KR100890290B1 - Display apparatus of the diffractive optical modulator having focus depth dependent on the numerical aperture - Google Patents

Abstract

The present invention relates to a display device using a diffractive optical modulator.

In particular, the present invention relates to a display apparatus using a diffraction type optical modulator having a depth of focus depending on the numerical aperture to appropriately adjust the numerical aperture of the illumination system to have an infinite focal depth.

Diffraction type, optical modulator, display, numerical aperture, depth of focus, infinite depth of focus

Description

Display apparatus of the diffractive optical modulator having focus depth dependent on the numerical aperture}

1 is a perspective view of an open hole-based diffractive optical modulator used in the present invention.

2 is a block diagram of a display apparatus using a diffractive optical modulator having a depth of focus depending on the numerical aperture according to an embodiment of the present invention.

3A is a perspective view of an illumination system including the light source system and the concave lens of FIG. 2, a first cylinder lens, and a second cylinder lens, and FIG. 3B is a light source system and the concave lens of FIG. 2, and a first cylinder lens and a second cylinder lens. 3C is a plan view of the illumination system including the light source system, the concave lens, the first cylinder lens, and the second cylinder lens.

4A is a front view of the projection system including the convex lens and the scanner of FIG. 2, and FIG. 4B is a plan view including the convex lens and the scanner of FIG. 2.

<Explanation of symbols for the main parts of the drawings>

102 display optical system 104 display electronic system

106: light source 108: lighting system

110: diffraction optical modulator 112: projection system

116: filter system 118: screen

The present invention relates to a display device using a diffractive optical modulator.

In particular, the present invention relates to a display apparatus using a diffraction type optical modulator having a depth of focus depending on the numerical aperture to appropriately adjust the numerical aperture of the illumination system to have an infinite focal depth.

As a next-generation display device, various flat panel displays (FPDs) are being actively researched. Among them, generalized display devices include liquid crystal displays (LCDs) using electro-optical characteristics of liquid crystals, and gases. And a plasma display panel (PDP) using discharge.

Among them, a liquid crystal display device (hereinafter, abbreviated as "LCD") has a narrow viewing angle and a slow response time, and requires a thin film transistor (TFT) and an electrode using a semiconductor manufacturing process. There is a difficulty.

Plasma display panel (PDP) has the advantage that it is advantageous to large area due to its simple manufacturing process, but it is difficult to consume large power, low discharge and luminous efficiency and high price.

The development of a new display device that can solve the problems of the flat panel display device is in progress, and recently, the pixel (Pixel) using a micro electromechanical system (hereinafter, abbreviated as "MEMS") is an ultra-fine processing technology. A display device capable of displaying an image by forming a fine spatial light modulator (SLM) has been proposed.

Here, the spatial light modulator (SLM) is a converter for modulating the incident light beams in a spatial pattern corresponding to the electrical or optical input. Incident light can be modulated in its phase, intensity, polarization or direction, and light modulation can be achieved by various materials with various electro-optic or magneto-optic effects, and by materials that modulate the light by surface modification. have.

Meanwhile, the spatial light modulator described above may be used in various applications, and for example, may be used in a display device.

In general, a display apparatus using an optical modulator according to the prior art includes a light source, an illumination lens, a diffractive light modulator, a projection system, a screen, and the like.

The light source includes a plurality of light sources, for example, a red light source, a green light source, and a blue light source.

Next, the illumination lens enters the light emitted from the light source into the light modulator. .

The diffractive light modulator performs light modulation when light is incident to form diffracted light having a plurality of diffraction orders. At this time, the diffracted light formed by the diffractive light modulator forms linear diffracted light when looking at each diffraction order. That is, the diffracted light emitted from the diffractive light modulator is arranged to be linearly arranged to form a plurality of scanning diffraction point lights corresponding to each other to form pixels of an image formed on the screen.

In addition, the projection system generates a 2D image by projecting and scanning a linear scan line formed by linearly arranging a plurality of scanning diffraction point lights onto a screen.

The projection and scanning optics according to the prior art of such a projection system generates a two-dimensional image by scanning a scanning line consisting of a plurality of scanning diffraction point light generated by the diffractive optical modulator on the screen.

The projection and scanning optics are composed of a condenser lens, a scanner and a projection lens, and project the incident diffracted light onto the screen.

Here, the condenser lens collects linear diffracted light, and the scanner scans the incident line image on the screen from left to right as an X scanning mirror, and then scans from right to left. , Repeat this operation. The projection lens adjusts the depth of focus so that the focus of the diffracted light is on the screen.

On the other hand, it is necessary to meet the requirements of thinning and miniaturization in the production of such a display device using a conventional diffractive optical modulator.

That is, in the recent display field, the thickness of the display device tends to become thinner and thinner, and it is necessary to satisfy this tendency.

In addition, in the recent display field, it is necessary to embed a display device in a portable terminal or the like, but it is necessary to meet such a need.

Therefore, the present invention has been devised to meet the above needs, and is a display device using a diffraction type optical modulator having a depth of focus depending on the numerical aperture to properly adjust the numerical aperture of the illumination lens to have an infinite focal depth. The purpose is to provide.

The present invention for solving the above problems, the light source for generating and emitting light; An illumination system for changing the light emitted from the light source system into linear parallel light having a small numerical aperture; A diffraction type optical modulator for modulating incident light incident from the illumination system to form diffracted light having a plurality of diffraction orders; And a projection system for generating an image image by projecting the diffracted light emitted from the diffractive light modulator onto a screen.

Hereinafter, with reference to the accompanying drawings will be described in detail a preferred embodiment of the present invention.

1 is a perspective view of an open hole-based diffractive light modulator used in the present invention.

Referring to the drawings, the open hole-based diffractive light modulator used in the present invention includes a substrate 11.

In addition, the open hole-based diffractive light modulator includes an insulating layer 12 formed on the substrate 11.

In addition, the open-hole-based diffractive optical modulator is formed in a portion of the insulating layer 12, and the space between the holes 16aa-16nb of the upper reflecting portions 16a-16n and the upper reflecting portions 16a-16n. A lower reflector 13 reflects light incident through the light.

In addition, the open hole-based diffractive optical modulator has a pair of side support members 14 and 14 'formed at positions spaced apart from each other on the surface of the substrate 11 with the lower reflector 13 positioned therebetween. It is included.

In addition, the open-hole-based diffractive optical modulator is supported on both sides by a pair of side support members 14 and 14 ', spaced apart from the substrate 11, and has a central portion movable up and down. Holes (not shown) corresponding to the holes 16aa to 16nb formed in the 16a to 16n are formed and include a plurality of laminate supporting plates 15a to 15n forming an array.

In addition, the open-hole-based diffraction type optical modulator is formed at the center portion of the laminate supporting plates 15a to 15n and has holes 16aa to 16nb at the center to partially reflect the incident light and partially to the holes 16aa. And upper reflectors 16a-16n passing through ˜16nb) and forming an array.

In addition, the open-hole-based diffractive optical modulators are formed on the laminate support plates 16a to 16n, and are spaced apart from each other, and are positioned on the side support members 14 and 14 ', and the laminate support plates 16a to 16n are disposed. A plurality of pairs of piezoelectric bodies 20a to 20n and 20a 'to 20n' for moving up and down are provided.

Here, the pair of piezoelectric materials 20a to 20n and 20a 'to 20n' include lower electrode layers 20aa to 20na and 20aa 'to 20na', piezoelectric material layers 20ab to 20nb and 20ab to 20nb ', and upper electrode layers 20ac. When a voltage is applied to ˜20 nc 20ac 'to 20 nc, the center portion of the laminate supporting plates 15a to 15n moves up and down by contraction and expansion of the piezoelectric material layers 20ab to 20nb and 20ab' to 20nb '. Accordingly, the upper reflecting portions 16a to 16n also move up and down. For convenience, each of the laminate supporting plates 16a to 16n, the upper reflecting portions 16a to 16n, and the pair of piezoelectric bodies 20a to 20n and 20a 'to 20n' is called an element.

On the other hand, when light is incident on the upper reflecting portions 16a to 16n of the open hole diffraction type optical modulator, the upper reflecting portions 16a to 16n reflect some light and some of the light through the holes 16aa to 16nb. The lower reflector 13 reflects the light passing through the holes 16aa-16nb of the upper reflector 16a-16n.

As a result, the reflected light reflected by the upper reflecting portions 16a to 16n and the reflected light reflected by the lower reflecting portion 13 form diffracted light having various diffraction coefficients, and the light intensity of the diffracted light is determined by the upper reflecting portion 16a. 16 n) and the step difference between the lower reflector 13 become the maximum when the wavelength of the incident light is λ, and becomes an odd multiple of λ / 4, and becomes the minimum when the even multiple becomes even.

2 is a block diagram of a display apparatus using a diffractive optical modulator having a depth of focus depending on the numerical aperture according to an embodiment of the present invention.

Referring to the drawings, a display apparatus using a diffraction type optical modulator having a depth of focus depending on the numerical aperture according to an embodiment of the present invention includes a display optical system 102 and a display electronic system 104.

The display optical system 102 includes a light source system 106 that generates and emits light, and the light source system 106 includes a vertical external cavity surface emitting laser (VECSEL) and a vertical resonance surface emitting laser (VCSEL). ; Light sources fabricated using semiconductors such as Vertical Cavity Surface Emitting Laser, Light Emitting Diode (LED), Laser Diode (LD), Super Luminescent Diode (SLED), etc. can be used. .

The light source system 106 emits laser illumination, the cross section of the laser illumination being circular (or elliptical), the intensity profile of the light having a Gaussian distribution, for example, the light source system 106 (actually an R light source). Laser, the G light source laser, and the B light source laser) may sequentially emit R light, G light, and B light.

In addition, the display optical system 102 converts the light emitted from the light source system 106 into linear parallel light having a low numerical aperture (NA) and parallel light having a linear shape to the diffractive optical modulator 110. It includes an illumination system 108 to irradiate.

The illumination system 108 converts the laser illumination emitted by the light source system 106 into linear long, narrow light having a low numerical aperture and then converts the laser light into parallel light and enters the diffracted light modulator 110.

When the illumination system 108 produces linear parallel light having a low numerical aperture and irradiates the diffractive light modulator 110, the diffracted light modulated by the diffractive light modulator 110 has an infinite depth of focus.

In general, all optics have holes that limit light passing through the optics, which may be the outer diameter of the lens or the aperture. This is called an aperture or stop, of which energy limiting is called an aperture stop, and when limiting the size of an object for forming an image, etc., it is called a field stop. This aperture stop is called an entrance pupil on the object side and an exit pupil on the upper side. When the lens forms an image of an object, the amount of light that can be received from the object is proportional to the entrance pupil of the lens or the area of the aperture. There are f-numbers and numerical apertures (NA). Among these, the numerical aperture can be expressed as follows.

Numerical aperture = NA = Nsinθ

Here, θ: the angle at which the light rays at the end of the opening converge, N is a proportional constant. At this time, when θ is small, the numerical aperture is NA ≒ θ.

The illumination system 108 is, for example, a first cylinder lens 108ba having a concave lens 108a and a curved surface in the Y-axis direction (Y-axis is shown in the figure) as shown in FIGS. 3A to 3C. And a second cylinder lens 108bb having a curved surface in the X-axis direction (X-axis is shown in the drawing).

That is, the illumination system 108 enlarges the light output from the light source system 106 in the Y-axis direction with respect to the optical path direction (shown in the drawing on the Z-axis), and changes the thus-expanded light into parallel light. The light converted into light is condensed in the X-axis direction, converted into linear light having a low convergence angle θ, and illuminated on the diffractive optical modulator 110. The concave lens 108a and the Y-axis direction (Y-axis are shown in the drawing) And a second cylinder lens 108bb having a curved surface in the X-axis direction (the X-axis is shown in the drawing).

This will be described in more detail with reference to FIGS. 3A to 3C as follows. 3A is a perspective view of an illumination system 108 consisting of a light source system 106 and a concave lens 108a, a first cylinder lens 108ba, and a second cylinder lens 108bb, and FIG. 3B is a concave light source system 106 and concave. It is a front view of the illumination system 108 which consists of the lens 108a, the 1st cylinder lens 108ba, and the 2nd cylinder lens 108bb, and FIG. 3C shows the light source system 106, the concave lens 108a, and the 1st cylinder lens ( 108ba), a plan view of the illumination system 108 composed of the second cylinder lens 108bb. Here, when light passes through the concave lens 108a, the light is enlarged in the Y-axis direction, and there is no change in the X-axis direction. Then, when light passes through the first cylinder lens 108ba, the light that is enlarged in the Y-axis direction becomes parallel light, and the X-axis direction remains unchanged. Next, when light passes through the second cylinder lens 108bb, there is no change in the Y-axis direction and the X-axis direction is focused. At this time, the convergence angle θ becomes NA. This numerical aperture NA must satisfy the following conditional expression (1) when the pitch of the diffractive optical modulator 110 is d and the wavelength of incident light is λ.

λ / d ≤ NA ------- (1)

On the other hand, the display optical system 102 includes a diffraction type optical modulator 110 to diffract the linear light irradiated from the illumination system 108 to generate diffracted light of a plurality of diffraction orders in which the light intensity of the diffracted light is adjusted.

Here, the diffracted light emitted by the diffractive light modulator 110 includes diffracted light having various diffraction orders, such as zero-order diffraction light, first-order diffraction light, second-order diffraction light, third-order diffraction light, and the like.

The diffracted light emitted by the diffractive light modulator 110 is a diffracted light having a long line shape and a narrow width (hereinafter, referred to as a line image).

Here, the diffractive light modulator 110 is, for example, vertically movable, and includes a plurality of upper reflectors that form an array, and a plurality of lower reflectors positioned between the upper reflectors and spaced apart from the upper reflectors by a predetermined distance. Consists of wealth. In addition, the diffractive optical modulator 110 may use electrostatic force and static magnetic force as driving means for driving the upper reflector, and may use a piezoelectric material layer having an upper electrode layer formed on one surface and a lower electrode layer formed on the other surface. have.

The diffracted light emitted from the diffractive light modulator 110 may be configured to diffract light corresponding to one pixel of an image formed on the screen 118 by diffracted light formed by one upper reflector and a lower reflector corresponding thereto. The diffracted light formed by the two or more upper reflectors and the lower reflector corresponding thereto may form diffracted light corresponding to one pixel formed on the screen 118.

Next, the display optical system 102 projects a diffracted light having a plurality of diffraction orders emitted from the diffractive light modulator 110 toward the screen 118 to perform scanning on the screen 118. ) Is included.

Here, the projection system 112 is to perform a scanning on the screen 118 to maintain a constant flux of the image displayed on the screen 118 by the control of the display electronic system 104.

The projection system 112 includes a convex lens 112a for collecting diffracted light emitted from the diffractive light modulator 110 and a scanner 112b for scanning the diffracted light toward the screen 118. .

The convex lens 112a serves to collect diffracted light, and the scanner 112b scans the diffracted light onto the screen 118.

This will be described below with reference to FIGS. 4A and 4B. 4A is a front view of the projection system that includes the convex lens 112a and the scanner 112b, and FIG. 4B is a plan view that includes the convex lens 112a and the scanner 112b. Here, the diffracted light generated by the diffractive light modulator 110 is focused in the Y-axis direction and the X-axis direction via the convex lens 112a. At this time, as can be seen in FIG. 4A, the light is rapidly focused in the Y-axis direction, and is rapidly enlarged beyond the Y-axis focus (here, the scanner 112b is positioned at the focus). However, as can be seen in FIG. 4B, the light is smoothly collected in the X-axis direction, and the focal length is largely dependent on the numerical aperture of the diffracted light emitted from the diffractive light modulator 110.

On the other hand, the sharpness of the image formed on the screen 118 largely depends on the depth of focus (Dof). Here, the depth of focus refers to information about how much clear images appear before and after the focused object, and the depth of focus is largely dependent on the numerical aperture. When the diffraction light with a low numerical aperture is used, the depth of focus is deep.

That is, the relationship between the depth of focus and the numerical aperture satisfies the following conditional expression (2).

Dof ∝ λ / NA ² ------- (2)

Therefore, when the illumination light having a small numerical aperture in the illumination system 108 is formed, even if the screen 118 is moved back and forth, since the depth of focus is deep, the sharpness is not greatly affected. Therefore, it is not necessary to adjust the focus according to the movement of the screen 118 back and forth, thereby simplifying the manufacture of the display device using the diffractive optical modulator.

In particular, the screen 118 is not fixed as in a case where a display using a diffraction type optical modulator is mounted on a portable terminal, but a depth of focus may be deep in an application in which the user arbitrarily sets the screen 108 and focuses using the naked eye. There is a need and the use of diffraction light with a low numerical aperture satisfies this need without providing a separate focus lens.

Here, the scanner 112b may be a galvanometer scanner or a polygon mirror scanner. The galvano scanner has a rectangular plank shape and a mirror is attached to one side. Rotate left and right about the axis within a predetermined angle range. Polygon mirror scanners have the shape of a polygonal column, with mirrors attached to the sides of the polygonal column. A mirror attached to each side and rotating in one direction about an axis changes an angle of reflection of light incident by the rotation to project an image on the screen 118.

In general, since the scanner 112b performs a rotational movement, a driving motor or the like is an essential component, and such a driving motor requires a lot of power consumption. However, when the display device using the diffractive optical modulator is used in a portable terminal, it is desirable that the power consumption is small.

On the other hand, the display optical system 102 is located between the projection system 112 and the screen 118, and the diffraction light of the order desired to be used in the various orders of diffracted light projected from the projection system 112 to the screen 118. It includes a filter system 116 to pass through. As an example of the filter system 116, slits may be used.

On the other hand, the display electromagnetic field 104 is connected to the light source system 106, the diffractive light modulator 110, and the projection system 112. The display electromagnetic field 104 provides power to the light source system 106. The display electromagnetic field 104 drives the upper reflector by providing a driving voltage to the upper electrode layer and the lower electrode layer of the piezoelectric body of the diffractive optical modulator 110.

On the other hand, according to the present invention as described above, in the projection system using a diffraction type optical modulator, there is an effect that can be miniaturized because it does not have a bulky and heavy focus lens separately.

In addition, according to the present invention, since the projection system using the diffractive optical modulator does not have to be provided with a bulky and heavy focus lens separately, there is an effect of enabling thinning.

In addition, according to the present invention, since the projection system using a diffractive optical modulator is not provided with a focusing lens separately, there is an effect of bringing down the cost.

Claims (6)

A light source system generating and emitting light; An illumination system for changing the light emitted from the light source system into linear parallel light having a small numerical aperture NA and emitting the light; A diffraction type optical modulator for modulating incident light incident from the illumination system to form diffracted light having a plurality of diffraction orders; And And a projection system for projecting diffracted light emitted from the diffractive light modulator onto a screen to generate an image image. The numerical aperture of the illumination light incident on the diffraction optical modulator by the illumination system satisfies λ / d ≦ NA when the pitch of the diffraction light modulator is d and the wavelength of the incident light is λ. Display device using a diffractive optical modulator having a dependent depth of focus. The method of claim 1, The illumination system, A collimator lens for enlarging the light emitted from the light source system; A first cylinder lens for converting light passing through the collimator lens into parallel light; And A display apparatus using a diffractive optical modulator having a depth of focus depending on the numerical aperture including a second cylinder lens for converting parallel light passing through the first cylinder lens into linear light having a low numerical aperture NA. delete The method of claim 1, A focal point dependent on the numerical aperture formed further at the rear end of the diffractive optical modulator and further including a filter system for passing the diffracted light having a desired diffraction order in the diffracted light having a plurality of diffraction orders emitted from the diffractive optical modulator Display device using a diffractive optical modulator having a depth. The method of claim 4, wherein The filter system, A Fourier lens that receives diffracted light having a plurality of diffraction orders from the diffraction type optical modulator and condenses and emits the light by orders And And a diffraction type optical modulator having a depth of focus depending on the numerical aperture including a filter for filtering the diffracted light having a desired diffraction order from the diffracted light collected for each order from the Fourier lens. The method of claim 1, The projection system, A condenser lens for condensing diffracted light emitted from the diffractive light modulator; And And a diffraction type optical modulator having a depth of focus depending on a numerical aperture including a scanner for projecting diffracted light emitted from the condenser lens onto a screen to generate an image image.

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