JPH0720429A - Optical device - Google Patents

Abstract

(57) [Summary] [Structure] A display device in which microlenses 76 and 74 for converging incident light into a predetermined size are provided at positions on the light incident side of the wobbling element 7 corresponding to the pixels 5 of the liquid crystal display element 2. [Effect] Pixel information can be accurately shifted to a predetermined position during wobbling. Therefore, in the case of a display device,
A plurality of field information is spatially separated, and the resolution can be sufficiently restored without the information of both fields overlapping, and a high resolution can be obtained. Further, in the image pickup apparatus, wobbling can be accurately performed on a target pixel, which also leads to improvement in resolution. Moreover, since it is not necessary to change the pixel spacing or the backlight for wobbling, it is possible to maintain the aperture ratio and increase the power consumption without increasing the power consumption.

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION The present invention relates to liquid crystal, plasma, EL
The present invention relates to an optical device including a display having discrete pixels such as (electroluminescence) or a wobbling element suitable for a solid-state image sensor represented by a CCD (charge coupled device) having discrete imaging pixels.

[0002]

2. Description of the Related Art When a line-sequential scanning pixel display is carried out by the NTSC system or the like for a display device having a discrete pixel array such as a liquid crystal, plasma, EL or the like in a mosaic pattern, a dot pattern, etc. The luminance signal, which should be a signal, is roughly sampled and the position information in the horizontal direction is lost. If the vertical pixel resolution cannot be implemented by the number of scanning lines, the positional resolution of the luminance signal or the like (that is,
Display resolution) was reduced.

For example, a TFT (T
In the hin-Film-Transistor) -TN (Twisted Nematic) liquid crystal viewfinder, in the NTSC system, one frame (that is, one picture displayed by the viewfinder) is an even scanning line as shown in FIG. By the first
It is formed by two fields consisting of a field and a second field by an odd number of scanning lines, and the frame frequency is 30 Hz (that is, the field frequency is 60 Hz) and one screen (one frame) is formed from the time resolution of the human naked eye. The time is set to 0.033 sec.

In the first field, the scanning line scans the screen every two lines, in the second field, the scanning line scans between the lines of the first field, and one screen is formed by combining with the second field. In this case, when the image receiving device has a sufficient resolution, the image formed as described above can be viewed without any discomfort.

However, when an image receiving device such as a liquid crystal display does not have a sufficient resolution as described above, when forming an image, for example, when the resolution of the liquid crystal display is only half the resolution of the image, the first field is displayed. In the second field, the scan lines scan exactly the same place. As a result, the image becomes as shown in FIG. 9A, and the resolution is reduced to half.

That is, since the current TFT viewfinder cannot mount 525 scanning lines of the NTSC system, the method of writing an odd field and an even field in the same pixel is adopted. Therefore, the vertical resolution is N
At present, it is lower than the principle of the TSC system.

Further, due to the large pixel size and the presence of joints of non-display pixel portions such as a black matrix, a mosaic-like screen having a discrete pixel array is conspicuous and the texture of the screen is deteriorated.

The above phenomenon similarly occurs in the image pickup by the CCD. That is, since the image pickup pixels forming the CCD are discrete, the image information of the subject is sampled at the constituent pixel pitch, which lowers the horizontal and vertical spatial resolution.

Therefore, by adopting a wobbling technique (spatial image information separation technique) and introducing picture element shifting elements (wobbling elements) to spatially shift the images of the odd field and the even field, the vertical resolution is improved. Have been proposed. This is also applied in the horizontal direction, and the horizontal resolution can be improved.

That is, as will be described later, for example, a wobbling element for changing the traveling direction of light is introduced on the light emitting side of a liquid crystal display to form first and second images.
When the field information is displayed on the screen, the light traveling direction is spatially changed. As a result, as shown in FIG. 9B, for example, the image of the second field is spatially displaced from the first field, the two fields are spatially separated, and the spatial field shown in FIG. It is possible to recover the information that was lost due to the overlapping condition.

Although the resolution can be improved in this way, as can be seen from FIG. 9B, the images of two spatially separated fields overlap each other in the shaded area in the figure. I will end up. With this, the resolution cannot be sufficiently restored. Such overlap between fields is caused by the pixel interval b (that is, the black matrix portion) being smaller than the pixel size a.

Therefore, in order to solve this overlap, it is conceivable that the pixel size and the pixel interval of the liquid crystal display are made equal and the amount of image shift between fields is set to the pixel size. However, this reduces the aperture ratio of the display and reduces the brightness of the display. In order to prevent this decrease in brightness, it is possible to increase the light amount of the illumination (backlight), but in this case, the power consumption is increased and at the same time, the heat absorption of the liquid crystal display is increased and the display characteristics deteriorate. Resulting in.

[0013]

SUMMARY OF THE INVENTION It is an object of the present invention to perform wobbling (picture element shifting) on a display composed of discrete pixels, a solid-state image pickup device composed of discrete light-receiving pixels, etc. without impairing its performance. It is an object of the present invention to provide an optical device capable of efficiently achieving a high resolution and improving a mosaic dot drawing screen or the like into a seamless continuous screen.

[0014]

That is, according to the present invention, the optical path of an optical element which is to be wobbling or made to have a high resolution (especially in the optical path between a display element and an observation position or between an object and an image pickup element). ) Is an optical device comprising a wobbling element arranged to shift the optical axis of the emitted light in a predetermined direction, and the incident light is provided at a position on the light incident side of the wobbling element corresponding to a pixel of the optical element. The present invention relates to an optical device provided with a light condensing unit (especially a microlens) for condensing light into a predetermined size.

In the present invention, the above-mentioned "optical device" means not only a wobbling element but also an optical system (for example, a display device or an image pickup device) incorporating this wobbling element.

[0016]

EXAMPLES Examples of the present invention will be described below.

1 to 3 schematically show an example of an optical device including a wobbling element according to the present invention.

In this example, the present invention is applied to a liquid crystal optical display device 1, in which a liquid crystal display element (LCD) 2 sequentially arranged in the same optical path along the traveling direction of light and a phase modulation optical device. A wobbling liquid crystal element (liquid crystal display) 3 as an element and a birefringent medium 4 made of a transparent substrate such as a crystal plate are combined.

The pixels 5 of the LCD 2 are composed of a discrete pixel array such as a mosaic pattern as a whole, and are made of ITO.
A transparent electrode such as (Indium tin oxide obtained by doping indium with tin) is formed on a transparent substrate 70 by applying a predetermined pattern such as a stripe shape. Pixel 5
A black matrix portion 73 of Cr or the like is provided between −5. Then, on the facing surface of the facing transparent substrate 71, ITO is formed.
Electrodes 72, etc. intersect the electrodes 5 and are applied in a predetermined pattern such as stripes.

Further, TN (twisted nematic), STN (super twisted nematic) and SH are provided between the opposing substrates.
(Super homeotropic), and further liquid crystal 83 made of FLC (ferroelectric liquid crystal) or the like is injected. This LC
Although not shown, D2 has a polarizing plate on the panel itself as is well known, and the output light has linearly polarized light.

The LCD 2 has a higher resolution by wobbling, but in this example, a hemispherical microlens 74 of the same size as the pixel is located at the position of each pixel 5 on the surface of the substrate 70 on the light emitting side. Is fixed. The microlens 74 has a function of narrowing light emitted from the pixel 5 of the liquid crystal display to each pixel.
In FIG. 2, the microlens 74 is indicated by diagonal lines.

Behind the LDC 2 is the above microlens.
The wobbling element 7 including 74 is arranged with the optical axis in common.

The wobbling element 7 is composed of a liquid crystal element having the same size as the LCD 2, and as shown in FIGS. 6 and 7, transparent electrodes (eg, transparent electrodes) on transparent glass substrates 20 and 21 are used.
100Ω / □ ITO) 13, 14 are provided, and further on that,
A polyimide film (not shown) is formed as a liquid crystal alignment film.

For example, 220 electrodes 13 are formed in stripes with the same width and at the same intervals corresponding to the above-mentioned pixels 5 (that is, the number of scanning lines), and a black stripe portion of Cr is provided between the electrodes 13 and 13. 75 (non-display part) is provided. The other electrode 14 may be deposited on the entire surface of the substrate 21.

The space between the two substrates 20-21 is sealed by a sealing material 25 in the peripheral portion, and the liquid crystal 15 is injected into the gap between them. Ferroelectric liquid crystal is preferable as the liquid crystal 15, which includes Chisso Co., Merck Co., BDH,
Alternatively, for example, a composition comprising a ferroelectric liquid crystal compound or a non-chiral liquid crystal described below is also possible, but there is no limitation thereto, and there is no need for limitation of the phase series thereof. Is to take.

The liquid crystal layer structure of the chiral smectic liquid crystal element used here has an X-ray structure having a bookshelf structure in antiparallel, a chevron structure in parallel or a pseudo bookshelf structure in parallel, depending on the combination of the alignment treatment directions. Clarified by analysis.

Then, on the surface of the substrate 20 on the light incident side, a semi-cylindrical microlens having the same width and the same interval as the transparent electrode 13 is formed.
For example, 220 stripes 76 are fixed. The microlens 76 is arranged so as to face the above-mentioned microlens 74 on the display side in common with the optical axis in common, and constitutes a condensing element 77 that condenses the light emitted from the display 2. In FIG. 3, the microlens 76 is indicated by diagonal lines.

Here, as clearly shown in FIG. 4, the width of the electrode 13 is w, the interval between the electrodes is l, the size of the pixel 5 is a,
When the distance between pixels is b (however, a> b), w = l = (a + b) / 2 (1) is satisfied, and this condition is presupposed. Between the focal length f _D of the lens 76 and the focal length f _W of the microlens 74, both micros are used so that the relationship of f _D / f _W = (a + b) / 2a (2) holds. Focus the lenses so that they are formed at a common location.

According to these conditional expressions, the display 2
The incident angle 6 from each pixel can be reliably focused on the microlens 76 via the microlens 74.
The parallel light having the same width or the same size as the transparent electrode 13 can be incident on the liquid crystal element 3 of FIG. Therefore, the width or size of the luminous flux of the incident light is the same as the width or size of the black stripe portion 75 (that is, the non-display portion).

As a result, the polarized light 6 emitted from the liquid crystal display 2 always enters the liquid crystal element 3 with the same width and the same pitch (w = 1), and the liquid crystal element 3 selectively causes the phase shift as described later. Is changed to change the polarization direction for each field. And further, this liquid crystal element 3
The birefringent medium 4 having a sufficient thickness, which is arranged at the rear of the optical axis, spatially changes the traveling direction of the light 11 incident from the liquid crystal element 3 by utilizing the birefringence.

In FIG. 1, the output light 12 is generated by such birefringence.
The state where the optical axis of the is shifted is shown by a broken line. The birefringent light 12 is obtained by a light flux corresponding to the non-display portion 75 adjacent to the transparent electrode 13 after being shifted by the length L from the solid line state not receiving the birefringence along the extraordinary optical axis forming the angle β. .

For example, when the birefringent medium 4 is quartz,
It is assumed that the optical axis of the crystal lies within the plane formed by the normal line of the cut surface of the crystal and the normal line of the scanning line. In the first field, if the polarization direction of light is perpendicular to the plane including the optical axis, the light vibrates without changing the vibration direction, but if it is perpendicular to this, the traveling direction of light is L.
Only (ie, w), shift upwards. Therefore, in the image after wobbling, the pixel size and the pixel interval are equal (Equation (1) above).

In this way, for example, in the first field, the polarization direction of the light is made perpendicular to the optical axis plane, and the image of the first field is formed in the direction in which the light goes straight. On the other hand, in the second field, the polarization direction of light is the optical axis plane,
The image of the second field is formed at a position separated by L above. As a result, as shown in FIG. 9C, the information in the two fields is spatially separated, and the information in the two fields does not overlap, so that the resolution can be sufficiently restored and a high resolution can be obtained. .

In this case, since the pixel interval of the liquid crystal display 2 is not changed and the backlight is not required to be changed, the aperture ratio of the display (that is, the brightness of the display) is maintained and the power consumption is increased. Without that, the display performance can be improved.

A microlens formed on the above-mentioned wobbling liquid crystal element 3 and liquid crystal display 2.
76 and 74 can be created by the following method, for example.

Microlens 74 on the liquid crystal display 2
Is spin-coated with an acrylic resin on the substrate 70 to a thickness of about several μm. Next, the coating film is cut into the same size as the pixel 5, and the substrate 70 is further heated, and the surface tension of the polymer is used to spontaneously shrink the resin to form the microlens 74 covering the surface of the pixel 5. .

The microlenses 76 on the liquid crystal element 3 are formed by the same method. However, here, the coated polymer film is cut in a stripe shape in the direction of the electrode 13. The cutting position is the central portion of the two transparent electrodes.

On the other hand, regarding the arrangement of the liquid crystal display 2 and the liquid crystal element 3, the wobbling element 7 is installed behind the liquid crystal display 2 so that the direct incident light coming from the liquid crystal display 2 can be completely transmitted through the wobbling element, and all the pixels are displayed. Is a positional relationship capable of wobbling. The distance between the liquid crystal display 2 and the liquid crystal wobbling element 7 is determined by the above equation (2).

Next, the above-mentioned microlens and its design will be described in more detail. In order to make the image after wobbling completely separable, the image size after wobbling should have the same pixel size and pixel interval, and (a +
b) / 2 must be set (equation (1) above). As a result, the microlens 74 attached to the surface of the display 2 to be wobbled and the liquid crystal element 3 to be wobbled
It can be seen from the geometrical optics that the focal length of the microlens 76 attached to the surface of is required to satisfy the relationship of the above equation (2).

The design of the microlens is carried out by designing the polymeric material and its curvature. Fabrication of the microlens is as follows.

1. The polymer film is coated on the place where it is formed, divided by lithography on the pixel, and by heating it, the film contracts due to the surface tension of the polymer, forming a hemispherical or semi-cylindrical microlens. To be done. 2. Microlens radius design. As shown in FIG. 5, assuming that the radius of the lens is R, the refractive index is n ₂ , the distance from the lens to the focal point is l, and the height of the light beam from the optical axis is d, the following relationships are found.

[0042]

Considering the Gaussian approximation, sin θ ₁ = θ, c
os θ ₁ = 1 and tan (θ ₂ −θ ₁ ) = θ ₂ −θ ₁ , and the equation (3) becomes the following equation (4).

[0044]

FIG. 10 shows the microlens 7 of the above example.
An example in which 4, 76 are built in the glass substrate 80 is shown. Other configurations are the same as those in FIG.

In the case of this example, the microlenses described above can be manufactured and designed separately from the liquid crystal elements 2 and 3. This can be easily realized by a method described later if the position and size of the microlens to be built in the glass plate 80 are determined in advance.

Among the above liquid crystal elements, a liquid crystal used for the wobbling element 3 may be a mixture of the following FLC or non-chiral compound.

[0048]

[Chemical 1]

[0049]

[Chemical 2]

[0050]

[Chemical 3]

[0051]

[Chemical 4]

[0052]

[Chemical 5]

Further, other than the chiral smectic liquid crystal, if the switching speed is high, for example, the following antiferroelectric liquid crystal (AFLC) and smectic A phase exhibiting the electroclinic effect can be applied.

<Anti-ferroelectric liquid crystal> The anti-ferroelectric liquid crystal is C
It was discovered by handani et al. in 1988 and is characterized by the following three points. (1) Utilizes switching between an antiferroelectric state and two stable states of three stable states. (2) A clear threshold value characteristic is exhibited, and a high contrast when driven by multiplex can be obtained. (3) Use positive and negative hysteresis alternately,
Since the occurrence of internal polarization is suppressed, the image sticking phenomenon is unlikely to occur.

The characteristics of this antiferroelectric liquid crystal material are:
Unlike ferroelectric liquid crystals, chiral liquid crystals are the majority of the composition (spontaneous polarization is large, almost 10 times that of ferroelectric liquid crystals), and the substituent for the asymmetric carbon is CH.
₃ group, CF ₃ group, compounds having C ₂ H ₅ group is readily indicates the antiferroelectric, the core structure is expanded. For example, there is CS-4000 manufactured by Chisso Corporation.

<Smectic liquid crystal exhibiting electroclinic effect> The electroclinic effect is a phenomenon in which the tilt angle of the orientation vector is induced by the electric field in the smectic A phase composed of chiral molecules when the temperature is constant. . In the smectic A phase, the orientation vector points in the normal direction of the smectic layer and rotates freely around the major axis. However, application of an electric field along the layer inhibits the free rotation, and the polarization P in the electric field direction is Induced.

Assuming that the linear combination of the polarization P and the inclination angle θ is P = kθ, P = (ε⊥ ^* −ε⊥0) ε _O Ε Therefore, θ = (ε⊥ ^* −ε⊥0) ε _O A tilt angle proportional to the applied electric field E occurs, such as Ε / k. Here, ε⊥ ^* and ε⊥0 are the permittivity of the racemate of the optically active substance, and ε _O is the permittivity of vacuum. From this, the larger the difference in the dielectric constants of the racemic chiral liquid crystals, the greater the electroclinic effect.

Next, a specific example of the above wobbling will be described. Example 1 It was confirmed that the resolution was improved by the conventional wobbling method. The display used was a Sony 0.7-inch, 100,000-pixel viewfinder. The vertical resolution of the display was 214.

A liquid crystal element for wobbling was prepared as follows. The glass substrate has a thickness of 1000Å, 100Ω / cm ²
A 0.7 mm thick glass substrate with a transparent electrode (ITO) was used. The size of the upper and lower glass substrates is 13.6, respectively.
mm × 14.2 mm and lower substrate 17.2 mm × 11.6 mm.

The upper substrate is coated with ITO on the entire surface, while the lower substrate has an I width of 24 μm and an interval of 24 μm.
It was a glass plate with TO. ITO on each substrate
A 500Å thick polyimide film was applied to the surface by spin coating. 240 ℃ after coating polyimide film
It was baked for 1 hour. The liquid crystal alignment treatment of this polyimide film was performed by rubbing the surface of the film with a rayon cloth (rubbing treatment).

Next, the two glass substrates were adhered to each other with an epoxy resin so that the rubbing directions were parallel to each other. The spacing between the glass substrates was controlled by 2.0 μm glass beads mixed with epoxy resin. A gap between the two glass substrates was formed for injecting liquid crystal.

The liquid crystal was injected through a gap formed in one corner of the epoxy resin sealing material. The liquid crystal was injected by heating the liquid crystal in a boat to an isotropic phase, and then removing the gas dissolved in the liquid crystal by vacuum deaeration. After this degassing is complete,
The injection port opened in the cell was submerged in the liquid crystal, and the vacuum was released. The liquid crystal was injected into the cell by atmospheric pressure. After that, the cell was gradually cooled to room temperature. The injected liquid crystal was CS-1014 manufactured by Chisso Corporation.

The microlenses on the surface of the wobbling element were formed by spin-coating an acrylic resin on the surface of the wobbling element before coating with the polyimide, dividing into a predetermined size by lithography, and then heating at 150 ° C.

The wobbling element thus obtained was placed behind a 0.7-inch liquid crystal display, precisely aligned, and then an attempt was made to display the projection type display. In this case, the wobbling effect was confirmed in FIG. 1 with and without the microlenses on the surface of the wobbling element.

As a result, the vertical resolution was improved to 350 without the microlens, but when the microlens was provided according to the present invention, the vertical resolution was doubled.
Improved to 40.

Example 2 A wobbling element as shown in FIG. 10 was produced. In the production of the liquid crystal element for the wobbling element, the two substrates had ITO of 100 Ω / cm ² . One substrate was provided with ITO on the entire surface, and the other substrate was etched so that the ITO electrode width and the distance between the electrodes were both 24 μm.

The glass substrate of the light converging element was manufactured as follows. A resist was coated on the front side of a glass substrate having a thickness of 5 mm by spin coating, and 48 μm holes were formed in the resist by lithography at predetermined intervals, and then the glass substrate was etched through the holes. By controlling the etching time, a circular recess having a diameter of 40 μm was formed on the substrate surface. Polycarbonate resin was poured into the depressions to form microlenses on the substrate. In the same way, on the other side of the glass substrate,
I built a m micro lens.

The glass substrate with a microlens produced in this manner was fixed so as to be in close contact between the liquid crystal viewfinder and the wobbling liquid crystal element as in Example 1.

As a result of evaluating the wobbling effect, it was confirmed that the vertical resolution of 214 lines was improved to 400 lines.

Next, the mechanism of the above wobbling operation will be described with reference to FIGS. It should be noted that, in the following figures, the above-mentioned light converging means (microlens) is not shown for simplification. Further, for ease of understanding, each constituent element is shown for each section corresponding to one constituent display pixel 5 of the liquid crystal display element LCD.

First, as shown in FIG. 11, the ferroelectric liquid crystal element 3
When the switch state of 1 is the state 1, since the polarization plane 9 of the light 6 emitted from the display element 2 side and the extraordinary optical axis 8 of the ferroelectric liquid crystal element 3 are parallel, the transmitted light 11 maintains the polarization plane. The crystal plate 4 having birefringence is irradiated. Since the crystal plate 4 includes the extraordinary optical axis 10 of the crystal in the plane of incident polarization, the light polarized in the Y-axis direction is refracted in the direction in which the extraordinary optical axis 10 of the crystal plate 4 is tilted, and the air layer is again formed. When it goes out to 12, it becomes parallel to the optical axis, and a deviation from the optical axis of the incident light occurs in the Y direction.

On the other hand, as shown in FIG. 12, the ferroelectric liquid crystal element 3
When the switch state of is the state 2, the polarization plane 9 and the extraordinary optical axis 8
Since the light has an angle of about 45 degrees, the transmitted light 11 rotates in the direction of the extraordinary optical axis and becomes linearly polarized light (Y-axis direction) → elliptically polarized light → circularly polarized light → elliptically polarized light → linearly polarized light (X-axis direction). The polarization plane is changed by 90 degrees from the initial state by changing the inside of the ferroelectric liquid crystal element 3, and the crystal plate 4 is irradiated with the polarized plane. In the crystal plate 4, since the extraordinary optical axis 10 of the crystal is not included in the plane of incident polarization, the light 11 is not refracted but maintains the optical axis as it is, and again exits to the air layer as outgoing light 12.

As described above, it is possible to shift the optical axis depending on whether the FLC 3 is switched, that is, in the presence or absence of refraction by the crystal plate 4 in the states 1 and 2, and use the shift of the optical axis as a principle of pixel shifting operation. it can.

Here, the cone angle of the liquid crystal that determines the switch state in the FLC 3 will be described. In the ferroelectric liquid crystal (the same applies to the anti-ferroelectric liquid crystal), the switching behavior of the liquid crystal director due to the application of the electric field is that liquid crystal molecules follow the South-Goldstone mode described in P150 of "Liquid Crystal Dictionary" (published by Baifukan). Move on a virtual cone. Furthermore, smectic A having an electroclinic effect
The liquid crystal (P145 of the same liquid crystal dictionary) has a cone angle unique to each liquid crystal composition similar to the cone angle even when the soft mode described in P119 of the same liquid crystal dictionary is used.

That is, consider a cone model of the liquid crystal 15 sandwiched between the transparent electrodes 13-14 made of ITO (Indium tin oxide in which tin is doped into indium) as shown in FIG. The opening angle of the cone is called the cone angle θr, and the projection of this cone angle on the glass substrate with the transparent electrode is called the apparent cone angle θ. Optically, the apparent cone angle θ may be considered.

Next, FIG. 14 shows a switch state of a concrete combination example of the respective elements constituting the liquid crystal optical device.
The liquid crystal display element 2 to be combined here may be of any type, such as an active matrix TN liquid crystal, an STN liquid crystal display element, a ferroelectric liquid crystal display element, an antiferroelectric liquid crystal display element, or an SH display element. Here, as an example,
An example of combination with a TN liquid crystal will be shown.

In the normally white TN liquid crystal display element shown in FIG. 15, light from the light source is transmitted without applying an electric field to the TN liquid crystal. Here, a combination of the backlight 17-polarizing plate 18-TN liquid crystal 2-polarizing plate 19 or reflection plate-polarizing plate 18-TN liquid crystal 2-polarizing plate 19 is used.
Shows the same TN liquid crystal display element as the conventional one.
Needless to say, the TN liquid crystal element 2 and the ferroelectric liquid crystal element 3 are provided with transparent electrodes on both sides thereof.

In this case, as the electric field strength increases, T
The twist of the N liquid crystal 2 is released, and light is gradually leaked through the polarizing plate to realize gradation display, but any transmitted light is polarized by the polarizing plate 19 in front of the ferroelectric liquid crystal element 3 and has the same linear polarization. Therefore, the pixel shifting can be performed according to the above-described operation principle.

In the normally black TN liquid crystal display element shown in FIG. 16, light is transmitted in a state where an electric field is applied to the TN liquid crystal, and the twist of the TN liquid crystal 2 gradually increases as the electric field strength decreases. It returns, it gets darker gradually,
Although gradation display is realized, since any transmitted light becomes the same linearly polarized light by the polarizing plate 19 in front of the ferroelectric liquid crystal element 3, the pixel shifting can be performed according to the above-described operation principle.

As described above, it is clear that the present invention can be applied to any type of liquid crystal display element as long as the light emitted from the display element is substantially linearly polarized light.

Although the above-mentioned example relates to a display element having polarized light, the present invention can of course be applied to a non-polarized display element.

As shown in FIG. 17, when the polarization degree of the light from the display pixel 5 is small, a polarizing plate 19 may be inserted in the optical path connecting the display element 2 and the pixel shifting element 7 in order to make the light polarized. good. The optical arrangement conditions are the same as in the case of the liquid crystal display element described above.

The non-polarizing display 2 that can be used here is a self-luminous display element such as a plasma display or an LED display.

As described above, based on the present invention, a phase modulation element such as a chiral smectic liquid crystal that can be driven at a video rate (ferroelectric liquid crystal, antiferroelectric liquid crystal, or smectic A liquid crystal having a large electroclinic effect). ) 3 is used to arrange the wobbling element 7 in the optical path connecting the display such as liquid crystal, plasma, LED, etc., which is composed of discrete pixels, and the retina of the observer, and wobbling (pixel shifting).
The following [1] can be used as the phase modulation element 3 and the following [2] can be used as the birefringent medium.

[1] At least two states exist in the switch state of the ferroelectric liquid crystal, antiferroelectric liquid crystal or smectic A liquid crystal having the electroclinic effect, which can be driven at the video rate, and at least two of them exist. A chiral smectic liquid crystal device with an extraordinary optical axis forming an angle of 26 to 64 degrees, which is optically arranged so that the plane of polarization can be rotated.

[2] A transparent substrate which shifts the optical axis depending on the polarization direction of the incident light, and is specifically arranged so as to have an equivalent uniaxial extraordinary optical axis component in the wobbling direction. element.

As a driving method for these ferroelectric liquid crystal elements, a conventional general FLC driving method can be applied. Figure 1
An example of drive waveforms of a frame and two fields is shown.

FIG. 18A shows a pulse drive with a reset pulse, which is a method of maintaining a neutral electrical condition in the field by adding a reset pulse immediately before writing, and a direct current component for a long time is generated in the liquid crystal. Hard to be applied. A in addition to FLC
It can also be used for FLC.

FIG. 18B shows pulse driving without a reset pulse, which is a method of maintaining an electrically neutral condition within one frame. It can be used for AFLC as well as FLC.

FIG. 18C shows a method of maintaining an electrical neutral condition in one frame in the case of square wave driving, in which the DC voltage is applied for a longer time than in pulse driving, but the element isolation If it is highly reliable, it is a highly reliable driving method. FL
In addition to C, it can be used for AFLC and electroclinic smectic A.

Fast response of FLC: Rising (10-90% T) as switching characteristic by the above driving waveform
Both, and the fall (90-10% T), show a high-speed response on the order of μsec, guaranteeing a sufficient response within one field and achieving an effective pixel shifting effect at the video rate. .

In particular, in wobbling (picture element shifting),
It is preferable that the response time of rising and falling is 1/3 or less of the field time, and the ratio of rising time and falling time does not exceed twice each other.

In this respect, when a nematic liquid crystal is used,
Even at high speeds, the rise time when an electric field is applied is relatively short, but the fall time when off is long, so switching in the field is not sufficient, and effective pixel shifting effects may not be obtained. . The twisted nematic pixel shift element has a minimum rise / fall time of about 15 msec (room temperature) when the transmittance change is 0 to 90%, and the NTSC 2: 1 line interlace scanning method (1/60 per field). Second (16.7 ms)), it is quite difficult to realize, and if the 4: 1 line interlace scanning method is applied with the same number of frames, 1/120 second (8.3 ms) per field
And, it becomes impossible to follow at all.

On the other hand, the pixel shifting method using the ferroelectric liquid crystal element is effective because its switching time is shorter than that of the TN liquid crystal. By the way, the rise and fall times of the ferroelectric liquid crystal element are in the order of μsec, and even the slowest one is several ms or less.

Table 1 below shows the response times of various liquid crystals for comparison, and the response speed of the liquid crystals usable in the present invention is extremely fast.

For example, the deviation L of the optical axis of the quartz plate is calculated by the following formula. As shown in FIG. 19, the birefringent transparent medium 4
The angle formed by the extraordinary optical axis 10 of
And the thickness of the crystal plate 4 is d. Here, the refractive index n _o of ordinary light and the refractive index n _e of extraordinary light of the quartz plate 4 are n _e = 1.55
336, n _o = 1.54425. Here, 0.7 inches,
L = 24.5 μm in order to increase the vertical resolution of an active matrix TN liquid crystal display with 1030,000 pixels
As values giving the deviation of β = 45 degrees, d = 4.17 mm.

[0097]

[Equation 1]

Here, the range of β effective for expressing the deviation L of the optical axis was 10 to 80 degrees. The deviation of the optical axis depends on the constituent pixel pitch.

If pixel shifting is performed in the vertical direction as in this example, the resolution is increased in the vertical direction as shown in FIG. Similarly, if the pixel shift is performed in the horizontal direction, the resolution in the horizontal direction is increased (FIG. 21). Further, if the pixel shifting is performed in the diagonal direction, the resolution is increased in the vertical and horizontal directions (FIG. 22).

In the case of a color liquid crystal display element having a color filter: In a normal color display element, one pixel is composed of trio of R, G and B color filters. R,
The G and B arrangement methods include an in-line arrangement (FIG. 23) and a delta arrangement (FIG. 24).

The pixel shift direction of such a pixel shift element can improve the resolution in the shifted direction by the two-dimensional pixel shift including not only the vertical direction but also the horizontal direction or the diagonal direction. Furthermore, the pixel shift range is
By setting the constituent pixel aperture L _A for the length component in the pixel shift direction to that of an RGB pixel trio and setting the length of the black matrix portion to L _B , the same conditions as those of the above-mentioned monochromatic display element are obtained. You can

Range of the number of divisions of the drive electrodes in the pixel shifting operation: The elements to be high resolution as described above are
In principle, a pixel shift synchronized with each switching per pixel is required. In this case, in the case of dot-sequential scanning, picture element shifting elements corresponding to the number of pixels like a TFT (Thin Film Transistor) matrix are required. Further, in the case of line-sequential scanning, it is necessary to divide the electrodes by the number of horizontal scanning lines.

Therefore, when the number of horizontal scanning lines of the display element whose resolution is to be increased is N, it is ideal to divide the transparent electrode into 1 / N in the vertical direction during line-sequential scanning. But,
In order to increase the resolution, it is necessary to use picture element shifting elements that are equivalent in cost. Therefore, the present inventor considered that the upper limit of electrode division can be lowered by a human factor to reduce the cost, and conducted the following experiment.

In combination with the above TFT color liquid crystal display element, the timing of switching the ferroelectric liquid crystal element was synchronized with the vertical synchronizing signal, and the FLC element on the entire surface of the panel was switched without considering the time series data. Even if it went, about 1/4 of the vertical direction of the panel was increased in resolution from 214 TV lines to over 400 TV lines.

From the experiment here, it was found that increasing the resolution is effective even in the vertical division up to about 1/4.
That is, in order to increase the resolution, the pixel shift element to be combined with the display element having the horizontal scanning line number N is divided into N in the vertical direction.
One division is sufficient, but N divisions to 3 divisions are preferable in order to increase the resolution of the entire panel. Furthermore, considering the electrode processing accuracy and cost, N / 2 or (N + 1)
It is preferably less than or equal to any integer division of / 2.

Specific example of high resolution of FLC picture element shifting element with 5-divided electrode configuration: FIG. 25 shows an example of combination of divided electrodes. This divided electrode is a transparent electrode (I
(TO) 13 and 14 were formed, and the electrode was etched so as to be divided into five parts. Distance between ITO electrodes (etching part) 10μ
m. It is necessary that the distance between the electrodes be larger than the cell gap (and shorter than the non-display portion) in order to prevent dielectric breakdown due to the potential difference between the electrodes, that is, withstand voltage.
Here, the cell gap is set to 1 μm to 3.0 μm. It is easily understood that the combination of the divided electrodes may be such that one side is the common electrode and both sides are the divided electrodes.

Further, a SiO alignment film is used as the alignment film, and the cell assembling method and the liquid crystal injecting method are the same as in the case of the unipolar cell. The liquid crystal alignment direction was set in consideration of the pixel shift direction.

Regarding the synchronization signal of the picture element shifting element: Interlace scanning moving image (for example, 24 frames per second for movies, 25 frames per second for television)
I'm sending one or thirty images. However, at 24 to 30 sheets per second, the flicker interference is great, and it can not be used at all.
For this reason, one frame is radiated twice each in a movie and 48 frames are repeated every second, and in television, the number of repetitions per second is increased by using the interlaced scanning method without increasing the transmission bandwidth. The Japanese domestic standard uses the 2: 1 line interlaced scanning method.

That is, as shown in FIG. 26, the scanning started from the point a reaches the point b in the horizontal scanning of N / 2 times, moves to the point c in the vertical retrace line period, and further the horizontal scanning is performed N / 2 times. The scanning reaches point d, and returns to point a again during the vertical baseline period. The period from d to b is called the first (odd) field, and the period from b to d is called the second (even) field. In the 2: 1 line interlace scanning system, one field (one frame) can be completed in two fields. In addition, there are 3: 1 and 5: 1 line interlace scanning systems.

When the line-sequential scanning screen display of the NTSC system or the like is used, the current CRT has an analog type, so there is little problem in its resolution, but liquid crystal, plasma, EL
For a display with discrete pixels, such as, for example, a considerable amount of horizontal position information is lost due to the discrete pixel array, scanning line information is lost, or the position resolution of the luminance signal is reduced ( That is, the resolution of the display is lowered) as described above.

Here, a specific method for setting the timing of the picture element shifting (wobbling) will be described. TV signal, Figure 27
As shown in, each field is composed of a luminance signal, a vertical synchronizing pulse, a horizontal synchronizing pulse, a color signal, and a color synchronizing pulse. Here, the vertical sync pulse of the odd field (first field) and the even field (second field) is detected, a sync signal is sent from this to the FLC driver, and then a delay is given to each channel in the driver. The drive waveform may be sent to the FLC cell.

Regarding the synchronization of the divided FLC element, the FLC drive circuit, and the video signal processing system: FIG. 28 shows the configuration of the electrodes, the connection of the drive circuit and the video signal processing system, and the synchronization method. That is, by the video signal processing device 40,
The respective sync pulses of the odd field (first field) and the even field (second field) and the RGB signal are supplied to the display element 2, and at the same time, the vertical sync pulse of each field is detected and the sync signal is sent to the FLC driver 41. Then, the drive waveform delayed in each channel in the driver 41 is sent to the FLC cell 3.

As shown in FIG. 29, the entire ITO side was used as a common electrode, the five-divided electrode side was divided into Ch1 to Ch5, and pulse driving was performed as shown. That is, the time of one field is divided into five with the detected vertical synchronizing signal as a reference, and each channel is sequentially delayed. Therefore, T
It is important that the driving of the N liquid crystal display element 2 and the driving of the FLC element 3 are synchronized. In addition, these drive waveforms are
A general FLC driving method and rectangular wave driving can be applied.

Further, a concrete method of changing the direction of shifting the picture elements will be described. A case of increasing the resolution in the vertical direction of the display element 2 (FIG. 30) and a method of increasing the resolution in the vertical and horizontal directions (FIG. 31) are shown. As a result, it was confirmed that the resolution was increased in each intended direction.

In the above 5-division FLC element, a high resolution was examined in consideration of drive conditions, optical arrangement, and pixel shift amount. As a result, a panel in a 0.7 inch, 103,000 pixel active matrix TN liquid crystal display was obtained. The resolution was increased from 214 TV lines to 400 TV lines or more over the entire surface, and the black matrix, which is a non-display area, became inconspicuous and a high-resolution and smooth screen was achieved.

These high resolution techniques can be used in any form such as direct-view type, reflective type, and projection type. this house,
32 to 33 show two examples of projection displays.

In the example of FIG. 32, the light from the halogen lamp 17 is guided to the display element 2 as a backlight through the cold filter 43, and the lens system is subjected to the above wobbling process.
An image is projected from 44 to screen 45.

FIG. 33 shows a mirror type display, which is a light source.
The light from 17 is passed through the filter 46, separated into predetermined wavelength lights (R, G, B) by the respective dichroic mirrors 47, made incident on the respective wobbling elements from the condenser lens 48, wobbled there, and then again. The combined image is projected on the screen 45.

The above-mentioned high resolution technique is applied in a visible light wavelength range for application as a display.

The present invention is not limited to the display element 2 described above,
It is also applied to the case where the above-mentioned wobbling element 7 is arranged in the optical path that connects the image pickup device such as CCD including discrete pixels and the object.

The image pickup apparatus 101 shown in FIGS. 34 to 36 according to the present invention.
Also in the case of applying to, the various conditions, principles, and explanations described in the above-mentioned display device are preferably adopted in the same manner. In the following, the contents similar to those of the above-described display device will not be particularly described repeatedly, but in comparison therewith, the description will be mainly given to those specific to the imaging device. Further, the light converging element 77 is not shown in the drawings after FIG. 35 for simplification.

When an image pickup device such as a CCD is used, for example, in order to increase the resolution of the 1/3 inch CCD in the horizontal direction, the vertical direction, or the horizontal and vertical directions simultaneously, β = 45
The amount of pixel shifting was adjusted by adjusting the thickness d of the crystal plate as a degree.

For example, in order to give a deviation of L = 3.7 μm, β = 45 degrees and d = 0.63 mm. Here, the range of β effective for expressing the deviation L of the optical axis was 10 to 80 degrees.

When the image pickup device is used, the subject and the image pickup device
In the optical path connecting 53, subject-polarizer-condenser-FLC
The elements are arranged in the order of birefringent substrate-imaging element. In this case, the lens system, the iris, and the wavelength limiting filter may be arranged anywhere in the optical path connecting the subject and the image sensor.

The incident light on the liquid crystal element 3 of the wobbling element 7 is constituted so as to be condensed as a luminous flux of width a by the combination of the microlenses 76 and 74 provided on the opposing transparent substrates 20 and 90, respectively. ing. In this case, the transparent electrode 13 of the liquid crystal element 3 is not divided unlike the case of the above-mentioned display device.

The microlenses 76 and 74 may be provided in a stripe shape with a width a and an interval a facing each other at substantially the same size and size corresponding to the pixel 91 of the CCD 53. Therefore, the incident light is not scattered by the condensing element 77 including the microlens, and the width a and the interval a
Incident on the liquid crystal element 3 while accurately holding
As shown by, the light component from the subject can be accurately wobbled on the pixel 91.

In this image pickup apparatus 101, as shown in FIG. 35, when the switching state of the ferroelectric liquid crystal element 3 is the state 1, the irradiation light component a from the subject 50 side passes through the lens 51 and the diaphragm 52. After that, it is polarized in the pixel shifting direction by the polarizing plate 19. Polarization plane of light and extraordinary optical axis 8 of ferroelectric liquid crystal element 3
Are parallel to each other, the transmitted light is applied to the crystal plate 4 having birefringence while maintaining the polarization plane. Since the crystal plate 4 includes the extraordinary optical axis of the crystal in the incident polarization plane, the light polarized in the Y-axis direction is refracted in the direction in which the extraordinary optical axis of the crystal plate is inclined,
When it goes out to the air layer again, it becomes parallel to the optical axis, a deviation from the optical axis of the incident light occurs, and each pixel of the CCD image pickup element 53 is irradiated.

On the other hand, as shown in FIG. 36, the ferroelectric liquid crystal element 3
When the switch state of is 2, the polarization plane and the extraordinary optical axis 8 form an angle of about 45 degrees, so the transmitted light rotates in the direction of the extraordinary optical axis, and linearly polarized light (Y-axis direction) → elliptically polarized light → Circular polarization →
The elliptically polarized light → linearly polarized light (X-axis direction) changes in the ferroelectric liquid crystal element, and the polarization plane rotates 90 degrees from the initial state.
Is irradiated. Since the crystal plate 4 does not include the extraordinary optical axis of the crystal in the plane of incident polarization, the optical axis is maintained as it is without refraction, and it exits to the air layer again and is irradiated to each pixel of the CCD image pickup element 53. . That is, the a'portion of the subject is imaged. The shift of the optical axis between the state 1 and the state 2 can be used as the operation principle of the pixel shifting.

FIG. 37 shows a specific arrangement example. In the case of an optical system such as a video camera or a still video camera, since incident light from the outside world is not substantially polarized, a polarizing plate is inserted between the outside world (subject) and the ferroelectric switching element. The positional relationship with respect to the diaphragm does not matter. Other optical arrangements are subject-lens-aperture-
The order is: polarizing plate-condensing element-ferroelectric switching element-transparent substrate having uniaxial optical anisotropy-imaging element.
The image pickup element to be combined here is a CCD or a MOS.
The mold element and the like may be of any type.

Since such an image pickup device is a light receiving device unlike a display device, it is possible to improve the spatial resolution (spatial separation ability) of a subject. Here, since it can be performed by the simultaneous method instead of the sequential method like the display element,
The switching part of the FLC element 3 may act on the entire surface of the CCD element at the same time and does not require spatial electrode division of the phase modulation element 3. That is, for example, the pixels of the CCD image sensor also
If there is no deviation of the optical axis because it is discrete, a for each pixel,
Although there are only b and c position resolutions, the frame is divided, and the information of a, b, and c are first accumulated in the simultaneous method and then transferred.
In the next field, the position information of a ', b', and c'is accumulated by the pixel shift of the ferroelectric liquid crystal element 3 by the simultaneous method,
By transferring and recombining with the first field, the vertical resolution is doubled.

A concrete example of mounting these cells on a video camera: Handycam TR-1 (manufactured by Sony Corporation) will be described. First, an infrared cut filter and a low pass filter which can be used therein will be described.

[1] Normal Imaging of Visible Light A semiconductor imaging device such as a CCD imaging device has a sensitivity range of
It extends to 380-1200nm. When a normal visible light image is captured, the near-infrared light region, which cannot be sensed by the human eye, is captured, which adversely affects the image. Therefore, it is necessary to insert the infrared cut filter 61 between the subject 50 and the CCD 53 as shown in FIG.

Here, an example is shown in which an infrared cut filter (cuts wavelengths of 700 nm or more) 61 is combined with the pixel shifting element. Further, since the quartz plate used for the wobbling element is insufficient in cutting high frequency components, an optical low pass filter is required. Therefore, a crystal low-pass filter (a plurality of crystal plates) for 7-point blur that is generally used in a high-quality CCD video camera
It consists of 64. ) Was incorporated (Fig. 38, Fig. 39).

In this low-pass filter, incident light is made into a two-point blur by utilizing its birefringence in one crystal plate, and a two-point image is formed by stacking another crystal plate rotated around the optical axis. It is possible to improve the low-pass filter characteristics by blurring the four-point image into a seven-point image on the third crystal plate.

That is, by blurring the incident light in this manner, it is possible to remove a component of image information having a high spatial frequency, and avoid problems such as moire fringes and color false signals. However, in the case of one crystal plate, the high frequency component can be cut or dispersed only in the y direction, but in the above, the high frequency component can be cut or dispersed in both the x and y directions, and the high frequency component of the high frequency component can be retained while maintaining the sensitivity of the low frequency component. It is possible to further eliminate the influence on the image (the generation of a moire fringe pattern or a color false signal in the image output of the formed image).

FIG. 40 shows an implementation example in which such a low-pass filter is not used, and FIG. 41 shows an implementation example in which the low-pass filter is used.
It was shown to. In each case, the picture element shifting element (wobbling element) 7 is provided in front of the CCD 53.

When the low-pass filter 64 is used, the first extraordinary optical axis of the low-pass filter is the polarization at the time of wobbling.
When the angle is 30 to 60 °, the effect of the low pass filter is obtained, but in other cases, the low pass filter characteristic changes in the field. At this time, by inserting a λ / 4 plate (not shown) between the picture element shifting element 7 and the optical low-pass filter, the difference in the low-pass filter characteristics between fields can be reduced and the low-pass filter characteristics can be sufficiently exhibited. Like

FIG. 42 shows a color separation camera system using three CCDs. However, CCD drive circuit,
The wobbling element drive circuit is omitted.

[2] In the case of imaging infrared light By utilizing the near infrared light region of a semiconductor image pickup device such as a CCD image pickup device, it is possible to take an image of only the near infrared light region which cannot be sensed by the human eye. . In this case, it is not necessary to intentionally insert an infrared cut filter.

In this case, to image only infrared light, it is necessary to insert a visible light cut filter (cuts 760 nm or less) between the subject and the CCD. Accordingly, the temperature distribution of the subject can be imaged. Since the imaging wavelength at this time extends to 700 to 1200 nm, the phase difference of the pixel shift element needs to be 350 to 600 nm, which is half the wavelength.

Although the embodiments of the present invention have been described above, the above embodiments can be further modified based on the technical idea of the present invention.

For example, the shape, size, material, arrangement, etc. of the above-mentioned microlenses may be variously changed. Further, another condensing element that replaces the microlens may be provided corresponding to the pixel.

Further, the kind of liquid crystal alignment film used in the above-mentioned liquid crystal element, the combination thereof and the like may be changed. The structure, material and shape of each component of the liquid crystal element, assembling method and the like may be variously changed. The substrate is not limited to the glass plate and may be any other optically transparent material. Various liquid crystals can be adopted.

The object to which the present invention is applied includes, of course, the optical system such as the display device and the image pickup device described above and the wobbling element which can be incorporated in the system.

[0145]

As described above, the present invention provides a light collecting means for collecting incident light in a predetermined size at a position on the light incident side of a wobbling element corresponding to a pixel of an optical element such as a display element or an image pickup element. Since it is provided, the pixel information can be accurately shifted to a predetermined position during wobbling. Therefore, in the case of a display device, a plurality of pieces of field information can be spatially separated, and the resolution can be sufficiently restored without the information of both fields overlapping, and a high resolution can be obtained. Also, in the image pickup device, wobbling can be accurately performed on the target pixel,
This also leads to an improvement in resolution.

Moreover, since it is not necessary to change the pixel interval or the backlight for wobbling, the aperture ratio is maintained and the power consumption is not increased, and the device performance can be improved.

[Brief description of drawings]

FIG. 1 is a schematic cross-sectional view of a liquid crystal optical display device to which the present invention is applicable (corresponding to a cross section taken along line IA-IA in FIG. 2 and line IB-IB in FIG. 3).

FIG. 2 is a schematic partial plan view of a liquid crystal display element in the display device.

FIG. 3 is a schematic partial plan view of a liquid crystal element for wobbling in the display device.

FIG. 4 is a schematic cross-sectional view similar to FIG. 1 for explaining a positional relationship of main parts in the display device.

FIG. 5 is a principle diagram for explaining a design of a microlens used for the wobbling.

FIG. 6 is a schematic plan view of the liquid crystal element for wobbling.

7 is a sectional view taken along line VII-VII of FIG.

FIG. 8 is an explanatory diagram of each field forming an image.

FIG. 9 is a schematic diagram for explaining wobbling of the display device.

FIG. 10 is a schematic cross-sectional view of another liquid crystal optical display device to which the present invention can be applied.

FIG. 11 is a schematic diagram in a state 1 of a display device using a liquid crystal element to which the present invention is applicable.

FIG. 12 is a schematic view of the same display device in a second state.

FIG. 13 is an explanatory diagram of a cone angle of a ferroelectric liquid crystal (FLC) used in the display device.

FIG. 14 is a schematic diagram of a specific example of the display device in each switch state.

FIG. 15 is a schematic diagram of a case where a normally white TN liquid crystal display element is used in the display device.

FIG. 16 is a schematic diagram of a case where a normally black TN liquid crystal display element is used in the display device.

FIG. 17 is a schematic diagram of a display device using a display element having a small degree of polarization.

FIG. 18 is a waveform diagram showing various driving methods of the same phase modulation element.

FIG. 19 is an explanatory diagram of an optical axis shift due to a birefringent medium.

FIG. 20 is an explanatory diagram of a wobbling state.

FIG. 21 is an explanatory diagram of another wobbling state.

FIG. 22 is an explanatory diagram of still another wobbling state.

FIG. 23 is an explanatory diagram of a wobbling state of an RGB in-line array display element.

FIG. 24 is an explanatory diagram of a wobbling state of an RGB delta array display element.

FIG. 25 is a schematic perspective view showing divided electrodes in the phase modulation element.

FIG. 26 is an explanatory diagram of an interlaced scanning method.

[Fig. 27] Fig. 27 is a waveform diagram of a synchronization signal in each field of the television.

FIG. 28 is a block diagram showing a connection relationship between respective elements of the display device.

[Fig. 29] Fig. 29 is a drive waveform diagram of an electrode-splitting type phase modulation element.

FIG. 30 is a schematic view of a display device using the same element.

FIG. 31 is a schematic view of another display device using the same element.

FIG. 32 is a cross-sectional view of a display to which the display device is applied.

[Fig. 33] Fig. 33 is a cross-sectional view of another example of application to a display.

FIG. 34 is a schematic cross-sectional view of an imaging device to which the present invention can be applied.

[Fig. 35] Fig. 35 is a schematic diagram of the same imaging device in state 1.

FIG. 36 is a schematic diagram of the same imaging device in state 2.

FIG. 37 is a schematic diagram of a specific example of the imaging apparatus.

FIG. 38 is a schematic diagram of a mounted state of a crystal optical low-pass filter.

[Fig. 39] Fig. 39 is a principle diagram illustrating blurring caused by three crystal filters of the same.

[Fig. 40] Fig. 40 is a cross-sectional view of a mounting example of the imaging device.

FIG. 41 is a cross-sectional view of another mounting example.

FIG. 42 is a cross-sectional view of still another mounting example.

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 1 ... (Liquid crystal optical) display device 2 ... (Liquid crystal) display element 3 ... Ferroelectric liquid crystal element (liquid crystal cell) 4 ... Birefringent medium 5 ... Display pixel 7 ... Wobbling Element (picture element shifting element) 8, 10 ... Extraordinary optical axis 9 ... Polarization direction 13, 14, 72 ... Transparent electrode 15, 83 ... Liquid crystal 17 ... Light source 18, 19 ... Polarizing plates 20, 21, 70, 71 ・ ・ ・ Transparent substrate 50 ・ ・ ・ Subject 53 ・ ・ ・ CCD element 73 ・ ・ ・ Black matrix section 74,76 ・ ・ ・ Micro lens 77 ・ ・ ・ Condensing element 80 ・ ・・ Glass substrate 101 ・ ・ ・ Imaging device

─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. ⁶ Identification number Reference number within the agency FI Technical indication location H04N 5/66 102 B 9186-5C (72) Inventor Hidehiko Takanashi 6-7 Kitashinagawa, Shinagawa-ku, Tokyo No. 35 In Sony Corporation (72) Inventor Eriko Matsui 6-7 Kita-Shinagawa, Shinagawa-ku, Tokyo No. 35 In Sony Corporation (72) Inventor Hidefumi Asahi 6-7 Kita-Shinagawa, Shinagawa-ku, Tokyo No. 35 Sony Corporation (72) Inventor Nobue Kataoka 6-7 35 Kita-Shinagawa, Shinagawa-ku, Tokyo Inside Sony Corporation

Claims (5)

[Claims] 1. An optical device comprising a wobbling element arranged to shift an optical axis of emitted light in a predetermined direction in an optical path of an optical element to be wobbled, the optical device corresponding to a pixel of the optical element. An optical device in which a condensing unit that condenses the incident light into a predetermined size is provided at a position on the light incident side of the wobbling element. 2. The optical device according to claim 1, wherein the light condensing unit comprises a microlens. 3. A plurality of optically transparent substrates provided with an optically transparent electrode and an alignment film in this order are arranged to face each other at a predetermined gap on the side of the electrode and the alignment film, A wobbling element is constituted by a liquid crystal element in which liquid crystal is injected into the gap, and at least one of the electrodes is divided by the number of scanning lines of the display element to be wobbled. w, l = (a + b) / 2, where w is the distance between the electrodes, l is the pixel size of the display element, and b is the pixel spacing. 2. The optical device described in 2. 4. A first microlens is provided on the light incident surface of the wobbling element, and a second microlens is provided in front of the light incident side opposite to the first microlens. 2. The light condensing means is configured so that the optical axis and the focal point are common with the two microlenses.
The optical device according to any one of 1. 5. When the focal length of the first microlens is f _D and the focal length of the second microlens is f _W , a relational expression of f _D / f _W = (a + b) / 2a is satisfied. The optical device according to claim 3 or 4.