The present disclosure relates to a diffractive optical element, an optical apparatus, a display apparatus, and an imaging apparatus.
Hitherto, there has been known a method of reducing chromatic aberration of a lens system by providing, in a part of an optical system, a diffractive optical element having a diffractive action. In addition to correction of the chromatic aberration, the diffractive optical element has been known to exhibit an effect as an aspherical surface by appropriately changing a grating pitch of its periodical structure.
Further, it is known that, in the diffractive optical element used as the lens of the optical system, when two diffraction gratings are arranged in close contact with each other and a material forming each diffraction grating and a grating height thereof are appropriately set, a high diffraction efficiency can be obtained in a wide wavelength band.
In International Publication No. WO2012/176388, there is described a diffractive optical element including: a body being formed of a first optical material and having a diffraction grating on a surface thereof, and an optical adjustment layer being formed of a second optical material and provided on the body so as to cover the diffraction grating. In the diffractive optical element described in International Publication No. WO2012/176388, the optical adjustment layer formed of the second optical material including a resin has a uniform thickness in a normal direction from an envelope, which is a curved surface passing through an edge of the diffraction grating. In this manner, in the diffractive optical element described in International Publication No. WO2012/176388, cracks are prevented from being caused by stress acting on the optical adjustment layer due to curing shrinkage of the second optical material during manufacture or the like.
In International Publication No. WO2012/176388, there is disclosed a technology of forming the optical adjustment layer which is a resin layer on the body to have a constant thickness so that cracks are prevented from being caused due to local concentration of stress on the optical adjustment layer at the time of curing shrinkage. However, when the body has an arc shape as that obtained by cutting a part of a circular lens shape, in plan view as viewed in an optical axis direction, the diffraction grating on the body has a circular shape on the inner side, but has an arc shape on the outer side. The diffraction grating having an arc shape has a different shrinkage behavior at the time of curing of the resin formed on the diffraction grating, as compared to that in the case of only the diffraction grating having a circular shape. Accordingly, in the case of the diffractive optical element in which the diffraction grating having a circular shape and the diffraction grating having an arc shape are provided on the body, even when the thickness of the resin layer on the body is kept constant as in the technology disclosed in International Publication No. WO2012/176388, reduction in the diffraction efficiency is caused due to a density difference of the resin layer, and thus an optical characteristic is liable to deteriorate.
The present disclosure has an object to provide a diffractive optical element with which deterioration of an optical characteristic can be reduced or prevented when, in plan view, a diffraction grating having a circular shape and a diffraction grating having an arc shape are provided.
According to one aspect of the present disclosure, there is provided a diffractive optical element including: a substrate having a surface on which a diffraction grating is provided; and a resin layer provided on the surface of the substrate so as to cover the diffraction grating, wherein, in plan view as viewed along an optical axis direction, the diffraction grating includes: a first diffraction grating having a circular shape; and a second diffraction grating having an arc shape, the second diffraction grating being arranged on an outer side of the first diffraction grating, wherein the diffractive optical element includes an optical effective region and a non-optical effective region surrounding the optical effective region, wherein the second diffraction grating has an arc end positioned in the non-optical effective region, and wherein a thickness of the resin layer provided in the non-optical effective region is larger than a thickness of the resin layer provided in the optical effective region.
According to another aspect of the present disclosure, there is provided a diffractive optical element including: a substrate having a surface on which a diffraction grating is provided; and a resin layer provided on the surface of the substrate so as to cover the diffraction grating, wherein, in plan view as viewed along an optical axis direction, the diffraction grating includes: a first diffraction grating having a circular shape; and a second diffraction grating having an arc shape, the second diffraction grating being arranged on an outer side of the first diffraction grating, wherein the diffractive optical element includes a first region in which the diffraction grating is provided and a second region in which the diffraction grating is not provided, the second region being arranged on an outer side of the first region, and wherein the diffractive optical element includes a region in which a first gradient in which a thickness of the resin layer increases toward an outer side from a center of a circle of the diffraction grating is 0.4 or more, in a third region including a boundary between the first region and the second region on a side on which the diffraction grating is discontinuous.
Further features of the present disclosure will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
A diffractive optical element according to one embodiment of the present disclosure and a method of manufacturing the diffractive optical element are described with reference to
First, a configuration of the diffractive optical element according to the first embodiment is described with reference to
The diffractive optical element 10 according to the first embodiment includes, as illustrated in
The substrate 11 is, for example, a convex-lens-shaped substrate, and may be a resin substrate formed by injection molding, or a glass substrate. The shape of the substrate 11 may be a concave lens shape other than the convex lens shape, or may be a convex spherical surface shape, a concave spherical surface shape, an aspherical surface shape, a planar shape, or other shapes. Further, a material forming the substrate 11 is not particularly limited as long as the material is a transparent material having transmittance with respect to light such as visible light which is a target of the diffractive optical element 10.
The term “transparent” means that, for example, the transmittance of light having a wavelength range of from 420 nm or more to 700 nm or less is 10% or more.
In plan view as viewed in the optical axis direction of the diffractive optical element 10, the substrate 11 has a planar shape including a segmental circular shape and a rectangular shape. The segmental circular shape is a shape enclosed between an arc and a chord connecting both ends of this arc to each other. The rectangular shape is coupled to this segmental circular shape. The segmental circular shape of the substrate 11 is a shape enclosed between a major arc having a central angle of more than 180° and a chord connecting both ends of this major arc to each other. The center of the circle of the segmental circular shape is an optical center of the diffractive optical element 10. The rectangular shape coupled to the segmental circular shape of the substrate 11 has the chord of the segmental circular shape as its longitudinal side. The substrate 11 includes a first portion 111 having a planer shape of the segmental circular shape, and a second portion 112 having a planer shape of the rectangular shape. The first portion 111 has a shape obtained by cutting a shape such as the above-mentioned lens shape along the optical axis direction at a position of the chord. The second portion 112 has a plate-like shape projecting from a middle of a cut portion at the position of the chord of the first portion 111. The shape including the planar shape of the substrate 11 is not limited to the shape illustrated in
The diffractive optical element 10 including the substrate 11 includes an optical effective region 14 and a non-optical effective region 15. The optical effective region 14 is a region within an optical effective diameter. The non-optical effective region 15 surrounds the optical effective region 14 in a region outside of the optical effective diameter. The optical effective region 14 is a region through which light being the target of the diffractive optical element 10 passes, and the non-optical effective region 15 is a region outside of the optical effective region 14. The non-optical effective region 15 includes an arc portion 113 and a chord portion 114. The arc portion 113 is an end portion of the first portion 111 on the arc side, and the chord portion 114 is formed of the second portion 112 and an end portion of the first portion 111 on the chord side.
The diffraction grating 13 is formed concentrically on one surface of the first portion 111 having a planar shape of the segmental circular shape of the substrate 11, with the center of the circle of the segmental circular shape through which the optical axis of the diffractive optical element 10 passes serving as a center. For example, the diffraction grating 13 is formed so that a slope surface and a wall surface are successively repeated toward an outer periphery from an element center through which the optical axis passes (see
The first portion 111 of the substrate 11 has a planar shape of the segmental circular shape, and hence the diffraction grating 13 includes a diffraction grating 13a having a circular shape on the inner side of the substrate 11, and a diffraction grating 13b having an arc shape on the outer side of the substrate 11. The diffraction grating 13b on the outer side of the substrate 11 is disconnected at an end of the chord portion 114 of the first portion 111 of the substrate 11, and hence has an arc shape. An arc end of the diffraction grating 13b having the arc shape is positioned at the chord portion 114 which is the non-optical effective region 15.
The resin layer 12 is provided on one surface of the first portion 111 and one surface of the second portion 112 of the substrate 11 so as to cover the diffraction grating 13. The resin forming the resin layer 12 is not particularly limited as long as the resin is a transparent resin having transmittance with respect to light such as visible light which is the target of the diffractive optical element 10, but it is preferred that the resin be a photocurable resin or a thermosetting resin from the viewpoint of easiness in manufacture.
As illustrated in
As illustrated in
With the transparent inorganic film 17 being provided, when the substrate 11 is made of a resin, penetration or dissolution of the resin material between the substrate 11 and the resin layer 12 can be reduced or prevented, and thus the deterioration of the diffraction efficiency can be reduced or prevented. Moreover, the transparent inorganic film 17 may be provided so that the thickness of the transparent inorganic film 17 at a grating edge of the diffraction grating 13 is larger than the thickness of the transparent inorganic film in the grating surface other than the grating edge of the diffraction grating 13. In this manner, while the initial influence of the transparent inorganic film on the optical performance is suppressed to be small, the deterioration of the diffraction efficiency due to penetration or dissolution of the resin material at the grating edge of the diffraction grating 13 can be reduced or prevented.
The resin layer 12 is provided so that, in the optical effective region 14 which is a region within the optical effective diameter, the resin layer 12 has substantially the same thickness “tc” with respect to an envelope which is a surface passing through an edge of the diffraction grating 13. Meanwhile, the resin layer 12 is provided so that, in the non-optical effective region 15 which is a region outside of the optical effective diameter, the resin layer 12 has a thickness larger than the thickness “tc” in the optical effective region 14.
Specifically, in the chord portion 114 in the non-optical effective region 15, the resin layer 12 is provided to have a thickness t1 larger than the thickness “tc”. Further, in the arc portion 113 in the non-optical effective region 15, the resin layer 12 is provided to have a thickness t2 larger than the thickness “tc”.
The thickness “tc” can be regarded as an average thickness of the resin layer 12 provided in the optical effective region 14 from the envelope of the diffraction grating 13. Further, the thickness t1 can be regarded as an average thickness of the resin layer 12 provided in the chord portion 114 in the non-optical effective region 15. Further, the thickness t2 can be regarded as an average thickness of the resin layer 12 provided in the arc portion 113 in the non-optical effective region 15. The thickness of the resin layer 12 can be measured through use of a shape measuring machine or the like. The thickness of the resin layer 12 can be obtained by taking a difference between a measured value of the surface shape of the diffractive optical element 10 obtained by the shape measuring machine or the like and the shape of the substrate 11.
The thicknesses t1 and t2 of the resin layer 12 provided in the non-optical effective region 15 are larger than the thickness “tc” of the resin layer 12 provided in the optical effective region 14 as described above so that, in consideration of shrinkage at the time of curing of the resin forming the resin layer 12, a density difference of the resin caused by the curing is suppressed to be small.
The phenomenon in which the density difference of the resin is caused by curing is described with reference to
When the diffractive optical element 10 according to the first embodiment is manufactured, first, as illustrated in
In
Further,
In the manufacturing method described above as illustrated in
In the diffractive optical element 10 according to the first embodiment, the thickness of the resin layer 12 provided in the non-optical effective region 15 outside of the optical effective diameter is larger than the thickness of the resin layer 12 provided in the optical effective region 14. Accordingly, in the first embodiment, the mold 21 for providing the resin layer 12 is a mold that allows the resin layer 12 to be provided thick in the non-optical effective region 15. Thus, as illustrated in
In this manner, in the first embodiment, the shrinkage of the resin 121 is reduced. Thus, occurrence of a refractive index difference due to the density difference of the resin layer 12 formed of the resin 121 can be suppressed or prevented, and thus reduction in the diffraction efficiency of the resin layer 12 can be suppressed to be small or prevented.
The shrinkage of the resin 121 in the chord portion 114 tends to be larger than the shrinkage of the resin 121 in the arc portion 113. Accordingly, it is preferred that the thickness t1 of the resin layer 12 provided in the chord portion 114 in the non-optical effective region 15 be larger than the thickness t2 of the resin layer 12 provided in the arc portion 113 in the non-optical effective region 15, that is, t1>t2 be satisfied.
Further, when the thickness t1 is excessively increased, there is a fear in that large curing stress may be generated in the thickness direction during a process at the time of curing of the resin 121, which may cause deformation of the diffractive optical element 10. The length from the optical center to the end portion of the substrate 11 is shorter in the chord portion 114 than in the arc portion 113. Accordingly, the substrate 11 has more advantage with respect to deformation in the chord portion 114 than in the arc portion 113, but it is preferred that the thickness t1 be kept to be no more than three times the thickness t2, that is, t1/t2<3 be satisfied.
Further, when a width of the resin layer 12 provided in the chord portion 114 is represented by w1, and a width of the resin layer 12 provided in the arc portion 113 is represented by w2, in consideration of also those widths together with the above-mentioned viewpoint, it is preferred that 1<(t1×w1)/(t2×w2)<3 be satisfied. The width w1 and the width w2 can each be an average value.
Further, when a grating height of the diffraction grating 13 is represented by “d”, it is preferred that 3<(t1−tc)/d<80 be satisfied. The grating height “d” is a height from a boundary between the protruding portion and the base of the diffraction grating 13 to a distal end of the protruding portion of the diffraction grating 13. The grating height “d” can be an average value of the diffraction grating 13 provided on the substrate 11.
Further, when the thickness t1 is excessively increased with respect to the thickness of the resin layer 12 at the center of the diffractive optical element 10, the diffractive optical element 10 is assumed to become thick and heavy. Accordingly, it is preferred that the thickness t1 be 1,000 μm or less.
As described above, according to the first embodiment, when the diffraction grating 13a having the circular shape and the diffraction grating 13b having the arc shape are provided, the deterioration of the optical characteristic of the diffractive optical element 10 can be reduced or prevented. The optical characteristic of the diffractive optical element 10 can be evaluated by measuring, as initial evaluation, the diffraction efficiency in a desired wavelength region such as a wavelength region of, for example, from 420 nm to 700 nm. In this case, for example, when the change of the diffraction efficiency is 2% or less as compared to the design value, there is no significant influence on the optical characteristic, and hence the optical characteristic can be evaluated as being good.
A diffractive optical element according to a second embodiment of the present disclosure is described with reference to
The diffractive optical element 10 according to the second embodiment is substantially similar to the configuration of the first embodiment. The diffractive optical element 10 according to the second embodiment is different from the configuration of the first embodiment in that the substrate 11 is formed of only the first portion 111 and includes no second portion 112.
In the second embodiment, the chord portion 114 does not include the second portion 112. In this chord portion 114, the resin layer 12 is provided so as to project to the outer side of the first portion 111.
As in the second embodiment, the substrate 11 is not always required to include the first portion 111 and the second portion 112, and may be formed of only the first portion 111. In the second embodiment, a distance r2 from the optical center of the resin layer 12 to an end portion of the resin layer 12 on the chord portion 114 side is longer than a distance r1 from the optical center of the substrate 11 to the chord portion 114, and r1<r2 is satisfied. When the substrate 11 has no second portion 112 for supporting the resin layer 12 in the chord portion 114 as described above, a further downsized and lightweight diffractive optical element 10 can be provided.
Next, the diffractive optical element according to each of the above-mentioned embodiments and the method of manufacturing the diffractive optical element are specifically described with reference to Examples.
A diffractive optical element according to Example 1 and a method of manufacturing the diffractive optical element are described with reference to
In Example 1, first, as the substrate 11, a substrate obtained by molding a polycarbonate-based resin material (EP4500, produced by MITSUBISHI GAS CHEMICAL COMPANY, INC.) by injection molding was prepared. The substrate 11 had an outer diameter of φ46 mm, an optical effective diameter of φ42 mm, and a center thickness of 2.5 mm. One surface of the substrate 11 had a convex shape, and the other surface thereof was a flat surface. The diffraction grating 13 having a grating height of 10 μm was provided on the other surface of the substrate 11. This diffraction grating 13 was arranged concentrically with respect to an outer diameter center of the substrate 11, and its grating interval was reduced toward the outer periphery from the center. In plan view as viewed in the optical axis direction, the substrate 11 had the first portion 111 having the segmental circular shape, and the outer-peripheral diffraction grating 13b was cut in the chord portion 114 at a position of 16 mm from the center. On the outer side of the chord portion 114 of the first portion 111 in the substrate 11, the flat second portion 112 having a width of 2.0 mm and a thickness of 2.0 mm was provided.
Next, through the steps illustrated in
The diffractive optical element 10 according to Example 1 manufactured as described above was subjected to shape measurement after release from the mold 21. The shape measurement used a surface shape/roughness measuring machine, Form Talysurf (manufactured by Taylor Hobson). In order to measure the thickness of the resin layer 12, the surface shape of the diffractive optical element 10 on the resin layer 12 side was measured at least at three positions from the optical axis center to the end portion in the chord portion and other regions.
When the thickness t1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the thicknesses t1 at the three positions were 450 μm, 350 μm, and 410 μm, and an average value of those values was about 400 μm. Further, when the width w1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the widths w1 at the three positions were 1.1 mm, 0.9 mm, and 1.05 mm, and an average value of those values was about 1.0 mm. Meanwhile, when the thickness t2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the thicknesses t2 at the three positions were 150 μm, 210 μm, and 230 μm, and an average value of those values was about 200 μm. Further, when the width w2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the widths w2 at the three positions were 0.8 mm, 1.1 mm, and 1.2 mm, and an average value of those values was about 1.0 mm. When the thickness “tc” of the resin layer 12 in the optical effective region 14 was similarly measured, the average value of the thickness “tc” was 100 μm.
As the initial evaluation of the diffractive optical element 10 according to Example 1, the diffraction efficiency in a wavelength range of from 420 nm to 700 nm was measured. In the initial evaluation, when the change of the diffraction efficiency was 2% or less as compared to the design value, there was no significant influence on the optical performance, and hence the diffraction efficiency was evaluated as being good. As a result, as shown in Table 1, it was confirmed that the diffraction efficiency was good.
In Example 2, the same substrate as that of Example 1 was used as the substrate 11. Further, in Example 2, the shape of the mold 21 was changed to a shape in which the thickness of the resin layer 12 in the non-optical effective region 15 became larger by 300 μm than the thickness of the resin layer 12 in the optical effective region 14 in both of the arc portion 113 and the chord portion 114. The other points were similar to those of Example 1. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 2 was also subjected to shape measurement after mold release, similarly to Example 1. When the thickness t1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the thicknesses t1 at the three positions were 300 μm, 510 μm, and 400 μm, and an average value of those values was about 400 μm. Further, when the width w1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the widths w1 at the three positions were 0.45 mm, 0.55 mm, and 0.52 mm, and an average value of those values was about 0.5 mm. Meanwhile, when the thickness t2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the thicknesses t2 at the three positions were 420 μm, 350 μm, and 440 μm, and an average value of those values was about 400 μm. Further, when the width w2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the widths w2 at the three positions were 0.49 mm, 0.53 mm, and 0.47 mm, and an average value of those values was about 0.5 mm. When the thickness “tc” of the resin layer 12 in the optical effective region 14 was similarly measured, the average value of the thickness “tc” was 100 μm.
As the initial evaluation of the diffractive optical element 10 according to Example 2, similarly to Example 1, the diffraction efficiency was measured and evaluated. Thus, as shown in Table 1, it was confirmed that the diffraction efficiency was good.
In Example 3, the same substrate as that of Example 1 was used as the substrate 11. Further, in Example 3, the shape of the mold 21 was changed to a shape in which the thickness of the resin layer 12 in the non-optical effective region 15 became larger by 200 μm in the arc portion 113 and larger by 700 μm in the chord portion 114 than the thickness of the resin layer 12 in the optical effective region 14. The other points were similar to those of Example 1. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 3 was also subjected to shape measurement after mold release, similarly to Example 1. When the thickness t1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the thicknesses t1 at the three positions were 610 μm, 910 μm, and 870 μm, and an average value of those values was about 800 am. Further, when the width w1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the widths w1 at the three positions were 0.095 mm, 0.11 mm, and 0.09 mm, and an average value of those values was about 0.1 mm. Meanwhile, when the thickness t2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the thicknesses t2 at the three positions were 370 μm, 240 μm, and 300 μm, and an average value of those values was about 300 μm. Further, when the width w2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the widths w2 at the three positions were 0.105 mm, 0.11 mm, and 0.09 mm, and an average value of those values was about 0.1 mm. When the thickness “tc” of the resin layer 12 in the optical effective region 14 was similarly measured, the average value of the thickness “tc” was 100 μm.
As the initial evaluation of the diffractive optical element 10 according to Example 3, similarly to Example 1, the diffraction efficiency was measured and evaluated. Thus, as shown in Table 1, it was confirmed that the diffraction efficiency was good.
A diffractive optical element according to Example 4 and a method of manufacturing the diffractive optical element are described with reference to
In Example 4, first, as the substrate 11, a substrate made of glass in which a diffraction grating was provided by a mold die or the like was prepared. The substrate 11 had an outer diameter of φ40 mm, an optical effective diameter of φ36 mm, and a center thickness of 5 mm. One surface of the substrate 11 had a convex shape, and the other surface thereof was a flat surface. The diffraction grating 13 having a grating height of 30 μm was provided on the other surface of the substrate 11. This diffraction grating 13 was arranged concentrically with respect to an outer diameter center of the substrate 11, and its grating interval was reduced toward the outer periphery from the center. In plan view along the optical axis direction, the substrate 11 was formed of only the first portion 111 having the segmental circular shape, and the outer-peripheral diffraction grating 13b and the substrate 11 were cut in the chord portion 114 at a position of 15 mm from the center.
Next, through the steps illustrated in
The diffractive optical element 10 according to Example 4 manufactured as described above was subjected to shape measurement after release from the mold 21 similarly to Example 1. When the thickness t1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the thicknesses t1 at the three positions were 240 μm, 310 μm, and 340 μm, and an average value of those values was about 300 μm. Further, when the width w1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the widths w1 at the three positions were 1.44 mm, 1.39 mm, and 1.36 mm, and an average value of those values was about 1.4 mm. Meanwhile, when the thickness t2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the thicknesses t2 at the three positions were 180 μm, 270 μm, and 310 μm, and an average value of those values was about 250 μm. Further, when the width w2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the widths w2 at the three positions were 1.55 mm, 1.65 mm, and 1.61 mm, and an average value of those values was about 1.6 mm.
When the thickness “tc” of the resin layer 12 in the optical effective region 14 was similarly measured, the average value of the thickness “tc” was 200 μm.
As the initial evaluation of the diffractive optical element 10 according to Example 4, similarly to Example 1, the diffraction efficiency was measured and evaluated. Thus, as shown in Table 1, it was confirmed that the diffraction efficiency was good.
In Comparative Example 1, the same substrate as that of Example 1 was used as the substrate 11. Further, in Comparative Example 1, the shape of the mold 21 was changed to a shape in which the thickness of the resin layer 12 in the non-optical effective region 15 in each of the arc portion 113 and the chord portion 114 became the same as the thickness of the resin layer 12 in the optical effective region 14. The other points were similar to those of Example 1. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Comparative Example 1 was also subjected to shape measurement after mold release, similarly to Example 1. When the thickness t1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the thicknesses t1 at the three positions were 100 μm, 80 μm, and 130 μm, and an average value of those values was about 100 μm. Further, when the width w1 of the resin layer 12 outside of the optical effective diameter in the chord portion 114 was measured at three positions, the widths w1 at the three positions were 1.05 mm, 0.85 mm, and 1.1 mm, and an average value of those values was about 1.0 mm. Meanwhile, when the thickness t2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the thicknesses t2 at the three positions were 70 μm, 110 μm, and 120 μm, and an average value of those values was about 100 μm. Further, when the width w2 of the resin layer 12 outside of the optical effective diameter in the arc portion 113 was measured at three positions, the widths w2 at the three positions were 1.07 mm, 0.79 mm, and 1.15 mm, and an average value of those values was about 1.0 mm. When the thickness “tc” of the resin layer 12 in the optical effective region 14 was similarly measured, the average value of the thickness “tc” was 100 μm.
As the initial evaluation of the diffractive optical element 10 according to Comparative Example 1, similarly to Example 1, the diffraction efficiency was measured and evaluated. Thus, as shown in Table 1, it was confirmed that the diffraction efficiency was deteriorated.
Measurement results and evaluation results for Example 1 to Example 4 and Comparative Example 1 described above are shown in Table 1 below. Table 1 also shows calculation results of t1/t2, (t1×w1)/(t2×w2), and (t1−tc)/d, which are calculated from the grating height “d” of the diffraction grating 13, the thickness t1 and the thickness t2 of the resin layer 12, and the width w1 and the width w2 of the resin layer 12.
A diffractive optical element according to a third embodiment of the present disclosure and a method of manufacturing the diffractive optical element are described with reference to
First, a configuration of the diffractive optical element according to the third embodiment is described with reference to
The diffractive optical element 10 according to the third embodiment includes, as illustrated in
The substrate 11 is, for example, a convex-lens-shaped substrate, and may be a resin substrate formed by injection molding, or a glass substrate. The shape of the substrate 11 may be a concave lens shape other than the convex lens shape, or may be a convex spherical surface shape, a concave spherical surface shape, an aspherical surface shape, a planar shape, or other shapes. Further, a material forming the substrate 11 is not particularly limited as long as the material is a transparent material having transmittance with respect to light such as visible light which is a target of the diffractive optical element 10.
The term “transparent” means that, for example, the transmittance of light having a wavelength range of from 420 nm or more to 700 nm or less is 10% or more.
In plan view as viewed in the optical axis direction of the diffractive optical element 10, the substrate 11 has a segmental circular shape which is a shape enclosed between an arc and a line connecting both ends of this arc to each other. In this case, the line connecting both ends of the arc to each other may be a straight line or a curved line. Further, the number of arcs may be one or more. That is, in the segmental circular shape, the number of segmental parts lacked from the circular shape may be one or more. The center of the circle of the segmental circular shape is the center of the circle of the diffraction grating 13, and is an optical center of the diffractive optical element 10. The shape including the planar shape of the substrate 11 is not limited to the shape illustrated in
The substrate 11 has a planar shape of the segmental circular shape, and hence the diffraction grating 13 includes a diffraction grating 13 having a circular shape on the inner side of the substrate 11, and a diffraction grating 13 having an arc shape on the outer side of the substrate 11. As in the shape illustrated in
The diffractive optical element 10 including the substrate 11 includes a first region 14 and a second region 15. The first region 14 has a grating shape of the diffraction grating 13. The second region 15 is arranged on the outer side of the first region 14, and has no grating shape of the diffraction grating 13. The first region 14 is a region in which the diffraction grating 13 is provided, and the second region 15 is a region in which no diffraction grating is provided. The first region 14 is substantially a region through which light being a target of the diffractive optical element 10 passes. The second region 15 is a region through which the light being the target of the diffractive optical element 10 does not pass.
As illustrated in
The diffraction grating 13 is formed concentrically on one surface having a planar shape of the segmental circular shape of the substrate 11, with the center of the circle of the segmental circular shape through which the optical axis of the diffractive optical element 10 passes serving as a center. In one example, the diffraction grating 13 is formed so that, as illustrated in
The resin layer 12 is provided on one surface of the substrate 11 so as to cover the diffraction grating 13. The resin forming the resin layer 12 is not particularly limited as long as the resin is a transparent resin having transmittance with respect to light such as visible light which is the target of the diffractive optical element 10, but it is preferred that the resin be a photocurable resin or a thermosetting resin from the viewpoint of easiness in manufacture.
As illustrated at the lower part of
A transparent inorganic film may be provided between the substrate 11 and the resin layer 12. That is, the transparent inorganic film may be provided on the diffraction grating 13 of the substrate 11, and the resin layer 12 may be provided on the substrate 11 through intermediation of the transparent inorganic film. In this case, the transparent inorganic film is a thin film made of a transparent inorganic material having transmittance with respect to light such as visible light which is the target of the diffractive optical element 10.
Examples of the inorganic material include an aluminum oxide (Al2O3), a silicon oxide (SiO2, SiO), a titanium oxide (TiOx), a tantalum oxide (TaOx), and a niobium oxide (NbOx). The transparent inorganic film can be provided along a grating surface of the diffraction grating 13 so as to cover the grating surface. The transparent inorganic film can be provided by using various film forming methods such as vacuum deposition and sputtering. With the transparent inorganic film being provided, when the substrate 11 is made of a resin, penetration or dissolution of the resin material between the substrate 11 and the resin layer 12 can be reduced or prevented, and thus the deterioration of the diffraction efficiency can be reduced or prevented.
The resin layer 12 is provided so that, as illustrated in
Moreover, the diffractive optical element 10 according to the third embodiment at least includes a region in which a thickness increase gradient G of the resin layer 12 is 0.4 or more, in the boundary region 16 including the boundary 19 between the first region 14 and the second region 15 on the side on which the diffraction grating 13 is discontinuous. The thickness increase gradient G of the resin layer 12 as used herein refers to a gradient in which the thickness “t” of the resin layer 12 increases toward the outer side from the center of the circle of the diffraction grating 13, that is, a degree of change of the thickness “t” of the resin layer toward the outer side from the center of the circle of the diffraction grating 13. The thickness increase gradient G can be obtained as a numerical value obtained as follows. Assuming that the boundary region 16 is a region between a position on the inner side by 0.5 mm and a position on the outer side by 0.5 mm from the boundary 19 serving as a center, the boundary region 16 is divided for each 0.05 mm in width, that is, divided into twenty sections, and a change amount of the average thickness of the resin layer 12 between adjacent sections is divided by the interval of 0.05 mm.
The thickness increase gradient G includes a thickness increase gradient Ga and a thickness increase gradient Gb. The thickness increase gradient Ga is a thickness increase gradient G in the boundary region 16 including the boundary 19 on the side on which the diffraction grating 13 is discontinuous. The thickness increase gradient Gb is a thickness increase gradient G in the boundary region 17 including the boundary 19 on the side on which the diffraction grating 13 is continuous. As described above, the diffractive optical element 10 according to the third embodiment at least includes a region in which the thickness increase gradient Ga is 0.4 or more.
In the first region 14, the thickness “t” of the resin layer 12 can be regarded as an average thickness of the resin layer 12 from the envelope of the diffraction grating 13. Further, in the second region 15, the thickness “t” of the resin layer 12 can be regarded as an average thickness of the resin layer 12 provided on the substrate 11. The thickness “t” of the resin layer can be measured through use of a shape measuring machine or the like. The thickness “t” of the resin layer can be obtained by taking a difference between a measured value of the surface shape of the diffractive optical element 10 obtained by the shape measuring machine or the like and the shape of the substrate 11. As another example, the diffractive optical element 10 can be cut along a plane passing through the center of the circle of the diffraction grating, and the sectional shape can be measured to measure the thickness “t” of the resin layer.
As described above, the diffractive optical element 10 according to the third embodiment at least includes a region in which the thickness increase gradient Ga of the resin layer 12 is 0.4 or more, in the boundary region 16 including the boundary 19 on the side on which the diffraction grating 13 is discontinuous. This configuration is adopted so that, in consideration of shrinkage at the time of curing of the resin forming the resin layer 12, the density difference of the resin caused by the curing is suppressed to be small.
The phenomenon in which the density difference of the resin is caused by curing is described with reference to
When the diffractive optical element 10 according to the third embodiment is manufactured, first, as illustrated in
In the manufacturing method described above as illustrated in
The diffractive optical element 10 according to the third embodiment at least includes a region in which the thickness increase gradient Ga of the resin layer 12 is 0.4 or more, in the boundary region 16 including the boundary 19 between the first region 14 and the second region 15 on the side on which the diffraction grating 13 is discontinuous. Accordingly, in the third embodiment, as illustrated in
Further, when the thickness increase gradient Ga of the resin layer 12 is 1.8 or more, the resin 121 can be sufficiently supplied at the time of curing shrinkage, and the reduction in the diffraction efficiency can be further prevented. However, when the thickness increase gradient Ga of the resin layer 12 is larger than 12, there is a fear in that large curing shrinkage stress may be generated in the thickness direction during a process at the time of curing of the resin 121, which may cause deformation of the diffractive optical element 10. Thus, it is preferred that the thickness increase gradient Ga be 1.8 or more and 12 or less, that is, 1.8≤Ga≤12 be satisfied. It suffices that the diffractive optical element 10 preferably include at least a region in which the thickness increase gradient Ga is 1.8 or more and 12 or less.
The shrinkage of the resin 121 in the boundary region 16 on the side on which the diffraction grating 13 is discontinuous tends to be larger than the shrinkage of the resin 121 in the boundary region 17 on the side on which the diffraction grating 13 is continuous. Accordingly, it is preferred that the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 is discontinuous be larger than the thickness increase gradient Gb of the resin layer 12 in the boundary region 17 on the side on which the diffraction grating 13 is continuous. That is, it is preferred that Ga>Gb be satisfied. It suffices that the diffractive optical element 10 preferably include at least a region in which the thickness increase gradient Ga is larger than the thickness increase gradient Gb.
Further, it is preferred that a grating height “d” of the diffraction grating 13 be 1 μm or more and 30 μm or less in order to sufficiently obtain the effect as the diffractive optical element 10. The grating height “d” is a height from a boundary between the protruding portion and the base of the diffraction grating 13 to a distal end of the protruding portion of the diffraction grating 13. The grating height “d” can be an average value of the diffraction grating 13 provided on the substrate 11.
Further, when the thickness “t” of the resin layer 12 is smaller than 10 μm, the internal refractive index becomes uneven, and thus the diffraction efficiency is reduced. When the thickness “t” is excessively large, the diffractive optical element 10 becomes thick and heavy. Accordingly, it is preferred that the thickness “t” of the resin layer 12 be 10 μm or more and 300 μm or less. The thickness “t” of the resin layer 12 as used here can be regarded as an average thickness of the resin layer 12 formed across the first region 14 and the second region 15.
Further, it is preferred that a pitch of the diffraction grating 13 in each of the boundary regions 16 and 17 including the boundary 19 between the first region 14 and the second region 15 be 10 μm or more and 300 μm or less. In this manner, an effect as the diffractive optical element 10 can be sufficiently obtained.
As described above, according to the third embodiment, in the diffractive optical element 10 in which the diffraction grating 13a having the circular shape and the diffraction grating 13b having the arc shape are provided, the deterioration of the optical characteristic can be reduced or prevented. The optical characteristic of the diffractive optical element 10 can be evaluated by measuring, as optical performance evaluation, the diffraction efficiency in a desired wavelength range such as a wavelength range of from 420 nm to 700 nm. In this case, for example, when the change of the diffraction efficiency is 2% or less as compared to the design value, there is no significant influence on the optical characteristic, and hence the optical characteristic can be evaluated as being good.
Next, the diffractive optical element 10 according to the above-mentioned third embodiment is specifically described with reference to Examples.
A diffractive optical element according to Example 5 and a method of manufacturing the diffractive optical element are described with reference to
In Example 5, first, as the substrate 11, a substrate obtained by molding a polycarbonate-based resin material (EP4500, produced by MITSUBISHI GAS CHEMICAL COMPANY, INC.) by injection molding was prepared. The substrate 11 had an outer diameter of φ46 mm, a diameter of a region in which the diffraction grating was present of φ42 mm, a center thickness of 2.5 mm, and an outer-peripheral thickness of 1.0 mm. One surface of the substrate 11 had a convex shape, and the other surface thereof was a flat surface. The diffraction grating 13 having a grating height of 10 μm was provided on the other surface of the substrate 11. This diffraction grating 13 was arranged concentrically with respect to an outer diameter center of the substrate 11, and its grating interval was reduced toward the outer periphery from the center. In plan view as viewed in the optical axis direction, the substrate 11 had a segmental circular shape, and had a shape obtained by cutting a circle with a straight line at a position of 18 mm from the center. As the diffraction grating 13, the diffraction grating 13 having a circular shape was provided in a range from the center to a position of 16 mm, that is, with a diameter of 32 mm, and the diffraction grating 13 in a range of a diameter of from 32 mm to 42 mm had an arc shape obtained by cutting a circle with a straight line at a position of 16 mm from the center in the same direction as that of the substrate 11.
Next, through the steps illustrated in
The diffractive optical element 10 according to Example 5 manufactured as described above was subjected to shape measurement after release from the mold 21. The shape measurement used a surface shape measuring machine, Form Talysurf (manufactured by Taylor Hobson). In order to measure the thickness of the resin layer 12, the surface shape of the diffractive optical element 10 on the resin layer 12 side was measured at least at three positions from the optical axis center to the end portion, in each of a direction of the boundary region 16 on the side on which the diffraction grating 13 is discontinuous and a direction of the boundary region 17 on the side on which the diffraction grating 13 is continuous.
When the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 is discontinuous, which included the boundary 19 between the first region 14 and the second region 15, was measured at three positions, the three positions each included a portion having the maximum Ga of 1.8. Specifically, the average thickness of the resin layer 12 from a position of 15.5 mm to a position of 16.5 mm from the center of the diffraction grating 13 for each 0.05 mm was as follows. That is, the average thickness of the resin layer 12 was 100 μm (15.5 mm to 15.9 mm), 190 μm (15.95 mm), 280 μm (16 mm), and 370 μm (16.05 mm to 16.5 mm). The thickness increase gradient Ga of the resin layer 12 was calculated as 0.0 (15.5 mm to 15.9 mm), 1.8 (15.95 mm to 16.05 mm), and 0.0 (16.1 mm to 16.5 mm). The boundary 19 between the first region 14 and the second region 15 was present at a position of 16 mm from the center of the diffraction grating 13.
Further, when the thickness increase gradient Gb of the resin layer in the boundary region 17 on the side on which the diffraction grating 13 is continuous, which included the boundary 19 between the first region 14 and the second region 15, was measured at three positions, the three positions each included a portion having the maximum Gb of 0.8. Specifically, the average thickness of the resin layer 12 from a position of 20.5 mm to a position of 21.5 mm from the center of the diffraction grating 13 for each 0.05 mm was as follows. That is, the average thickness of the resin layer 12 was 100 μm (20.5 mm to 20.9 mm), 140 μm (20.95 mm), 180 μm (21 mm), and 220 μm (21.05 mm to 21.5 mm). The thickness increase gradient Gb of the resin layer 12 was calculated as 0.0 (20.5 mm to 20.9 mm), 0.8 (20.95 mm to 21.05 mm), and 0.0 (21.1 mm to 21.5 mm). The boundary 19 between the first region 14 and the second region 15 in which the diffraction grating was not present was present at a position of 21 mm from the center of the diffraction grating 13.
As the optical performance evaluation of the diffractive optical element 10 according to Example 5, a diffraction efficiency in a wavelength range of from 420 nm to 700 nm was measured. In the optical performance evaluation, when the change of the diffraction efficiency was 1% or less as compared to the design value, there was no significant influence on the optical performance, and hence the optical performance was evaluated as “a” representing very good. When the change of the diffraction efficiency was more than 1% and 2% or less as compared to the design value, there was no significant problem on the optical performance, and hence the optical performance was evaluated as “b” representing good. When the change of the diffraction efficiency was more than 2% as compared to the design value, the deterioration of the optical performance was unignorable, and hence the optical performance was evaluated as “c” representing bad. Further, as the shape accuracy evaluation of the diffractive optical element 10, the shape of the surface of the resin layer 12 was compared to the design shape. When the difference from the design shape was 1 μm or less, there was no significant influence on the optical performance, and hence the shape accuracy was evaluated as “a” representing very good. When the difference from the design shape was more than 1 μm and 2 μm or less, there was no significant problem on the optical performance, and hence the shape accuracy was evaluated as “b” representing good. When the difference from the design shape was more than 2 μm, the deterioration of the optical performance was unignorable, and hence the shape accuracy was evaluated as “c” representing bad. As a result, for the diffractive optical element 10 according to Example 5, as shown in Table 2, it was confirmed that both of the optical performance and the shape accuracy were very good.
In Example 6, the same substrate as that of Example 5 was used as the substrate 11. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 was discontinuous was 0.4. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Gb of the resin layer 12 in the boundary region 17 on the side on which the diffraction grating 13 was continuous was 0.2. The other points were similar to those of Example 5. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 6 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 0.4. Further, the three positions each included a portion having the maximum thickness increase gradient Gb of 0.2.
For the diffractive optical element 10 according to Example 6, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that the optical performance was good and the shape accuracy was very good.
In Example 7, the same substrate as that of Example 5 was used as the substrate 11. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 was discontinuous was 1.8. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Gb of the resin layer 12 in the boundary region 17 on the side on which the diffraction grating 13 was continuous was 1.8. The other points were similar to those of Example 5. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 7 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 1.8. The three positions each included a portion having the maximum thickness increase gradient Gb of 1.8.
For the diffractive optical element 10 according to Example 7, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that the optical performance was very good and the shape accuracy was good.
In Example 8, the same substrate as that of Example 5 was used as the substrate 11. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 was discontinuous was 0.4. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed to have a region in which the thickness increase gradient Gb of the resin layer 12 in the boundary region 17 on the side on which the diffraction grating 13 was continuous was 0.8. The other points were similar to those of Example 5. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 8 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 0.4. The three positions each included a portion having the maximum thickness increase gradient Gb of 0.8.
For the diffractive optical element 10 according to Example 8, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that both of the optical performance and the shape accuracy were good.
In Example 9, the diffractive optical element 10 having the shape illustrated in
The diffractive optical element 10 according to Example 9 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 1.8. The three positions each included a portion having the maximum thickness increase gradient Gb of 0.8.
For the diffractive optical element 10 according to Example 9, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that both of the optical performance and the shape accuracy were very good.
In Example 10, the resin layer 12 was molded so that the thickness of the resin layer 12 from the envelope of the diffraction grating 13 became 12 μm. The other points were similar to those of Example 5. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Example 10 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 1.8. The three positions each included a portion having the maximum thickness increase gradient Gb of 0.8.
For the diffractive optical element 10 according to Example 10, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that both of the optical performance and the shape accuracy were very good.
In Comparative Example 2, the same substrate as that of Example 5 was used as the substrate 11. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed so that the thickness increase gradient Ga of the resin layer 12 in the boundary region 16 on the side on which the diffraction grating 13 was discontinuous became 0, that is, the resin layer 12 became flat. Further, the shape of the mold 21 was a shape in which the resin layer 12 was to be formed so that the thickness increase gradient Gb of the resin layer 12 in the boundary region 17 on the side on which the diffraction grating 13 was continuous became 0, that is, the resin layer 12 became flat. The other points were similar to those of Example 5. In this manner, the resin layer 12 was molded so that the diffractive optical element 10 was manufactured.
The diffractive optical element 10 according to Comparative Example 2 was also subjected to shape measurement after mold release similarly to Example 5. The three positions each included a portion having the maximum thickness increase gradient Ga of 0.0. The three positions each included a portion having the maximum thickness increase gradient Gb of 0.0.
For the diffractive optical element 10 according to Comparative Example 2, the optical performance and the shape accuracy were measured and evaluated similarly to Example 5. As a result, as shown in Table 2, it was confirmed that both of the optical performance and the shape accuracy were bad.
Evaluation results for Example 5 to Example 10 and Comparative Example 2 described above are shown in Table 2 below.
The diffractive optical element 10 according to each of the first embodiment to the third embodiment described above can be applied to various apparatus and devices such as an optical apparatus, a display apparatus, and an imaging apparatus. In a fourth embodiment of the present disclosure, an optical apparatus, a display apparatus, and an imaging apparatus are described as specific application examples of the diffractive optical element 10 according to each of the first embodiment and the second embodiment.
The specific application examples of the diffractive optical element 10 according to each of the first embodiment to the third embodiment include: a lens for forming an optical apparatus (image taking optical system) for a camera or a video camera; and a lens for forming an optical apparatus (projecting optical system) for a liquid crystal projector. In addition, the diffractive optical element may be used in a pickup lens of a DVD recorder or the like. Those optical systems each include at least one lens arranged in a housing, and the diffractive optical element 10 according to the first embodiment can be used as at least one of the lenses.
As illustrated in
As illustrated in
Herein, the display apparatus has been described by using the HMD. However, the diffractive optical element 10 may be similarly used in a projector or the like.
An image of light from an object is taken through an optical system formed of, for example, a plurality of lenses 203 and 205 arranged on the optical axis of an image taking optical system in a housing 220 of the lens barrel 201. The diffractive optical element 10 according to the first embodiment may be used in, for example, each of the lenses 203 and 205. Herein, the lens 205 is supported by an inner barrel 204, and is movably supported with respect to an outer barrel of the lens barrel 201 for focusing and zooming.
In an observation period before the image taking, the light from the object is reflected by a main mirror 207 in a housing 221 of the camera main body to be transmitted through a prism 211. After that, the taken image is projected to a photographer through a finder lens 212. The main mirror 207 is, for example, a half mirror, and the light that has been transmitted through the main mirror 207 is reflected toward an autofocus (AF) unit 213 by a submirror 208. The reflected light is used in, for example, distance measurement. In addition, the main mirror 207 is mounted on and supported by a main mirror holder 240 through bonding or the like. At the time of the image taking, the main mirror 207 and the submirror 208 are moved to the outside of an optical path via a driving mechanism (not shown) to open a shutter 209 so that an imaging element 210 may receive the light that has entered from the lens barrel 201 and has passed through the image taking optical system to form a taken light image. In addition, a diaphragm 206 is configured to be capable of changing brightness and a focal depth at the time of the image taking by changing its opening area.
Herein, the imaging apparatus has been described by using the single-lens reflex digital camera. However, the diffractive optical element 10 may be similarly used in, for example, a smartphone, a compact digital camera, or a drone.
According to the present disclosure, when, in plan view, a diffraction grating having a circular shape and a diffraction grating having an arc shape are provided, deterioration of the optical characteristic can be reduced or prevented.
While the present disclosure has been described with reference to exemplary embodiments, it is to be understood that the disclosure is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2023-046875, filed Mar. 23, 2023, and Japanese Patent Application No. 2023-142311, filed Sep. 1, 2023, which are hereby incorporated by reference herein in their entirety.
Number | Date | Country | Kind |
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2023-046875 | Mar 2023 | JP | national |
2023-142311 | Sep 2023 | JP | national |