Patent Application
20240077658
The present invention relates to a diffuser plate, a display device, a projecting device, and a lighting device.
In order to change an optical diffusion property, a diffuser plate that diffuses incident light to a desired direction is used. The diffuser plate is widely utilized in various devices such as, for example, a display device such as a display, a projecting device such as a projector, or various types of lighting devices. A type of diffuser plate utilizes light refraction resulting from the surface shape of the diffuser plate to diffuse incident light at a desired diffusion angle. As a diffuser plate of that type, a diffuser plate of a microlens array type in which a plurality of microlenses having sizes of approximately several tens of micrometers are arranged is known.
Such a diffuser plate of a microlens array type has problems in that, as a result of interference of a wavefront of light from each of microlenses, a diffraction wave due to a periodic structure of a microlens array occurs, which causes unevenness in intensity distribution of diffused light. Thus, a technology of varying the arrangement of microlenses, the shapes of lens surfaces, and the shapes of apertures to reduce unevenness in intensity distribution of diffused light caused by interference or diffraction has been proposed.
For example, Patent Literature 1 describes a diffuser plate including a plurality of microlenses regularly arranged on a principal surface in the form of a rectangular grid, in which a plurality of microlenses having sectional shapes different from each other and having no symmetrical axis are used. In addition, Patent Literature 2 describes arranging lens vertex positions of a plurality of microlenses disposed in the form of a rectangular grid away from grid points of a reference grid.
However, in an array structure in which a plurality of microlenses having no symmetrical axis and having sectional shapes different from each other are disposed regularly in the form of a rectangular grid as described in Patent Literature 1 above, unevenness in intensity distribution of diffused light is reduced merely by means of phase changes of light between microlenses adjacent to each other. Therefore, the effect of uniformly diffusing diffused light in two directions of the rectangular grid orthogonal to each other is restrictive. In addition, in an array structure disposed regularly in the form of a rectangular grid as described in Patent Literature 2, highly uniform light distribution control in the two directions of the rectangular grid cannot be achieved merely by shifting the vertex positions of the respective microlenses.
The present invention was therefore made in view of the above circumstances, and an object of the present invention is to reduce unevenness in a luminance distribution and improve uniformity of light distribution in two directions of microlenses disposed in the form of a rectangular grid.
According to an aspect of the present invention in order to solve the above-mentioned problems, provided is a diffuser plate of a microlens array type including a base material, and a microlens array composed of a plurality of microlenses disposed on an X-Y plane on at least one surface of the base material using a rectangular grid as a reference, in which grid intervals Wx in an X direction of the microlenses disposed in the X direction of the rectangular grid are different from each other, grid intervals Wy in a Y direction of the microlenses disposed in the Y direction of the rectangular grid are different from each other, and surface shapes of the plurality of microlenses are different from each other.
The grid intervals Wx in the X direction may be each varied at random at a varying rate δWx within ±10% to ±50% using a reference grid interval Wx_k as a reference, and the grid intervals Wy in the Y direction may be each varied at random at a varying rate δWy within ±10% to ±50% using a reference grid interval Wy_k as a reference.
Curvature radii Rx in the X direction of the microlenses disposed in the X direction may be varied from each other, and curvature radii Ry in the Y direction of the microlenses disposed in the Y direction may be varied from each other.
The curvature radii Rx in the X direction may be each varied at random at a varying rate δRx within ±10% to ±50% using a reference curvature radius Rx_k as a reference, and the curvature radii Ry in the Y direction may be each varied at random at a varying rate δRy within ±10% to ±50% using a reference curvature radius Ry_k as a reference.
The grid intervals Wx in the X direction may be each varied at random at a varying rate δWx within ±10% to ±50% using a reference grid interval Wx_k as a reference, the grid intervals δWy in the Y direction may be each varied at random at a varying rate δWy within ±10% to ±50% using a reference grid interval Wy_k as a reference, the reference grid intervals Wx_k, Wy_k and the reference curvature radii Rx_k, Ry_k may satisfy relational expressions (A) and (B) below, and a diffusion angle (a full width at half maximum) achieved by the diffuser plate may be less than or equal to 20°:
Rx_k/Wx_k≥1.85 (A); and
Ry_k/Wy_k≥1.85 (B).
A planar position of a vertex of each of the microlenses disposed in the X direction and the Y direction may be off-centered from a central point of each of rectangles of the rectangular grid.
When distances in the X direction and the Y direction from the central point of each of the rectangles to the planar position of the vertex of each of the microlenses having been off-centered are denoted by an off-centering amount Ecx and an off-centering amount Ecy, respectively, and proportions of the off-centering amounts Ecx and Ecy with respect to the grid intervals Wx and Wy of the rectangular grid are denoted by an off-centering rate δEcx and an off-centering rate δEcy, respectively, the planar position of the vertex of each of the microlens may be off-centered at random at the off-centering rates δEcx and δEcy within ±10% to ±50%.
Height positions of vertices of the plurality of microlenses disposed in the X direction and the Y direction may be different from each other.
The microlenses disposed in the X direction and the Y direction may be arranged continuously with no gap between each other.
A boundary line between adjacent ones of the microlenses may include a straight line and a curve.
The microlens array may include a plurality of unit cells which are basic arrangement patterns of the microlenses, and the microlens array may be configured by disposing the plurality of unit cells with no gap between each other while maintaining continuity of the microlenses at boundary portions between the plurality of unit cells.
Surface shapes of the microlenses may be spherical shapes, or aspherical shapes having anisotropy in the X direction or the Y direction.
According to another aspect of the present invention in order to solve the above-mentioned problems, a display device including the above-described diffuser plate is provided.
According to another aspect of the present invention in order to solve the above-mentioned problems, a projecting device including the above-described diffuser plate is provided.
According to another aspect of the present invention in order to solve the above-mentioned problems, a lighting device including the above-described diffuser plate is provided.
As described above, the present invention can reduce unevenness in a luminance distribution and improve uniformity of light distribution in two directions of microlenses disposed in the form of a rectangular grid.
Hereinafter, (a) preferred embodiment(s) of the present invention will be described in detail with reference to the appended drawings. Note that, in the present specification and the drawings, structural elements that have substantially the same function and structure are denoted with the same reference numerals, and repeated explanation is omitted.
First, an overview of a diffuser plate according to an embodiment of the present invention will be described.
The diffuser plate according to the present embodiment which will be described below in detail is a diffuser plate of a microlens array type having a function of uniformly diffusing light. Such a diffuser plate has a microlens array formed on the X-Y plane on at least one surface (a principal surface) of a base material. The microlens array is composed of a plurality of microlenses disposed and deployed in the form of a rectangular grid. The microlens has a convex structure (convex lens) or a concave structure (concave lens) having a light diffusing function, and has a lens diameter of approximately several tens of micrometers.
Then, in the diffuser plate according to the present embodiment, the plurality of microlenses are disposed in the form of a rectangular grid (in the form of a matrix) using a rectangular grid having irregularity as a reference. In this rectangular grid having irregularity, a plurality of grid intervals Wx in the X direction (a row direction) are varied at random and different from each other, and a plurality of grid intervals Wy in the Y direction (a column direction) are also varied at random and different from each other. Furthermore, curvature radii Rx and Ry of the plurality of microlenses disposed in the X and Y directions are varied at random (irregularly) to be different from each other. In addition, the planar position of the vertex of each of the microlenses is varied at random (off-centered) so as to be shifted from the central point of each of rectangles of the rectangular grid. In addition, the height positions in the Z direction of the vertices of the plurality of microlenses (the positions in the thickness direction of the diffuser plate) are also vaned at random and different from each other. By varying the grid intervals Wx, Wy, the curvature radii Rx, Ry, the planar positions and height positions of the lens vertices, and the like at random in this manner, the surface shapes of the plurality of microlenses deployed in the form of a rectangular grid are varied at random and have shapes different from each other.
In this manner, the diffuser plate according to the present embodiment achieves a three-dimensional surface structure of a highly random microlens array by varying the respective varying elements of the plurality of microlenses at random. This enables an overlapping state of phases of light emitted from the respective microlenses to be controlled. As a result, a surface structure of a diffuser plate can be provided which has highly-transmissive luminance properties, satisfies uniformity of light distribution in two directions (the X and Y directions) orthogonal to each other, and may control sufficient anisotropy in light distribution and a cut-off property of intensity distribution of diffused light.
Furthermore, according to the present embodiment, the plurality of microlenses are disposed on the X-Y plane using the irregular rectangular grid having the grid intervals Wx and Wy different from each other as a reference. This enables the plurality of microlenses to be arranged continuously with no gap between each other on the surface of the diffuser plate while ensuring randomness of the surface shape of each of the microlenses. This can prevent a flat portion from existing at the boundary portion between the microlenses adjacent to each other when possible. Thus, unevenness in intensity distribution of diffused light can further be reduced to further improve uniformity of light distribution in the two directions (the X and Y directions).
Hereinafter, the diffuser plate according to the present embodiment having characteristics as described above will be described in detail.
First, an overall configuration of the diffuser plate according to an embodiment of the present invention and a layout pattern of microlenses will be described with reference to
The diffuser plate 1 according to the present embodiment is a diffuser plate of a microlens array type in which a microlens array composed of a plurality of microlenses (single lenses) is arranged on a substrate. The microlens array of the diffuser plate 1 is composed of a plurality of unit cells 3 as shown in
Herein,
In the example of
In addition, as schematically shown in a magnified view on the right in
In this manner, in the diffuser plate 1 according to the present embodiment, the microlens array is formed by disposing the unit cells 3 (basic structures) of the microlens array with no gap while maintaining continuity of the boundaries. This can prevent an unintended defect such as diffraction, reflection, or scattering of light from occurring at the boundary portions between the unit cells 3 to obtain a desired light distribution property with the diffuser plate 1.
A configuration of the diffuser plate 1 according to the present embodiment will now be described in more detail with reference to
As shown in
First, the base material 10 will be described. The base material 10 is a substrate for supporting the microlens array 20. The base material 10 may be film like or plate like. The base material 10 shown in
The base material 10 is a transparent base material capable of transmitting light. The base material 10 is formed of a material that can be assumed as being transparent in a wavelength band of light incident on the diffuser plate 1. For example, the base material 10 may be formed of a material having a light transmittance of more than or equal to 70% in a wavelength band corresponding to visible light.
The base material 10 may be formed of publicly-known resin such as polymenthyl methacrylate (PMMA), Polyethylene terephthalate (PET), polycarbonate (PC), Cyclo Olefin Copolymer (COC), Cyclo Olefin Polymer (COP), or Triacetylcellulose (TAC), for example. Alternatively, the base material 10 may be formed of publicly-known optical glass such as quartz glass, borosilicate glass, or high transmission crown glass.
The microlens array 20 will now be described. The microlens array 20 is provided on at least one surface (a principal surface) of the base material 10. The microlens array 20 is an assembly of the plurality of microlenses 21 (single lenses) disposed on the surface of the base material 10. In the present embodiment, the microlens array 20 is formed on one surface of the base material 10 as shown in FIG. 2. However, this is not a limitation, and the microlens array 20 may be formed on both principal surfaces (front and rear surfaces) of the base material 10.
The microlenses 21 are fine optical lenses on the order of several tens of micrometers, for example. The microlenses 21 constitute single lenses of the microlens array 20. The microlens 21 may have a concave structure (concave lens) formed to be recessed in the thickness direction of the diffuser plate 1, or may have a convex structure (convex lens) formed to protrude in the thickness direction of the diffuser plate 1. The present embodiment will describe an example in which the microlenses 21 have concave structures (concave lenses) as shown in
The surface shape of each of the microlenses 21 is not particularly limited as long as it is a curved surface shape including a curved surface component. The surface shape of the microlens 21 may be a spherical shape only including a spherical component, for example, or may be an aspherical shape including a spherical component and an aspherical component, or may be an aspherical shape only including an aspherical component.
As shown in
Note that, in order to reduce the 0-th order transmitted light component, the filling rate of the microlenses 21 on the base material 10 preferably is more than or equal to 90%, and more preferably is 100%. Herein, the filling rate is the proportion of the area of a portion occupied by the plurality of microlenses 21 on the surface of the base material 10. If the filling rate is 100%, the surface of the microlens array 20 is formed by a curved surface component, and will hardly include a flat surface component.
However, since the curved surfaces of the plurality of microlenses 21 are connected continuously in actual manufacturing of the microlens array 20, the vicinity of an inflection point at the boundary between the microlenses 21 adjacent to each other may become generally flat. In such a case, the width of a region in the vicinity of the inflection point (the width of the boundary line between the microlenses 21) which becomes generally flat at the boundary between the microlenses 21 preferably is less than or equal to 1 μm. The 0-th order transmitted light component can thereby be reduced sufficiently.
In addition, in the microlens array 20 according to the present embodiment, the plurality of microlenses 21 are not arranged at random (irregularly), but as shown in
In the present embodiment, the plurality of microlenses 21 are arranged quasi-regularly using a rectangular grid having irregularity as a reference. Then, the surface shapes and planar shapes of the microlenses 21 are varied at random. As shown in
In this manner, in the present embodiment, the curvature radii Rx, Ry and the aperture sizes Dx, Dy of the respective microlenses 21 are vaned at random, and have variations. Note that the aperture sizes Dx and Dy of the microlenses 21 are equivalent to lens diameters of single lenses. The phase distribution of an optical aperture of each of the microlenses 21 differs depending on the orientation. The plurality of microlenses 21 are arranged continuously on the surface of the base material 10 in a manner overlapping each other, and the curvature radii Rx, Ry and the aperture sizes Dx, Dy (lens diameters) of the respective microlenses 21 have variations. Accordingly, the shapes (surface shapes and planar shapes) of the plurality of microlenses 21 are not identical shapes to each other. Therefore, the plurality of microlenses 21 have various shapes as shown in
As a result, as shown in
Specifically, in a case of seeing a microlens 21 in plan view in the Z direction vertical to the surface of the base material 10 as shown in
A method of arranging the microlenses 21 according to the present embodiment will now be described in detail with reference to
The microlens array 20 in which the plurality of microlenses 21 having characteristics as described above are disposed can be achieved by the arrangement method according to the present embodiment which will be described below.
First, as shown in
In this reference arrangement method, upon experiencing the quasi-regular disposition of the microlenses 21 (see
(1) Initial Disposition State of the Microlenses 21 Using the Irregular Rectangular Grid as a Reference (
In the reference arrangement method according to the present embodiment, the initial disposition state to be used as a reference for the arrangement of the microlenses 21 is set first. Specifically, in the initial disposition state, the plurality of microlenses 21 are disposed on the X-Y plane of a reference surface regularly to some extent (quasi-regularly) using a rectangular grid having irregularity as a reference as shown in
The rectangular grid according to the present embodiment may be composed of rectangles or squares. As shown in
Herein, the above-described irregular rectangular grid is such a rectangular grid in which the grid intervals Wx in the X direction are varied at random and different from each other, and the grid intervals Wy in the Y direction are varied at random and different from each other, as shown in
A method of varying the grid intervals Wx and the grid intervals Wy at random is as follows, for example. First, constant reference values Wx_k and Wy_k (hereinafter referred to as reference grid intervals Wx_k and Wy_k) to be used as references for varying the grid intervals Wx and Wy in the X direction and the Y direction are set. Then, the reference grid intervals Wx_k and Wy_k are varied at random within ranges of predetermined varying rates δWx and δWy [±%] to set the grid intervals Wx and Wy (Wx=Wx_k×(100±δWx [%]), Wy=Wy_k×(100±δWy [%])). This is repeated by the number of rectangles of the rectangular grid to set the plurality of grid intervals Wx1, Wx2, Wx3, . . . , and Wy1, Wy2, Wy3, . . . in the X direction and the Y direction, respectively.
Herein, the varying rates δWx and Wy preferably fall within a range of ±10% to ±50%. If the varying rates δWx and δWy are set to be less than ±10%, variations in the grid intervals Wx and Wy will be insufficient, which could make it difficult to provide the microlens array 20 with sufficient aperiodicity, and uniformity of diffused light through the microlens array 20 could be degraded. On the other hand, if the varying rates δWx and δWy are set to be more than ±50%, variations in the grid intervals W will be excessively large, which could make it difficult to continuously dispose the plurality of microlenses 21 on the X-Y plane with no gap.
For example, in the case in which the varying rates δWx and δWy are set at “±10%”, the grid intervals Wx and Wy are set at values shifted at random from the reference grid intervals Wx_k and Wy_k within the range of less than or equal to “±10%” using the reference grid intervals Wx_k and Wy_k as references (that is, more than or equal to values of 90% and less than or equal to values of 110% of Wx_k and Wy_k).
In the foregoing manner, the plurality of grid intervals Wx1, Wx2. Wx3, . . . , and Wy1, Wy2, Wy3, . . . in the X direction and the Y direction are set at values different from each other at random in the present embodiment. Then, using the grid intervals Wx1, Wx2, Wx3, . . . , and Wy1, Wy2. Wy3, . . . , an irregular rectangular grid (see
Then, the plurality of microlenses 21 are disposed on the X-Y plane using the above-described irregular rectangular grid as a reference, as shown in
In addition, the surface shape of each of the microlenses 21 in the initial disposition state is a shape obtained by cutting out a predetermined reference shape previously set (for example, an aspherical reference shape) with a rectangle corresponding to each of the microlenses 21. Herein, since the grid intervals Wx and Wy corresponding to the respective microlenses 21 are different from each other, the aperture sizes Dx, Dy and the surface shapes of the plurality of microlenses 21 are different from each other. In other words, by disposing the plurality of microlenses 21 using the above-described irregular rectangular grid as a reference, the plurality of microlenses 21 can be arranged such that the aperture sizes Dx, Dy and the surface shapes of the microlenses 21 are different from each other in the initial disposition state.
(2) First Varied Disposition State of the Microlenses 21 Obtained by Varying the Curvature Radii Rx and Ry (
By varying the curvature radii Rx and Ry of the microlenses 21 at random as shown in
The curvature radius R includes the curvature radius Rx of a sectional shape of the microlens 21 cut by a section in the X direction and the curvature radius Ry of a sectional shape of the microlens 21 cut by a section in the Y direction. In a case in which the surface shape of the microlens 21 is a spherical shape, Rx and Ry are the same value. On the other hand, in a case in which the surface shape of the microlens 21 is an aspherical shape having anisotropy, Rx and Ry may be different values.
The method of varying the curvature radii Rx and Ry of the microlenses 21 in the above-described initial disposition state at random is as follows, for example. First, constant reference values Rx_k and Ry_k (hereinafter referred to as reference curvature radii Rx_k and Ry_k) to be used as references for varying the curvature radii Rx and Ry in the X direction and the Y direction are set. Then, the reference curvature radii Rx_k and Ry_k are varied at random within ranges of predetermined varying rates δRx and δRy [%] to set the curvature radii Rx and Ry (Rx=Rx_k×(100±δRx [%]), Ry=Ry_k×(100±δRy [%])). This is repeated by the number of the respective microlenses 21 to respectively set curvature radii Rx11, Ry11, Rx21, Ry21, . . . , Rxnm, and Rynm in the X direction and the Y direction for the respective microlenses 21. Note that n indicates the number of the microlenses 21 disposed in the X direction, and m indicates the number of the microlenses 21 disposed in the Y direction.
Herein, the varying rates δRx and δRy preferably fall within the range of ±10% to ±50%. If the varying rates δRx and δRy are set to be less than ±10%, variations in the curvature radii Rx and Ry will be insufficient, which could make it difficult to provide the microlens array 20 with sufficient aperiodicity, and uniformity of diffused light through the microlens array 20 could be degraded. On the other hand, if the varying rates δRx and δRy are set to be more than ±50%, variations in the curvature radii Rx and Ry will become excessively large, which could make it difficult to continuously dispose the plurality of microlenses 21 on the X-Y plane with no gap.
In the foregoing manner, the curvature radii Rx and Ry of each of the microlenses 21 in the initial disposition state are varied at random (the first varied disposition state). As a result, the curvature radii Rx in the X direction of the microlenses 21 disposed in the X direction have values different from each other as shown in
In the first varied disposition state, the planar shapes of the respective microlenses 21 have shapes shifted from the rectangles as shown in
In this manner, in the first varied disposition state obtained by varying the curvature radii Rx and Ry of the microlenses 21 at random, the plurality of microlenses 21 can be arranged such that the aperture sizes Dx, Dy and the surface shapes of the microlenses 21 are further different from each other relative to those in the initial disposition state.
(3) Second Varied Disposition State of the Microlenses 21 Obtained by Varying Lens Vertex Positions (
After setting the first varied disposition state as described above, a second varied disposition state obtained by off-centering the planar positions of the vertices 22 of the microlenses 21 at random from the central points 23 of the above-described rectangles is set as shown in
A method of off-centering the planar positions of the vertices 22 of the microlenses 21 in the above-described first varied disposition state at random is as follows, for example.
First, an off-centering amount Ec of the planar position of the vertex 22 of the microlens 21 (which hereinafter may be referred to as a lens vertex position 22) is set. The off-centering amount Ec is a shift amount (distance) of the lens vertex position 22 from the central point 23 of the rectangle. The off-centering amount Ec is expressed by an off-centering amount Ecx in the X direction and an off-centering amount Ecy in the Y direction. The off-centering amount Ecx is a shift amount of the lens vertex position 22 in the X direction from the central point 23 of the rectangle, and the off-centering amount Ecy is a shift amount of the lens vertex position 22 in the Y direction from the central point 23 of the rectangle.
Then, off-centering rates δEcx and δEcy in the X direction and the Y direction are set. The off-centering rate δEcx in the X direction is a proportion (percentage) of the off-centering amount Ecx with respect to the grid interval Wx of the above-described rectangle. The off-centering rate δEcy in the Y direction is a proportion (percentage) of the off-centering amount Ecy with respect to the grid interval Wy of the above-described rectangle. The off-centering rates δEcx and δEcy are expressed by the following expressions.
δEcx[%]=Ecx/Wx×100
δEcy[%]=Ecy/Wy×100
Then, the lens vertex position is off-centered based on the off-centering rates δEcx and δEcy set as described above. Describing in detail, the lens vertex position 22 of each of the microlenses 21 is off-centered at random at the off-centering rates δEcx and δEcy within ±10% to ±50%.
Herein, the off-centering rates δEcx and δEcy preferably fall within the range of ±10% to ±50%. If the off-centering rates δEcx and δEcy are set to be less than ±10%, the off-centering amounts Ecx and Ecy of the lens vertex position 22 will be insufficient, which could make it difficult to provide the microlens array 20 with sufficient aperiodicity, and uniformity of diffused light in the X direction and the Y direction through the microlens array 20 could be degraded. On the other hand, if the off-centering rates δEcx and δEcy are set to be more than ±50%, the off-centering amounts Ecx and Ecy of the lens vertex will be excessively large, which could make it difficult to continuously dispose the plurality of microlenses 21 on the X-Y plane with no gap.
In the foregoing manner, the planar position of the vertex 22 of each of the microlenses 21 in the first varied disposition state is varied at random from the central point 23 of the rectangle (the second varied disposition state). As a result, as shown in
As a result, in the second varied disposition state, the planar shapes of the respective microlenses 21 have shapes shifted from the rectangular shapes corresponding to the rectangles further than in the above-described first varied disposition state (see
In this manner, in the second varied disposition state obtained by off-centering the planar positions of the vertices 22 of the microlenses 21 at random, the plurality of microlenses 21 can be arranged such that the surface shapes and the aperture sizes Dx, Dy of the microlenses 21 are different from each other further than in the first varied disposition state.
In addition, in the above-described second varied disposition state, the height positions of the vertices 22 of the plurality of microlenses 21 (the positions in the thickness direction of the diffuser plate 1) are varied from each other. Describing in detail, as shown in
In the foregoing manner, the method of arranging the microlenses 21 according to the present embodiment first disposes the plurality of microlenses 21 quasi-regularly using the irregular rectangular grid having the grid intervals Wx and Wy different from each other as a reference (the initial disposition state:
Thereafter, the curvature radii Rx and Ry, the surface shapes, and the lens vertex positions 22 of the plurality of microlenses 21 having been disposed are varied at random (the first and second varied disposition states:
Therefore, the microlens array 20 according to the present embodiment enables an overlapping state of phases of light emitted from the respective microlenses 21 to be controlled appropriately. This can appropriately reduce interference of diffused light from the respective microlenses 21 and diffraction due to a periodic structure of the microlens array. Thus, unevenness in intensity distribution of diffused light can be reduced to improve uniformity of light distribution in the X and Y directions orthogonal to each other. Furthermore, anisotropy of light distribution in the X and Y directions and a cut-off property of intensity distribution of diffused light can also be controlled.
Note that the cut-off property indicates that diffused light from the microlens array 20 has what is called a top hat diffusion property. The top hat diffusion property refers to an optical function that, with respect to collimated light in a visible light region or telecentric light having a principal ray with a collimating property and having a certain aperture, uniformity of energy distribution is very high within an angular component in a certain region, and if the certain region of this angular component is exceeded, energy may be reduced abruptly. When the top hat diffusion property is achieved, a luminance distribution of diffused light of light incident on the microlens array 20 becomes generally even within the range of predetermined diffusion angles, and within the range of the predetermined diffusion angles, a state is achieved in which a luminance value of diffused light falls within the range of ±20%, for example, centering on an average value of peak levels.
With the microlens array 20 according to the present embodiment, the plurality of microlenses 21 are disposed in the form of a rectangular grid by the above-described arrangement method, the curvature radii Rx, Ry, the lens vertex position 22, and the like of each of the microlenses 21 are controlled properly, and aspherical shapes are introduced into the surface shapes of the microlenses 21. This can achieve a desired diffusion property of the microlens array 20, so that the top hat diffusion property can be achieved more reliably.
Furthermore, according to the present embodiment, upon disposing the plurality of microlenses 21 quasi-regularly on the X-Y plane (the initial disposition state) using the irregular rectangular grid having the grid intervals Wx and Wy different from each other as a reference, the curvature radii Rx, Ry and the lens vertex positions 22 are varied (the first and second varied disposition states). This enables the plurality of microlenses 21 to be arranged continuously with no gap between each other on the surface of the diffuser plate 1 while ensuring randomness of the surface shapes of the respective microlenses 21. Therefore, a flat portion can be prevented from existing at the boundary portion between the microlenses 21 adjacent to each other, so that a component (0-th order transmitted light component) of incident light that is transmitted as it is without scattering on the surface of the diffuser plate can be reduced. As a result, uniformity of light distribution in the X and Y directions orthogonal to each other and diffusion performance can be improved further.
Examples in which the surface shapes of the microlenses 21 according to the present embodiment are aspherical shapes having anisotropy will now be described.
In the present embodiment, the plurality of microlenses 21 having anisotropy in a common direction may be disposed in the form of a rectangular grid all over the microlens array 20. The microlenses 21 having anisotropy are microlenses each having a planar shape whose length in one direction (longitudinal direction) is longer than the length in the other direction (shorter side direction) orthogonal to the one direction, for example. The plurality of microlenses 21 having anisotropy are disposed on the X-Y plane of the base material 10 such that the longitudinal direction of each of the microlenses 21 is directed to the same direction.
This enables an anisotropic shape of diffused light on a projection surface to be controlled. For example, on the diffuser plate 1, a diffusion width of light in the longitudinal direction of the microlenses 21 is reduced, and a diffusion width of light in the shorter side direction is increased. This enables the anisotropic shape of light diffused by the diffuser plate 1 to be controlled in accordance with the shape of the projection surface.
Hereinafter, a case in which the surface shapes (three-dimensional stereoscopic shapes) of the individual microlenses 21 are aspherical shapes having anisotropy will be described in more detail with reference to
(1) First Aspherical Shape Example (Anamorphic Shape)
First, an example of aspherical shapes (anamorphic shapes) of the microlenses 21 will be described with reference to
The microlenses 21 shown in
Herein, a method of setting the surface shape of the microlens 21 having the anamorphic shape will be described with reference to
Note that Expression 1 includes the following respective parameters.
Cx=1/Rx
Cy=1/Ry
As shown in
(2) Second Aspherical Shape Example (Toric Shape)
Another example of aspherical shapes (toric shapes) of the microlenses 21 will now be described with reference to
As shown in
As shown in
Herein, a method of setting the surface shape of the microlens 21 having the toric shape will be described with reference to
[Ex. 2]
Z=√{square root over ((R±√{square root over (r2−x2)})2−y2)} (2)
As shown in
Note that, as the surface shapes (aspherical shapes having anisotropy) of the microlenses 21 according to the present embodiment, aspherical shapes cut out from spheroids, for example, can be used besides the above-described first and second aspherical shape examples.
A method of designing microlenses according to the present embodiment will now be described with reference to
(S10) Setting of Grid Parameters
As shown in
Specifically, set values of the grid parameters can be set at the following numeric values, for example.
(S12) Production of Grid
Then, a plurality of rectangles disposed in the X and Y directions are produced on the basis of the grid parameters set in S10 (S12).
The grid intervals Wx in the X direction are set at values obtained by varying the reference grid interval Wx_k [μm] at random at the varying rate δWx [±%]. Similarly, the grid intervals Wy in the Y direction are set at values obtained by varying the reference grid interval Wy_k [μm] at random at the varying rate δWy [±%]. For example, in a case in which the set values of the grid parameters are numeric values in the above-described specific example (Wx_k=120 μm, δWx=±20%), the grid intervals Wx are set at random values within the range of 96 μm to 144 μm (values of 80% to 120% of 120 μm) centering on 120 μm (Wx_k). The grid intervals Wy are also set similarly. As a result, as shown in
(S14) Processing of Off-Centering Grid Center
Thereafter, off-centering processing of varying the position of a central point (hereinafter referred to as a “grid center”) of each of the rectangles at random is executed (S14).
As shown in
(S16 to S24) Production of Microlenses
Then, on the basis of the rectangles produced in S12 above and the grid centers off-centered in S14, the microlenses 21 corresponding to the respective rectangles are arranged. Specifically, a basic shape of the surface shapes (lens surfaces) of the microlenses 21 is selected first (S16). Then, parameters (lens parameters) concerning the selected basic shape are set (S18, S20). Thereafter, on the basis of the set lens parameters, the shape of the microlens 21 in each of the rectangles is determined, and a Z coordinate position representing the shape of the microlens 21 is computed to produce the microlens 21 (S22, S24).
Specifically, in the present embodiment, an anamorphic shape or a toric shape is selected, for example as the basic shape of the microlenses 21 (hereinafter referred to as a lens shape) (S16). However, this is not a limitation, and another type of aspherical shape or spherical shape may be selected as the lens shape.
In a case in which the anamorphic shape is selected in S16, various lens parameters concerning the anamorphic shape are set (S18). The lens parameters of the anamorphic shape include the following parameters, for example.
Specifically, set values of the lens parameters of the anamorphic shape can be set at the following numeric values, for example.
Then, on the basis of the lens parameters set in S18, the surface shape of the microlens 21 having the anamorphic shape is produced (S22). Describing in detail, on the basis of the lens parameters, the surface shape of each of the microlenses 21 is determined, and each of the microlenses 21 is disposed on each of the rectangles. In other words, the Z coordinate value of each point of the lens surface having the anamorphic shape is computed.
The curvature radius Rx in the X direction is set at a value obtained by varying the reference curvature radius Rx_k [μm] at random at the varying rate δRx [±%]. Similarly, the curvature radius Ry in the Y direction is set at a value obtained by varying the reference curvature radius Ry_k [μm] at random at the varying rate δRy [±%]. For example, in a case in which set values of the lens parameters are numeric values in the above-described specific example (Rx_k=240 μm, δRx=±10%), the curvature radius Rx is set at a random value within the range of 216 μm to 264 μm (a value of 90% to 110% of 240 μm) centering on 240 μm (Rx_k). The curvature radius Ry is also set similarly. As a result, as shown in
On the other hand, in a case in which the toric shape is selected in S16 above, various lens parameters concerning the toric shape are set (S20). The lens parameters of the toric shape include the following parameters, for example. Note that the smaller circle radius r and the larger circle radius R are curvature radii that define the toric shape shown in
Specifically, the set values of the lens parameters of the toric shape can be set at the following numeric values, for example.
Then, on the basis of the lens parameters set in S20, the surface shape of the microlens 21 having the toric shape is produced (S24). Describing in detail, the surface shape of each of the microlenses 21 is determined on the basis of the lens parameters, and each of the microlenses 21 is disposed on each of the rectangles. In other words, the Z coordinate value of each point of the lens surface having the toric shape is computed. The toric lens production processing in the present step S24 is similar to the anamorphic lens production processing in S22 above, and a detailed description is omitted.
(S26) Output of Lens Pattern
Thereafter, a lens pattern representing the shapes and arrangement of the microlenses 21 produced in S20 or S24 above is output (S26). For example, a file of XYZ coordinate values representing the lens pattern and an image file expressing the Z coordinate values of the lens pattern by grayscale gradation are output.
It is therefore appreciated that the plurality of microlenses 21 have aspherical shapes (for example, anamorphic shapes or toric shapes) different from each other. In addition, the plurality of microlenses 21 have planar shapes different from each other. The planar shapes of the respective microlenses 21 schematically have generally rectangular shapes along the above-described rectangles, but are shapes varied individually. The four side portions of the boundary line between the microlenses 21 are substantially composed of straight lines, whereas the four corner portions are composed of curves.
Furthermore, the plurality of microlenses 21 are arranged so as to overlap each other with no gap between each other, and a flat portion does not exist at the boundary portion between the microlenses 21 adjacent to each other.
In the foregoing manner, by the method of designing the microlenses 21 according to the present embodiment, the plurality of microlenses 21 are arranged quasi-regularly using the aforementioned irregular rectangular grid as a reference, and the respective varying elements (such as the grid intervals Wx, Wy, the curvature radii Rx, Ry, and the lens vertex position 22) of the microlenses 21 are varied at random. This can provide the respective microlenses 21 with diffusion properties different from each other while disposing a plurality of the microlens arrays 20 on the X-Y plane continuously with no gap between each other. The microlens array having such a configuration has various light distribution control properties in which variations in macroscopic light amount depending on the lens surface structure and changes in light amount due to diffracted light are small, and uniformity is high.
A method of manufacturing the diffuser plate 1 according to the present embodiment will now be described with reference to
As shown in
Then, a resist is formed on a surface of the base material after cleaning (step S103). For example, a resist layer can be formed of a resist through use of a metal oxide. Specifically, on the rolled base material, the resist layer can be formed by resist spray coating or dipping treatment. On the other hand, on the flat plate-like base material, the resist layer can be formed by performing various types of resist coating treatment. Note that, as the resist, a positive photoresist may be used, or a negative photoresist may be used. In addition, a coupling agent may be used to increase adhesion between the base material and the resist.
Furthermore, the resist layer is exposed using a pattern corresponding to the shape of the microlens array 20 (step S105). To the exposure processing, a publicly-known exposure method such as, for example, exposure through use of a grayscale mask, multi-exposure performed by overlaying a plurality of grayscale masks, or laser exposure through use of picosecond pulsed laser, femtosecond pulsed laser, or the like is applied as appropriate.
Thereafter, the resist layer after the exposure is developed (S107). A pattern is formed in the resist layer through this development processing. The development processing can be executed using a developing solution appropriate for the material of the resist layer. For example, in a case in which the resist layer is formed of a resist through use of a metal oxide, the resist layer can be subjected to alkaline development using an inorganic or organic alkaline solution.
Then, by performing sputtering treatment or etching treatment using the resist layer after development (S109), a master original, in a surface of which the shape of the microlens array 20 has been formed, is completed (S111). Specifically, a glass base material is subjected to glass etching using the resist layer on which a pattern has been formed as a mask, so that a glass master can be manufactured. Alternatively, the resist layer on which a pattern has been formed is subjected to Ni sputtering or nickel plating (NED treatment) to form a nickel laver to which the pattern has been transferred, and then the base material is separated, so that a metal master can be manufactured. For example, the metal master original can be manufactured by forming a nickel layer to which the resist pattern has been transferred through Ni sputtering to a film thickness of approximately 50 nm, nickel plating (for example, nickel sulfamate bath) to a film thickness of 100 μm to 200 μm, or the like.
Furthermore, by transferring (imprinting) the pattern to a resin film or the like using the master original (for example, the glass master original or the metal master original) completed in S111 above, a soft mold, in a surface of which an inverted shape of the microlens array 20 has been formed, is created (S113).
Thereafter, by transferring the pattern of the microlens array 20 to the glass substrate, the film base material, or the like using the soft mold (S115), and further depositing a protective film, an anti-reflective film, or the like according to necessity (S117), the diffuser plate 1 according to the present embodiment is manufactured.
Note that the foregoing has described the example of manufacturing the soft mold (S113) using the master original (S111), and then manufacturing the diffuser plate 1 through transfer using the soft mold (S115). However, this is not a limitation, and a master original (for example, an inorganic glass original) in which an inverted shape of the microlens array 20 has been formed may be manufactured, and the diffuser plate 1 may be manufactured through imprinting using the master original. The diffuser plate 1 can be manufactured by, for example, applying a light curing acrylic resin to a base material made of PET (PolyEthylene Terephthalate) or PC (PolyCarbonate), transferring the pattern of the master original to the applied light curing acrylic resin, and UV curing the light curing acrylic resin.
On the other hand, in a case of directly processing a glass base material itself to manufacture the diffuser plate 1, the diffuser plate 1 according to the present embodiment is manufactured by, subsequent to the development processing in step S107, subjecting the base material 10 to dry etching treatment using a publicly known compound such as CF4 (S119), and thereafter depositing a protective film, an anti-reflective film, or the like according to necessity (S121).
Note that the manufacturing method shown in
Application examples of the diffuser plate 1 according to the present embodiment will now be described.
The diffuser plate 1 as described above can be mounted as appropriate on a device that needs to diffuse light in order to achieve its functions. Examples of such a device can include a display device such as various displays (for example, an LED and organic EL display), a projecting device such as a projector, and various lighting devices.
For example, the diffuser plate 1 is also applicable to a backlight of a liquid crystal display device, a diffuser plate-integrated lens, and the like, and also applicable to light shaping applications. In addition, the diffuser plate 1 is also applicable to a transmissive screen of a projecting device, a Fresnel lens, a reflective screen, and the like. In addition, the diffuser plate 1 is also applicable to various lighting devices to be utilized for spot illumination, base illumination, and the like, various specialized lightings, various screens such as an intermediate screen and a final screen, and the like. Furthermore, the diffuser plate 1 is also applicable to applications such as control over diffusion of light source light in an optical device, and can also be applied to light distribution control in an LED light source device, light distribution control in a laser light source device, distribution control over incident light to various light valve systems, and the like.
Note that devices to which the diffuser plate 1 is applied are not limited to the above-described application examples, but the diffuser plate 1 is also applicable to any publicly-known device that utilizes distribution of light.
Diffuser plates according to examples of the present invention will now be described. Note that the following examples are mere examples for indicating the effects and practicability of the diffuser plate according to the present invention, and the present invention is not limited to the following examples.
Diffuser plates according to the examples and comparative examples were manufactured by a manufacturing method which will be described below with the surface structure of the microlens array changed.
Specifically, a glass base material was cleaned first, and then, a photoresist was applied to one surface (a principal surface) of the glass base material to a resist thickness of 2 μm to 15 μm. As the photoresist, a positive photoresist such as, for example, PMER-LA900 (made by TOKYO OHKA KOGYO CO., LTD.) or AZ4620 (registered trademark) (made by AZ Electronic Materials) was used.
Next, a pattern was drawn on the resist on the glass base material with a laser drawing device through use of laser having a wavelength of 405 nm, and the resist layer was exposed. Note that the resist layer may be exposed by subjecting the resist on the glass base material to mask exposure with a stepper exposure device through use of g-line.
Subsequently, the resist layer was developed to form a pattern on the resist. As a developing solution, a tetramethylammonium hydroxide (TMAH) solution such as, for example, NMD-W (made by TOKYO OHKA KOGYO CO., LTD.) or PMER P7G (made by TOKYO OHKA KOGYO CO., LTD.) was used.
Next, the glass base material was etched using the resist on which the pattern had been formed to manufacture a diffuser plate. Specifically, the resist pattern was formed on the glass base material by glass etching through use of Ar gas or CF4 gas to manufacture a diffuser plate.
Table 1 relates to diffuser plates according to the examples and comparative examples manufactured as described above, and shows designing conditions for the surface structures of the microlens arrays and evaluation results of uniformity of light distribution achieved by the diffuser plates.
In each of the examples and comparative examples shown in Table 1, a microlens array was designed by the aforementioned designing method shown in
As shown in Table 1, in Examples 1 to 9, the grid intervals Wx and Wy of each of the microlenses were varied at random when designing the surface structure of the microlens array. In contrast, in Comparative Examples 1 to 4, the grid intervals of all the microlenses were set at the constant reference grid intervals Wx_k and Wy_k without varying the grid intervals Wx and Wy.
In addition, the curvature radius Rx and the curvature radius Ry were set at fixed values or random varying values in each of the examples and comparative examples, as shown in Table 1. It means that, in the case in which the varying rates δRx and δRy=±0%, the curvature radii Rx and Ry of each of the microlenses were set at fixed values without being varied, and in the case in which the varying rates δRx and δRy=±10% and ±15%, the curvature radii Rx and Ry were varied at random within the ranges of the varying rates δRx and Ry. In addition, off-centering of the lens vertex position on the X-Y plane means that, in the case in which the off-centering rates δEcx and δEcy=±0%, the lens vertex position was not off-centered, and in the case in which the off-centering rates δEcx and δEcy=±10% and ±15%, the lens vertex position was off-centered at random within the ranges of the off-centering rates δEcx and δEcy.
In addition, the surface shapes of the microlenses had spherical shapes in Examples 1 to 4, 8, 9 and Comparative Examples 1 to 3, and had aspherical shapes (for example, anamorphic shapes) in Examples 5 to 7. In addition, the planar shapes of the microlens arrays were square in Examples 1 to 7 and Comparative Examples 1 to 3, and were rectangular (rectangular shape longer in the X direction) in Examples 8, 9 and Comparative Example 4.
The surface shapes of the microlens arrays of the diffuser plates according to Examples 1 to 9 and Comparative Examples 1 to 4 manufactured as described above were observed with a laser microscope. Furthermore, a light distribution pattern of each of the diffuser plates was simulated with Virtual-Lab (made by LightTrans GmbH), and a light distribution property of each of the diffuser plates was measured with a light distribution property measuring instrument, Mini-Diff (made by Light Tec). In addition, in order to measure the light distribution properties of the diffuser plates, an intensity distribution of diffused light was measured from captured images of laser light intensity (far-field pattern measurement which will be described later).
Simulation results and actual measurement results of patterns of the surface shapes of the microlens arrays, light distribution properties of diffused light, luminance distributions, and the like of the diffuser plates according to Examples 1 to 9 and Comparative Examples 1 to 4 are shown in
In
In addition, in
In addition, in
The light distribution properties (such as uniformity of light distribution) of the diffuser plates according to Examples 1 to 9 and Comparative Examples 1 to 3 as described above were evaluated on three scales (grades A, B, and C) according to the following evaluation criteria. Such evaluation results are shown in Table 1.
Evaluation results of Examples 1 to 9 and Comparative Examples 1 to 4 will be described below in comparison.
(1) Comparison Between Examples 1 to 9 and Comparative Examples 1 to 4 (Effects of Irregularity of Grid Intervals)
In Comparative Examples 1 to 4, the luminance significantly increased and decreased periodically in the luminance distribution of diffused light, and unevenness in the form of a rectangular grid occurred in the luminance distribution of diffused light as shown in
In Comparative Examples 1 to 4, the rectangular grid to be used as a reference of disposition of the microlenses was a regular rectangular grid, and the grid intervals in the X and Y directions were fixed at the constant values Wx_k and Wy_k (δWx and δWy=±0%). It is therefore considered that the periodic structure of microlens disposition in the form of the regular rectangular grid caused diffraction in diffused light from each of the microlenses, so that unevenness occurred in the luminance distribution, and the uniformity of light distribution was degraded.
In this respect, off-centering the lens vertex position as in Comparative Example 2 or varying the curvature radii Rx and Ry at random as in Comparative Example 3 allowed the uniformity of luminance distribution to be improved to some degree. However, it is considered that, in the case in which the grid intervals Wx and Wy were constant as in Comparative Examples 1 to 4, luminance unevenness caused by diffraction resulting from the periodicity of the grid intervals exceeded the effect of improving the uniformity by varying the lens vertex positions and the curvature radii Rx and Ry, which interfered with the uniformity of light distribution.
In contrast, in Examples 1 to 9, the luminance varied in the luminance distribution of diffused light, but periodic increase/decrease or periodic peaks were not observed, so that unevenness in the luminance distribution of diffused light was sufficiently reduced, and the uniformity of light distribution of diffused light was excellent. The reason is considered as follows.
In Examples 1 to 9, microlenses were disposed on the X-Y plane using the rectangular grid as a reference. Herein, the rectangular grids of Examples 1 to 9 were not regular rectangular grids as in the comparative examples, but were quasi-regular rectangular grids having irregularity in the grid intervals Wx and Wy. In other words, as shown in
As a result, as shown in
The above results reveal that the use of the diffuser plate of the present invention can reduce unevenness in the luminance distribution in the two directions orthogonal to each other (the X and Y directions) to sufficiently improve the uniformity of light distribution.
(2) Comparison Between Example 1 and Examples 2 to 9 (Effects of Varying Curvature Radii and Off-Centering Lens Vertices)
As shown in Table 1, only the grid intervals Wx and Wy were varied in Example 1. In contrast, in Examples 2 to 9, the curvature radii Rx and Ry were varied in addition to the grid intervals Wx and Wy, and the lens vertex positions were off-centered.
As a result, Examples 2 to 9 (grade A) were able to reduce unevenness in the luminance distribution more effectively than in Example 1 (grade B) to improve the uniformity of light distribution of diffused light. This reveals that, from the perspective of improvement of the uniformity of light distribution, varying the curvature radii Rx and Ry in addition to the grid intervals Wx and Wy and off-centering the lens vertex positions are effective.
Furthermore, in Examples 2, 3, and 5, the curvature radii Rx and Ry were vaned, or the lens vertex positions were off-centered. In contrast, in Examples 4 and 6 to 9, the curvature radii Rx and Ry were varied, and the lens vertex positions were also off-centered. As a result, Examples 4 and 6 to 9 were able to reduce unevenness in the luminance distribution further to improve the uniformity of light distribution of diffused light further, as shown in the electromagnetic field analysis images at (b) and the graphs of luminance distribution at (c) in
(3) Comparison Between Examples 1 to 4 and Examples 5 to 7 (Effects of Aspherical Lens Shape)
As shown in Table 1, spherical lenses were used in Examples 1 to 4 as the basic shape of microlenses. In contrast, aspherical lenses (for example, the anamorphic lenses shown in
As a result, as shown in the electromagnetic field analysis images at (b) and the graphs of luminance distribution at (c) in
(4) Diffusion Properties of Example 7 (Excellent Light Distribution Uniformity and Cut-Off Property)
As shown in Table 1, in Example 7, the reference curvature radii Rx_k and Ry_k were set at a relatively large value (150 μm), and the curvature radii Rx and Ry were varied within the ranges of ±10% of Rx_k and Ry_k, and the lens vertex positions were off-centered within the range of the off-centering rates δEcx and δEcy=±10%.
Furthermore, the surface shapes of the microlenses in Example 7 were aspherical shapes in which the ratio between the reference curvature radii Rx_k, Ry_k [μm] and the reference grid intervals Wx_k, Wy_k [μm] satisfied relational expressions (A) and (B) below. In Example 7, (Rx_k/Wx_k)=(Ry_k/Wy_k)=(150/80)=1.875.
Rx_k/Wx_k≥1.85 (A)
Ry_k/Wy_k≥1.85 (B)
The surface shapes of the microlenses according to Example 7 were aspherical shapes having anisotropy as described above, and the grid intervals Wx, Wy, and the curvature radii Rx, Ry were varied, and the lens vertex positions were off-centered under the conditions shown in Table 1, and the reference curvature radii Rx_k, Ry_k [μm] and the reference grid intervals Wx_k, Wy_k [μm] were adjusted so as to satisfy the relational expressions (A) and (B) above. Furthermore, the diffusion angle (full width at half maximum (FWHM)) of diffused light output from the diffuser plate fell within a range of less than or equal to 20°. This enabled what is called the top hat diffusion property to be achieved more reliably.
As shown in the graph of FFP measurement result in
The above results reveal that the use of a diffuser plate similar to that of Example 7 above enables, within the range in which the diffusion angle (full width at half maximum) is less than or equal to 20°, anisotropy of light distribution in the X and Y directions and the cut-off property of intensity distribution of diffused light to be controlled properly while sufficiently improving uniformity of light distribution in the two directions (the X and Y directions) orthogonal to each other.
(7) Comparison Between Examples 8, 9 and Comparative Example 4 (Effects of Rectangular Aspherical Lens Shape)
For the diffuser plates according to Examples 8, 9 and Comparative Example 4, rectangular microlens arrays extending long in the X direction were used. The reference grid intervals Wx_k=50 μm, Wy_k=40 μm, and the reference grid interval Wx_k in the longitudinal direction (the X direction) of the microlens arrays was set to be larger than the reference grid interval Wy_k in the shorter side direction (the Y direction) (Wx_k>Wy_k).
In the rectangular microlens arrays, the grid intervals Wx and Wy were not varied in Comparative Example 4. On the other hand, in Examples 8 and 9, the grid intervals Wx and Wy were varied at random within the range of ±10% or ±15%, and the curvature radii Rx and Ry were vaned at random within the range of ±10% or ±15%. Furthermore, in Examples 8 and 9, the lens vertex positions were also off-centered at random within the range of ±10% or ±15%.
As a result, in Comparative Example 4, the luminance distribution of diffused light significantly increased and decreased periodically, unevenness in the form of a rectangular grid occurred remarkably, and the uniformity of light distribution of diffused light was insufficient, as shown in
The above results reveal that, even in a case of using a rectangular microlens array as in Examples 8 and 9, uniformity of light distribution can be improved sufficiently in the two directions (the X and Y directions) orthogonal to each other.
The preferred embodiment(s) of the present invention has/have been described above with reference to the accompanying drawings, whilst the present invention is not limited to the above examples. A person skilled in the art may find various alterations or modifications within the scope of the appended claims, and it should be understood that they will naturally come under the technical scope of the present invention.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2019-194363 | Oct 2019 | JP | national |
| 2020-175853 | Oct 2020 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2020/039657 | 10/22/2020 | WO |
