JP2955617B2 - Reflective liquid crystal electro-optical device - Google Patents

Description

Description: TECHNICAL FIELD The present invention relates to a reflection type liquid crystal electro-optical device provided with a switching element array.

[Prior Art] A conventional reflection type liquid crystal electro-optical device provided with a switching element array is described in Nikkei Electronics No. 1981.2 / 16, p.
As described above, a transparent substrate is used for the counter electrode, and a substrate provided with a reflective electrode is used for the switching element array substrate.

[Problems to be Solved by the Invention] However, in the conventional reflective liquid crystal electro-optical device, it is necessary to use a pixel portion of a substrate on which a switching element array is disposed as a reflector, which increases the number of manufacturing steps and increases the number of transparent electrodes. Established process changes required. Further, there is a problem that the position of the switching element array must be aligned with the light shielding mask covering the periphery of the pixel on the counter substrate. Therefore, an object of the present invention is to provide a reflection-type electro-optical device that can use a conventional switching element array as it is and does not require alignment with a light-shielding mask.

[Means for Solving the Problems] According to the present invention, a liquid crystal layer is sandwiched between a pair of substrates,
In a reflective liquid crystal electro-optical device having a reflector at a pixel portion in the pair of substrates, a pixel electrode disposed in a matrix on one of the pair of substrates, and a switching element connected to the pixel electrode. Wherein the reflector has an insulating property and is formed on the inner surface of the one substrate on the liquid crystal layer side so as to overlap the pixel electrode.

The present invention is characterized in that the reflector comprises a dielectric multilayer film.

According to the present invention, a liquid crystal is sandwiched between a pair of substrates, and a pixel electrode arranged in a matrix on one of the pair of substrates and a switching element connected to the pixel electrode are formed. In the reflection type liquid crystal electro-optical device, an insulating reflector is formed on the inner surface of the one substrate on the liquid crystal layer side, and the one of the one substrate is parallel or perpendicular to the molecular axis of the incident surface of the liquid crystal layer. Means for allowing incident light of linearly polarized light to be incident, the light becomes substantially circularly polarized on the reflection surface after passing through the liquid crystal layer, and on the emission surface which has passed through the liquid crystal layer after reflection on the reflection surface, the incident light and The liquid crystal layer is characterized in that the liquid crystal layer is set so that the plane of polarization of the liquid crystal is rotated by about 90 degrees and becomes linearly polarized light.

EXAMPLES Example 1 FIG. 1 is a sectional view of a reflection type electro-optical device according to the present invention. Insulating reflector 1 on switching element array substrate 103
01 is provided, and has a basic structure in which a liquid crystal 104 is interposed between the liquid crystal 104 and the counter substrate 102. Here, a nematic liquid crystal (hereinafter referred to as TN) twisted in the liquid crystal layer was used. 105 is a pixel electrode, 106 is a polarizing plate, and 107 is a switching element. The other electrode 108 for applying an electric field is formed of a transparent electrode. Further, an anti-reflection coating is applied to the entrance / exit surface and the transparent electrode surface to suppress unnecessary light reflection.

Next, the reflection type liquid crystal display mode used in this embodiment will be described. Although a general field-effect birefringence display mode (hereinafter referred to as ECB) can be used, in this embodiment, an ECB mode using a twisted nematic liquid crystal is used.

In this embodiment, the switching element substrate is provided with the TF shown in Table 1.
T active matrix method, TN-E described above for the liquid crystal layer
CB mode is used. Detailed driving method and configuration are described in Nikkei Electronics No.351 (1981) p.211, SID'83 DIGEST
p.156 (1983), SID'85DIGEST p.278 (1985), Japa
n According to those described in Display'89 p.192. Table 1 Driving method TFT active matrix Number of pixels 480 × 440 Effective display area 96 × 88 mm Display mode TN-ECB (Field effect birefringence) Liquid crystal layer thickness 2.4 μm Δnd 0.2 Twist angle 63 ° Reflector Si-SiO ₂ dielectric film FIG. 2 shows a multi-layer mirror (on the switching element substrate) .
0 nm). First, the case where the voltage is zero will be described.
When the linearly polarized light 302 enters, the trajectory of the elliptically polarized light rotates as shown in FIG. At the reflector surface, the light becomes substantially circularly polarized light 301, and the phase is rotated by 180 degrees and reflected. The linearly polarized light 303 is transmitted through the liquid crystal layer again, and the plane of polarization is rotated by almost 90 degrees on the exit surface.
And emitted. Therefore, the light is blocked by the polarizing element, and the reflectance is reduced (OFF state). Next, a case where a voltage is applied will be described. The liquid crystal molecules rearrange in the direction of the electric field due to the anisotropy of the dielectric constant. As a result, the anisotropy of birefringence with respect to the incident light is eliminated, and the incident linearly polarized light is maintained, reflected, and emitted. Therefore, there is no decrease in reflectance (ON state).

Such a change in polarization occurs under limited conditions, and as a result of intensive studies on these conditions, the present invention has been achieved. The optical characteristics required of the liquid crystal layer are that, for linearly polarized light, it becomes circularly polarized after transmission, and that the phase is 180
The polarization plane is rotated by 90 degrees when transmitted through the liquid crystal layer.

4 (a) and 4 (b) are graphs showing Δnd and off-state reflectance. The twist angle of the liquid crystal layer was taken as a parameter, and the plane of polarization of the incident light was adjusted to the director of the liquid crystal molecules on the plane of incidence. The reflectance at the time of ON is determined by the transmittance of the polarizing element and is almost constant. According to this, about 60
It was found that the reflectivity was almost zero when the twist angle in degrees, Δnd = 0.2. Further examination revealed that a twist angle of 63 degrees was optimal. Looking at the trajectory of the elliptically polarized light at this time, as shown in FIG. 3, it becomes polarized light on the reflecting surface, and becomes linear polarized light rotated 90 degrees from the incident surface on the emitting surface. Compared to the case of a 1 / 4λ plate, since polarized light is incident along the director of the liquid crystal, birefringence is hardly perceived, and a large Δnd is required to receive the same phase change, Δnd Is characterized by a low periodicity with respect to. This allows the thickness of the liquid crystal layer to be set relatively large, and secures a margin in manufacturing.

The Δn effect works exactly the same when linearly polarized light is perpendicularly incident on the director of the liquid crystal. This is because Δn has no sign.

FIGS. 5 (a) and 5 (b) show the relationship between the Δnd and the reflectance by taking the arrangement angle of the polarizing element with respect to the director of the liquid crystal as a parameter. According to this, there is a condition that the reflectance is zero even when the direction of the polarizing element is +30 degrees. The locus of the elliptically polarized light in this case is circularly polarized on the reflection surface as in FIG.

You can find other such conditions by shaking the parameters. However, it is necessary to set the minimum Δnd in order to suppress the variation in the reflectance due to the wavelength. If the Δnd is extremely small, the liquid crystal thickness becomes too small. In the reflection type in which the optical length is doubled, the allowable liquid crystal thickness in the transmission type liquid crystal element poses a problem in manufacturing. Therefore, it is required that Δnd is as large as possible. This is to increase the margin for manufacturing the element. Looking at the above condition of Δnd = 0.2,
When Δn is a typical value of a small liquid crystal and Δn = 0.08, d is
2.5 μm. On the other hand, in the case of the type twisted by 45 degrees described in the conventional example, the optimum liquid crystal thickness is less than 2 μm, which is a factor of reducing the uniformity and the yield of the device.

In addition, since such a liquid crystal mode can be set to a non-transmissive state (black) when there is no electric field, a light-shielding mask in a portion where no pixel electrode is provided becomes unnecessary.

Example 2 FIG. 6 shows that a polarizing beam splitter (hereinafter, referred to as a polarizing beam splitter)
FIG. 3 is a configuration diagram of a reflection type liquid crystal electro-optical device using PBS (referred to as PBS).

601 is a PBS which linearly polarizes the light source light 603 and
02 incident. The configuration of the liquid crystal panel and the process up to emission are the same as in the first embodiment. The means to detect the emitted light is PB
In S, it is shifted by 90 degrees from that at the time of incidence. Therefore, the reflected output light 604
Becomes smaller when there is no electric field, and the characteristics of applied voltage and reflectance are
This is symmetrical with respect to FIG. 3 of the first embodiment and the vertical axis.

Embodiment 3 The present invention can be applied to an active matrix in which diodes and the like are arrayed here.

FIG. 7 is a sectional view of a MIM liquid crystal electro-optical device using a metal-insulator-metal element (hereinafter referred to as MIM) as a diode element. Basic structure is M with insulating reflector 701 installed
The liquid crystal 704 is sandwiched between the IM substrate 702 and the counter substrate 703. Reference numeral 705 denotes a transparent electrode on the opposite substrate for applying an electric field to the liquid crystal layer, and is a stripe electrode corresponding to the pixel size. In this embodiment, a mirror made of a dielectric multilayer film is used as the insulating reflector. The mirror made of the dielectric multilayer film can be set up or down the MIM element. It comprises a line-shaped signal transmission wiring 707 on a substrate 706, a MIM element 708 made of a thin insulator formed on a part thereof, and a pixel electrode 712 electrically connected thereto. The pixel electrode is M
The other metal thin film that constitutes the IM also serves as the reflective film of the electro-optical element. 710 is an anti-reflection coating, and 711 is a polarizing element.

Table 2 shows a more specific configuration. Table 2 Number of pixels 220 × 320 Pixel pitch 80 × 90 μm MIM substrate MIM element Ta−Ta ₂ O ₅ −Cr Ta ₂ O ₅ 500Å Oxidation method Wet anodic oxidation Signal transmission wiring Ta Pixel electrode Cr reflective film Reflector Dielectric multilayer film Display Mode TN-ECB (Field Effect Birefringence) Liquid Crystal Layer Thickness 2.4 μm Δnd 0.2 Twist Angle 63 ° Although the embodiments have been described above, the present invention is not limited to the above embodiments, but is widely applied to a reflection type light control device. Is possible.

[Effects of the Invention] As described above, according to the present invention, the following effects can be obtained.

(A) Since the reflector is formed on the inner surface of one of the substrates on the liquid crystal layer side, no parallax occurs due to the distance between the reflector and the liquid crystal layer. Therefore, double images and shadows can be prevented.

(B) Since the reflector is insulative, the reflector does not affect the switching element or the wiring connecting the switching element, so that crosstalk can be prevented.

[Brief description of the drawings]

FIG. 1 is a sectional view of a reflective electro-optical device according to the present invention. FIG. 2 is a characteristic diagram of the applied voltage and the reflectance (550 nm) of the apparatus of FIG. FIG. 3 is a diagram showing the trajectory of the elliptically polarized light in FIG. FIGS. 4A and 4B are graphs showing the relationship between Δnd and reflectance. FIGS. 5 (a) and 5 (b) show the relationship between the Δnd and the reflectance by taking the arrangement angle of the polarizing element with respect to the director as a parameter, and FIG. 6 shows the reflection type using PBS for the polarizing element. FIG. 2 is a configuration diagram of a liquid crystal electro-optical device. FIG. 7 is a sectional view of a reflective electro-optical device addressed by a MIM diode. 101: insulating reflector 102: opposing substrate 103: switching element array substrate 104: liquid crystal layer 301: circularly polarized light at the reflecting surface 601: PBS 701: insulating reflector 702: MIM substrate 703 …… Counter substrate 704 …… Liquid crystal 705 …… Counter electrode 706 …… Substrate 707 …… Signal transmission wiring 708 …… MIM element

Claims (3)

(57) [Claims] A liquid crystal layer sandwiched between a pair of substrates;
In a reflective liquid crystal electro-optical device having a reflector at a pixel portion in the pair of substrates, a pixel electrode disposed in a matrix on one of the pair of substrates, and a switching element connected to the pixel electrode. Wherein the reflector has insulating properties and is formed on the inner surface of the one substrate on the liquid crystal layer side so as to overlap the pixel electrode. 2. The reflection type liquid crystal electro-optical device according to claim 1, wherein said reflector comprises a dielectric multilayer film. 3. A liquid crystal is sandwiched between a pair of substrates, and a pixel electrode arranged in a matrix on one of the pair of substrates and a switching element connected to the pixel electrode are formed. In the reflection type liquid crystal electro-optical device, an insulating reflector is formed on the inner surface of the one substrate on the liquid crystal layer side, and the one of the one substrate is parallel or perpendicular to a molecular axis of an incident surface of the liquid crystal layer. Means for making incident light of linearly polarized light incident thereon, the light becomes substantially circularly polarized on the reflection surface after passing through the liquid crystal layer, and the incident light is transmitted through the liquid crystal layer after reflection on the reflection surface. A reflective liquid crystal electro-optical device, wherein the liquid crystal layer is set so that the polarization plane of the liquid crystal is rotated by approximately 90 degrees.