Liquid crystal display

Technical Field

0001The present invention relates to liquid crystal displays, and more particularly to segmented-pixel liquid crystal displays.

Background Art

0002Liquid crystal displays are flat displays that boast of high resolution, slimness, lightweight, low electric power consumption, and other advantages. In recent years, liquid crystal displays have seen improvement of display performance, improvement of fabrication capacity, and price competitiveness against other types of display, and accordingly they have been enjoying a rapidly growing market.

0003More recently, as the display quality of liquid crystal displays has been further improved, a problem in viewing angle characteristics has become apparent: the gamma characteristic varies between in orthogonal viewing and in oblique viewing; in other words, the gamma characteristic depends on the viewing angle. Here, the gamma characteristic denotes the dependence of display brightness on halftone levels. Thus, the fact that the gamma characteristic varies between in orthogonal viewing and in oblique viewing means that the way different halftone levels are displayed varies with the direction of viewing. This is annoying especially during the display of photograph images or of TV broadcasts, among others.

0004This problem of the viewing-angle dependence of the gamma characteristic is more remarkable in the multi-domain vertical alignment mode (MVA mode, as disclosed in <patcit id="pcit0001" dnum="JPH11242225A"><text>JP-A-H11-242225</text></patcit>) and in the axisymmetric aligned mode (ASM mode, as disclosed in <patcit id="pcit0002" dnum="JPH10186330A"><text>JP-A-H10-186330</text></patcit>) than in the in-plane switching mode (IPS mode, as disclosed in <patcit id="pcit0003" dnum="JPS63021907B"><text>JP-B-S63-021907</text></patcit>). On the other hand, with the IPS mode, it is more difficult, than with the MVA or ASM mode, to fabricate liquid crystal panels that offer high contrast in orthogonal viewing with satisfactory productivity. Hence, improvements addressing the viewing-angle dependence of the gamma characteristic are sought especially eagerly in MVA and ASM mode liquid crystal displays.

0005Under this background, the applicant of the present invention once proposed a technology whereby each pixel is segmented into two sub-pixels to which different voltages are applied to mitigate the viewing-angle dependence of the gamma characteristic (for example, in Patent Document 1 listed below). <ul id="ul0001" list-style="none" compact="compact"><li>Patent Document 1: <patcit id="pcit0004" dnum="JP2004078157A"><text>JP-A-2004-078157</text></patcit>, Claims</li><li>Patent Document 2: <patcit id="pcit0005" dnum="JPH6332009A"><text>JP-A-H6-332009</text></patcit>, Claims</li><li>Patent Document 3: <patcit id="pcit0006" dnum="JP2004062146A"><text>JP-A-2004-062146</text></patcit>, Embodiments</li></ul>

Disclosure of the Invention

Problems to be Solved by the Invention

0006Incidentally, the human eye tends to recognize pixels and borders by being attracted by light spots and areas. On the other hand, the recent trend toward increasingly large-screen liquid crystal displays has resulted in their having larger pixels than they have conventionally had. Under these circumstances, segmenting each pixel into two sub-pixels causes an inconvenience: as a result of the human eye recognizing pixels by tracing the lighter sub-pixel of each pixel, when an image with a straight border is displayed, the line of sight moves in a zigzag along the border, from one pixel with one halftone level to another having a different halftone level, often causing the viewer to perceive unsmoothness or unnatural hues. To be sure, in conventional liquid crystal displays, certain improvements have been made to address the viewing-angle dependence of the gamma characteristic; these improvements, however, are not quite satisfactory.

0007An object of the present invention is to provide a segmented-pixel liquid crystal display that does not produce unnaturalness even when displaying an image with a straight border and that offers a further improved gamma characteristic.

Means for Solving the Problem

0008To achieve the above object, according to one aspect of the invention, in a liquid crystal display, a plurality of pixels, each having a plurality of electrodes for applying an electric field to a liquid crystal layer, are arrayed in a matrix; in each pixel, three sub-pixels, namely one middle and two side sub-pixels, are arranged next to one another in the column or row direction; the three sub-pixels have at least two different brightness levels when the pixel as a whole is in a given middle halftone state, and the middle sub-pixel has the highest brightness level. In the present specification, "a middle halftone state" denotes any intermediate state between the highest and lowest halftone levels.

0009Here, preferably, the two side sub-pixels are given an identical brightness level.

0010From the viewpoint of further improving the gamma characteristic of the liquid crystal display, preferably, the ratio of the aperture area of the middle sub-pixel to the total aperture area of the two side sub-pixels is in the range from 1 : 1 to 1 : 4 and, preferably, the ratio between aperture areas of the two side sub-pixels is in the range from 1 : 1 to 1 : 4.

0011According to a preferred embodiment, in the liquid crystal display, preferably, the three sub-pixels each have: a liquid crystal capacitance between a sub-pixel electrode and an common electrode disposed opposite each other across the liquid crystal layer; and an auxiliary capacitance between an auxiliary capacitance electrode electrically connecting to the sub-pixel electrode and an auxiliary capacitance common electrode disposed opposite the auxiliary capacitance electrode and connecting to an auxiliary capacitance conductor. Moreover, a single electrode may be shared as the common electrodes of the three sub-pixels; moreover, at least two different auxiliary capacitance conductors may provided, one for the middle sub-pixel and another for the side sub-pixels. Here, preferably, an insulating layer is interposed between the auxiliary capacitance electrode and the auxiliary capacitance common electrode.

0012Preferably, there are provided: scanning lines extending in the row direction; signal lines extending in the column direction; and, for each pixel, at least two switching devices that are provided one for the middle sub-pixel and another for the side sub-pixels and that connect to a scanning line and a signal line each common to the three sub-pixels of the pixel. Moreover, preferably, the switching devices are turned on and off by a scanning signal voltage supplied to the common scanning line and, when the switching devices are on, a display signal voltage is supplied from the common signal line to the sub-pixel electrode and the auxiliary capacitance electrode of each of the middle and side sub-pixels; moreover, preferably, after the switching devices are turned off, the auxiliary capacitance common voltages at the auxiliary capacitance common electrodes of the middle and side sub-pixels vary such that the variations in those voltages as defined by the directions and degrees in which they vary differ between the middle sub-pixel and the side sub-pixels.

0013Here, for a higher aperture ratio, preferably, the switching devices are TFTs, and these TFTs are formed with a single semiconductor layer.

0014The auxiliary capacitance common voltages may invert the polarities thereof periodically. Preferably, the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrode of the middle sub-pixel and the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrodes of the side sub-pixels are 180 degrees out of phase with each other. Preferably, the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrode of the middle sub-pixel and the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrodes of the side sub-pixels have an equal amplitude.

0015Preferably, between every two mutually adjacent signal lines, display signal voltages applied thereto are given opposite polarities and, between every two pixels mutually adjacent in the row direction, the auxiliary capacitance electrodes and the auxiliary capacitance common electrodes of the middle and side sub-pixels are disposed in reversed patterns.

0016From the viewpoint of improving the aperture ration, preferably, the scanning lines are laid between mutually adjacent pixels, and, in each pixel, the two auxiliary capacitance conductors are laid parallel to the scanning lines and between the sub-pixels. Here, from the viewpoint of improving image quality, preferably, the conductor electrode via which the display signal voltage is supplied to the sub-pixel electrode of the middle sub-pixel is so formed as to cross the two auxiliary capacitance conductors.

0017The sub-pixel electrodes of the three sub-pixels may be separate from one another, or may be continuous with each other.

0018From the viewpoint of preventing disturbed alignment in the liquid crystal layer and improving display quality, preferably, a metal layer is formed under a contact hole via which the conductor electrode via which the display signal voltage is supplied connects to the sub-pixel electrode, with an insulating layer interposed between the metal layer and the contact hole.

Advantages of the Invention

0019According to the present invention, in each pixel, three sub-pixels are formed that are arranged next to one another in the column or row direction. This helps further mitigate the viewing-angle dependence of the gamma characteristic as compared with that conventionally observed. Moreover, the three sub-pixels have at least two different brightness levels when the pixel as a whole is in a given middle halftone state, and the middle sub-pixel has the highest brightness level. Thus, even when an image with a straight border is displayed, the line of sight, as it moves along the border, moves across pixels having the same halftone level, unlike in a case where each pixel has two sub-pixels. This prevents the viewer from perceiving unsmoothness or unnatural hues at a border between different halftone levels.

0020Here, preferably, the two side sub-pixels are given an identical brightness level. This helps reduce the numbers of switching devices, auxiliary capacitance conductors, and other elements, and thus helps prevent undue lowering of the aperture ratio.

0021Preferably, the ratio of the aperture area of the middle sub-pixel to the total aperture area of the two side sub-pixels is in the range from 1 : 1 to 1 : 4 and, preferably, the ratio between aperture areas of the two side sub-pixels is in the range from 1 : 1 to 1 : 4. This helps further improve the gamma characteristic of the liquid crystal display.

0022Preferably, the three sub-pixels each have: a liquid crystal capacitance between a sub-pixel electrode and an common electrode disposed opposite each other across the liquid crystal layer; and an auxiliary capacitance between an auxiliary capacitance electrode electrically connecting to the pixel electrode and an auxiliary capacitance common electrode disposed opposite the auxiliary capacitance electrode and connecting to an auxiliary capacitance conductor; moreover, a single electrode may be shared as the common electrodes of the three sub-pixels; moreover, at least two different auxiliary capacitance conductors may provided, one for the middle sub-pixel and another for the side sub-pixels. This helps improve the controllability of the voltages applied to the sub-pixels.

0023Here, preferably, an insulating layer is interposed between the auxiliary capacitance electrode and the auxiliary capacitance common electrode. This allows those electrodes to overlap to form an auxiliary electrode, and thus helps increase the aperture ratio. Preferably, there are provided: scanning lines extending in the row direction; signal lines extending in the column direction; and, for each pixel, at least two switching devices that are provided one for the middle sub-pixel and another for the side sub-pixels and that connect to a scanning line and a signal line each common to the three sub-pixels of the pixel. Moreover, preferably, the switching devices are turned on and off by a scanning signal voltage supplied to the common scanning line and, when the switching devices are on, a display signal voltage is supplied from the common signal line to the sub-pixel electrode and the auxiliary capacitance electrode of each of the middle and side sub-pixels; moreover, preferably, after the switching devices are turned off, the auxiliary capacitance common voltages at the auxiliary capacitance common electrodes of the middle and side sub-pixels vary such that the variations in those voltages as defined by the directions and degrees in which they vary differ between the middle sub-pixel and the side sub-pixels. This helps further improve the controllability of the voltages applied to the sub-pixels.

0024Here, preferably, the switching devices are TFTs, and these TFTs are formed with a single semiconductor layer. This helps increase the aperture ratio of the pixel.

0025The auxiliary capacitance common voltages may invert the polarities thereof periodically; preferably, the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrode of the middle sub-pixel and the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrodes of the side sub-pixels are 180 degrees out of phase with each other; and, preferably, the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrode of the middle sub-pixel and the auxiliary capacitance common voltage applied to the auxiliary capacitance common electrodes of the side sub-pixels have an equal amplitude. This helps further improve the controllability of the voltages applied to the sub-pixels.

0026Preferably, between every two mutually adjacent signal lines, display signal voltages applied thereto are given opposite polarities, in which case, preferably, between every two pixels mutually adjacent in the row direction, the auxiliary capacitance electrodes and the auxiliary capacitance common electrodes of the middle and side sub-pixels are disposed in reversed patterns. This allows the center sub-pixel to have the highest brightness.

0027Preferably, the scanning lines are laid between mutually adjacent pixels, and, in each pixel, the two auxiliary capacitance conductors are laid parallel to the scanning lines and between the sub-pixels. This helps improve the aperture ratio. Moreover, preferably, the conductor electrode via which the display signal voltage is supplied to the sub-pixel electrode of the middle sub-pixel is so formed as to cross the two auxiliary capacitance conductors. This helps cancel out the two parasitic capacitances formed where the conductor electrode crosses the auxiliary capacitance conductors, and thus helps improve image quality.

0028Preferably, a metal layer is formed under a contact hole via which the conductor electrode via which the display signal voltage is supplied connects to the sub-pixel electrode. This helps shield disturbed alignment in the liquid crystal layer, and thus helps improve image quality.

Brief Description of Drawings

0029[<figref idref="f0001">Fig. 1</figref>] A plan view schematically showing the pixel structure in a liquid crystal display according to the invention. <ul id="ul0002" list-style="none" compact="compact"><li>[<figref idref="f0002">Fig. 2</figref>] A cross-sectional view along line A-A shown in <figref idref="f0001">Fig. 1</figref>.</li><li>[<figref idref="f0002">Fig. 3</figref>] A cross-sectional view along line B-B shown in <figref idref="f0001">Fig. 1</figref>.</li><li>[<figref idref="f0002">Fig. 4</figref>] A graph showing the viewing-angle dependence of the gamma characteristic in relation to the ratio of the aperture area of the middle sub-pixel to the ratio of the total aperture area of the side sub-pixels.</li><li>[<figref idref="f0003">Fig. 5</figref>] An enlarged plan view of the TFTs shown in <figref idref="f0001">Fig. 1</figref>.</li><li>[<figref idref="f0004">Fig. 6</figref>] A circuit diagram electrically equivalent to the pixel structure in the liquid crystal display shown in <figref idref="f0001">Fig. 1</figref>.</li><li>[<figref idref="f0005">Fig. 7</figref>] A diagram schematically showing an example of the voltage waveforms with which the liquid crystal display according to the invention is driven.</li><li>[<figref idref="f0006">Fig. 8</figref>] A plan view schematically showing the pixel structure in another liquid crystal display according to the invention.</li><li>[<figref idref="f0007">Fig. 9</figref>] A plan view schematically showing another example of the sub-pixel electrodes usable in the invention.</li></ul>

List of Reference Symbols

003010a, 10b, 10c sub-pixels <ul id="ul0003" list-style="none" compact="compact"><li>11a, 11b, 11c, 11d sub-pixel electrodes</li><li>12 scanning lines</li><li>13 signal lines</li><li>140, 14E auxiliary capacitance conductors</li><li>15a, 15b, 15c TFTs (switching devices)</li><li>16a, 16b, 16c, 16d, 16e, 16a', 16b' extensions from drain electrodes</li><li>17a, 17b auxiliary capacitance electrodes</li><li>18a, 18b, 18c contact holes</li><li>19 metal layer</li><li>21 common electrode</li><li>141, 142, 141', 142' auxiliary capacitance common electrode</li><li>SC semiconductor layer</li><li>ClcO, ClcE₁, ClcE₂ liquid crystal capacitances</li><li>CcsO, CcsE auxiliary capacitances</li></ul>

Best Mode for Carrying Out the Invention

0031Hereinafter, liquid crystal displays embodying the present invention will be described with reference to the accompanying drawings. It should be understood that these embodiments are not meant to limit in any way how the invention is implemented.

0032<figref idref="f0001">Fig. 1</figref> is a plan view schematically showing the pixel structure on the active matrix substrate of a liquid crystal display according to the invention, focusing on the pixel at line n, column m. <figref idref="f0002">Figs. 2 and 3</figref> are cross-sectional view along lines A-A and B-B, respectively, shown in <figref idref="f0001">Fig. 1</figref>. Sub-pixel electrodes 11a-11c are arranged next to one another in the column direction. A scanning line 12(<i>n</i>) is laid between pixels to run laterally as seen in <figref idref="f0001">Fig. 1</figref>; a signal line 13(m) is laid between pixels to run longitudinally as seen in <figref idref="f0001">Fig. 1</figref>. Two auxiliary capacitance conductors 140 and 14E are laid parallel to the scanning line 12(<i>n</i>), between the sub-pixel electrodes 11a, 11b; and 11c. As switching devices, TFTs 15a-15c are provided at the intersection between the scanning line 12(<i>n</i>) and the signal line 13(<i>m</i>).

0033A drain electrode extension 16a from the TFT 15a runs over the auxiliary capacitance conductor 14E to reach above the auxiliary capacitance conductor 140, where a portion of the drain electrode extension 16a faces, across an insulating layer (unillustrated), an auxiliary capacitance common electrode 141 formed integrally with the auxiliary capacitance conductor 140 to function as an auxiliary capacitance electrode 17a. In this auxiliary capacitance electrode 17a, a contact hole 18a is formed to connect the drain electrode extension 16a to the sub-pixel electrode 11 a. Likewise, drain electrode extensions 16b and 16c merge together on the way to reach above the auxiliary capacitance conductor 14E, where a portion of the drain electrodes extension 16b and 16c faces, across an insulating layer (unillustrated), an auxiliary capacitance common electrode 142 formed integrally with the auxiliary capacitance conductor 14E to function as an auxiliary capacitance electrode 17b. In this auxiliary capacitance electrode 17b, a contact hole 18b is formed to connect the drain electrodes extension 16b and 16c to the sub-pixel electrode 11b (see <figref idref="f0002">Fig 2</figref>). From the auxiliary capacitance electrode 17b, a drain electrode extension 16d further extends to run over the auxiliary capacitance conductor 140 to reach above the sub-pixel electrode 11c, where the drain electrode extension 16d connects via a contact hole 18c to the sub-pixel electrode 11c (see <figref idref="f0002">Fig. 3</figref>).

0034As shown in <figref idref="f0002">Figs. 2 and 3</figref>, under the contact hole 18b, the auxiliary capacitance conductor 14E is formed with an insulating layer 21a interposed in between; under the contact hole 18c, a metal layer 19 forming an island is formed with an insulating layer 21 b interposed in between. This helps shield disturbed alignment in the liquid crystal layer, and thus helps improve image quality. The insulating layer 21 a, which forms an auxiliary capacitance, and the insulating layer 21b under the contact hole 18c are each, for example, the gate insulating layer of a TFT.

0035With this structure, an equal effective voltage is applied to the sub-pixel electrodes 11 b and 11c. Moreover, as will be described later, by supplying different auxiliary capacitance common voltages to the two auxiliary capacitance conductors 140 and 14E, it is possible to make the effective voltage at the sub-pixel electrode 11a higher than the effective voltage at the sub-pixel electrodes 11b and 11c. Thus, it is possible to make the brightness level of a sub-pixel 10a higher than the brightness level of sub-pixels 10b and 10c. This helps eliminate unnaturalness as is conventionally produced when an image with a straight border is displayed, and also helps further mitigate the viewing-angle dependence of the gamma characteristic.

0036Through experiments, the applicant has come to know that an effective way to mitigate the viewing-angle dependence of the gamma characteristic is to reduce the proportion of the aperture area of the sub-pixel 10a that has a higher brightness level. In <figref idref="f0002">Fig. 4</figref> is a graph showing the viewing-angle dependence in relation to the ratio of the aperture area of the higher-brightness sub-pixel 10a (indicated as "high" in the graph) to the total aperture area of the lower-brightness sub-pixels 10b and 10c (indicated as "low" in the graph). In <figref idref="f0002">Fig. 4</figref>, the horizontal axis represents the halftone level observed in orthogonal viewing, and the vertical axis represents the viewing-angle dependence of the gamma characteristic observed at different aperture area ratios, namely "with no pixel segmentation", "at a high-to-low ratio of 1:1 ", "at a high-to-low ratio of 1:3", and "at a high-to-low ratio of 1:4", by using the halftone level observed in oblique viewing from 45 degrees upward, downward, leftward, and rightward. This graph shows the following. As the proportion of the "high" brightness aperture area decreases, the gamma characteristic becomes increasingly close to the ideal straight line, becoming closest to it when the high-to-low ratio is 1 : 3; as the "high" brightness aperture area further decreases (to 1:4), the gamma characteristic then becomes increasingly less close to the ideal straight line. Hence, the ratio of the aperture area of the higher brightness sub-pixel 10a to the total aperture area of the lower sub-pixels 10b and 10c is preferably in the range between 1 : 1 to 1 : 4, and further preferably in the range between 1 : 2.5 to 1 : 3.5. Incidentally, the relationship between, on one hand, the just mentioned viewing-angle dependence of the gamma characteristic in relation to the aperture area ratio and, on the other hand, transmissivity is explained in <patcit id="pcit0007" dnum="JP2004062146A"><text>JP-A-2004-062146</text></patcit>, a prior application by the same applicant.

0037Moreover, the ratio between the aperture areas of the sub-pixels 10b and 10c is preferably in the range from 1 : 1 to 1 : 4, and further preferably in the range from 1 : 1 to 1 : 2. With the higher-brightness sub-pixel located in a deviated position, an evaluation of the display quality of an image of a person revealed an unintended change in color at the border of a skin-color area, like where a skin-color area, such as representing the chin of a person, overlaps a single-color background, such as clothes. This phenomenon was alleviated when the higher-brightness sub-pixel was located closer to the center.

0038In the embodiment under discussion, TFTs (thin-film transistors) are used as switching devices. <figref idref="f0003">Fig. 5</figref> is an enlarged view of the TFTs in the liquid crystal display shown in <figref idref="f0001">Fig. 1</figref>. On top of a gate electrode G formed as part of the scanning line 12(<i>n</i>), a gate insulating film (unillustrated) is formed, and, further on top, a semiconductor layer SC is formed. On top of this semiconductor layer SC, a source electrode S and three drain electrodes D₁, D₂, and D₃ are formed. From the source electrode S, a plurality of extensions extend substantially in the shape of a comb. The drain electrodes D₁, D₂, and D₃ are formed between these extensions, with a predetermined distance secured from them.

0039Forming the three TFTs 15a to 15c on a single semiconductor layer SC in this way helps give the pixel a larger aperture ratio than when they are formed separately. Moreover, by varying the width W and length L of the channel regions formed between the extensions of the source electrode S and the drain electrodes D₁, D₂, and D₃, it is possible to supply the desired current that suits the capacity of the pixel.

0040There are no particular restrictions on the shapes of the source electrode S, the drain electrodes D₁, D₂, and D₃, and the semiconductor layer SC; these may be given any shapes so long as no current leakage occurs. As switching devices, any conventionally known switching devices other than TFTs may instead be used, such as MIMs (metal insulator metals).

0041<figref idref="f0004">Fig. 6</figref> is a schematic diagram showing a circuit equivalent to the liquid crystal display shown in <figref idref="f0001">Fig. 1</figref>. In this diagram, the liquid crystal capacitance corresponding to the sub-pixel 10a is indicated as ClcO, and the liquid crystal capacitances corresponding to the sub-pixels 10b and 10c is indicated as ClcE₁ and ClcE₂. The liquid crystal capacitances ClcO, ClcE₁, and ClcE₂ of the sub-pixels 10a, 10b, and 10c are formed by the sub-pixel electrodes 11 a to 11c, a common electrode 21, and the liquid crystal layer lying in between. The sub-pixel electrodes 11a to 11c are connected via the TFTs 15a to 15c to the signal line 13(<i>m</i>), and the gate electrode G (shown in <figref idref="f0003">Fig. 5</figref>) of the TFTs is connected to the scanning line 12(n)

0042A first auxiliary capacitance provided for the sub-pixel 10a and a second auxiliary capacitance provided for the sub-pixels 10b and 10c are indicated as CcsO and CscE in <figref idref="f0004">Fig. 6</figref>. The auxiliary capacitance electrode 17a of the first auxiliary capacitance CcsO is connected via the drain electrode extension 16a to the drain of the TFT 15a. The auxiliary capacitance electrode 17b of the second auxiliary capacitance CcsE is connected via the drain electrode extensions 16b and 16c to the drains of the TFTs 15b and 15c. The auxiliary capacitance electrodes 17a and 17b may be connected in any manner other than specifically illustrated, so long as they are electrically so connected as to receive voltages equal to those applied to the corresponding sub-pixel electrodes, namely the sub-pixel electrode 11a and the sub-pixel electrodes 11b and 11c, respectively; that is, the sub-pixel electrode 11a and the sub-pixel electrodes 11b and 11c have simply to be electrically connected, either directly or indirectly, to the corresponding auxiliary capacitance electrodes 17a and 17b, respectively.

0043The auxiliary capacitance common electrode 141 of the first auxiliary capacitance CcsO is connected to the auxiliary capacitance conductor 140, and the auxiliary capacitance common electrode 142 of the second auxiliary capacitance CcsE is connected to the auxiliary capacitance conductor 14E. With this structure, it is possible to apply different auxiliary capacitance common voltages to the auxiliary capacitance common electrodes 141 and 142 of the first and second auxiliary capacitance CcsO and CcsE, respectively. As will be described later, how the auxiliary capacitance common electrodes 141 and 142 are connected to the first and second auxiliary capacitances CcsO and CcsE is selected to suit the driving method adopted (for example, dot-inversion driving).

0044Next, a description will be given of the mechanism by which different voltages are applied, on one hand, to the sub-pixel electrode 11 a and, on the other hand, to the sub-pixel electrodes 11 b and 11c.

0045<figref idref="f0005">Fig. 7</figref> shows the voltage waveforms of the signals fed to the pixel (n, m) shown in <figref idref="f0004">Fig. 6</figref>; that is, it shows how those signals change their voltage levels over time. In <figref idref="f0005">Fig. 7</figref>, at (a) is shown the waveform of the display signal voltage (halftone signal voltage) Vs supplied to a signal line 13; at (b) is shown the waveform of the scanning signal voltage Vg supplied to a scanning line 12; at (c) and (d) are shown the waveforms of the auxiliary capacitance common voltages VcsO and Vcse supplied to the auxiliary capacitance conductors 140 and 14E, respectively; at (e) and (f) are shown the waveforms of the voltages VlcO and VlcE applied to the liquid crystal capacitances ClcE₁ and ClcE₂ of the sub-pixel 10a and of the sub-pixels 10b and 10c, respectively.

0046The driving method shown in <figref idref="f0005">Fig. 7</figref> is adopted when the invention is applied to a liquid crystal display that operates on a "1H dot inversion plus frame inversion" basis.

0047The display signal voltage Vs applied to a signal line 13 inverts its polarity every time a scanning line is selected (every 1H); in addition, between every two mutually adjacent signal lines, the display signal voltages applied thereto have opposite polarities (1H inversion). Moreover, the display signal voltages Vs on all the signal lines 13 invert their polarities every frame (frame inversion).

0048In the example under discussion, the cycle at which the auxiliary capacitance common voltages VcsO and Vcse invert their polarities is 2H; moreover, the auxiliary capacitance common voltages VcsO and Vcse have waveforms such that they have an equal amplitude and are 180 degrees out of phase with each other. The cycle at which the auxiliary capacitance common voltages VcsO and Vcse invert their polarities may be longer than 2H.

0049Now, with reference to <figref idref="f0005">Fig. 7</figref>, a description will be given of why the voltages VlcO and VlcE applied to the liquid crystal capacitance ClcO and to the liquid crystal capacitances ClcE₁ and ClcE₂ change their voltage levels as shown in <figref idref="f0005">Fig. 7</figref>.

0050At time T₁, the scanning signal voltage Vg turns from low (VgL) to high (VgH), and thereby brings the TFTs 15a to 15c into a conducting state, allowing the display signal voltage Vs on the signal line 13 to be applied to the sub-pixel electrodes 10a to 10c. The voltages applied across the liquid crystal capacitance ClcO and across the liquid crystal capacitances ClcE₁ and ClcE₂ are the differences between the voltages at the sub-pixel electrodes 11a to 11c and the voltage (Vcom) at the common electrode 21. That is, VlcO = VlcE₁ = VlcE₂ = Vs - Vcom.

0051At time T₂, the scanning signal voltage Vg turns from high (VgH) to low (VgL, &lt; Vs), and thereby brings the TFTs 15a to 15c into a non-conducting state (off state), electrically insulating all the sub-pixels and the auxiliary capacitances from the signal line 13. At this point, under the influence of the parasitic capacitances etc. of the TFTs 15a to 15c, the voltages at the sub-pixel electrodes 11a to 11c momentarily fall by ΔVd, a phenomenon called "pulling".

0052At time T₃, the voltage VlcO at the liquid crystal capacitance ClcO changes under the influence of the voltage VcsO at the auxiliary capacitance common electrode 141 of the auxiliary capacitance CcsO, which electrode is electrically connected to the sub-pixel electrode 11a of the liquid crystal capacitance ClcO. Moreover, the voltage VlcE at the liquid crystal capacitances ClcE₁ and ClcE₂ changes under the influence of the voltage VcsE at the auxiliary capacitance common electrode 142 of the second auxiliary capacitance CcsE, which electrode is electrically connected to the sub-pixel electrodes 11 b and 11 c of the liquid crystal capacitances ClcE₁ and ClcE₂.

0053Here, suppose that, at time T₃, the auxiliary capacitance common voltage VcsO increases by VcsOp > 0 and the auxiliary capacitance common voltage VcsE decreases by VcsEp > 0. That is, let the whole amplitude Vp - p of the auxiliary capacitance common voltage VcsO be VcsOp, and let the whole amplitude of the auxiliary capacitance common voltage VcsE be VceEp.

0054Moreover, let the total capacitance of the liquid crystal capacitance ClcO and the auxiliary capacitance CcsO be C_pixO, and let the total capacitance of the liquid crystal capacitances ClcE₁ and ClcE₂ and the auxiliary capacitance CcsE be C_pixE. Then, <maths id="math0001" num=""><math display="block"><mi>VlcO</mi><mo mathvariant="normal">=</mo><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo mathvariant="normal">+</mo><mi>VcsOp</mi><mfenced separators=""><mi>CcsO</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">O</mi></mfenced><mo mathvariant="normal">-</mo><mi>Vcom</mi><mo mathvariant="normal">,</mo></math><img file="EP1978398A2_D0001.tif" /></maths> and <maths id="math0002" num=""><math display="block"><mi>VlcE</mi><mo mathvariant="normal">=</mo><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo mathvariant="normal">+</mo><mi>VcsEp</mi><mfenced separators=""><mi>CcsE</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">E</mi></mfenced><mo mathvariant="normal">-</mo><mi>Vcom</mi><mn>.</mn></math><img file="EP1978398A2_D0002.tif" /></maths>

0055Next, at time T₄, likewise under the influence of the voltages VcsO and VceE at the auxiliary capacitance common electrodes, the voltages VlcO and VlcE restore their voltages at time T₂. <maths id="math0003" num=""><math display="block"><mi>VlcO</mi><mo>=</mo><mi>Vs</mi><mo>-</mo><mi mathvariant="normal">ΔVd</mi><mo>-</mo><mi>Vcom</mi><mo>,</mo></math><img file="EP1978398A2_D0003.tif" /></maths> and <maths id="math0004" num=""><math display="block"><mi>VlcE</mi><mo>=</mo><mi>Vs</mi><mo>-</mo><mi mathvariant="normal">ΔVd</mi><mo>-</mo><mi>Vcom</mi><mn>.</mn></math><img file="EP1978398A2_D0004.tif" /></maths>

0056These changes in voltage are repeated until the voltage Vg(<i>n</i>) turns to VgH in the next frame. As a result, the voltages VlcO and VlcE come to have different effective values. Specifically, let the effective value of the voltage VlcO be VlcO_rms, and let the effective value of the voltage VlcE be VlcE_rms, then <maths id="math0005" num=""><math display="block"><msub><mi>VlcO</mi><mi>rms</mi></msub><mo mathvariant="normal">=</mo><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo mathvariant="normal">+</mo><mfenced separators=""><mn>1</mn><mo>/</mo><mn>2</mn></mfenced><mo>⁢</mo><mi>VcsOp</mi><mfenced separators=""><mi>CcsO</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">O</mi></mfenced><mo mathvariant="normal">-</mo><mi>Vcom</mi><mo>,</mo></math><img file="EP1978398A2_D0005.tif" /></maths> and <maths id="math0006" num=""><math display="block"><msub><mi>VlcE</mi><mi>rms</mi></msub><mo mathvariant="normal">=</mo><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo>-</mo><mfenced separators=""><mn>1</mn><mo>/</mo><mn>2</mn></mfenced><mo>⁢</mo><mi>VcsEp</mi><mfenced separators=""><mi>CcsE</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">E</mi></mfenced><mo mathvariant="normal">-</mo><mi>Vcom</mi></math><img file="EP1978398A2_D0006.tif" /></maths><maths id="math0007" num=""><math display="block"><mrow><mo mathvariant="normal">(</mo><mi>provided that</mi><mo>⁢</mo><mfenced separators=""><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo mathvariant="normal">-</mo><mi>Vcom</mi></mfenced><mo mathvariant="normal">≫</mo><mi>VcsOp</mi><mfenced separators=""><mi>CcsO</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">O</mi></mfenced><mo mathvariant="normal">,</mo></mrow></math><img file="EP1978398A2_D0007.tif" /></maths> and <maths id="math0008" num=""><math display="block"><mrow><mfenced separators=""><mi>Vs</mi><mo mathvariant="normal">-</mo><mi mathvariant="normal">ΔVd</mi><mo mathvariant="normal">-</mo><mi>Vcom</mi></mfenced><mo mathvariant="normal">≫</mo><mi>VcsEp</mi><mfenced separators=""><mi>CcsE</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">E</mi></mfenced><mo>)</mo></mrow><mn>.</mn></math><img file="EP1978398A2_D0008.tif" /></maths> Hence, let the differences between these effective values be ΔVlc = VlcO_rms - VlcE_rms, then <maths id="math0009" num=""><math display="block"><mi>DVlc</mi><mo mathvariant="normal">=</mo><mfenced open="[" close="]" separators=""><mi>VcsOp</mi><mfenced separators=""><mi>CcsO</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">O</mi></mfenced><mo mathvariant="normal">+</mo><mi>VcsEp</mi><mfenced separators=""><mi>CcsE</mi><mo mathvariant="normal">/</mo><msub><mi mathvariant="normal">C</mi><mi>pix</mi></msub><mo>⁢</mo><mi mathvariant="normal">E</mi></mfenced></mfenced><mo mathvariant="normal">/</mo><mn mathvariant="normal">2.</mn></math><img file="EP1978398A2_D0009.tif" /></maths> In this way, by controlling the voltages applied to the auxiliary capacitance common electrodes 141 and 142 of the auxiliary capacitances CcsO and CcsE connected to the sub-pixel electrodes 11a to 11c, it is possible to apply different voltages to the sub-pixel electrode 11a and to the sub-pixel electrodes 11b and 11c.

0057By interchanging the voltages VcsO and VcsE, it is possible to give the voltage VlcO a smaller effective value and the voltage VlcE a greater effective value. Alternatively, also by reversing the combination of the auxiliary capacitance conductors 140 and 14E connected to the auxiliary capacitance common electrodes 141 and 142 of the auxiliary capacitances CcsO and CcsE, it is possible to give the voltage VIcO a smaller effective value and the voltage VIcE a greater effective value.

0058Here, since the driving method adopted involves frame inversion, in the next frame, the polarity of the voltage Vs is inverted, so that Vlc &lt; 0. Even then, the same results as described above can be obtained by inverting the polarities of VcsO and VcsE in synchronism with frame inversion.

0059Moreover, here, since the driving method adopted involves dot inversion, between every two mutually adjacent signal lines 13 (<i>m</i>) and 13(<i>m</i>+1), the display signal voltages supplied thereto have opposite polarities. Thus, to make the effective voltage applied to the sub-pixel electrode 11a' always higher than the effective voltage applied to the sub-pixel electrodes 11b' and 11c' even in the pixel (n, <i>m</i>+1) in the next frame, as shown in <figref idref="f0006">Fig. 8</figref>, it is necessary that the auxiliary capacitance electrode 17a' of the sub-pixel electrode 11a' face the auxiliary capacitance common electrode 142' of the auxiliary capacitance conductor 14E and that the auxiliary capacitance electrode 17b' of the sub-pixel electrodes 11b' and 11c' face the auxiliary capacitance common electrode 141' of the auxiliary capacitance conductor 140.

0060Here, in the pixel <i>(n, m),</i> since the drain electrode extension 16a of the sub-pixel electrode 11a crosses the two auxiliary capacitance conductors 140 and 14E, and the voltages applied to the auxiliary capacitance conductors 140 and 14E are 180 degrees out of phase with each other, the parasitic capacitances attributable to the drain electrode extension 16a and attributable to the auxiliary capacitance conductors 140 and 14E cancel out. On the other hand, in the pixel (n, <i>m</i>+1), although the drain electrode extension 16a' of the sub-pixel electrode 11a' does not need to cross the auxiliary capacitance conductor 140, if the drain electrode extension 16a' of the sub-pixel electrode 11a' crosses only the auxiliary capacitance conductor 14E, the above-mentioned parasitic capacitances do not cancel out, and cause uneven display between the sub-pixel electrodes 11a and 11a'. To overcome this inconvenience, it is recommended that a drain electrode extension 16e be formed to extend further from the auxiliary capacitance electrode 17a' of the sub-pixel electrode 11a' to reach above the auxiliary capacitance conductor 140 so that together the drain electrode extensions cross the two auxiliary capacitance conductors 140 and 14E.

0061In the liquid crystal display described above, the sub-pixel electrodes 11 a to 11c of the sub-pixels 10a to 10c are formed separately from one another (see <figref idref="f0001">Fig. 1</figref>); it is however also possible to form the sub-pixel electrodes 11 b and 11c as a single sub-pixel electrode 11d as shown in <figref idref="f0007">Fig. 9</figref>. Even in that case, just as described previously, by controlling the voltages applied to the auxiliary capacitance common electrodes 141 and 142 connected to the sub-pixel electrodes 11a and 11d, it is possible to apply different voltages to the sub-pixel electrodes 11a and 11d. In the liquid crystal display described above, the sub-pixels are arranged next to one another in the column direction; needless to say, it is also possible to arrange them in the row direction instead.

0062The embodiment described above demonstrates that the present invention contributes to improving the gamma characteristic in normally black mode liquid crystal displays, in particular MVA mode liquid crystal displays. It should however be understood that the present invention finds application in any other type of liquid crystal display, among others, IPS liquid crystal displays.

Industrial Applicability

0063Liquid crystal displays according to the invention offer an improved gamma characteristic with less viewing angle dependence than ever, and do not produce unsmoothness or unnatural hues along a border even when an image with a straight border is displayed. This makes liquid crystal displays according to the invention suitable for use in, for example, television monitors with large screens.