-shielding region SR immediately after the voltage is applied to the liquid crystal layer, and FIG. 3) shows the light shielding region SR in FIG. FIGS. 26A to 26C schematically show the light-shielding region SR in the liquid crystal domain when the polarizing axis of the polarizing plate is provided to be inclined at an angle of about 13 ° with respect to the 12:00 direction. 26A shows the polarization axis of the polarizing plate at this time, and FIG. 26B shows the light-shielding region SR immediately after the voltage is applied to the liquid crystal layer. c) shows the light shielding region SR when the alignment is stable (steady state).

  First, a case where one polarization axis of a pair of polarizing plates is provided in parallel with the 12 o'clock direction as shown in FIG. When the polarizer is provided in this manner, when the liquid crystal molecules immediately after the voltage application have a simple radial tilt alignment, the light-shielding region SR is located at the center of the liquid crystal domain as shown in FIG. On the other hand, it is observed at 12 o'clock, 3 o'clock, 6 o'clock, and 9 o'clock. When the alignment is stable, the light shielding region SR is shifted clockwise from the 12 o'clock direction, the 3 o'clock direction, the 6 o'clock direction, and the 9 o'clock direction with respect to the center of the liquid crystal domain, as shown in FIG. Observed.

  Assuming that the area of the light-shielding region SR immediately after the voltage application shown in FIG. 25B is S1 ′ and the area of the light-shielding region SR when the orientation is stable shown in FIG. 25C is S1, S1 is larger than S1 ′. In addition, the transmittance immediately after voltage application is higher than the transmittance when the alignment is stable. Therefore, as shown in FIG. 23, when displaying an image in which a black square (box) moves from left to right in the halftone background, the picture element area immediately after the black square passes, that is, The picture element area that changes from the display state to the halftone display state transitoryly has a transmittance higher than the transmittance in the halftone state (the transmittance when the orientation is stable), and is observed as a white tailed afterimage. Is done.

  On the other hand, as shown in FIG. 26A, if one of the polarizing plates of the pair of polarizing plates is provided so as to be inclined at an angle of about 13 ° with respect to the 12 o'clock direction, the voltage becomes higher. When the liquid crystal molecules immediately after the application have a simple radial tilt alignment, the light-shielding region SR is positioned at 12 o'clock, 3 o'clock, and 6 o'clock with respect to the center of the liquid crystal domain, as shown in FIG. And observed in a direction deviated counterclockwise from the 9 o'clock direction. Further, when the alignment is stable, the light-shielding region SR is observed in the directions of 12 o'clock, 3 o'clock, 6 o'clock, and 9 o'clock with respect to the center of the liquid crystal domain, as shown in FIG.

  Assuming that the area of the light-shielding region SR immediately after the voltage application shown in FIG. 26B is S2 ′ and the area of the light-shielding region SR when the orientation is stable shown in FIG. 25C is S2, S2 is smaller than S2 ′. In addition, the transmittance at the time of stable alignment is higher than the transmittance immediately after voltage application. Further, when the polarizing plate is arranged in this manner, the transmittance becomes highest when the alignment is stable. Therefore, as shown in FIG. 24, when displaying an image in which a black square (box) moves from left to right in the halftone background, a picture element area immediately after the black square passes, that is, black display The picture element region that changes from the state to the halftone display state does not transiently go through a state in which the transmittance is higher than the transmittance in the halftone state (the transmittance when the orientation is stable). As a result, in the liquid crystal display device in which the polarizing plate is disposed as described above, the occurrence of the white tailing phenomenon is reliably prevented.

  FIG. 27 shows the case where the polarization axis is provided in parallel with the 12 o'clock direction and the case where the polarization axis is provided so as to be inclined at an angle of about 13 ° with respect to the 12 o'clock direction. 7 shows a temporal change in transmittance when a certain pixel region is changed from a black display state to a halftone display state. Here, the transmittance in the halftone state is set to 1.00, and the time when a voltage is applied to the liquid crystal layer in this picture element region is set to 0 sec.

  When the polarization axis is provided in parallel to the 12 o'clock direction, as shown by the solid line in FIG. 27, the transmittance greatly exceeds 1.00 immediately after the application of the voltage, and thereafter, the predetermined transmittance ( (Transmittance in the halftone state). Therefore, when the polarizing plate is arranged in this manner, a white tail phenomenon may occur.

  On the other hand, when the polarization axis is provided so as to be inclined at an angle of about 13 ° with respect to the 12 o'clock direction, as shown by a dashed line in FIG. The rate does not greatly exceed 1.00. Therefore, when the polarizing plate is arranged in this way, the occurrence of the white tailing phenomenon is reliably prevented.

  In the above description, as an example of the arrangement of the polarizing plate for preventing the occurrence of the white tailing phenomenon, a case where the polarization axis is inclined at an angle of about 13 ° (that is, θ) with respect to the 12:00 direction will be described. explained. When the polarizing plate is arranged in this manner, as described above, the transmittance becomes highest when the alignment is stable, so that the occurrence of the white tailing phenomenon is reliably prevented.

  However, the configuration for suppressing the occurrence of the white tailing phenomenon is not limited to the configuration having the highest transmittance when the alignment is stable, but the highest transmittance that is transiently taken and the transmittance when the alignment is stable. Is smaller than the case where the polarization axis is provided in parallel with the 12 o'clock direction, thereby suppressing the occurrence of the white tailing phenomenon.

  For example, when the polarization axis is inclined at an angle of more than 0 ° and not more than θ in the same direction as the inclination direction of the liquid crystal molecules with respect to the 12 o'clock direction, the occurrence of the white tailing phenomenon is suppressed, and high quality is achieved. Is displayed. When the polarization axis is set within the above-mentioned angle range, not only the occurrence of the white tailing phenomenon is suppressed, but also the transmittance at the time of stable alignment is improved, and a bright display is realized. Within the above-mentioned angle range, the larger the inclination angle of the polarization axis is, the more difficult the white tailing phenomenon is to occur. When the tilt angle of the polarization axis is tilted at substantially the same angle as θ / 2, the occurrence of the white tailing phenomenon is substantially prevented.

  The configuration for suppressing the occurrence of the white tailing phenomenon is not limited to the configuration illustrated, but depending on the arrangement of the polarizing plate, the change in transmittance when changing the picture element region from the black display state to the halftone display state may occur. It may be too slow, and the black tail phenomenon may occur.

  Similar to the white tailing phenomenon, the black tailing phenomenon may occur, for example, when an image in which a black square (box) moves in the background of the halftone display state is displayed on the liquid crystal display device. FIG. 28 is a diagram schematically illustrating the black tailing phenomenon. As shown in FIG. 28, when an image in which a black square (box) moves from left to right in the figure in the halftone background is displayed, the left side of the black square has a higher luminance than the black display state and a lower halftone state than the black display state. Has a region with low luminance, and may be observed as a black tailed afterimage.

  The above-described black tailing phenomenon is relatively likely to occur when the polarization axis of the polarizing plate is provided at an angle exceeding θ with respect to the 12:00 direction. For example, when the polarization axis is inclined at about 20 ° with respect to the 12 o'clock direction, the transmittance changes from the black display state to the halftone state as schematically shown by a two-dot chain line in FIG. Too loose. Therefore, when the image in which the black square moves is displayed as described above, the pixel region immediately after the black square passes cannot be in the halftone display state quickly, and the black tailing phenomenon may occur. is there.

  For example, when the polarization axis is inclined at an angle of more than 0 ° and not more than θ in the same direction as the tilt direction of the liquid crystal molecules with respect to the 12 o'clock direction, the occurrence of the black tailing phenomenon is suppressed, and high quality is achieved. Is displayed. When the polarization axis is set within the above-mentioned angle range, not only the occurrence of the black tailing phenomenon is suppressed, but also the transmittance at the time of stable alignment is improved, and a bright display is realized. In the angle range where the tilt angle of the polarization axis with respect to the 12 o'clock direction is greater than 0 ° and θ or less in the same direction as the tilt direction of the liquid crystal molecules, the smaller the tilt angle of the polarization axis, the more difficult it is for black tailing to occur. . When the inclination angle of the polarization axis is inclined at substantially the same angle as θ / 2, the occurrence of the black tail phenomenon is substantially prevented.

  As described above, by optimizing the arrangement of the polarizing plates, the occurrence of the white tail phenomenon or the black tail phenomenon is suppressed. From the viewpoint of suppressing the occurrence of the tailing phenomenon and improving the transmittance, the polarization axis of the polarizing plate (one polarization axis of the pair of polarizing plates) is set to 0 in the same direction as the direction in which the liquid crystal molecules are inclined. It is preferable to arrange the polarizing plate so as to be inclined at an angle of more than ° and not more than θ. By arranging the polarizing plate in this manner, bright display is realized, and the occurrence of tailing phenomena (white tailing and black tailing) is suppressed, and high-quality display is realized. Furthermore, when the polarizing plate is arranged such that the polarizing axis of the polarizing plate is inclined at substantially the same angle as θ / 2, the occurrence of the white tail phenomenon and the black tail phenomenon is substantially prevented, and higher quality is achieved. The display is realized.

  Note that the configuration in which the liquid crystal domains take a spiral alignment state is realized, for example, by using a liquid crystal material to which a chiral agent is added as the liquid crystal material. Accordingly, there are a case where the alignment of the liquid crystal molecules changes spirally along the thickness direction of the liquid crystal layer, and a case where such a spiral alignment change hardly occurs. In any case, the display quality can be improved by optimizing the arrangement of the polarizing plates as described above.

(Branch width, number)
As described above, the pixel electrodes 14 included in the liquid crystal display devices 100 and 200 according to the present invention have the plurality of openings 14a and the solid portions 14b. The unit solid portions 14b ′ located in the unit cell formed by the openings 14a are typically electrically connected to the adjacent unit solid portions 14b ′, but are adjacent to each other. Naturally, the same potential as that of the other portions is also applied to a portion which plays a role of connecting the portions 14b 'to each other, for example, a branch portion extending from a circular portion as shown in FIG. Therefore, the branch also affects the alignment regulation effect by the oblique electric field.

  As shown in FIG. 29, the solid portion 14b typically has a plurality of islands 14c and a plurality of branches 14d each of which electrically connects adjacent islands 14c to each other. ing. Here, the island-shaped portion 14c refers to a portion of the conductive film located in the unit cell except for the branch portion 14d.

  The alignment of the liquid crystal molecules 30a of the liquid crystal layer 30 located on the island 14c is controlled by an oblique electric field generated at the boundary between the island 14c and the opening 14a (the edge of the opening 14a). In order to realize a stable alignment state and good response characteristics, it is necessary to apply an oblique electric field for controlling the alignment of the liquid crystal molecules 30a to many liquid crystal molecules 30a. Are preferably formed.

  As shown in FIG. 29, if the branch 14d exists between the islands 14c, the boundary between the island 14c and the opening 14a is reduced by the existence of the branch 14d, and the island 14c Edge portions for forming an oblique electric field for controlling the alignment of the upper liquid crystal molecules 30a are reduced. That is, the branch portions 14d existing between the island-shaped portions 14c reduce the alignment control effect by the oblique electric field. Therefore, as the width of the branches 14d is smaller or the number of the branches 14d is smaller, a decrease in the alignment control effect is suppressed, and the response characteristics are improved.

  Further, since an oblique electric field is generated at the boundary between the branch 14d and the opening 14a, the alignment direction of the liquid crystal molecules 30a located on the branch 14d is regulated. The alignment of the liquid crystal molecules 30a on the branch portions 14d also affects the alignment state of the liquid crystal molecules 30a on the island portions 14c, thereby affecting the responsiveness. The details will be described below.

  First, the alignment state of the liquid crystal layer 30 located on the island portion 14c will be described with reference to FIGS. FIG. 30 is a top view schematically illustrating an alignment state of the liquid crystal molecules 30a when a voltage is applied, and FIG. 31 is a cross-sectional view taken along lines 31A-31A ′ and 31B-31B ′ in FIG. . Here, the shape of the island-shaped portion 14c is a barrel shape (corners are arc-shaped squares), a material to which a chiral agent is added as a liquid crystal material is used, and the liquid crystal layer 30 has a spiral radially inclined orientation. 1 shows a liquid crystal display device in a state. Here, as shown in FIG. 31, on the counter electrode 22 provided on the counter substrate 100b, the center of the radially inclined alignment is fixed at a position near the center of the unit solid portion 14b ', and the alignment is performed. Although a bowl-shaped projection (a projection having a surface composed of a part of a spherical surface) 24 for improving stability is provided, even when such a projection 24 is not provided, the following will be described. There is no difference in the description.

  As shown in FIG. 30, when a voltage is applied to the liquid crystal layer 30, the orientation direction of the liquid crystal molecules 30a is caused by an oblique electric field generated at the boundary between the opening 14a and the island 14c (the edge of the opening 14a). Is regulated, and the liquid crystal layer 30 on the island-shaped portion 14c is in a spiral radially inclined alignment state.

  In a cross section along a direction in which the branch portion 14d does not exist, such as a cross section along the lines 31A-31A 'and 31B-31B' in FIG. 30, as shown in FIG. 31, all the liquid crystal molecules 30a have openings. The orientation regulating force acts so as to incline from the edge of the portion 14a toward the center of the island 14c. When the shape of the island portion 14c is circular, the magnitude of the alignment regulating force is the same in any cross section along the direction in which the branch portion 14d does not exist. However, as shown in FIG. When the shape of the shape 14c is a barrel shape, the magnitude of the alignment control force depends on the distance from the center of the island 14c to the edge.

  As described above, the liquid crystal layer 30 located on the island portion 14c stably forms a spiral radial inclined alignment having an alignment center near the center of the island portion 14c when a voltage is applied. This state is referred to as a first stable state for the sake of simplicity of the description to be described later.

  Next, the alignment state of the liquid crystal layer 30 located on the opening 14a will be described with reference to FIGS. FIG. 32 is a top view schematically illustrating an alignment state of the liquid crystal molecules 30a when a voltage is applied, and FIG. 33 is a cross-sectional view taken along lines 33A-33A ′ and 33B-33B ′ in FIG. .

  In the cross section along the direction in which the branch 14d does not exist, such as the cross section along the lines 33A-33A 'and 33B-33B' in FIG. 32, as shown in FIG. The orientation regulating force acts so as to incline from the edge of the portion 14a toward the center of the opening 14a. However, since the liquid crystal molecules 30a of the liquid crystal layer 30 located in the shape of the opening 14a are not directly affected by the electric field generated by the electrodes, the liquid crystal molecules 30a are inclined more than the liquid crystal molecules 30a located on the island 14c. The angle to do is small.

  As described above, the liquid crystal layer 30 located on the opening 14a stably forms a radially inclined alignment having an alignment center near the center of the opening 14a when a voltage is applied.

  Subsequently, the alignment state of the liquid crystal layer 30 located on the branch portion 14d will be described with reference to FIGS. 34, 35A and 35B. FIG. 34 is a top view schematically illustrating an alignment state of the liquid crystal molecules 30a when a voltage is applied. FIG. 35A is a cross-sectional view taken along a line 35A-35A ′ in FIG. FIG. 36B is a cross-sectional view of FIG. 34 taken along the line 35B-35B ′.

  As shown in FIG. 35A, in a cross section along a direction crossing the boundary between the branch 14d and the opening 14a, as in a cross section taken along line 35A-35A 'in FIG. The orientation direction of the liquid crystal molecules 30a is regulated by the oblique electric field generated at the boundary between the opening 14d and the opening 14a. On the other hand, as shown in FIG. 35 (b), in a cross section along a direction that traverses the branch portion 14d and the island-shaped portion 14c like a cross section along line 35B-35B ′ in FIG. The liquid crystal molecules 30a are tilted so as to match the alignment state of the liquid crystal layer 30 on the adjacent island portion 14c.

  Accordingly, as shown in FIG. 36, the liquid crystal molecules 30a of the liquid crystal layer 30 located on the branch portions 14d have the alignment of the liquid crystal molecules 30a on the adjacent island portions 14c and the alignment of the liquid crystal molecules 30a on the opening portions 14a. Orient to align (corresponding to the first stable state described above). In FIG. 36, the liquid crystal molecules 30a whose orientation axis direction is up and down (12 o'clock and 6 o'clock) on the display surface and the liquid crystal molecules 30a whose display surface is right and left (3 o'clock and 9 o'clock) are shown. Is shown.

  The alignment control force (a very weak alignment control force acting to maintain the continuity of the surrounding alignment) in the cross section along the 35B-35B 'line is affected by the alignment control force of the oblique electric field formed at the edge of the opening 14a. In addition, the inclination direction of the liquid crystal molecules 30a due to the above-described alignment control force is extremely weak. ) Is in the opposite direction (the liquid crystal molecules 30a are oriented in an open cone shape) (the lower side (substrate 100a side) is oriented in an open cone shape). The balance of the alignment regulating force acting on the molecule 30a is likely to be lost.

  For this reason, the liquid crystal molecules 30a (orientation) that are vertically aligned in a cross section (corresponding to a cross section taken along line 35A-35A 'in FIG. 34) along the direction crossing the boundary between the branch 14d and the opening 14a. As shown in FIGS. 37A and 37B, the center liquid crystal molecule 30a) easily moves to the boundary between the branch 14d and the opening 14a.

  Under the influence of the misalignment of the liquid crystal molecules 30a on the branch portions 14d (the misalignment of the vertically aligned liquid crystal molecules 30a), the spiral orientation of the liquid crystal layer 30 on the island portions 14c is changed as shown in FIG. 38 changes from the first stable state shown in FIG. 38 to the second stable state shown in FIG. This affects the response characteristics of the liquid crystal display device, and it takes a relatively long time for the alignment to be stable and to be in a steady state.

  As described above, the alignment state of the liquid crystal molecules 30a on the branches 14d that affects the response characteristics largely depends on the presence (the number) of the branches 14d and the width of the branches 14d. As shown in FIG. 39B, when the width of the branch portion 14d is relatively large, the balance of the alignment control force with respect to the liquid crystal molecules 30a on the branch portion 14d tends to be lost, and the alignment of the liquid crystal molecules 30a on the island portion 14 is stabilized. It greatly affects the condition. On the other hand, as shown in FIG. 39A, when the width of the branch portion 14d is relatively narrow, the alignment regulating force for the liquid crystal molecules 30a on the branch portion 14d is well balanced, and the liquid crystal on the island-like portion 14c is well-balanced. The alignment state of the molecules 30a is stabilized relatively quickly, and the response characteristics of the liquid crystal display device are improved.

  With reference to FIG. 40, the effect of the width of the branch portion 14d on the response characteristic will be described more specifically. FIG. 40 shows the time change of the transmittance when a voltage is applied to the liquid crystal layer 30 when the width of the branch 14d is relatively narrow (for example, 5.5 μm) and when it is relatively wide (for example, 7.5 μm). It is a graph shown typically. Here, it is assumed that the polarization axes of the pair of polarizing plates are set to be parallel to the 12 o'clock direction and the 3 o'clock direction, respectively.

  As described with reference to FIG. 27, when the polarization axis of the polarizing plate is set parallel to the 12 o'clock direction, the transmittance temporarily reaches a maximum immediately after the application of the voltage (the maximum transmittance Ip in FIG. 40). , Then becomes almost constant. The liquid crystal layer 30 takes a simple radial tilt alignment immediately after voltage application, and then changes into a spiral radial tilt alignment. At this time, the liquid crystal layer 30 goes through the first stable state shown in FIG. The second stable state shown in FIG.

  As shown in FIG. 40, the time Ta required to reach the second stable state when the width of the branch 14d is relatively narrow is equal to the time Ta required to reach the second stable state when the width of the branch 14d is relatively wide. (Ta <Tb). As described above, the narrower the width of the branch portion 14d, the better the response characteristics can be obtained (the higher the response speed).

  Further, the transmittance Ia in the second stable state when the width of the branch 14d is relatively narrow is higher than the transmittance Ib in the second stable state when the width of the branch 14d is relatively wide (Ia>). Ib).

  The reason will be described with reference to FIGS. 41 (a) and 41 (b). FIGS. 41A and 41B schematically show the liquid crystal molecules 30a oriented in a direction parallel to the polarization axis in the second stable state. FIG. 41A shows the branch 14d. 41B shows a case where the width of the branch portion 14d is relatively wide. The arrows shown in FIGS. 41A and 41B indicate the directions of the polarization axes of the pair of polarizers. Here, the polarization axes of the pair of polarizers are 12 o'clock and 3 o'clock, respectively. It is set parallel to the direction.

  When the polarizing plate is arranged as described above, the region where the liquid crystal molecules 30a oriented in the direction parallel to the polarization axis of the polarizing plate exists is a light-shielding region through which light hardly passes.

  As shown in FIG. 41 (a), when the width of the branch portion 14d is relatively narrow, the liquid crystal molecules 30a oriented in the direction parallel to the polarization axis are in the 12 o'clock direction, the 3 o'clock direction, and the 6 o'clock direction. And the light shielding region is observed substantially along the polarization axis because it exists substantially along the 9 o'clock direction. On the other hand, as shown in FIG. 41B, when the width of the branch portion 14d is relatively large, the liquid crystal molecules 30a oriented in the direction parallel to the polarization axis are in the 12 o'clock direction and the 3 o'clock direction. Direction, the 6 o'clock direction, and the 9 o'clock direction, the position is different from the case shown in FIG.

  Since the area of the light-blocking region is smallest when the light-blocking region is observed along the polarization axis, the area of the light-blocking region is smaller than that in the case where the width of the branch portion 14d is relatively wide as shown in FIG. As shown in a), the area of the light shielding region is smaller when the width of the branch portion 14d is relatively narrow. Therefore, the transmittance in the second stable state is higher when the width of the branch 14d is relatively narrow.

  As described above, the transmittance Ia in the second stable state when the width of the branch 14d is relatively narrow is higher than the transmittance Ib in the second stable state when the width of the branch 14d is relatively wide. Therefore, in the case where the width of the branch 14d is relatively narrow, the change ΔIa in transmittance between immediately after the voltage application and the second stable state is equal to that in the case where the width of the branch 14d is relatively wide. It is smaller than the transmittance change amount ΔIb between the second stable state (ΔIa <ΔIb). Therefore, when the width of the branch portion 14d is relatively narrow, the white tailing phenomenon as shown in FIG. 23 is less likely to be observed than when the width is relatively wide, so that excellent response characteristics can be obtained.

  As described above, the response characteristics are improved as the width of the branch portions 14d is smaller. However, the response characteristics can also be improved by relatively reducing the number of the branch portions 14d.

  The pixel electrode 14 included in the liquid crystal display device according to the present invention may be configured such that all the island-shaped portions 14c adjacent to each other are connected to each other by the branch portions 14d as shown in FIG. The response characteristics can be improved by appropriately omitting the branch portions 14d. The pixel electrodes 14 are connected to switching elements, for example, in contact holes 19 provided in the light-shielding region 18 shown in FIG. 42, and the island-shaped portions 14c are electrically connected to each other by the branch portions 14d. They are connected and function substantially as one conductive film. The light-shielding region 18 is, for example, a region on the auxiliary capacitance wiring in the TFT substrate, and is a region through which light from the backlight does not transmit and does not contribute to display.

  Specifically, for example, as shown in FIGS. 43 and 44, when the number of the branch portions 14d is two or less per one island-shaped portion 14c, excellent response characteristics are obtained.

  An area that does not contribute to the display, for example, the branch 14d located in the light-shielding area 18 has almost no effect on the response characteristics. Therefore, as shown in FIG. The configuration may be such that there are two or less per unit 14c.

  Of course, the configuration of the solid portion 14b is not limited to the configuration described above. As shown in FIG. 46, when a configuration in which the branch portion 14d is partially omitted and the island portion 14c has redundancy is adopted as compared with the configuration shown in FIG. Further, a liquid crystal display device having a high yield rate is provided.

  As shown in FIG. 42, the response characteristics can be improved by reducing the number of the branches 14d as compared with a case where all the islands 14c adjacent to each other are connected to each other by the branches 14d. Can be improved. The number of branches 14d, that is, how much the branches 14d are omitted, may be determined according to a desired response characteristic or the like.

  For example, when the plurality of islands 14c are arranged in a matrix of m rows and n columns (m and n are natural numbers of 2 or more), all adjacent islands 14c are connected to each other by the branch 14d. In this case, the number of the branch portions 14d is (2mn-mn). Therefore, when the island portions 14c are arranged in a matrix of m rows and n columns, the response characteristic is improved by configuring the number of branch portions to be smaller than (2mn-mn). be able to.

  As described above, by optimizing the width and the number of the branch portions 14d, excellent response characteristics can be obtained.

  Note that the present invention is not limited to the illustrated liquid crystal display device, and one of a pair of electrodes for applying a voltage to the liquid crystal layer in the pixel region has a plurality of openings arranged at least at the corners of the pixel region. The liquid crystal display device having a wide viewing angle characteristic is realized by adopting a configuration having a solid portion and a solid portion. With the above configuration, an oblique electric field is formed at the edge of the opening of the electrode when a voltage is applied. Therefore, due to the oblique electric field generated at least at the edges of the plurality of openings arranged at the corners, the liquid crystal layer forms a liquid crystal domain that assumes a radially inclined alignment state in a voltage applied state, and thus has a wide field of view. An angular characteristic is obtained.

  A unit solid portion (a region of a solid portion substantially surrounded by an opening) existing in a certain pixel region may be a plurality of unit solid portions or an opening arranged at a corner. May be one unit solid part surrounded by. When the unit solid part existing in a certain pixel region is one unit solid part, the opening surrounding the unit solid part may be a plurality of openings arranged at the corners, A plurality of openings arranged at the corners may be continuous, substantially one opening.

  Since the region of the solid portion substantially surrounded by the opening (unit solid portion) has rotational symmetry, it is possible to enhance the stability of the radially inclined alignment of the liquid crystal domains formed in the solid portion. it can. For example, the shape of the unit solid portion may be substantially circular, substantially square, or substantially rectangular.

  When the shape of the unit solid portion is substantially circular, the radially inclined alignment of the liquid crystal domains formed in the solid portion of the electrode can be stabilized. One liquid crystal domain formed in a solid portion formed from a continuous conductive film is formed corresponding to the unit solid portion, so that the opening of the unit solid portion becomes substantially circular. What is necessary is just to determine the shape of a part and its arrangement. Further, by adopting a configuration in which the unit solid portion has a substantially rectangular shape in which the corners are substantially arc-shaped, a liquid crystal display device having relatively high alignment stability and transmittance (effective aperture ratio) can be obtained.

It is a figure which shows typically the structure of one picture element area | region of the liquid crystal display device 100 of Embodiment 1 by this invention, (a) is a top view, (b) is 1B-1B 'line in (a). It is sectional drawing along. 5A and 5B are diagrams illustrating a state in which a voltage is applied to the liquid crystal layer 30 of the liquid crystal display device 100, in which FIG. 5A schematically illustrates a state in which the alignment has begun to change (ON initial state), and FIG. Is schematically shown. (A)-(d) is a figure which shows typically the relationship between the line of electric force and the orientation of a liquid crystal molecule. (A)-(c) is a figure which shows typically the orientation state of the liquid crystal molecule seen from the substrate normal direction in the liquid crystal display device 100 of Embodiment 1 by this invention. (A)-(c) is a figure which shows typically the example of the radial inclination alignment of a liquid crystal molecule. (A) and (b) are top views schematically showing another picture element electrode used for the liquid crystal display device of Embodiment 1 according to the present invention. (A) And (b) is a top view which shows typically another picture element electrode used for the liquid crystal display device of Embodiment 1 by this invention. (A) And (b) is a top view which shows typically another picture element electrode used for the liquid crystal display device of Embodiment 1 by this invention. FIG. 11 is a top view schematically showing still another picture element electrode used in the liquid crystal display device of Embodiment 1 according to the present invention. (A) And (b) is a top view which shows typically another picture element electrode used for the liquid crystal display device of Embodiment 1 by this invention. 9A is a diagram schematically illustrating a unit lattice of the pattern illustrated in FIG. 1A, and FIG. 9B is a diagram schematically illustrating a unit lattice of the pattern illustrated in FIG. c) is a graph showing the relationship between the pitch p and the solid part area ratio. (A) is a figure which shows typically the unit lattice of the picture element electrode which has the unit solid part formed in the substantially circular shape, (b) and (c) are the substantially square whose corner part is substantially arc-shaped. FIG. 4D is a diagram schematically illustrating a unit lattice of a pixel electrode having a unit solid portion formed in FIG. 3D, and FIG. 4D schematically illustrates a unit lattice of a pixel electrode having a unit solid portion formed in a substantially square shape. FIG. It is a figure which shows typically the structure of one picture element area | region of the liquid crystal display device 200 of Embodiment 2 by this invention, (a) is a top view, (b) is 13B-13B 'line in (a). It is sectional drawing along. (A)-(d) is a schematic diagram for demonstrating the relationship between the orientation of the liquid crystal molecules 30a and the shape of the surface having vertical alignment. 5A and 5B are diagrams illustrating a state in which a voltage is applied to the liquid crystal layer 30 of the liquid crystal display device 200, where FIG. 5A schematically illustrates a state in which the alignment starts to change (ON initial state), and FIG. Is schematically shown. (A)-(c) is typical sectional drawing of the liquid crystal display device 200A, 200B, and 200C of Embodiment 2 from which the arrangement | positioning relationship of an opening part and a convex part differs. FIG. 14 is a diagram schematically illustrating a cross-sectional structure of the liquid crystal display device 200, and is a cross-sectional view taken along line 17A-17A ′ in FIG. It is a figure which shows typically the structure of one picture element area of the liquid crystal display device 200D of Embodiment 2 by this invention, (a) is a top view, (b) is 18B-18B 'line in (a). It is sectional drawing along. (A) is a diagram schematically showing the alignment state of liquid crystal molecules immediately after voltage application, and (b) and (c) are top views schematically showing the alignment state of liquid crystal molecules when alignment is stable (steady state). FIG. 7 is a graph showing the transmittance of a liquid crystal display device according to an embodiment of the present invention in a white display state on the vertical axis, and showing the angle formed by the polarization axis with respect to the 12:00 direction on the vertical axis. (A) is a diagram schematically showing the arrangement of a polarizing plate, and (b) is a diagram schematically showing a light shielding region SR in a liquid crystal domain when the polarizing plate is arranged as shown in (a). FIG. (A) is a diagram schematically showing the arrangement of a polarizing plate, and (b) is a diagram schematically showing a light shielding region SR in a liquid crystal domain when the polarizing plate is arranged as shown in (a). FIG. It is a figure which shows the white tailing phenomenon typically. It is a figure which shows typically a mode that the tailing phenomenon is prevented in the certain liquid crystal display device by this invention. (A) is a diagram schematically showing the arrangement of the polarizing plates, and (b) is a diagram schematically showing the light shielding region SR immediately after voltage application when the polarizing plates are arranged as shown in (a). FIG. 3C is a diagram schematically showing a light-shielding region SR when the orientation is stable (steady state) when a polarizing plate is arranged as shown in FIG. (A) is a diagram schematically showing the arrangement of the polarizing plates, and (b) is a diagram schematically showing the light shielding region SR immediately after voltage application when the polarizing plates are arranged as shown in (a). FIG. 3C is a diagram schematically showing a light-shielding region SR when the orientation is stable (steady state) when a polarizing plate is arranged as shown in FIG. When the angle of the polarization axis with respect to the 12:00 direction is 0 °, about 13 °, and about 20 °, the transmittance changes over time when a certain pixel region is changed from a black display state to a halftone display state. FIG. It is a figure which shows the black tailing phenomenon typically. FIG. 3 is a top view schematically showing a picture element electrode used in the liquid crystal display device of the embodiment according to the present invention. FIG. 3 is a top view schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied. FIG. 31 is a diagram schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied, and is a cross-sectional view taken along lines 31A-31A ′ and 31B-31B ′ in FIG. FIG. 3 is a top view schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied. FIG. 33 is a diagram schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied, and is a cross-sectional view taken along lines 33A-33A ′ and 33B-33B ′ in FIG. FIG. 3 is a top view schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied. (A) and (b) are diagrams schematically showing an alignment state of liquid crystal molecules when a voltage is applied, (a) is a cross-sectional view taken along line 35A-35A 'in FIG. 34) is a sectional view taken along the line 35B-35B 'in FIG. FIG. 3 is a top view schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied. (A) and (b) are cross-sectional views schematically showing an alignment state of liquid crystal molecules when a voltage is applied. (A) corresponds to a cross section taken along line 35A-35A 'in FIG. b) corresponds to a section taken along line 35B-35B 'in FIG. FIG. 3 is a top view schematically illustrating an alignment state of liquid crystal molecules when a voltage is applied. (A) and (b) are top views schematically showing an alignment state of liquid crystal molecules when a voltage is applied, (a) shows a case where the width of a branch portion of a pixel electrode is relatively narrow, (b) shows the case where the width of the branch of the pixel electrode is relatively narrow. 9 is a graph schematically showing a temporal change in transmittance when a voltage is applied to the liquid crystal layer when the width of the branch portion is relatively narrow and when it is relatively wide. (A) and (b) are top views schematically showing liquid crystal molecules oriented in a direction parallel to the polarization axis in the second stable state, and (a) shows a comparison of the width of the branch 14d. (B) shows a case where the width of the branch portion 14d is relatively wide. FIG. 3 is a top view schematically showing a picture element electrode used in the liquid crystal display device of the embodiment according to the present invention. FIG. 9 is a top view schematically showing another picture element electrode used for the liquid crystal display device of the embodiment according to the present invention. FIG. 9 is a top view schematically showing another picture element electrode used for the liquid crystal display device of the embodiment according to the present invention. FIG. 9 is a top view schematically showing another picture element electrode used for the liquid crystal display device of the embodiment according to the present invention. FIG. 9 is a top view schematically showing another picture element electrode used for the liquid crystal display device of the embodiment according to the present invention.

Explanation of reference numerals

11, 21 Transparent insulating substrate 14, 14A, 14B, 14C, 14D, 14E, 14
F Pixel electrode 14G, 14H, 14I Pixel electrode 14a Opening 14b Solid part (conductive film)
14b ′ Unit solid portion 14c Island portion 14d Branch portion 22 Counter electrode 30 Liquid crystal layer 30a Liquid crystal molecules 40, 40A, 40B, 40C, 40D Convex portion 40s Convex side surface 40t Convex top surface 100, 200 Liquid crystal display device 100a, 200a TFT substrate 100b Counter substrate

Claims (20)

A first substrate, a second substrate, and a liquid crystal layer provided between the first substrate and the second substrate;
A plurality of electrodes each defined by a first electrode provided on the liquid crystal layer side of the first substrate and a second electrode provided on the second substrate and facing the first electrode via the liquid crystal layer. Having a pixel area of
In each of the plurality of picture element regions, the first electrode has a plurality of openings and a solid portion, and the liquid crystal layer applies a voltage between the first electrode and the second electrode. It takes a vertical alignment state when not performed, and is generated at the edges of the plurality of openings of the first electrode when a voltage is applied between the first electrode and the second electrode. A plurality of liquid crystal domains each having a radially inclined alignment state are formed in the plurality of openings and the solid portion by an oblique electric field, and the alignment state of the plurality of liquid crystal domains changes according to an applied voltage. A liquid crystal display device that performs display by doing.   2. The at least one opening of the plurality of openings has substantially the same shape and the same size, and forms at least one unit cell arranged to have rotational symmetry. 3. The liquid crystal display device according to 1.   The liquid crystal display device according to claim 2, wherein each of the at least some of the plurality of openings has a rotational symmetry.   4. The liquid crystal display device according to claim 2, wherein each of the at least some of the plurality of openings is substantially circular.   4. The liquid crystal display device according to claim 2, wherein each of the regions of the solid portion surrounded by the at least one opening is substantially circular. 5.   4. The liquid crystal display device according to claim 2, wherein each of the regions of the solid portion surrounded by the at least a part of the opening has a substantially rectangular shape having a substantially arc-shaped corner portion. 5.   7. The device according to claim 1, wherein in each of the plurality of picture element regions, a total area of the plurality of openings of the first electrode is smaller than an area of the solid portion of the first electrode. 8. Liquid crystal display device.   A projection is further provided inside each of the plurality of openings, and a cross-sectional shape of the projection in an in-plane direction of the substrate is the same as a shape of the plurality of openings, and a side surface of the projection is The liquid crystal display device according to any one of claims 1 to 7, wherein the liquid crystal display device has an alignment control force in the same direction as the alignment control direction by the oblique electric field with respect to the liquid crystal molecules of the liquid crystal layer.   9. The liquid crystal display device according to claim 1, wherein the plurality of liquid crystal domains are in a spiral radially inclined alignment state. Further comprising a pair of polarizing plates provided outside the first substrate and the second substrate and arranged so that polarization axes are substantially orthogonal to each other;
In each of the plurality of liquid crystal domains, the liquid crystal molecules of the liquid crystal layer, which are positioned at 12 o'clock on the display surface with respect to the center of each of the plurality of liquid crystal domains, form with respect to 12 o'clock on the display surface. When the angle is θ, one of the polarization axes of the pair of polarizing plates is in the same direction as the direction in which the liquid crystal molecules positioned in the display surface 12 o'clock direction are inclined with respect to the display surface 12 o'clock direction. The liquid crystal display device according to claim 9, wherein the liquid crystal display device is inclined at an angle of more than 0 ° and less than 2θ with respect to the 12:00 display surface.   The liquid crystal display device according to claim 10, wherein the one polarization axis of the pair of polarizing plates is inclined at an angle of more than 0 ° and not more than θ.   The liquid crystal display device according to claim 10, wherein the one polarization axis of the pair of polarizing plates is inclined at substantially the same angle as θ / 2.   The liquid crystal display device according to claim 10, wherein the one polarization axis of the pair of polarizing plates is inclined at substantially the same angle as θ. The solid portion includes a plurality of islands arranged in a matrix of m rows and n columns, and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands to one another. And a part,
14. The liquid crystal display device according to claim 1, wherein the plurality of branches are a number of branches smaller than (2mn−mn). The first substrate further includes an active element provided corresponding to each of the plurality of picture element regions,
The first electrode is a pixel electrode provided for each of the plurality of pixel regions and is switched by the active element, and the second electrode is at least one counter electrode facing the plurality of pixel electrodes. The liquid crystal display device according to claim 1, wherein: A first substrate, a second substrate, and a liquid crystal layer provided between the first substrate and the second substrate;
A plurality of electrodes each defined by a first electrode provided on the liquid crystal layer side of the first substrate and a second electrode provided on the second substrate and facing the first electrode via the liquid crystal layer. Having a pixel area of
In each of the plurality of picture element regions, the liquid crystal layer assumes a vertical alignment state when no voltage is applied between the first electrode and the second electrode, and the first electrode includes the plurality of pixel regions. A liquid crystal display device comprising: a plurality of openings arranged at least at each corner of each of the picture element regions; and a solid portion.   17. The liquid crystal display device according to claim 16, wherein a shape of the region of the solid portion surrounded by at least a part of the plurality of openings has a rotational symmetry.   18. The liquid crystal display device according to claim 16, wherein a region of the solid portion surrounded by at least a part of the plurality of openings is substantially circular.   18. The liquid crystal display device according to claim 16, wherein a region of the solid portion surrounded by at least a part of the plurality of openings has a substantially rectangular shape having a substantially arc-shaped corner. The solid portion includes a plurality of islands arranged in a matrix of m rows and n columns, and a plurality of branches each of which electrically connects adjacent ones of the plurality of islands to one another. And a part,
20. The liquid crystal display device according to claim 16, wherein the plurality of branches are a number of branches smaller than (2mn-mn).