WO2019189289A1 - Optical apparatus - Google Patents
Optical apparatus Download PDFInfo
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- WO2019189289A1 WO2019189289A1 PCT/JP2019/013059 JP2019013059W WO2019189289A1 WO 2019189289 A1 WO2019189289 A1 WO 2019189289A1 JP 2019013059 W JP2019013059 W JP 2019013059W WO 2019189289 A1 WO2019189289 A1 WO 2019189289A1
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- Prior art keywords
- optical system
- imaging optical
- imaging
- image
- present
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N23/00—Cameras or camera modules comprising electronic image sensors; Control thereof
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B7/00—Mountings, adjusting means, or light-tight connections, for optical elements
- G02B7/02—Mountings, adjusting means, or light-tight connections, for optical elements for lenses
- G02B7/14—Mountings, adjusting means, or light-tight connections, for optical elements for lenses adapted to interchange lenses
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B15/00—Special procedures for taking photographs; Apparatus therefor
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B17/00—Details of cameras or camera bodies; Accessories therefor
- G03B17/02—Bodies
- G03B17/12—Bodies with means for supporting objectives, supplementary lenses, filters, masks, or turrets
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B3/00—Focusing arrangements of general interest for cameras, projectors or printers
- G03B3/04—Focusing arrangements of general interest for cameras, projectors or printers adjusting position of image plane without moving lens
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B5/00—Adjustment of optical system relative to image or object surface other than for focusing
Definitions
- the present invention relates to an optical device, and is suitable for a digital camera, a surveillance camera, an in-vehicle camera, and a camera mounted on a UAV (Unmanned Aerial Vehicle) such as a drone.
- UAV Unmanned Aerial Vehicle
- An imaging apparatus having a plurality of imaging optical systems and capable of switching the imaging optical system used for photographing is known.
- Patent Document 1 describes an imaging apparatus that has two imaging optical systems and can change the imaging optical system used for photographing by moving one imaging element.
- Patent Document 1 since the imaging apparatus described in Patent Document 1 has a configuration in which a plurality of imaging optical systems are fixed and the imaging element is moved, the space in the housing for the imaging optical system that is not used is always wasted. It was.
- an object of the present invention is to realize an optical device that can effectively use a space in a housing while allowing a plurality of imaging optical systems to be switched.
- the optical apparatus of the present invention includes first and second imaging optical systems, and is an optical apparatus that can be used by switching between the first and second imaging optical systems.
- the second imaging optical system In a state in which the optical system is used, the second imaging optical system is disposed at a position that does not block an optical path of the first imaging optical system, and in a state in which the second imaging optical system is used.
- the second imaging optical system is disposed at a position that blocks the optical path.
- another optical device of the present invention is an optical device that includes first and second imaging optical systems and an imaging device, and can be used by switching between the first and second imaging optical systems.
- an image is acquired using the imaging device, and the switching is performed using the first and second imaging optical systems.
- the relative positional relationship of the second imaging optical system is determined so that the second imaging optical system is retracted from the space through which the light beam imaged by the first imaging optical system passes, It is performed by changing between the state in which the second imaging optical system is inserted, and the relative positional relationship between the first imaging optical system and the imaging element does not change before and after the switching. It is characterized by.
- an optical device that can effectively use the space in the housing while allowing a plurality of imaging optical systems to be switched.
- FIG. 1 is a schematic diagram of an imaging apparatus according to Embodiment 1.
- FIG. 2 is a cross-sectional view of an imaging optical system in the imaging apparatus of Embodiment 1.
- FIG. 3 is a diagram illustrating distortion of the image forming optical system according to the first embodiment.
- 2 is a lateral aberration diagram of the imaging optical system according to Example 1.
- FIG. FIG. 6 is a schematic diagram of an imaging apparatus according to a second embodiment.
- FIG. FIG. 6 is a diagram illustrating distortion of the image forming optical system according to the second embodiment.
- FIG. 6 is a lateral aberration diagram of the image forming optical system according to Example 2.
- FIG. 6 is a cross-sectional view of an imaging optical system in an imaging apparatus according to Embodiment 3.
- FIG. 6 is a diagram illustrating distortion of the image forming optical system according to the third embodiment.
- 6 is a lateral aberration diagram of the image forming optical system according to Example 3.
- FIG. 6 is a cross-sectional view of an imaging optical system in an imaging apparatus of Embodiment 4.
- FIG. 10 is a diagram illustrating distortion of the image forming optical system according to the fourth embodiment.
- FIG. 6 is a lateral aberration diagram of the image forming optical system according to Example 4.
- 7 is a cross-sectional view of an imaging optical system in an imaging apparatus according to Embodiment 5.
- FIG. 5 is a cross-sectional view of an imaging optical system in an imaging apparatus according to Embodiment 5.
- FIG. 10 is a diagram illustrating distortion of the image forming optical system according to the fifth embodiment.
- 6 is a lateral aberration diagram of the imaging optical system according to Example 5.
- FIG. It is a figure explaining the coordinate system used by this-application specification. It is a figure which shows the position on the image pick-up element which evaluated the aberration. It is a figure explaining the modification regarding the mechanism which moves a 2nd imaging optical system.
- FIG. 19 is a diagram illustrating a coordinate system used when describing the imaging optical system of each embodiment.
- one light beam that passes from the object side (subject side) toward the image side (image plane side formed on the image sensor) through the center of a pupil (aperture) (not shown) and reaches the center of the image plane.
- the central principal ray (reference axis ray) is indicated by a one-dot chain line in FIG.
- the path followed by the central principal ray is defined as the reference axis.
- the i-th optical surface (i-th surface) from the object side along the reference axis is the i-th surface Ri.
- the first surface R1 is the stop surface (incidence pupil part)
- the second surface R2 is the reflecting surface tilted with respect to the first surface R1
- the third surface R3 and the fourth surface R4 are the respective front surfaces. The reflecting surface is shifted and tilted with respect to the reflecting surface.
- At least one of the first imaging optical system and the second imaging optical system in each embodiment to be described later is an off-axial optical system.
- Each surface constituting the Off-Axial optical system does not have a common optical axis. Therefore, an absolute coordinate system with the center of the first surface R1 as the origin is set. The position of the origin corresponds to the center position of the first surface R1 (the stop surface or the entrance pupil). Therefore, the reference axis passes through the origin of the absolute coordinate system.
- the central principal ray passes through the center of the first surface R1 (the origin of the absolute coordinate system) and reaches the center of the final surface (image surface), and is refracted or reflected by each optical surface.
- the reference axis extends to the final surface while bending in turn on each optical surface.
- the image plane side and the object side mean which side is along the reference axis.
- a straight line passing through the origin and parallel to the reference axis extending from the first surface is called the Z-axis (the direction from the first surface toward the second surface is positive).
- the axis in the paper of FIG. 19 that passes through the origin and forms 90 ° counterclockwise with respect to the Z-axis in accordance with the definition of the right-handed coordinate system is called the Y-axis.
- a straight line that passes through the origin and is perpendicular to the Z-axis and the Y-axis is referred to as an X-axis (the direction toward the back of the page in FIG. 19 is positive).
- a local coordinate system is defined to represent the surface shape and tilt angle of the optical surface after the first surface R1 in the imaging optical system.
- a local coordinate system is defined for each optical surface after the first surface R1. The surface shape of the optical surface in the imaging optical system of each embodiment will be described using local coordinates.
- the origin of the local coordinate system is the point where the reference axis and the i-th surface Ri intersect.
- the z axis in the local coordinate system of the i-th surface Ri is a surface normal at a point on the reference axis of the i-th surface.
- the y axis in the local coordinate system passes through the origin of the local coordinate and is an axis in the plane of FIG. 19 that forms 90 ° counterclockwise with respect to the z direction according to the definition of the right hand coordinate system.
- the x-axis of the local coordinate system is a straight line that passes through the origin of the local coordinates and is perpendicular to the z-axis and the y-axis.
- the tilt angle ⁇ xi (°) in the yz plane of the i-th surface is an acute angle formed in the yz-plane with respect to the reference axis extending from the i-1th plane in the local coordinate system (counterclockwise direction Positive).
- the tilt angle ⁇ yi (°) in the xz plane of the i-th surface is an acute angle formed in the xz plane with respect to the reference axis extending from the i ⁇ 1 plane (the counterclockwise direction is positive).
- the direction of the arrow of each axis in FIG. 19 represents the positive direction of each axis.
- FIGS. 1A to 1D are schematic views showing a configuration of an imaging apparatus 100 as an optical apparatus in the present embodiment.
- 2A to 2C are cross-sectional views of the imaging optical system included in the imaging apparatus 100.
- FIG. 1A to 1D are schematic views showing a configuration of an imaging apparatus 100 as an optical apparatus in the present embodiment.
- 2A to 2C are cross-sectional views of the imaging optical system included in the imaging apparatus 100.
- the imaging apparatus 100 of the present embodiment includes a first imaging optical system L1, a second imaging optical system L2, and a member that holds each imaging optical system.
- the member that holds the second imaging optical system L2 is configured to be movable with respect to the member that holds the first imaging optical system L1, and the imaging apparatus 100 can switch the imaging optical system to be used. it can.
- the imaging apparatus 100 of the present embodiment when the first imaging optical system L1 is used, the light beam imaged by the first imaging optical system L1 passes through the second imaging optical system L2. It arrange
- the optical system to be used is switched to the second imaging optical system L2, a light beam imaged by the first imaging optical system L1 passes when the first imaging optical system L1 is used.
- the second imaging optical system L2 is inserted at a second position in the space.
- the first imaging optical system L1 when the first imaging optical system L1 is used, the first imaging optical system L2 is arranged at a position that does not block the optical path of the first imaging optical system L1.
- the optical path of the imaging optical system L1 is made effective. At this time, light from the object enters the first imaging optical system L1 and is imaged by the first imaging optical system L1. on the other hand.
- the second imaging optical system L2 when the second imaging optical system L2 is used, the second imaging optical system L2 is disposed at a position that blocks the optical path of the first imaging optical system L1, and the first imaging optical system is used.
- the optical path of the second imaging optical system L2 is validated while invalidating the optical path of L1. At this time, light from the object enters the second imaging optical system L2, and is imaged by the second imaging optical system L2.
- the imaging optical system to be used is switched by changing the relative positional relationship between the first imaging optical system L1 and the second imaging optical system L2.
- the second imaging optical system L2 is used, the second imaging optical system L2 is imaged inside the first imaging optical system L1 (by the first imaging optical system L1). Therefore, the space in the housing can be used effectively.
- FIG. 1A is a view of the imaging device 100 in a state in which the second imaging optical system L2 is used as seen from a direction parallel to the Z axis.
- FIG. 1B is a diagram of the imaging device 100 in a state where the first imaging optical system L1 is used as seen from a direction parallel to the Z axis.
- 1C is a perspective view of the imaging device 100 corresponding to FIG. 1A
- FIG. 1D is a perspective view of the imaging device 100 corresponding to FIG.
- SP1 is an opening through which light imaged by the first imaging optical system L1 enters
- SP2 is an opening through which light imaged by the second imaging optical system L2 enters.
- SP1 and SP2 also function as a diaphragm of each imaging optical system.
- IMG is an image plane.
- the image plane IMG corresponds to the final plane in each imaging optical system. This is different from an intermediate imaging plane described later, which is in the middle of the optical path of the imaging optical system.
- a light receiving surface of an image sensor such as a CCD or a CMOS sensor is arranged on the image plane IMG. The image sensor is shared regardless of the imaging optical system used.
- the imaging apparatus 100 as an optical apparatus has an imaging element
- the imaging element may be separate from the optical apparatus.
- the imaging optical system L2 when the second imaging optical system L2 is used, the imaging optical system L2 is housed inside the first imaging optical system L1. Thus, the second imaging optical system L2 is arranged. At this time, since the optical path of the first imaging optical system L1 is blocked by the second imaging optical system L2, the first imaging optical system L1 is invalid (the first imaging optical system L1). Light does not enter the system L1). For this reason, an image by the second imaging optical system L2 is formed on the image plane IMG.
- FIGS. 1B and 1D when the first imaging optical system L1 is used, the second imaging optical system from the inside of the first imaging optical system L1 is used. By retracting L2, the optical path of the first imaging optical system L1 is validated.
- the arrows shown in FIGS. 1B and 1D indicate the moving direction when the second imaging optical system L2 is retracted by a slide mechanism (not shown).
- the first connection is made on the image plane IMG. An image is formed by the image optical system L1.
- the mechanism for moving the second imaging optical system L2 is not particularly limited.
- the movement of the second imaging optical system L2 may be performed manually or electrically by a driving means such as a motor.
- An elastic member such as a spring or rubber may be provided so that only one of insertion and removal from the inside of the first imaging optical system L1 is performed by the elastic force of the elastic member.
- FIGS. 1A to 1D illustrate a mechanism for inserting / removing the second imaging optical system L2 by translating the second imaging optical system L2, but the present invention is not limited to this. It is not limited to.
- FIGS. 21A to 21D are diagrams showing modifications of the moving mechanism of the second imaging optical system L2. As shown in FIGS. 21A to 21D, the first imaging optical system L1 and the second imaging optical system L2 are connected by the axis P, and the second imaging optical system L2 is centered on the axis P. You may insert / extract with respect to the 1st imaging optical system L1 by rotating.
- the optical surface of the second imaging optical system L2 is constituted by a reflecting surface, and when using the first imaging optical system L1, each optical surface of the second imaging optical system L2 is You may make it tilt or shift so that the optical path of the 1st imaging optical system L1 may not be interrupted.
- FIG. 2A is a sectional view of the first imaging optical system L1 in the present embodiment.
- FIG. 2B is a sectional view of the second imaging optical system L2 in the present embodiment.
- FIG. 2C shows a state in which the second imaging optical system L2 is inserted in the first imaging optical system L1 in the imaging apparatus 100 of the present embodiment (FIGS. 1A and 1C are shown). It is sectional drawing of the state shown.
- the first imaging optical system L1 and the second imaging optical system L2 are both off-axial optical systems having five free-form reflecting surfaces.
- the space between the optical surfaces in each imaging optical system is filled with air.
- Each reflecting surface is a mirror made of metal, glass, plastic or the like.
- the reflective surface can be formed by vapor-depositing a material having high reflectivity in a visible light region or an infrared light region such as silver or aluminum on a substrate.
- the region through which the light beam imaged by the first imaging optical system L1 passes is larger than the region through which the light beam imaged by the second imaging optical system L2 passes. For this reason, there is a space in which the second imaging optical system L2 can be accommodated inside the first imaging optical system L1.
- the light incident on the first surface R10 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R11 to the sixth surface R15, and the image surface. Imaging with IMG.
- the first surface R10 corresponds to the opening (aperture stop) SP1 in FIGS.
- the first surface R10 corresponds to the entrance pupil of the first imaging optical system L1.
- the aperture diameter of the aperture (aperture stop) SP1 may be variable.
- M1 shown in FIG. 2A indicates an intermediate imaging plane in the first imaging optical system L1.
- the light incident on the first surface R20 of the second imaging optical system L2 is reflected in order while converging or diverging from the second surface R21 to the sixth surface R25, and the image surface. Imaging with IMG.
- the first surface R20 corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d).
- the first surface R20 corresponds to the entrance pupil of the second imaging optical system L2.
- the aperture diameter of the aperture (aperture stop) SP2 may be variable as in the aperture SP1.
- M2 shown in FIG. 2B indicates an intermediate imaging plane in the second imaging optical system L2.
- FIG. 2C is a cross-sectional view when the second imaging optical system L2 is inserted into the first imaging optical system L1.
- the XY coordinates of the centers of the first surfaces R10 (opening portion SP1) and R20 (opening portion SP2) of the first imaging optical system L1 and the second imaging optical system L2 coincide with each other.
- the first image forming optical system L1 and the second image forming optical system L2 are arranged so that their image planes coincide with the image plane IMG.
- the optical path of the first imaging optical system L1 is blocked by the second imaging optical system L2.
- the light incident on the first surface R10 (opening SP1) of the first imaging optical system L1 does not reach the sixth surface R15 from the second surface R11 of the first imaging optical system L1.
- Part of the light incident on the first surface R10 (opening SP1) of the first imaging optical system L1 enters the first surface R20 (opening SP2) of the second imaging optical system L2, and then The light is reflected from the second surface R21 to the sixth surface R25 and reaches the image surface IMG. That is, an image by the second imaging optical system L2 is formed on the image plane IMG.
- the first imaging optical system L2 in the state in which the second imaging optical system L2 is retracted from the space inside the first imaging optical system L1 (FIG. 2A), the first imaging optical on the image plane IMG. An image is formed by the system L1. That is, in this case, the first imaging optical system is used.
- the second imaging optical system L2 in a state where the second imaging optical system L2 is inserted into the space inside the first imaging optical system L1 (FIG. 2C), the second imaging optical system L2 is present on the image plane IMG. An image is formed. That is, the second imaging optical system L2 is used.
- 3 (a) and 3 (b) show distortion of the imaging optical system of the present embodiment.
- 3A shows distortion in the first imaging optical system L1
- FIG. 3B shows distortion in the second imaging optical system L2.
- the horizontal axis is the coordinate value on the image plane IMG in the X-axis direction (corresponding to the X angle of view (X FOV))
- the vertical axis is on the image plane in the Y-axis direction. Coordinate values (equivalent to Y angle of view (Y FOV)).
- Y FOV Y angle of view
- an ideal lattice without distortion Paraxial FOV
- Actual FOV actual ray tracing result lattice
- FIGS. 4A and 4B are lateral aberration diagrams of the imaging optical system of the present example.
- 4A is a lateral aberration diagram of the first imaging optical system L1
- FIG. 4B is a lateral aberration diagram of the second imaging optical system L2.
- the lateral aberration diagrams shown in FIGS. 4A and 4B are shown with respect to positions 1 to 5 on the image sensor shown in FIG.
- the horizontal axis represents the X axis or Y axis on the pupil plane
- the vertical axis represents the amount of aberration on the image plane.
- the wavelength of the evaluation light beam is d-line.
- ⁇ is a half angle of view.
- a lateral aberration is shown on a scale of ⁇ 0.0025 mm.
- the focal length of the first imaging optical system L1 is 71.65 mm, and the F number is 8.0.
- the focal length of the second imaging optical system L2 is 17.91 mm, and the F number is 8.0.
- the field angle of the first imaging optical system L1 and the field angle of the second imaging optical system L2 are different from each other. As a result, it is possible to switch the angle of view taken by switching the imaging optical system described above.
- a zoom lens that moves the lens included in the optical system in the optical axis direction is known, but a complicated mechanism is required because it is necessary to move multiple lenses along different trajectories Met. In addition, since it is necessary to move the lens along the movement trajectory, the angle of view cannot be switched instantaneously.
- the angle of view can be switched instantaneously, but the imaging performance after insertion of the extender depends on the imaging performance of the master lens. It has been difficult to change the angle of view while maintaining image performance.
- the angle of view of the first imaging optical system L1 and the second imaging optical system L2 in the imaging apparatus 100 of the present embodiment can be instantaneously switched with a simple mechanism.
- the imaging apparatus 100 according to the present embodiment changes the angle of view by switching the imaging optical system itself, each imaging optical system can be individually designed to switch the angle of view while obtaining high imaging performance. Is possible.
- the second imaging optical system L2 is preferably configured to have a wider angle of view than the first imaging optical system L1.
- the optical path length of the imaging optical system becomes longer as the angle of view becomes narrower. Therefore, even if a reflection surface is provided in the imaging optical system and the optical path is bent, the imaging optical system is likely to be enlarged as the angle of view becomes narrower. For this reason, the design of the first imaging optical system L1 can be facilitated by setting the second imaging optical system L2 that can be inserted into the first imaging optical system L1 to have a wider angle. It becomes.
- the first imaging optical system L1 is preferably configured to include a plurality of reflecting surfaces, and the space between the reflecting surfaces is preferably filled with gas (air). Such a configuration is called a hollow mirror configuration.
- the second imaging optical system L2 can be inserted into the first imaging optical system L1 while improving the imaging performance of the first imaging optical system L1. Space can be secured.
- the first image-forming optical system L1 may be composed only of a reflecting surface.
- it does not have a refracting surface having optical power, it is assumed that it is composed only of a reflecting surface even if a diaphragm surface or a cover glass that does not contribute to light image formation is provided. This makes it easy to secure a sufficient space for housing the second imaging optical system.
- the first imaging optical system L1 can be configured to be lightweight, the imaging device 100 can be reduced in weight.
- the first imaging optical system L1 includes at least one free-form reflecting surface.
- the second imaging optical system L2 includes at least one free-form reflecting surface. This makes it possible to easily correct aberrations caused by the eccentric arrangement of the reflecting surfaces in each imaging optical system.
- the entrance pupil position of the first imaging optical system L1 is closer to the object side than the reflecting surface closest to the object side.
- the opening SP1 that functions as an aperture stop corresponds to the entrance pupil. This can prevent an excessive increase in the size of each reflecting surface in the first imaging optical system L1.
- the incident light and the reflected light on each reflecting surface can pass through the same space, downsizing is facilitated. Note that the entrance pupil position does not necessarily coincide with the opening SP1.
- the imaging apparatus 100 can be configured more compactly.
- the image sensor may be movable. For example, focusing may be performed by moving the image sensor in the direction of the reference axis and moving the image sensor.
- the focus mechanism can be shared by the first imaging optical system L1 and the second imaging optical system L2. Further, when the positions of the image planes of the first imaging optical system L1 and the second imaging optical system L2 are different in the reference axis direction, the image pickup device is moved in accordance with the switching of the imaging optical system.
- the image sensor may be movable in the xz plane, and camera shake correction (image blur correction) may be performed by moving the image sensor.
- the image stabilization mechanism can be shared by the first imaging optical system L1 and the second imaging optical system L2.
- At least one of the first imaging optical system L1 and the second imaging optical system L2 has at least one intermediate imaging plane that forms a real image in the optical path at a position different from the image plane IMG. It is preferable to have one.
- the imaging optical system By providing an intermediate imaging plane in the imaging optical system, it is possible to suppress excessive spread of the light beam in the optical system. As a result, the shape and angle of view of the imaging optical system can be easily controlled, and an imaging optical system having desired characteristics can be configured without being excessively large.
- the open F numbers for the axial light beams of the first imaging optical system L1 and the second imaging optical system L2 are the same. Thereby, when the imaging optical system is switched between the first imaging optical system L1 and the second imaging optical system L2, the brightness of the acquired image can be made constant. If the difference between the open F numbers of the first image forming optical system L1 and the second image forming optical system L2 is less than 1 ⁇ 2, the open F numbers can be regarded as the same.
- the “axial light beam” is a light beam that forms an image at the center of the image plane. That is, the axial light beam includes the reference axis light beam.
- an optical element such as a cover glass or a lens having a transmittance characteristic that transmits light having a wavelength necessary for imaging may be added to positions near the openings SP1 and SP2 and the image plane IMG. By doing so, it is possible to prevent dust and dust from adhering in the first image forming optical system L1 and the second image forming optical system L2 and the image pickup device.
- a common optical system can be added to the first imaging optical system L1 and the second imaging optical system L2.
- a close-up lens that enables close-up photography can be attached to the object side of the opening SP1, or an extender for changing the magnification can be inserted and removed near the image plane IMG.
- Example 2 Next, Example 2 will be described.
- the image pickup apparatus according to the present embodiment is different from the first embodiment in that a third image forming optical system is further provided in addition to the first image forming optical system L1 and the second image forming optical system L2. Since the first imaging optical system L1 and the second imaging optical system L2 in the present embodiment are the same as those in the first embodiment, description thereof is omitted.
- FIGS. 6 (a) to 6 (c) are schematic views showing the imaging apparatus 100 of the present embodiment.
- FIG. 5A is a diagram of the imaging device 100 in a state where the second imaging optical system L2 is used as seen from a direction parallel to the Z axis.
- FIG. 5B is a diagram of the imaging apparatus 100 in a state in which the first imaging optical system L1 is used as seen from a direction parallel to the Z axis.
- FIG. 5C is a diagram of the imaging device 100 in a state where the third imaging optical system L3 is used as seen from a direction parallel to the Z axis.
- FIG. 6A is a perspective view of the imaging apparatus 100 corresponding to FIG. 5A
- FIG. 6B is a perspective view of the imaging apparatus 100 corresponding to FIG. 5B
- FIG. ) Is a perspective view of the imaging apparatus 100 corresponding to FIG.
- the third imaging optical system L3 in this embodiment is configured to be larger than the first imaging optical system L1.
- the first imaging optical system can be inserted into the third imaging optical system L3.
- the first imaging optical system from the inside of the third imaging optical system L3 is used.
- L1 and the second imaging optical system L2 are retracted, and the optical path of the third imaging optical system L3 is validated. That is, light incident from the aperture SP3 of the third imaging optical system L3 (which also functions as an aperture stop of the third imaging optical system L3) is transmitted through each optical surface of the third imaging optical system L3. An image is formed on the image plane IMG while being converged or diverged.
- the present invention even if there are three or more imaging optical systems to be switched, it is possible to effectively use the space in the housing while enabling switching of the imaging optical system to be used.
- 5C and 6C show a state in which the second imaging optical system L2 is retracted from the optical path of the first imaging optical system L1, the third result is shown.
- the second imaging optical system L2 may be inserted into the first imaging optical system L1.
- the space for disposing the imaging optical system in the imaging apparatus 100 can be further reduced, and further miniaturization can be achieved.
- FIG. 7A is a cross-sectional view of the third imaging optical system L3 in the present embodiment.
- FIG. 7B shows a state in which the first imaging optical system L1 and the second imaging optical system L2 are inserted into the third imaging optical system L3 in this embodiment (FIGS. 5A and 6). It is sectional drawing of the state shown to (a).
- FIG. 7C is a cross section of a state in which the first imaging optical system L1 is inserted into the third imaging optical system L3 in this embodiment (the state shown in FIGS. 5B and 6B).
- the third imaging optical system L3 is an Off-Axial optical system having five reflecting surfaces. Also in this embodiment, the space between the optical surfaces in each imaging optical system is filled with air.
- the region through which the light beam imaged by the third imaging optical system L3 passes is larger than the region through which the light beam imaged by the first imaging optical system L1 passes. For this reason, a space in which the first imaging optical system L1 can be accommodated is provided inside the third imaging optical system L3.
- the light incident on the first surface R30 of the third imaging optical system L3 is reflected in order while converging or diverging from the second surface R31 to the sixth surface R35, and the image surface. Imaging with IMG.
- the first surface R30 corresponds to the opening (aperture stop) SP3 in FIGS. 5 (a) to 5 (c).
- the first surface R30 corresponds to the entrance pupil of the third imaging optical system L3.
- the aperture diameter of the aperture (aperture stop) SP3 may be variable.
- M3 shown in FIG. 7A indicates an intermediate imaging plane in the third imaging optical system L3.
- the aperture The light incident from the part SP3 does not reach the sixth surface R35 from the second surface R31 of the third imaging optical system L3.
- the light incident from the opening SP3 is imaged on the image plane IMG by the imaging optical system arranged on the innermost side. That is, the imaging optical system to be used can be switched by inserting and removing the imaging optical system.
- FIG. 8 shows distortion of the third imaging optical system L3 of the present embodiment.
- the distortion of the third imaging optical system L3 is extremely small as shown in FIG.
- FIG. 9 shows a lateral aberration diagram of the third imaging optical system L3 of the present example.
- the lateral aberration diagram shown in FIG. 9 is shown with respect to positions 1 to 5 on the image sensor shown in FIG.
- the focal length of the third imaging optical system L3 is 214.95 mm, and the F number is 11.0.
- an optical element such as a cover glass or a lens having a transmittance characteristic that transmits a wavelength necessary for imaging may be added at a position near the opening SP3. Thereby, it is possible to prevent dust and dirt from adhering to the inside of the third imaging optical system L3 and the image sensor.
- the imaging apparatus of the present embodiment has two imaging optical systems as in the first embodiment.
- the appearance of the image pickup apparatus of the present embodiment is the same as that shown in FIGS. 1 (a) to 1 (d).
- the optical characteristics of the two imaging optical systems in this embodiment are different from those in the first embodiment.
- the second imaging optical system that is inserted into and extracted from the first imaging optical system is not a hollow mirror structure, but is composed of a solid prism having a plurality of reflecting surfaces.
- the optical path length can be increased, and the second imaging optical system can be further miniaturized. As a result, there is a merit that it is easy to insert and remove from the first imaging optical system.
- the first imaging optical system L1 is an off-axial optical system having four free-form reflecting surfaces.
- the space between the optical surfaces in the first imaging optical system is filled with air.
- the second imaging optical system L2 is an off-axial optical system having four free-form curved reflecting surfaces and two free-form refracting surfaces.
- FIG. 10A is a sectional view of the first imaging optical system L1 in the present embodiment.
- FIG. 10B is a cross-sectional view of the second imaging optical system L2 in the present embodiment.
- FIG. 10C is a cross-sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
- the light incident on the first surface R40 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R41 to the fifth surface R44, and the image surface. Imaging with IMG.
- the first surface R40 is an entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d).
- the light incident on the first surface R50 that is a refractive surface is sequentially converged or diverged from the second surface R51 to the fifth surface R54. Reflected. Then, the light passes through the sixth surface R55, which is a refractive surface, and forms an image on the image surface IMG.
- the first surface R50 is an entrance pupil of the second imaging optical system L2, and corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d).
- An aperture stop having a variable aperture diameter may be provided on the object side of the first surface R50.
- M5 shown in FIG. 10B indicates an intermediate imaging plane in the second imaging optical system L2.
- FIG. 10C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1.
- the first imaging optical system L1 and the second imaging optical system L2 have the same XY coordinates of the center of the first surface R40 (opening SP1) and the center of R50 (opening SP2). To be arranged. Further, the first imaging optical system L1 and the second imaging optical system L2 are arranged so that their image planes coincide with the image plane IMG.
- FIGS. 11A and 11B show distortion of the imaging optical system of the present embodiment.
- FIG. 11A shows distortion in the first imaging optical system L1
- FIG. 11B shows distortion in the second imaging optical system L2.
- the distortion of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment is extremely small as shown in FIGS. 11 (a) and 11 (b).
- FIGS. 12A and 12B show lateral aberration diagrams of the imaging optical system of the present example.
- FIG. 12A is a lateral aberration diagram of the first imaging optical system L1
- FIG. 12B is a lateral aberration diagram of the second imaging optical system L2.
- the lateral aberration diagram shown in FIG. 12A is shown for positions 1 to 5 on the image sensor shown in FIG.
- the lateral aberration diagram shown in FIG. 12B is shown with respect to positions 1 to 5 on the image sensor shown in FIG.
- the focal length of the first imaging optical system L1 of the present example is 71.65 mm, and the F number is 8.0.
- the focal length of the second imaging optical system L2 is 17.91 mm, and the F number is 8.0.
- the imaging apparatus of the present embodiment has two imaging optical systems as in the first and third embodiments.
- the appearance of the image pickup apparatus according to the present embodiment is the same as that shown in FIGS. 1A to 1D except for the size relationship between the diameters of the openings.
- the optical characteristics of the two imaging optical systems in this embodiment are different from those in the first and third embodiments.
- the field angle of the first imaging optical system in the present embodiment is larger than the field angle of the second imaging optical system.
- the opening for capturing light into the first imaging optical system (also functions as an aperture stop) is more than the opening for capturing light into the second imaging optical system (also functions as an aperture stop). Is also small.
- the first imaging optical system L1 is an off-axial optical system having five free-form reflecting surfaces.
- the second imaging optical system L2 is an Off-Axial optical system having five free-form reflecting surfaces.
- FIG. 13A is a sectional view of the first imaging optical system L1 in the present embodiment.
- FIG. 13B is a cross-sectional view of the second imaging optical system L2 in the present embodiment.
- FIG. 13C is a cross-sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
- the light incident on the first surface R60 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R61 to the sixth surface R65, and the image surface. Imaging with IMG.
- the first surface R60 is the entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d).
- M6 shown in FIG. 13A indicates an intermediate imaging plane in the first imaging optical system L1.
- the light incident on the first surface R70 is reflected in order while converging or diverging from the second surface R71 to the sixth surface R75, and the image An image is formed on the surface IMG.
- the first surface R70 is an entrance pupil of the second imaging optical system L2, and corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d).
- M7 shown in FIG. 13B indicates an intermediate imaging plane in the second imaging optical system L2.
- FIG. 13C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1.
- the first imaging optical system L1 and the second imaging optical system L2 have the same XY coordinates of the center of the first surface R60 (opening SP1) and the center of R70 (opening SP2). To be arranged. Further, the first imaging optical system L1 and the second imaging optical system L2 are arranged so that their image planes coincide with the image plane IMG.
- the diameter of the first surface R60 (opening SP1) of the first imaging optical system L1 is the same as that of the first surface R70 (opening SP2) of the second imaging optical system L2. Smaller than the diameter. Therefore, the diameter of the opening SP1 in the first imaging optical system L1 is configured to be variable, and the second imaging optical system L2 is the first imaging optical system L1 as shown in FIG. 13C. It is preferable to increase the diameter of the opening SP1 when inserted into the inside. Alternatively, another opening having an opening diameter larger than that of the opening SP1 is provided, and when the second imaging optical system L2 is inserted into the first imaging optical system L1, the opening SP1 is replaced with another opening. You may comprise so that it may switch to a part. As a result, the light beam imaged by the second imaging optical system L2 is not scattered by the first imaging optical system L1.
- FIGS. 14A and 14B show the distortion of the imaging optical system of the present embodiment.
- FIG. 14A shows distortion in the first imaging optical system L1
- FIG. 14B shows distortion in the second imaging optical system L2.
- the distortions of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment are extremely small as shown in FIGS. 14 (a) and 14 (b).
- FIGS. 15A and 15B are lateral aberration diagrams of the imaging optical system of the present example.
- FIG. 15A is a lateral aberration diagram of the first imaging optical system L1
- FIG. 15B is a lateral aberration diagram of the second imaging optical system L2.
- the lateral aberration diagrams shown in FIGS. 15A and 15B are shown with respect to positions 1 to 5 on the image sensor shown in FIG.
- the focal length of the first imaging optical system L1 of the present embodiment is 17.91 mm, and the F number is 5.97.
- the focal length of the second imaging optical system L2 is 71.65 mm, and the F number is 8.0.
- Example 5 Next, Example 5 will be described.
- the imaging apparatus of the present embodiment has two imaging optical systems as in the first, third, and fourth embodiments.
- the appearance of the image pickup apparatus of the present embodiment is the same as that shown in FIGS. 1 (a) to 1 (d).
- the optical characteristics of the two imaging optical systems in the present embodiment are different from those in the first, third, and fourth embodiments.
- the second imaging optical system that is inserted into and extracted from the first imaging optical system is composed of a plurality of lenses and prisms.
- the first imaging optical system L1 is an off-axial optical system having four free-form reflecting surfaces.
- the second imaging optical system L2 is an Off-Axial optical system including four spherical lenses and one triangular prism.
- FIG. 16A is a cross-sectional view of the first imaging optical system L1 in the present embodiment.
- FIG. 16B is a cross-sectional view of the second imaging optical system L2 in the present embodiment.
- FIG. 16C is a sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
- the light incident on the first surface R80 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R81 to the fifth surface R84, and the image surface. Imaging with IMG.
- the first surface R80 is the entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d).
- the second imaging optical system L2 is arranged in order from the object side to the image side, and a meniscus positive lens having a convex surface facing the image side, a meniscus negative lens having a convex surface facing the image side, and a reflecting surface A triangular prism, a biconvex positive lens, and a negative lens with a convex surface facing the image side.
- the positive lens disposed closest to the object side in the second imaging optical system L2 also serves as an aperture stop and corresponds to an entrance pupil.
- the second imaging optical system L2 of the present embodiment configured to include a refractive optical element has an advantage that it is easy to manufacture compared to a reflective optical system having a plurality of free-form surfaces.
- FIG. 16C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1.
- FIGS. 17A and 17B show distortion of the imaging optical system of the present embodiment.
- FIG. 17A shows distortion in the first imaging optical system L1
- FIG. 17B shows distortion in the second imaging optical system L2.
- the distortions of the first imaging optical system L1 and the second imaging optical system L2 of this embodiment are extremely small as shown in FIGS. 17 (a) and 17 (b).
- FIGS. 18A and 18B are lateral aberration diagrams of the imaging optical system of this example.
- FIG. 18A is a lateral aberration diagram of the first imaging optical system L1
- FIG. 18B is a lateral aberration diagram of the second imaging optical system L2.
- the lateral aberration diagram shown in FIG. 18A is shown for positions 1 to 5 on the image sensor shown in FIG.
- the lateral aberration diagram shown in FIG. 18B is shown for positions 1 to 5 on the image circle shown in FIG.
- the focal length of the first imaging optical system L1 of the present example is 71.65 mm, and the F number is 8.0.
- the focal length of the second imaging optical system L2 is 17.91 mm, and the F number is 8.0.
- Each numerical example is in a state of focusing on an object at infinity.
- the surface data indicates the coordinates (mm) in the absolute coordinate system of the points on the reference axis in each surface and the tilt angle (°) of the surface, excluding the second imaging optical system of Numerical Example 5.
- Di is a scalar quantity representing the distance between the origins of the local coordinates of the i-th surface and the (i + 1) -th surface.
- i is the order of the surfaces from the object side
- ri is the radius of curvature of the i-th surface from the object side
- di is the i-th surface from the object side.
- Ndi and ⁇ di represent the refractive index and Abbe number of the optical member between the i-th surface and the (i + 1) -th surface.
- BF is the back focus in terms of air.
- E—X represents 10 —X .
- the spherical shape is expressed by the following equation (1), where ri is the radius of curvature of the i-th surface and x and y are coordinates in each local coordinate system of the i-th surface.
- the free-form surface shape is expressed by the following equation (2).
- Equation (2) is only an even-order term with respect to x, the free-form surface defined by Equation (2) has a plane-symmetric shape with the yz plane as the symmetry plane.
- the angle of view is ⁇ 1.86 ° in the X direction and ⁇ 2.48 ° in the Y direction.
- the focal length is 71.65 mm in the X direction and 71.65 mm in the Y direction.
- the image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
- the first surface R10 is circular and has a diameter of 8.96 mm.
- the F value in the X axis direction is 8.00
- the F value in the Y axis direction is 8.00.
- the angle of view is ⁇ 7.40 ° in the X direction and ⁇ 9.82 ° in the Y direction.
- the focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
- the image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
- the first surface R20 is circular and has a diameter of 2.24 mm.
- the F value in the X axis direction is 8.00
- the F value in the Y axis direction is 8.00.
- the angle of view is ⁇ 0.62 ° in the X direction and ⁇ 0.83 ° in the Y direction.
- the focal length is 214.98 mm in the X direction and 214.95 mm in the Y direction.
- the image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
- the first surface R30 is circular and has a diameter of 19.5 mm.
- the F value in the X-axis direction is 11.02
- the F value in the Y-axis direction is 11.02.
- the angle of view is ⁇ 2.48 ° in the X direction and ⁇ 1.86 ° in the Y direction.
- the focal length is 71.63 mm in the X direction and 71.65 mm in the Y direction.
- the image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
- the first surface R40 is circular and has a diameter of 8.96 mm.
- the F value in the X axis direction is 8.00
- the F value in the Y axis direction is 8.00.
- the angle of view is ⁇ 9.82 ° in the X direction and ⁇ 7.40 ° in the Y direction.
- the focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
- the image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
- the first surface R50 is circular and has a diameter of 2.24 mm.
- the F value in the X axis direction is 8.00
- the F value in the Y axis direction is 8.00.
- the angle of view is ⁇ 7.40 ° in the X direction and ⁇ 9.82 ° in the Y direction.
- the focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
- the image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
- the first surface R60 is circular and has a diameter of 3.00 mm.
- the F value in the X axis direction is 5.97
- the F value in the Y axis direction is 5.97.
- the angle of view is ⁇ 1.86 ° in the X direction and ⁇ 2.48 ° in the Y direction.
- the focal length is 71.65 mm in the X direction and 71.65 mm in the Y direction.
- the image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
- the first surface R70 is circular and has a diameter of 8.96 mm.
- the F value in the X axis direction is 7.9
- the F value in the Y axis direction is 7.9.
- the angle of view is ⁇ 2.48 ° in the X direction and ⁇ 1.86 ° in the Y direction.
- the focal length is 71.63 mm in the X direction and 71.65 mm in the Y direction.
- the image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
- the first surface R80 is circular and has a diameter of 8.96 mm.
- the F value in the X-axis direction is 7.99, and the F value in the Y-axis direction is 8.00.
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Abstract
Description
本発明は、光学装置に関し、デジタルカメラ、監視カメラ、車載カメラや、ドローン等のUAV(Unmanned Aerial Vehicle)に搭載されるカメラに好適なものである。 The present invention relates to an optical device, and is suitable for a digital camera, a surveillance camera, an in-vehicle camera, and a camera mounted on a UAV (Unmanned Aerial Vehicle) such as a drone.
複数の結像光学系を有し、撮影に使用する結像光学系を切り替えることが可能な撮像装置が知られている。 An imaging apparatus having a plurality of imaging optical systems and capable of switching the imaging optical system used for photographing is known.
特許文献1には、2つの結像光学系を有し、1つの撮像素子を移動させることによって撮影に用いる結像光学系を異ならせることのできる撮像装置が記載されている。
しかしながら特許文献1に記載の撮像装置では、複数の結像光学系を固定し撮像素子を移動させる構成であるため、使用されていない結像光学系のための筐体内のスペースは常に無駄となっていた。
However, since the imaging apparatus described in
そこで本発明は、複数の結像光学系を切り替え可能としつつ、筐体内のスペースを有効に活用できる光学装置を実現することを目的とする。 Therefore, an object of the present invention is to realize an optical device that can effectively use a space in a housing while allowing a plurality of imaging optical systems to be switched.
本発明の光学装置は、第1及び第2の結像光学系を有し、前記第1及び第2の結像光学系を切り替えて使用可能な光学装置であって、前記第1の結像光学系が使用される状態において、前記第2の結像光学系は前記第1の結像光学系の光路を遮らない位置に配置され、前記第2の結像光学系が使用される状態において、前記第2の結像光学系は前記光路を遮る位置に配置されることを特徴とする。 The optical apparatus of the present invention includes first and second imaging optical systems, and is an optical apparatus that can be used by switching between the first and second imaging optical systems. In a state in which the optical system is used, the second imaging optical system is disposed at a position that does not block an optical path of the first imaging optical system, and in a state in which the second imaging optical system is used. The second imaging optical system is disposed at a position that blocks the optical path.
また、本発明の他の光学装置は、第1及び第2の結像光学系と、撮像素子を有し、前記第1及び第2の結像光学系を切り替えて使用可能な光学装置であって、前記第1の結像光学系と前記第2の結像光学系のいずれが使用される場合であっても、前記撮像素子を用いて画像が取得され、前記切り替えは、前記第1及び第2の結像光学系の相対位置関係を、前記第1の結像光学系によって結像される光線が通る空間から前記第2の結像光学系が退避された状態と、前記空間内に前記第2の結像光学系が挿入された状態との間で変化させることによって行われ、前記切り替えの前後で、前記第1の結像光学系と前記撮像素子の相対位置関係は変化しないことを特徴とする。 In addition, another optical device of the present invention is an optical device that includes first and second imaging optical systems and an imaging device, and can be used by switching between the first and second imaging optical systems. Thus, regardless of which of the first imaging optical system and the second imaging optical system is used, an image is acquired using the imaging device, and the switching is performed using the first and second imaging optical systems. The relative positional relationship of the second imaging optical system is determined so that the second imaging optical system is retracted from the space through which the light beam imaged by the first imaging optical system passes, It is performed by changing between the state in which the second imaging optical system is inserted, and the relative positional relationship between the first imaging optical system and the imaging element does not change before and after the switching. It is characterized by.
本発明によれば、複数の結像光学系を切り替え可能としつつ、筐体内のスペースを有効に活用できる光学装置を提供することができる。 According to the present invention, it is possible to provide an optical device that can effectively use the space in the housing while allowing a plurality of imaging optical systems to be switched.
本発明の光学装置の実施例に関する説明に先立ち、本願明細書における種々の定義について述べる。 Prior to the description of the embodiments of the optical apparatus of the present invention, various definitions in the present specification will be described.
図19は、各実施形態の結像光学系を説明する際に用いられる座標系を説明する図である。本願明細書では、物体側(被写体側)から像側(撮像素子に形成される像面側)に向かって、不図示の瞳(絞り)の中心を通って像面の中心に至る1つの光線を中心主光線または基準軸光線と定義する。中心主光線(基準軸光線)は、図19中に一点鎖線で示されている。 FIG. 19 is a diagram illustrating a coordinate system used when describing the imaging optical system of each embodiment. In the specification of the present application, one light beam that passes from the object side (subject side) toward the image side (image plane side formed on the image sensor) through the center of a pupil (aperture) (not shown) and reaches the center of the image plane. Is defined as the central chief ray or reference axis ray. The central principal ray (reference axis ray) is indicated by a one-dot chain line in FIG.
また、中心主光線(基準軸光線)が辿る経路を基準軸と定義する。 Also, the path followed by the central principal ray (reference axis ray) is defined as the reference axis.
図19において、基準軸に沿って物体側からi番目の光学面(第i面)を第i面Riとする。図19において、第1面R1は絞り面(入射瞳部)、第2面R2は第1面R1に対してチルトした反射面、第3面R3及び第4面R4はそれぞれの前の面に対してシフト及びチルトした反射面である。 In FIG. 19, the i-th optical surface (i-th surface) from the object side along the reference axis is the i-th surface Ri. In FIG. 19, the first surface R1 is the stop surface (incidence pupil part), the second surface R2 is the reflecting surface tilted with respect to the first surface R1, and the third surface R3 and the fourth surface R4 are the respective front surfaces. The reflecting surface is shifted and tilted with respect to the reflecting surface.
後述する各実施形態における第1の結像光学系と第2の結像光学系のうち少なくとも1つはOff-Axial光学系である。Off-Axial光学系を構成する各面は共通の光軸を有さない。そこで、第1面R1の中心を原点とする絶対座標系を設定する。原点の位置は第1面R1(絞り面または入射瞳部)の中心位置に相当する。したがって、基準軸は絶対座標系の原点を通る。 At least one of the first imaging optical system and the second imaging optical system in each embodiment to be described later is an off-axial optical system. Each surface constituting the Off-Axial optical system does not have a common optical axis. Therefore, an absolute coordinate system with the center of the first surface R1 as the origin is set. The position of the origin corresponds to the center position of the first surface R1 (the stop surface or the entrance pupil). Therefore, the reference axis passes through the origin of the absolute coordinate system.
中心主光線(基準軸光線)は、第1面R1の中心(絶対座標系の原点)を通り最終面(像面)の中心へ至るまでに、各光学面で屈折または反射される。基準軸は、各光学面で順番に折れ曲がりながら最終面まで伸びている。以下の説明において、像面側及び物体側とはそれぞれ、基準軸に沿っていずれの側であるかを意味している。 The central principal ray (reference axis ray) passes through the center of the first surface R1 (the origin of the absolute coordinate system) and reaches the center of the final surface (image surface), and is refracted or reflected by each optical surface. The reference axis extends to the final surface while bending in turn on each optical surface. In the following description, the image plane side and the object side mean which side is along the reference axis.
絶対座標系において、原点を通り第1面から伸びる基準軸に平行な直線をZ軸と呼ぶ(第1面から第2面に向かう方向を正とする)。また、原点を通り右手座標系の定義に従ってZ軸に対して反時計回り方向に90゜をなす図19の紙面内の軸をY軸と呼ぶ。また、原点を通りZ軸及びY軸に垂直な直線をX軸と呼ぶ(図19の紙面奥に向かう方向を正とする)。 In the absolute coordinate system, a straight line passing through the origin and parallel to the reference axis extending from the first surface is called the Z-axis (the direction from the first surface toward the second surface is positive). Further, the axis in the paper of FIG. 19 that passes through the origin and forms 90 ° counterclockwise with respect to the Z-axis in accordance with the definition of the right-handed coordinate system is called the Y-axis. A straight line that passes through the origin and is perpendicular to the Z-axis and the Y-axis is referred to as an X-axis (the direction toward the back of the page in FIG. 19 is positive).
また、結像光学系において第1面R1以降の光学面の面形状及びチルト角を表すためにローカル座標系を定義する。ローカル座標系は第1面R1以降の各光学面に対してそれぞれ定義される。各実施例の結像光学系における光学面の面形状はローカル座標で表して説明する。 In addition, a local coordinate system is defined to represent the surface shape and tilt angle of the optical surface after the first surface R1 in the imaging optical system. A local coordinate system is defined for each optical surface after the first surface R1. The surface shape of the optical surface in the imaging optical system of each embodiment will be described using local coordinates.
ローカル座標系の原点は基準軸と第i面Riが交差する点とする。 The origin of the local coordinate system is the point where the reference axis and the i-th surface Ri intersect.
第i面Riのローカル座標系におけるz軸は第i面の基準軸上の点における面法線である。ローカル座標系におけるy軸はローカル座標の原点を通り、右手座標系の定義に従ってz方向に対し反時計方向に90゜をなす図19の紙面内の軸である。ローカル座標系のx軸はローカル座標の原点を通り、z軸及びy軸に垂直な直線である。 The z axis in the local coordinate system of the i-th surface Ri is a surface normal at a point on the reference axis of the i-th surface. The y axis in the local coordinate system passes through the origin of the local coordinate and is an axis in the plane of FIG. 19 that forms 90 ° counterclockwise with respect to the z direction according to the definition of the right hand coordinate system. The x-axis of the local coordinate system is a straight line that passes through the origin of the local coordinates and is perpendicular to the z-axis and the y-axis.
第i面のyz面内でのチルト角θxi(°)は、ローカル座標系のz軸が第i-1面から伸びる基準軸に対してyz面内で成す鋭角である(反時計回り方向を正)。また、第i面のxz面内でのチルト角θyi(°)は、z軸がi-1面から伸びる基準軸に対してxz面内で成す鋭角である(反時計回り方向を正)。図19の各軸の矢印の方向は、各軸の正の方向を表している。 The tilt angle θxi (°) in the yz plane of the i-th surface is an acute angle formed in the yz-plane with respect to the reference axis extending from the i-1th plane in the local coordinate system (counterclockwise direction Positive). The tilt angle θyi (°) in the xz plane of the i-th surface is an acute angle formed in the xz plane with respect to the reference axis extending from the i−1 plane (the counterclockwise direction is positive). The direction of the arrow of each axis in FIG. 19 represents the positive direction of each axis.
次に、本発明の光学装置に関する各実施例について説明する。 Next, each example relating to the optical device of the present invention will be described.
[実施例1]
図1(a)~(d)は、本実施例における光学装置としての撮像装置100の構成を示す概略図である。図2(a)~(c)は、撮像装置100の有する結像光学系の断面図である。
[Example 1]
FIGS. 1A to 1D are schematic views showing a configuration of an
本実施例の撮像装置100は第1の結像光学系L1と、第2の結像光学系L2と、各結像光学系を保持する部材を有する。第2の結像光学系L2を保持する部材は第1の結像光学系L1を保持する部材に対して移動可能に構成されており、撮像装置100は使用する結像光学系を切り替えることができる。
The
本実施例の撮像装置100では、第1の結像光学系L1を使用する際には、第2の結像光学系L2を、第1の結像光学系L1によって結像される光線が通る空間から退避した位置である第1の位置に配置する。一方、使用する光学系を第2の結像光学系L2に切り替える際には、第1の結像光学系L1を使用する際に第1の結像光学系L1によって結像される光線が通る空間内である第2の位置に第2の結像光学系L2が挿入される。
In the
すなわち、第1の結像光学系L1を使用する場合には、第2の結像光学系L2を第1の結像光学系L1の光路を遮らないような位置に配置することで第1の結像光学系L1の光路を有効にする。このとき、物体からの光は第1の結像光学系L1に入射し、第1の結像光学系L1によって結像される。一方。第2の結像光学系L2を使用する場合には、第1の結像光学系L1の光路を遮るような位置に第2の結像光学系L2を配置し、第1の結像光学系L1の光路を無効にしつつ第2の結像光学系L2の光路を有効にする。このとき、物体からの光は第2の結像光学系L2に入射し、第2の結像光学系L2によって結像される。 That is, when the first imaging optical system L1 is used, the first imaging optical system L2 is arranged at a position that does not block the optical path of the first imaging optical system L1. The optical path of the imaging optical system L1 is made effective. At this time, light from the object enters the first imaging optical system L1 and is imaged by the first imaging optical system L1. on the other hand. When the second imaging optical system L2 is used, the second imaging optical system L2 is disposed at a position that blocks the optical path of the first imaging optical system L1, and the first imaging optical system is used. The optical path of the second imaging optical system L2 is validated while invalidating the optical path of L1. At this time, light from the object enters the second imaging optical system L2, and is imaged by the second imaging optical system L2.
このように本実施例では、第1の結像光学系L1と第2の結像光学系L2の相対位置関係を変化させることで使用する結像光学系を切り替える。これによって、第2の結像光学系L2を使用する際には、第2の結像光学系L2は第1の結像光学系L1の内部(第1の結像光学系L1によって結像される光線が通る空間)に収納されるように配置されるため、筐体内のスペースを有効に活用することができる。 Thus, in this embodiment, the imaging optical system to be used is switched by changing the relative positional relationship between the first imaging optical system L1 and the second imaging optical system L2. Thus, when the second imaging optical system L2 is used, the second imaging optical system L2 is imaged inside the first imaging optical system L1 (by the first imaging optical system L1). Therefore, the space in the housing can be used effectively.
図1(a)は、第2の結像光学系L2が使用される状態の撮像装置100をZ軸に平行な方向から見た図である。図1(b)は、第1の結像光学系L1が使用される状態の撮像装置100をZ軸に平行な方向から見た図である。図1(c)は図1(a)に対応する撮像装置100の斜視図であり、図1(d)は図1(b)に対応する撮像装置100の斜視図である。
FIG. 1A is a view of the
ここで、SP1は第1の結像光学系L1によって結像される光が入射する開口部であり、SP2は第2の結像光学系L2によって結像される光が入射する開口部である。SP1及びSP2はそれぞれの結像光学系の絞りとしても機能する。また、IMGは像面である。像面IMGは各結像光学系における最終面に相当する。結像光学系の光路の途中にあるような後述する中間結像面とは異なる。本実施例では像面IMGにはCCDやCMOSセンサなど撮像素子の受光面が配置される。撮像素子は使用される結像光学系に依らず共用される。 Here, SP1 is an opening through which light imaged by the first imaging optical system L1 enters, and SP2 is an opening through which light imaged by the second imaging optical system L2 enters. . SP1 and SP2 also function as a diaphragm of each imaging optical system. IMG is an image plane. The image plane IMG corresponds to the final plane in each imaging optical system. This is different from an intermediate imaging plane described later, which is in the middle of the optical path of the imaging optical system. In this embodiment, a light receiving surface of an image sensor such as a CCD or a CMOS sensor is arranged on the image plane IMG. The image sensor is shared regardless of the imaging optical system used.
なお、本実施例では光学装置としての撮像装置100が撮像素子を有している場合について示しているが、撮像素子は光学装置と別体であっても良い。
In addition, although the present embodiment shows a case where the
図1(a)及び(c)に示すように、第2の結像光学系L2が使用される際には、第1の結像光学系L1の内部に結像光学系L2が収納されるように第2の結像光学系L2が配置されている。このとき、第1の結像光学系L1の光路は第2の結像光学系L2によって遮られているため、第1の結像光学系L1は無効となっている(第1の結像光学系L1には光は入射しない)。このため、像面IMGには第2の結像光学系L2による像が結像される。 As shown in FIGS. 1A and 1C, when the second imaging optical system L2 is used, the imaging optical system L2 is housed inside the first imaging optical system L1. Thus, the second imaging optical system L2 is arranged. At this time, since the optical path of the first imaging optical system L1 is blocked by the second imaging optical system L2, the first imaging optical system L1 is invalid (the first imaging optical system L1). Light does not enter the system L1). For this reason, an image by the second imaging optical system L2 is formed on the image plane IMG.
また、図1(b)及び(d)に示すように、第1の結像光学系L1が使用される際には、第1の結像光学系L1の内部から第2の結像光学系L2が退避することで、第1の結像光学系L1の光路が有効化される。図1(b)及び(d)に示した矢印は、不図示のスライド機構によって第2の結像光学系L2を退避する際の移動方向を示している。このとき、第1の結像光学系L1の光路は有効化されている(第1の結像光学系L1に光が入射するようになっている)ため、像面IMGには第1の結像光学系L1による像が結像される。 Further, as shown in FIGS. 1B and 1D, when the first imaging optical system L1 is used, the second imaging optical system from the inside of the first imaging optical system L1 is used. By retracting L2, the optical path of the first imaging optical system L1 is validated. The arrows shown in FIGS. 1B and 1D indicate the moving direction when the second imaging optical system L2 is retracted by a slide mechanism (not shown). At this time, since the optical path of the first imaging optical system L1 is validated (light is incident on the first imaging optical system L1), the first connection is made on the image plane IMG. An image is formed by the image optical system L1.
なお、第2の結像光学系L2を移動させるための機構は特に限定されない。第2の結像光学系L2の移動は手動で行うようにしても良いし、モーター等の駆動手段によって電気的に行っても良い。バネやゴム等の弾性部材を設け、第1の結像光学系L1の内部への挿入または抜去の一方のみを弾性部材の弾性力で行うようにしても良い。 Note that the mechanism for moving the second imaging optical system L2 is not particularly limited. The movement of the second imaging optical system L2 may be performed manually or electrically by a driving means such as a motor. An elastic member such as a spring or rubber may be provided so that only one of insertion and removal from the inside of the first imaging optical system L1 is performed by the elastic force of the elastic member.
さらに、図1(a)~(d)には第2の結像光学系L2を平行移動することによって第1の結像光学系L1に対して挿抜する機構を例示したが、本発明はこれに限定されない。図21(a)~(d)は第2の結像光学系L2の移動機構の変形例を示す図である。図21(a)~(d)に示すように第1の結像光学系L1と第2の結像光学系L2を軸Pでつなぎ、軸Pを中心に第2の結像光学系L2を回動させることで第1の結像光学系L1に対して挿抜しても良い。 Further, FIGS. 1A to 1D illustrate a mechanism for inserting / removing the second imaging optical system L2 by translating the second imaging optical system L2, but the present invention is not limited to this. It is not limited to. FIGS. 21A to 21D are diagrams showing modifications of the moving mechanism of the second imaging optical system L2. As shown in FIGS. 21A to 21D, the first imaging optical system L1 and the second imaging optical system L2 are connected by the axis P, and the second imaging optical system L2 is centered on the axis P. You may insert / extract with respect to the 1st imaging optical system L1 by rotating.
さらに、第1の結像光学系L1を使用する際に必ずしも第2の結像光学系L2を一体的に第1の結像光学系L1から退避させる必要はない。第1の結像光学系L1を使用する際に第1の結像光学系L1の光路が遮られず、第2の結像光学系L2を使用する際に第1の結像光学系L1の光路が遮られれば良い。このため、第2の結像光学系L2の光学面を反射面で構成し、第1の結像光学系L1を使用する際には第2の結像光学系L2の各光学面のそれぞれを第1の結像光学系L1の光路を遮らないようにチルトまたはシフトするようにしても良い。 Further, when the first imaging optical system L1 is used, it is not always necessary to retract the second imaging optical system L2 integrally from the first imaging optical system L1. When the first imaging optical system L1 is used, the optical path of the first imaging optical system L1 is not blocked, and when the second imaging optical system L2 is used, the first imaging optical system L1 It is sufficient if the light path is blocked. For this reason, the optical surface of the second imaging optical system L2 is constituted by a reflecting surface, and when using the first imaging optical system L1, each optical surface of the second imaging optical system L2 is You may make it tilt or shift so that the optical path of the 1st imaging optical system L1 may not be interrupted.
次に、本実施例の撮像装置100における第1の結像光学系L1及び第2の結像光学系L2について述べる。
Next, the first imaging optical system L1 and the second imaging optical system L2 in the
図2(a)は本実施例における第1の結像光学系L1の断面図である。図2(b)は本実施例における第2の結像光学系L2の断面図である。図2(c)は本実施例の撮像装置100において、第1の結像光学系L1の内部に第2の結像光学系L2が挿入された状態(図1(a)及び(c)に示す状態)の断面図である。
FIG. 2A is a sectional view of the first imaging optical system L1 in the present embodiment. FIG. 2B is a sectional view of the second imaging optical system L2 in the present embodiment. FIG. 2C shows a state in which the second imaging optical system L2 is inserted in the first imaging optical system L1 in the
本実施例において、第1の結像光学系L1と第2の結像光学系L2は共に5面の自由曲面形状の反射面を有するOff-Axial光学系である。本実施例において各結像光学系における光学面間は空気によって満たされている。各反射面は、金属、ガラス、プラスチックなどで構成されるミラーである。反射面は銀やアルミなど可視光領域や赤外光領域などで反射率の高い材料を基板に蒸着して形成することができる。 In this embodiment, the first imaging optical system L1 and the second imaging optical system L2 are both off-axial optical systems having five free-form reflecting surfaces. In this embodiment, the space between the optical surfaces in each imaging optical system is filled with air. Each reflecting surface is a mirror made of metal, glass, plastic or the like. The reflective surface can be formed by vapor-depositing a material having high reflectivity in a visible light region or an infrared light region such as silver or aluminum on a substrate.
第1の結像光学系L1によって結像される光線が通る領域は第2の結像光学系L2によって結像される光線が通る領域よりも大きい。このため、第1の結像光学系L1の内側には第2の結像光学系L2を収納することのできる空間が存在する。 The region through which the light beam imaged by the first imaging optical system L1 passes is larger than the region through which the light beam imaged by the second imaging optical system L2 passes. For this reason, there is a space in which the second imaging optical system L2 can be accommodated inside the first imaging optical system L1.
図2(a)に示すように、第1の結像光学系L1の第1面R10に入射した光は、第2面R11から第6面R15で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R10は図1(a)~(d)における開口部(開口絞り)SP1に相当する。また、第1面R10は第1の結像光学系L1の入射瞳に相当する。開口部(開口絞り)SP1の開口径は可変としても良い。また、図2(a)に示したM1は第1の結像光学系L1における中間結像面を示している。 As shown in FIG. 2A, the light incident on the first surface R10 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R11 to the sixth surface R15, and the image surface. Imaging with IMG. The first surface R10 corresponds to the opening (aperture stop) SP1 in FIGS. The first surface R10 corresponds to the entrance pupil of the first imaging optical system L1. The aperture diameter of the aperture (aperture stop) SP1 may be variable. Further, M1 shown in FIG. 2A indicates an intermediate imaging plane in the first imaging optical system L1.
図2(b)に示すように、第2の結像光学系L2の第1面R20に入射した光は、第2面R21から第6面R25で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R20は図1(a)~(d)における開口部(開口絞り)SP2に相当する。また、第1面R20は第2の結像光学系L2の入射瞳に相当する。開口部(開口絞り)SP2の開口径は、開口部SP1と同様に、可変としても良い。また、図2(b)に示したM2は第2の結像光学系L2における中間結像面を示している。 As shown in FIG. 2B, the light incident on the first surface R20 of the second imaging optical system L2 is reflected in order while converging or diverging from the second surface R21 to the sixth surface R25, and the image surface. Imaging with IMG. The first surface R20 corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d). The first surface R20 corresponds to the entrance pupil of the second imaging optical system L2. The aperture diameter of the aperture (aperture stop) SP2 may be variable as in the aperture SP1. Further, M2 shown in FIG. 2B indicates an intermediate imaging plane in the second imaging optical system L2.
第1の結像光学系L1及び第2の結像光学系L2のより詳しい形状等は、後の数値実施例1において説明する。 More detailed shapes and the like of the first image forming optical system L1 and the second image forming optical system L2 will be described in Numerical Example 1 later.
図2(c)は、第2の結像光学系L2を第1の結像光学系L1の内部に挿入した際の断面図である。このとき本実施例では、第1の結像光学系L1と第2の結像光学系L2の第1面R10(開口部SP1)及びR20(開口部SP2)の中心のXY座標が一致するように配置される。また、本実施例では、第1の結像光学系L1と第2の結像光学系L2はそれぞれの像面が像面IMGに一致するように配置される。 FIG. 2C is a cross-sectional view when the second imaging optical system L2 is inserted into the first imaging optical system L1. At this time, in this embodiment, the XY coordinates of the centers of the first surfaces R10 (opening portion SP1) and R20 (opening portion SP2) of the first imaging optical system L1 and the second imaging optical system L2 coincide with each other. Placed in. In the present embodiment, the first image forming optical system L1 and the second image forming optical system L2 are arranged so that their image planes coincide with the image plane IMG.
図2(c)に示す配置において、第1の結像光学系L1の光路は第2の結像光学系L2によって遮られている。このため第1の結像光学系L1の第1面R10(開口部SP1)に入射した光は第1の結像光学系L1の第2面R11から第6面R15には到達しない。第1の結像光学系L1の第1面R10(開口部SP1)に入射した光の一部は、第2の結像光学系L2の第1面R20(開口部SP2)に入射し、その後第2面R21から第6面R25にて反射され、像面IMGに到達する。すなわち、像面IMGには第2の結像光学系L2による像が形成されることになる。 In the arrangement shown in FIG. 2 (c), the optical path of the first imaging optical system L1 is blocked by the second imaging optical system L2. For this reason, the light incident on the first surface R10 (opening SP1) of the first imaging optical system L1 does not reach the sixth surface R15 from the second surface R11 of the first imaging optical system L1. Part of the light incident on the first surface R10 (opening SP1) of the first imaging optical system L1 enters the first surface R20 (opening SP2) of the second imaging optical system L2, and then The light is reflected from the second surface R21 to the sixth surface R25 and reaches the image surface IMG. That is, an image by the second imaging optical system L2 is formed on the image plane IMG.
このように、第2の結像光学系L2を第1の結像光学系L1の内部の空間から退避させた状態(図2(a))では、像面IMGには第1の結像光学系L1による像が形成される。すなわち、この場合第1の結像光学系が使用される状態となる。一方、第2の結像光学系L2が第1の結像光学系L1の内部の空間に挿入された状態(図2(c))では、像面IMGには第2の結像光学系L2による像が形成される。すなわち第2の結像光学系L2が使用される状態となる。 As described above, in the state in which the second imaging optical system L2 is retracted from the space inside the first imaging optical system L1 (FIG. 2A), the first imaging optical on the image plane IMG. An image is formed by the system L1. That is, in this case, the first imaging optical system is used. On the other hand, in a state where the second imaging optical system L2 is inserted into the space inside the first imaging optical system L1 (FIG. 2C), the second imaging optical system L2 is present on the image plane IMG. An image is formed. That is, the second imaging optical system L2 is used.
次に、本実施例における第1の結像光学系L1及び第2の結像光学系L2の光学特性について述べる。 Next, the optical characteristics of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment will be described.
図3(a)及び(b)に、本実施例の結像光学系のディストーションを示す。図3(a)は第1の結像光学系L1におけるディストーション、図3(b)は第2の結像光学系L2におけるディストーションを表している。図3(a)及び(b)において、横軸はX軸方向の像面IMG上での座標値(X画角(X FOV)に相当)、縦軸はY軸方向の像面上での座標値(Y画角(Y FOV)に相当)である。また、ディストーションの無い理想格子(Paraxial FOV)と実際の光線追跡結果の格子(Actual FOV)を重ねて描いている。ディストーションの大きな光学系ではActual FOVとParaxial FOVの乖離が大きくなるが、本実施例の第1の結像光学系L1及び第2の結像光学系L2のディストーションは図3(a)及び(b)に示すように極めて小さい。 3 (a) and 3 (b) show distortion of the imaging optical system of the present embodiment. 3A shows distortion in the first imaging optical system L1, and FIG. 3B shows distortion in the second imaging optical system L2. 3A and 3B, the horizontal axis is the coordinate value on the image plane IMG in the X-axis direction (corresponding to the X angle of view (X FOV)), and the vertical axis is on the image plane in the Y-axis direction. Coordinate values (equivalent to Y angle of view (Y FOV)). In addition, an ideal lattice without distortion (Paraxial FOV) and an actual ray tracing result lattice (Actual FOV) are drawn in an overlapping manner. In an optical system with a large distortion, the difference between the Actual FOV and the Paraxial FOV is large, but the distortions of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment are shown in FIGS. ) Is extremely small as shown in
図4(a)及び(b)に本実施例の結像光学系の横収差図を示す。図4(a)は第1の結像光学系L1の横収差図、図4(b)は第2の結像光学系L2の横収差図である。図4(a)及び(b)に示す横収差図は、図20(a)に示す撮像素子上の位置1から5に対して示している。図4(a)及び(b)に示す各横収差図において、横軸は瞳面上でのX軸或いはY軸、縦軸は像面上での収差量である。評価光線の波長はd線である。ωは半画角である。収差図では、後述する数値実施例1に示す結像光学系において、横収差±0.0025mmのスケールで示されている。YZ断面において、第1の結像光学系L1の焦点距離は71.65mm、Fナンバーは8.0である。また、YZ断面において、第2の結像光学系L2の焦点距離は17.91mm、Fナンバーは8.0である。
FIGS. 4A and 4B are lateral aberration diagrams of the imaging optical system of the present example. 4A is a lateral aberration diagram of the first imaging optical system L1, and FIG. 4B is a lateral aberration diagram of the second imaging optical system L2. The lateral aberration diagrams shown in FIGS. 4A and 4B are shown with respect to
次に、本実施例の撮像装置100における好ましい構成について述べる。
Next, a preferable configuration of the
第1の結像光学系L1の画角と第2の結像光学系L2の画角は互いに異なることが好ましい。これによって、上述した結像光学系の切り替えによって撮影される画角を切り替えることが可能となる。 It is preferable that the field angle of the first imaging optical system L1 and the field angle of the second imaging optical system L2 are different from each other. As a result, it is possible to switch the angle of view taken by switching the imaging optical system described above.
画角を切り替えることのできるレンズとして、光学系に含まれるレンズを光軸方向に移動させるズームレンズが知られているが、複数のレンズを異なる軌跡で動かす必要があるために複雑な機構が必要であった。また、レンズを移動軌跡に沿って移動させる必要があるため、瞬時に画角を切り替えることはできなかった。 As a lens that can switch the angle of view, a zoom lens that moves the lens included in the optical system in the optical axis direction is known, but a complicated mechanism is required because it is necessary to move multiple lenses along different trajectories Met. In addition, since it is necessary to move the lens along the movement trajectory, the angle of view cannot be switched instantaneously.
また、光路に対して挿抜可能なエクステンダを内蔵したレンズ装置では瞬間的な画角の切り替えが可能であるが、エクステンダの挿入後の結像性能はマスターレンズの結像性能に依存するため、結像性能を維持しつつ画角を大幅に変えることは困難であった。 In addition, in a lens device incorporating an extender that can be inserted into and removed from the optical path, the angle of view can be switched instantaneously, but the imaging performance after insertion of the extender depends on the imaging performance of the master lens. It has been difficult to change the angle of view while maintaining image performance.
一方、本実施例の撮像装置100において第1の結像光学系L1と第2の結像光学系L2の画角を異ならせることで、簡易な機構で瞬時に画角を切り替えることが可能となる。また、本実施例の撮像装置100では結像光学系自体を切り替えることで画角を変化させるため、それぞれの結像光学系を個別に設計でき、高い結像性能を得つつ画角を切り替えることが可能となる。
On the other hand, by changing the angle of view of the first imaging optical system L1 and the second imaging optical system L2 in the
また、第2の結像光学系L2は第1の結像光学系L1よりも広い画角を有するように構成することが好ましい。一般的に結像光学系の光路長は画角が狭くなるほど長くなる。それゆえ、結像光学系内に反射面を設けて光路を折り曲げたとしても、画角が狭くなるほど結像光学系は大型化し易い。このため、第1の結像光学系L1の内部に挿入され得る第2の結像光学系L2をより広角とすることで、第1の結像光学系L1の設計を容易にすることが可能となる。 The second imaging optical system L2 is preferably configured to have a wider angle of view than the first imaging optical system L1. In general, the optical path length of the imaging optical system becomes longer as the angle of view becomes narrower. Therefore, even if a reflection surface is provided in the imaging optical system and the optical path is bent, the imaging optical system is likely to be enlarged as the angle of view becomes narrower. For this reason, the design of the first imaging optical system L1 can be facilitated by setting the second imaging optical system L2 that can be inserted into the first imaging optical system L1 to have a wider angle. It becomes.
また、第1の結像光学系L1は複数の反射面を含んで構成され、各反射面間は気体(空気)で満たされていることが好ましい。このような構成を中空ミラー構成と呼ぶ。 The first imaging optical system L1 is preferably configured to include a plurality of reflecting surfaces, and the space between the reflecting surfaces is preferably filled with gas (air). Such a configuration is called a hollow mirror configuration.
中空ミラー構成では色収差がほとんど発生しないため、第1の結像光学系L1の結像性能を高めつつ、第1の結像光学系L1の内部に第2の結像光学系L2が挿入され得るスペースを確保することができる。 Since the hollow mirror configuration hardly causes chromatic aberration, the second imaging optical system L2 can be inserted into the first imaging optical system L1 while improving the imaging performance of the first imaging optical system L1. Space can be secured.
より好ましくは、第1の結像光学系L1は反射面のみで構成されていると良い。なお、光学的パワーを有する屈折面を有していなければ、光の結像に寄与しない絞り面やカバーガラスが設けられていたとしても反射面のみで構成されているとする。これによって、第2の結像光学系を収納するための十分なスペースを確保しやすくなる。また、第1の結像光学系L1を軽量に構成することができるため、撮像装置100を軽量化することができる。
More preferably, the first image-forming optical system L1 may be composed only of a reflecting surface. In addition, if it does not have a refracting surface having optical power, it is assumed that it is composed only of a reflecting surface even if a diaphragm surface or a cover glass that does not contribute to light image formation is provided. This makes it easy to secure a sufficient space for housing the second imaging optical system. In addition, since the first imaging optical system L1 can be configured to be lightweight, the
また、第1の結像光学系L1は少なくとも1面の自由曲面形状の反射面を備えることが好ましい。同様に、第2の結像光学系L2は少なくとも1面の自由曲面形状の反射面を備えることが好ましい。これによって、それぞれの結像光学系において反射面の偏心配置によって生じる収差を容易に補正することが可能となる。 Further, it is preferable that the first imaging optical system L1 includes at least one free-form reflecting surface. Similarly, it is preferable that the second imaging optical system L2 includes at least one free-form reflecting surface. This makes it possible to easily correct aberrations caused by the eccentric arrangement of the reflecting surfaces in each imaging optical system.
また、第1の結像光学系L1の入射瞳位置は最も物体側の反射面よりも物体側であることが好ましい。本実施例の第1の結像光学系L1では、開口絞りとして機能する開口部SP1が入射瞳に相当する。これによって、第1の結像光学系L1における各反射面の過度な大型化を防ぐことができる。また各反射面への入射光と反射光が同じ空間を通ることが可能となるため、小型化が容易となる。なお、入射瞳位置は必ずしも開口部SP1と一致していなくとも良い。 Further, it is preferable that the entrance pupil position of the first imaging optical system L1 is closer to the object side than the reflecting surface closest to the object side. In the first imaging optical system L1 of the present embodiment, the opening SP1 that functions as an aperture stop corresponds to the entrance pupil. This can prevent an excessive increase in the size of each reflecting surface in the first imaging optical system L1. In addition, since the incident light and the reflected light on each reflecting surface can pass through the same space, downsizing is facilitated. Note that the entrance pupil position does not necessarily coincide with the opening SP1.
また、第1及び第2の結像光学系のいずれが使用される場合であっても、共通の撮像素子を用いることが好ましい。ゆえに、第1の結像光学系L1が使用される状態における第1の結像光学系L1の像面の位置と第2の結像光学系L2が使用される状態における第2の結像光学系L2の像面は一致していることが好ましい。撮像素子の共通化によって、撮像装置100をより小型に構成することが可能となる。
In addition, it is preferable to use a common image sensor regardless of which of the first and second imaging optical systems is used. Therefore, the position of the image plane of the first imaging optical system L1 in the state where the first imaging optical system L1 is used and the second imaging optical in the state where the second imaging optical system L2 is used. The image planes of the system L2 are preferably coincident. By sharing the imaging element, the
さらに、撮像素子を可動としても良い。例えば、撮像素子を基準軸方向に可動とし、撮像素子を移動させることでフォーカシングを行っても良い。この場合、第1の結像光学系L1と第2の結像光学系L2でフォーカス機構を共通化することができる。また、第1の結像光学系L1と第2の結像光学系L2の像面の位置が基準軸方向に異なるような場合に、結像光学系の切り替えに応じて撮像素子を移動させるようにしても良い。 Furthermore, the image sensor may be movable. For example, focusing may be performed by moving the image sensor in the direction of the reference axis and moving the image sensor. In this case, the focus mechanism can be shared by the first imaging optical system L1 and the second imaging optical system L2. Further, when the positions of the image planes of the first imaging optical system L1 and the second imaging optical system L2 are different in the reference axis direction, the image pickup device is moved in accordance with the switching of the imaging optical system. Anyway.
さらに、撮像素子をxz平面内で可動とし、撮像素子を移動させることで手振れ補正(像ぶれ補正)を行っても良い。この場合、第1の結像光学系L1と第2の結像光学系L2で防振機構を共通化することができる。 Furthermore, the image sensor may be movable in the xz plane, and camera shake correction (image blur correction) may be performed by moving the image sensor. In this case, the image stabilization mechanism can be shared by the first imaging optical system L1 and the second imaging optical system L2.
また、第1の結像光学系L1と第2の結像光学系L2のうちの少なくとも一方は、像面IMGとは別の位置で光路中に実像を結像する中間結像面を少なくとも1つ有することが好ましい。 In addition, at least one of the first imaging optical system L1 and the second imaging optical system L2 has at least one intermediate imaging plane that forms a real image in the optical path at a position different from the image plane IMG. It is preferable to have one.
結像光学系内に中間結像面を設けることで、光学系内における光束の過度な広がりを抑制できる。これにより結像光学系の形状や画角の制御が容易となり、過度な大型化を伴わずに所望の特性を備える結像光学系を構成することが可能となる。 By providing an intermediate imaging plane in the imaging optical system, it is possible to suppress excessive spread of the light beam in the optical system. As a result, the shape and angle of view of the imaging optical system can be easily controlled, and an imaging optical system having desired characteristics can be configured without being excessively large.
また、第1の結像光学系L1と第2の結像光学系L2の軸上光束に対する開放Fナンバーは同じであることが好ましい。これによって、第1の結像光学系L1と第2の結像光学系L2の間で結像光学系を切り替える場合において、取得される画像の明るさを一定とすることができる。なお、第1の結像光学系L1と第2の結像光学系L2の開放Fナンバーの差が1/2段未満であれば開放Fナンバーは同じであるとみなすことができる。なお、「軸上光束」とは、像面の中心に結像する光束である。すなわち、軸上光束は基準軸光線を含む。 Further, it is preferable that the open F numbers for the axial light beams of the first imaging optical system L1 and the second imaging optical system L2 are the same. Thereby, when the imaging optical system is switched between the first imaging optical system L1 and the second imaging optical system L2, the brightness of the acquired image can be made constant. If the difference between the open F numbers of the first image forming optical system L1 and the second image forming optical system L2 is less than ½, the open F numbers can be regarded as the same. The “axial light beam” is a light beam that forms an image at the center of the image plane. That is, the axial light beam includes the reference axis light beam.
また、開口部SP1やSP2、像面IMG付近の位置に、撮像に必要な波長の光が透過する透過率特性を有したカバーガラスやレンズ等の光学素子を付加しても良い。こうすることで、第1の結像光学系L1及び第2の結像光学系L2内や撮像素子にごみや埃が付着することを防ぐことができる。 Further, an optical element such as a cover glass or a lens having a transmittance characteristic that transmits light having a wavelength necessary for imaging may be added to positions near the openings SP1 and SP2 and the image plane IMG. By doing so, it is possible to prevent dust and dust from adhering in the first image forming optical system L1 and the second image forming optical system L2 and the image pickup device.
さらに、第1の結像光学系L1と第2の結像光学系L2に共通な光学系を付加できるように構成しても良い。たとえば、開口部SP1よりも物体側に接写撮影を可能にするクローズアップレンズを装着したり、像面IMG付近に倍率を変更するためのエクステンダを挿抜できる構成にしても良い。 Furthermore, it may be configured such that a common optical system can be added to the first imaging optical system L1 and the second imaging optical system L2. For example, a close-up lens that enables close-up photography can be attached to the object side of the opening SP1, or an extender for changing the magnification can be inserted and removed near the image plane IMG.
[実施例2]
次に実施例2について述べる。本実施例の撮像装置は、第1の結像光学系L1及び第2の結像光学系L2に加えて、さらに第3の結像光学系を有する点で実施例1と異なる。本実施例における第1の結像光学系L1及び第2の結像光学系L2は実施例1と同様であるため説明を省略する。
[Example 2]
Next, Example 2 will be described. The image pickup apparatus according to the present embodiment is different from the first embodiment in that a third image forming optical system is further provided in addition to the first image forming optical system L1 and the second image forming optical system L2. Since the first imaging optical system L1 and the second imaging optical system L2 in the present embodiment are the same as those in the first embodiment, description thereof is omitted.
図5(a)~(c)、及び図6(a)~(c)は、本実施例の撮像装置100を示す概略図である。
5 (a) to 5 (c) and FIGS. 6 (a) to 6 (c) are schematic views showing the
図5(a)は、第2の結像光学系L2が使用される状態の撮像装置100をZ軸に平行な方向から見た図である。図5(b)は、第1の結像光学系L1が使用される状態の撮像装置100をZ軸に平行な方向から見た図である。図5(c)は、第3の結像光学系L3が使用される状態の撮像装置100をZ軸に平行な方向から見た図である。
FIG. 5A is a diagram of the
図6(a)は図5(a)に対応する撮像装置100の斜視図であり、図6(b)は図5(b)に対応する撮像装置100の斜視図であり、図6(c)は図5(c)に対応する撮像装置100の斜視図である。
6A is a perspective view of the
図5(a)~(c)、及び図6(a)~(c)に示すように、本実施例における第3の結像光学系L3は第1の結像光学系L1よりも大きく構成され、第1の結像光学系を第3の結像光学系L3の内部に挿入できるように構成されている。 As shown in FIGS. 5A to 5C and FIGS. 6A to 6C, the third imaging optical system L3 in this embodiment is configured to be larger than the first imaging optical system L1. Thus, the first imaging optical system can be inserted into the third imaging optical system L3.
第3の結像光学系L3が使用される際には、図5(c)及び図6(c)に示すように、第3の結像光学系L3の内部から第1の結像光学系L1及び第2の結像光学系L2が退避され、第3の結像光学系L3の光路が有効化される。すなわち、第3の結像光学系L3の開口部SP3(第3の結像光学系L3の開口絞りとしても機能する)から入射した光は、第3の結像光学系L3の各光学面で収斂または発散されながら像面IMGにて結像される。 When the third imaging optical system L3 is used, as shown in FIGS. 5C and 6C, the first imaging optical system from the inside of the third imaging optical system L3 is used. L1 and the second imaging optical system L2 are retracted, and the optical path of the third imaging optical system L3 is validated. That is, light incident from the aperture SP3 of the third imaging optical system L3 (which also functions as an aperture stop of the third imaging optical system L3) is transmitted through each optical surface of the third imaging optical system L3. An image is formed on the image plane IMG while being converged or diverged.
このように、本発明は切り替えられる結像光学系が3つ以上であっても、使用される結像光学系を切り替えて可能としつつ筐体内のスペースを有効に活用することができる。 As described above, according to the present invention, even if there are three or more imaging optical systems to be switched, it is possible to effectively use the space in the housing while enabling switching of the imaging optical system to be used.
なお、図5(c)及び図6(c)において、第1の結像光学系L1の光路から第2の結像光学系L2が退避している状態を示しているが、第3の結像光学系L3が使用される際には第2の結像光学系L2は第1の結像光学系L1の内部に挿入されていても良い。これによって撮像装置100内において結像光学系を配置するためのスペースをさらに減じることができ、さらなる小型化を達成することが可能となる。
5C and 6C show a state in which the second imaging optical system L2 is retracted from the optical path of the first imaging optical system L1, the third result is shown. When the image optical system L3 is used, the second imaging optical system L2 may be inserted into the first imaging optical system L1. As a result, the space for disposing the imaging optical system in the
次に、本実施例における第3の結像光学系L3について述べる。図7(a)は本実施例における第3の結像光学系L3の断面図である。図7(b)は本実施例における第3の結像光学系L3に第1の結像光学系L1及び第2の結像光学系L2が挿入された状態(図5(a)及び図6(a)に示す状態)の断面図である。図7(c)は本実施例における第3の結像光学系L3に第1の結像光学系L1が挿入された状態(図5(b)及び図6(b)に示す状態)の断面図である。 Next, the third imaging optical system L3 in this embodiment will be described. FIG. 7A is a cross-sectional view of the third imaging optical system L3 in the present embodiment. FIG. 7B shows a state in which the first imaging optical system L1 and the second imaging optical system L2 are inserted into the third imaging optical system L3 in this embodiment (FIGS. 5A and 6). It is sectional drawing of the state shown to (a). FIG. 7C is a cross section of a state in which the first imaging optical system L1 is inserted into the third imaging optical system L3 in this embodiment (the state shown in FIGS. 5B and 6B). FIG.
本実施例において、第3の結像光学系L3は5面の反射面を有するOff-Axial光学系である。本実施例においても各結像光学系における光学面間は空気によって満たされている。 In the present embodiment, the third imaging optical system L3 is an Off-Axial optical system having five reflecting surfaces. Also in this embodiment, the space between the optical surfaces in each imaging optical system is filled with air.
第3の結像光学系L3によって結像される光線が通る領域は第1の結像光学系L1によって結像される光線が通る領域よりも大きい。このため、第3の結像光学系L3の内側には第1の結像光学系L1を収納することのできる空間が設けられている。 The region through which the light beam imaged by the third imaging optical system L3 passes is larger than the region through which the light beam imaged by the first imaging optical system L1 passes. For this reason, a space in which the first imaging optical system L1 can be accommodated is provided inside the third imaging optical system L3.
図7(a)に示すように、第3の結像光学系L3の第1面R30に入射した光は、第2面R31から第6面R35で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R30は図5(a)~(c)における開口部(開口絞り)SP3に相当する。また、第1面R30は第3の結像光学系L3の入射瞳に相当する。開口部(開口絞り)SP3の開口径は可変としても良い。また、図7(a)に示したM3は第3の結像光学系L3における中間結像面を示している。 As shown in FIG. 7A, the light incident on the first surface R30 of the third imaging optical system L3 is reflected in order while converging or diverging from the second surface R31 to the sixth surface R35, and the image surface. Imaging with IMG. The first surface R30 corresponds to the opening (aperture stop) SP3 in FIGS. 5 (a) to 5 (c). The first surface R30 corresponds to the entrance pupil of the third imaging optical system L3. The aperture diameter of the aperture (aperture stop) SP3 may be variable. Further, M3 shown in FIG. 7A indicates an intermediate imaging plane in the third imaging optical system L3.
第3の結像光学系L3のより詳しい形状等は、後の数値実施例2において説明する。 A more detailed shape of the third imaging optical system L3 will be described later in Numerical Example 2.
図7(b)及び(c)に示すように、第3の結像光学系L3の内部に第1の結像光学系L1や第2の結像光学系L2が挿入されている場合、開口部SP3から入射した光は第3の結像光学系L3の第2面R31から第6面R35には到達しない。この時、開口部SP3から入射した光は、最も内側に配置された結像光学系によって像面IMGに結像されることになる。すなわち、結像光学系の挿抜によって、使用される結像光学系が切り替えることが可能となっている。 As shown in FIGS. 7B and 7C, when the first imaging optical system L1 and the second imaging optical system L2 are inserted into the third imaging optical system L3, the aperture The light incident from the part SP3 does not reach the sixth surface R35 from the second surface R31 of the third imaging optical system L3. At this time, the light incident from the opening SP3 is imaged on the image plane IMG by the imaging optical system arranged on the innermost side. That is, the imaging optical system to be used can be switched by inserting and removing the imaging optical system.
次に、本実施例における第3の結像光学系L3の光学特性について述べる。 Next, the optical characteristics of the third imaging optical system L3 in this embodiment will be described.
図8に、本実施例の第3の結像光学系L3のディストーションを示す。第3の結像光学系L3のディストーションは、図8に示すように極めて小さい。 FIG. 8 shows distortion of the third imaging optical system L3 of the present embodiment. The distortion of the third imaging optical system L3 is extremely small as shown in FIG.
図9に、本実施例の第3の結像光学系L3の横収差図を示す。図9に示す横収差図は、図20(a)に示す撮像素子上の位置1から5に対して示している。
FIG. 9 shows a lateral aberration diagram of the third imaging optical system L3 of the present example. The lateral aberration diagram shown in FIG. 9 is shown with respect to
また、YZ断面において、第3の結像光学系L3の焦点距離は214.95mm、Fナンバーは11.0である。 In the YZ section, the focal length of the third imaging optical system L3 is 214.95 mm, and the F number is 11.0.
なお、開口部SP3の付近の位置に、撮像に必要な波長が透過する透過率特性を有したカバーガラスやレンズ等の光学素子を付加してもよい。これによって、第3の結像光学系L3内や撮像素子にごみや埃が付着することを防ぐことができる。 It should be noted that an optical element such as a cover glass or a lens having a transmittance characteristic that transmits a wavelength necessary for imaging may be added at a position near the opening SP3. Thereby, it is possible to prevent dust and dirt from adhering to the inside of the third imaging optical system L3 and the image sensor.
[実施例3]
次に実施例3について述べる。本実施例の撮像装置は実施例1と同様に2つの結像光学系を有する。本実施例の撮像装置の外観は、図1(a)~(d)に示したものと同様である。ただし、本実施例における2つの結像光学系の光学特性は共に実施例1とは異なる。本実施例において、第1の結像光学系に対して挿抜される第2の結像光学系は、中空ミラー構造ではなく、複数の反射面を有する固体プリズムで構成されている。本実施例のように、第2の結像光学系をプリズムで構成することで、光路長を稼ぐことができ、第2の結像光学系をより小型化することができる。これによって、第1の結像光学系に対して挿抜し易くなるメリットがある。
[Example 3]
Next, Example 3 will be described. The imaging apparatus of the present embodiment has two imaging optical systems as in the first embodiment. The appearance of the image pickup apparatus of the present embodiment is the same as that shown in FIGS. 1 (a) to 1 (d). However, the optical characteristics of the two imaging optical systems in this embodiment are different from those in the first embodiment. In the present embodiment, the second imaging optical system that is inserted into and extracted from the first imaging optical system is not a hollow mirror structure, but is composed of a solid prism having a plurality of reflecting surfaces. By configuring the second imaging optical system with a prism as in this embodiment, the optical path length can be increased, and the second imaging optical system can be further miniaturized. As a result, there is a merit that it is easy to insert and remove from the first imaging optical system.
本実施例において、第1の結像光学系L1は4面の自由曲面形状の反射面を有するOff-Axial光学系である。本実施例において第1の結像光学系における光学面間は空気によって満たされている。また、本実施例において第2の結像光学系L2は4面の自由曲面形状の反射面と、2面の自由曲面形状の屈折面を有するOff-Axial光学系である。 In the present embodiment, the first imaging optical system L1 is an off-axial optical system having four free-form reflecting surfaces. In this embodiment, the space between the optical surfaces in the first imaging optical system is filled with air. In the present embodiment, the second imaging optical system L2 is an off-axial optical system having four free-form curved reflecting surfaces and two free-form refracting surfaces.
図10(a)は本実施例における第1の結像光学系L1の断面図である。図10(b)は本実施例における第2の結像光学系L2の断面図である。図10(c)は本実施例における第1の結像光学系L1に第2の結像光学系L2が挿入された状態の断面図である。 FIG. 10A is a sectional view of the first imaging optical system L1 in the present embodiment. FIG. 10B is a cross-sectional view of the second imaging optical system L2 in the present embodiment. FIG. 10C is a cross-sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
図10(a)に示すように、第1の結像光学系L1の第1面R40に入射した光は、第2面R41から第5面R44で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R40は第1の結像光学系L1の入射瞳であり、図1(a)~(d)における開口部(開口絞り)SP1に相当する。 As shown in FIG. 10A, the light incident on the first surface R40 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R41 to the fifth surface R44, and the image surface. Imaging with IMG. The first surface R40 is an entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d).
図10(b)に示すように、第2の結像光学系L2において、屈折面である第1面R50に入射した光は、第2面R51から第5面R54で収斂または発散しながら順に反射される。そして、屈折面である第6面R55を通り、像面IMGで結像する。第1面R50は第2の結像光学系L2の入射瞳であり、図1(a)~(d)における開口部(開口絞り)SP2に相当する。なお、第1面R50の物体側にさらに開口径が可変である開口絞りを設けても良い。また、図10(b)に示したM5は第2の結像光学系L2における中間結像面を示している。 As shown in FIG. 10B, in the second imaging optical system L2, the light incident on the first surface R50 that is a refractive surface is sequentially converged or diverged from the second surface R51 to the fifth surface R54. Reflected. Then, the light passes through the sixth surface R55, which is a refractive surface, and forms an image on the image surface IMG. The first surface R50 is an entrance pupil of the second imaging optical system L2, and corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d). An aperture stop having a variable aperture diameter may be provided on the object side of the first surface R50. Further, M5 shown in FIG. 10B indicates an intermediate imaging plane in the second imaging optical system L2.
本実施例における第1の結像光学系L1及び第2の結像光学系L2のより詳しい形状等は、後の数値実施例3において説明する。 More detailed shapes and the like of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment will be described in Numerical Example 3 later.
図10(c)は、本実施例の第2の結像光学系L2を第1の結像光学系L1の内部に挿入した際の断面図である。本実施例においても、第1の結像光学系L1と第2の結像光学系L2は、第1面R40(開口部SP1)の中心とR50(開口部SP2)の中心のXY座標が一致するように配置される。また、第1の結像光学系L1と第2の結像光学系L2はそれぞれの像面が像面IMGに一致するように配置される。 FIG. 10C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1. Also in the present embodiment, the first imaging optical system L1 and the second imaging optical system L2 have the same XY coordinates of the center of the first surface R40 (opening SP1) and the center of R50 (opening SP2). To be arranged. Further, the first imaging optical system L1 and the second imaging optical system L2 are arranged so that their image planes coincide with the image plane IMG.
次に、本実施例における第1の結像光学系L1及び第2の結像光学系L2の光学特性について述べる。 Next, the optical characteristics of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment will be described.
図11(a)及び(b)に、本実施例の結像光学系のディストーションを示す。図11(a)は第1の結像光学系L1におけるディストーション、図11(b)は第2の結像光学系L2におけるディストーションを表している。本実施例の第1の結像光学系L1及び第2の結像光学系L2のディストーションは、図11(a)及び(b)に示すように極めて小さい。 FIGS. 11A and 11B show distortion of the imaging optical system of the present embodiment. FIG. 11A shows distortion in the first imaging optical system L1, and FIG. 11B shows distortion in the second imaging optical system L2. The distortion of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment is extremely small as shown in FIGS. 11 (a) and 11 (b).
図12(a)及び(b)に、本実施例の結像光学系の横収差図を示す。図12(a)は第1の結像光学系L1の横収差図、図12(b)は第2の結像光学系L2の横収差図である。図12(a)に示す横収差図は図20(b)に示す撮像素子上の位置1から5に対して示している。また、図12(b)に示す横収差図は図20(c)に示す撮像素子上の位置1から5に対して示している。
FIGS. 12A and 12B show lateral aberration diagrams of the imaging optical system of the present example. FIG. 12A is a lateral aberration diagram of the first imaging optical system L1, and FIG. 12B is a lateral aberration diagram of the second imaging optical system L2. The lateral aberration diagram shown in FIG. 12A is shown for
YZ断面において、本実施例の第1の結像光学系L1の焦点距離は71.65mm、Fナンバーは8.0である。また、YZ断面において、第2の結像光学系L2の焦点距離は17.91mm、Fナンバーは8.0である。 In the YZ cross section, the focal length of the first imaging optical system L1 of the present example is 71.65 mm, and the F number is 8.0. In the YZ section, the focal length of the second imaging optical system L2 is 17.91 mm, and the F number is 8.0.
[実施例4]
次に実施例4について述べる。本実施例の撮像装置は実施例1や3と同様に2つの結像光学系を有する。本実施例の撮像装置の外観は、図1(a)~(d)に示したものと開口部の径の大小関係を除き同様である。本実施例における2つの結像光学系の光学特性は共に実施例1や3とは異なる。具体的には、本実施例における第1の結像光学系の画角は、第2の結像光学系の画角よりも大きい。また、第1の結像光学系に光を取り込むための開口部(開口絞りとしても機能する)は第2の結像光学系に光を取り込むための開口部(開口絞りとしても機能する)よりも小さい。
[Example 4]
Next, Example 4 will be described. The imaging apparatus of the present embodiment has two imaging optical systems as in the first and third embodiments. The appearance of the image pickup apparatus according to the present embodiment is the same as that shown in FIGS. 1A to 1D except for the size relationship between the diameters of the openings. The optical characteristics of the two imaging optical systems in this embodiment are different from those in the first and third embodiments. Specifically, the field angle of the first imaging optical system in the present embodiment is larger than the field angle of the second imaging optical system. Further, the opening for capturing light into the first imaging optical system (also functions as an aperture stop) is more than the opening for capturing light into the second imaging optical system (also functions as an aperture stop). Is also small.
本実施例において、第1の結像光学系L1は5面の自由曲面形状の反射面を有するOff-Axial光学系である。また、本実施例において第2の結像光学系L2は5面の自由曲面形状の反射面を有するOff-Axial光学系である。 In this embodiment, the first imaging optical system L1 is an off-axial optical system having five free-form reflecting surfaces. In this embodiment, the second imaging optical system L2 is an Off-Axial optical system having five free-form reflecting surfaces.
図13(a)は本実施例における第1の結像光学系L1の断面図である。図13(b)は本実施例における第2の結像光学系L2の断面図である。図13(c)は本実施例における第1の結像光学系L1に第2の結像光学系L2が挿入された状態の断面図である。 FIG. 13A is a sectional view of the first imaging optical system L1 in the present embodiment. FIG. 13B is a cross-sectional view of the second imaging optical system L2 in the present embodiment. FIG. 13C is a cross-sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
図13(a)に示すように、第1の結像光学系L1の第1面R60に入射した光は、第2面R61から第6面R65で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R60は第1の結像光学系L1の入射瞳であり、図1(a)~(d)における開口部(開口絞り)SP1に相当する。また、図13(a)に示したM6は第1の結像光学系L1における中間結像面を示している。 As shown in FIG. 13A, the light incident on the first surface R60 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R61 to the sixth surface R65, and the image surface. Imaging with IMG. The first surface R60 is the entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d). Further, M6 shown in FIG. 13A indicates an intermediate imaging plane in the first imaging optical system L1.
図13(b)に示すように、第2の結像光学系L2において、第1面R70に入射した光は、第2面R71から第6面R75で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R70は第2の結像光学系L2の入射瞳であり、図1(a)~(d)における開口部(開口絞り)SP2に相当する。また、図13(b)に示したM7は第2の結像光学系L2における中間結像面を示している。 As shown in FIG. 13B, in the second imaging optical system L2, the light incident on the first surface R70 is reflected in order while converging or diverging from the second surface R71 to the sixth surface R75, and the image An image is formed on the surface IMG. The first surface R70 is an entrance pupil of the second imaging optical system L2, and corresponds to the aperture (aperture stop) SP2 in FIGS. 1 (a) to 1 (d). Further, M7 shown in FIG. 13B indicates an intermediate imaging plane in the second imaging optical system L2.
本実施例における第1の結像光学系L1及び第2の結像光学系L2のより詳しい形状等は、後の数値実施例4において説明する。 More detailed shapes and the like of the first image forming optical system L1 and the second image forming optical system L2 in this embodiment will be described in Numerical Example 4 later.
図13(c)は、本実施例の第2の結像光学系L2を第1の結像光学系L1の内部に挿入した際の断面図である。本実施例においても、第1の結像光学系L1と第2の結像光学系L2は、第1面R60(開口部SP1)の中心とR70(開口部SP2)の中心のXY座標が一致するように配置される。また、第1の結像光学系L1と第2の結像光学系L2はそれぞれの像面が像面IMGに一致するように配置される。 FIG. 13C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1. Also in the present embodiment, the first imaging optical system L1 and the second imaging optical system L2 have the same XY coordinates of the center of the first surface R60 (opening SP1) and the center of R70 (opening SP2). To be arranged. Further, the first imaging optical system L1 and the second imaging optical system L2 are arranged so that their image planes coincide with the image plane IMG.
なお本実施例では、前述のように第1の結像光学系L1の第1面R60(開口部SP1)の径は第2の結像光学系L2の第1面R70(開口部SP2)の径よりも小さい。ゆえに、第1の結像光学系L1における開口部SP1の径を可変に構成しておき、図13(c)のように第2の結像光学系L2が第1の結像光学系L1の内部に挿入される際に開口部SP1の径を広げるようにすることが好ましい。あるいは、開口部SP1よりも開口径の大きい他の開口部を設け、第2の結像光学系L2が第1の結像光学系L1の内部に挿入される際に開口部SP1が他の開口部に切り替わるように構成しても良い。これによって、第2の結像光学系L2で結像される光線が第1の結像光学系L1によってけられることがなくなる。 In this embodiment, as described above, the diameter of the first surface R60 (opening SP1) of the first imaging optical system L1 is the same as that of the first surface R70 (opening SP2) of the second imaging optical system L2. Smaller than the diameter. Therefore, the diameter of the opening SP1 in the first imaging optical system L1 is configured to be variable, and the second imaging optical system L2 is the first imaging optical system L1 as shown in FIG. 13C. It is preferable to increase the diameter of the opening SP1 when inserted into the inside. Alternatively, another opening having an opening diameter larger than that of the opening SP1 is provided, and when the second imaging optical system L2 is inserted into the first imaging optical system L1, the opening SP1 is replaced with another opening. You may comprise so that it may switch to a part. As a result, the light beam imaged by the second imaging optical system L2 is not scattered by the first imaging optical system L1.
次に、本実施例における第1の結像光学系L1及び第2の結像光学系L2の光学特性について述べる。 Next, the optical characteristics of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment will be described.
図14(a)及び(b)に、本実施例の結像光学系のディストーションを示す。図14(a)は第1の結像光学系L1におけるディストーション、図14(b)は第2の結像光学系L2におけるディストーションを表している。本実施例の第1の結像光学系L1及び第2の結像光学系L2のディストーションは、図14(a)及び(b)に示すように極めて小さい。 FIGS. 14A and 14B show the distortion of the imaging optical system of the present embodiment. FIG. 14A shows distortion in the first imaging optical system L1, and FIG. 14B shows distortion in the second imaging optical system L2. The distortions of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment are extremely small as shown in FIGS. 14 (a) and 14 (b).
図15(a)及び(b)に、本実施例の結像光学系の横収差図を示す。図15(a)は第1の結像光学系L1の横収差図、図15(b)は第2の結像光学系L2の横収差図である。図15(a)及び(b)に示す横収差図は図20(a)に示す撮像素子上の位置1から5に対して示している。
FIGS. 15A and 15B are lateral aberration diagrams of the imaging optical system of the present example. FIG. 15A is a lateral aberration diagram of the first imaging optical system L1, and FIG. 15B is a lateral aberration diagram of the second imaging optical system L2. The lateral aberration diagrams shown in FIGS. 15A and 15B are shown with respect to
YZ断面において、本実施例の第1の結像光学系L1の焦点距離は17.91mm、Fナンバーは5.97である。また、YZ断面において、第2の結像光学系L2の焦点距離は71.65mm、Fナンバーは8.0である。 In the YZ section, the focal length of the first imaging optical system L1 of the present embodiment is 17.91 mm, and the F number is 5.97. In the YZ section, the focal length of the second imaging optical system L2 is 71.65 mm, and the F number is 8.0.
[実施例5]
次に実施例5について述べる。本実施例の撮像装置は実施例1,3,4と同様に2つの結像光学系を有する。本実施例の撮像装置の外観は、図1(a)~(d)に示したものと同様である。ただし、本実施例における2つの結像光学系の光学特性は共に実施例1,3,4とは異なる。本実施例において、第1の結像光学系に対して挿抜される第2の結像光学系は複数のレンズとプリズムで構成されている。
[Example 5]
Next, Example 5 will be described. The imaging apparatus of the present embodiment has two imaging optical systems as in the first, third, and fourth embodiments. The appearance of the image pickup apparatus of the present embodiment is the same as that shown in FIGS. 1 (a) to 1 (d). However, the optical characteristics of the two imaging optical systems in the present embodiment are different from those in the first, third, and fourth embodiments. In this embodiment, the second imaging optical system that is inserted into and extracted from the first imaging optical system is composed of a plurality of lenses and prisms.
本実施例において、第1の結像光学系L1は4面の自由曲面形状の反射面を有するOff-Axial光学系である。また、本実施例において第2の結像光学系L2は4枚の球面レンズと1つの三角プリズムで構成されたOff-Axial光学系である。 In the present embodiment, the first imaging optical system L1 is an off-axial optical system having four free-form reflecting surfaces. In the present embodiment, the second imaging optical system L2 is an Off-Axial optical system including four spherical lenses and one triangular prism.
図16(a)は本実施例における第1の結像光学系L1の断面図である。図16(b)は本実施例における第2の結像光学系L2の断面図である。図16(c)は本実施例における第1の結像光学系L1に第2の結像光学系L2が挿入された状態の断面図である。 FIG. 16A is a cross-sectional view of the first imaging optical system L1 in the present embodiment. FIG. 16B is a cross-sectional view of the second imaging optical system L2 in the present embodiment. FIG. 16C is a sectional view showing a state in which the second imaging optical system L2 is inserted into the first imaging optical system L1 in the present embodiment.
図16(a)に示すように、第1の結像光学系L1の第1面R80に入射した光は、第2面R81から第5面R84で収斂または発散しながら順に反射され、像面IMGで結像する。第1面R80は第1の結像光学系L1の入射瞳であり、図1(a)~(d)における開口部(開口絞り)SP1に相当する。 As shown in FIG. 16A, the light incident on the first surface R80 of the first imaging optical system L1 is reflected in order while converging or diverging from the second surface R81 to the fifth surface R84, and the image surface. Imaging with IMG. The first surface R80 is the entrance pupil of the first imaging optical system L1, and corresponds to the aperture (aperture stop) SP1 in FIGS. 1 (a) to 1 (d).
また、第2の結像光学系L2は物体側から像側へ順に配置された、像側に凸面を向けたメニスカス形状の正レンズ、像側に凸面を向けたメニスカス形状の負レンズ、反射面を有する三角プリズム、両凸の正レンズ、像側に凸面を向けた負レンズで構成される。第2の結像光学系L2において最も物体側に配置された正レンズは開口絞りの役割も果たしており、入射瞳に相当する。屈折光学素子を含んで構成される本実施例の第2の結像光学系L2には、複数の自由曲面を有する反射光学系と比較して製造は容易であるというメリットがある。 The second imaging optical system L2 is arranged in order from the object side to the image side, and a meniscus positive lens having a convex surface facing the image side, a meniscus negative lens having a convex surface facing the image side, and a reflecting surface A triangular prism, a biconvex positive lens, and a negative lens with a convex surface facing the image side. The positive lens disposed closest to the object side in the second imaging optical system L2 also serves as an aperture stop and corresponds to an entrance pupil. The second imaging optical system L2 of the present embodiment configured to include a refractive optical element has an advantage that it is easy to manufacture compared to a reflective optical system having a plurality of free-form surfaces.
本実施例における第1の結像光学系L1及び第2の結像光学系L2のより詳しい形状等は、後の数値実施例5において説明する。 More detailed shapes and the like of the first imaging optical system L1 and the second imaging optical system L2 in the present embodiment will be described in Numerical Example 5 later.
図16(c)は、本実施例の第2の結像光学系L2を第1の結像光学系L1の内部に挿入した際の断面図である。 FIG. 16C is a cross-sectional view when the second imaging optical system L2 of the present embodiment is inserted into the first imaging optical system L1.
次に、本実施例における第1の結像光学系L1及び第2の結像光学系L2の光学特性について述べる。 Next, the optical characteristics of the first imaging optical system L1 and the second imaging optical system L2 in this embodiment will be described.
図17(a)及び(b)に、本実施例の結像光学系のディストーションを示す。図17(a)は第1の結像光学系L1におけるディストーション、図17(b)は第2の結像光学系L2におけるディストーションを表している。本実施例の第1の結像光学系L1及び第2の結像光学系L2のディストーションは、図17(a)及び(b)に示すように極めて小さい。 FIGS. 17A and 17B show distortion of the imaging optical system of the present embodiment. FIG. 17A shows distortion in the first imaging optical system L1, and FIG. 17B shows distortion in the second imaging optical system L2. The distortions of the first imaging optical system L1 and the second imaging optical system L2 of this embodiment are extremely small as shown in FIGS. 17 (a) and 17 (b).
図18(a)及び(b)に、本実施例の結像光学系の横収差図を示す。図18(a)は第1の結像光学系L1の横収差図、図18(b)は第2の結像光学系L2の横収差図である。図18(a)に示す横収差図は図20(b)に示す撮像素子上の位置1から5に対して示している。図18(b)に示す横収差図は図20(d)に示すイメージサークル上の位置1から5に対して示している。
FIGS. 18A and 18B are lateral aberration diagrams of the imaging optical system of this example. FIG. 18A is a lateral aberration diagram of the first imaging optical system L1, and FIG. 18B is a lateral aberration diagram of the second imaging optical system L2. The lateral aberration diagram shown in FIG. 18A is shown for
YZ断面において、本実施例の第1の結像光学系L1の焦点距離は71.65mm、Fナンバーは8.0である。また、YZ断面において、第2の結像光学系L2の焦点距離は17.91mm、Fナンバーは8.0である。 In the YZ cross section, the focal length of the first imaging optical system L1 of the present example is 71.65 mm, and the F number is 8.0. In the YZ section, the focal length of the second imaging optical system L2 is 17.91 mm, and the F number is 8.0.
次に、上述した各実施例における結像光学系に対応した数値実施例を示す。各数値実施例は無限遠物体に合焦した状態である。面データは、数値実施例5の第2の結像光学系を除き、各面における基準軸上の点の絶対座標系における座標(mm)、面のチルト角(°)を示している。また、Diは第i面と第(i+1)面とのローカル座標の原点間の間隔を表すスカラー量である。 Next, numerical examples corresponding to the imaging optical system in each of the above-described embodiments will be shown. Each numerical example is in a state of focusing on an object at infinity. The surface data indicates the coordinates (mm) in the absolute coordinate system of the points on the reference axis in each surface and the tilt angle (°) of the surface, excluding the second imaging optical system of Numerical Example 5. Di is a scalar quantity representing the distance between the origins of the local coordinates of the i-th surface and the (i + 1) -th surface.
数値実施例5の第2の結像光学系の面データにおいて、iを物体側からの面の順序として、riは物体側より第i番目の面の曲率半径、diは物体側より第i番目の面と第i+1番目の面との間隔、ndiとνdiは第i番目の面と第i+1番目の面との間の光学部材の屈折率とアッベ数を表している。BFは空気換算値でのバックフォーカスである。E-Xは、10-Xを表す。 In the surface data of the second imaging optical system of Numerical Example 5, i is the order of the surfaces from the object side, ri is the radius of curvature of the i-th surface from the object side, and di is the i-th surface from the object side. Ndi and νdi represent the refractive index and Abbe number of the optical member between the i-th surface and the (i + 1) -th surface. BF is the back focus in terms of air. E—X represents 10 —X .
また、各実施例において球面形状はriを第i面の曲率半径、x、yを第i面の各ローカル座標系での座標とした時、以下の式(1)で表す。 In each embodiment, the spherical shape is expressed by the following equation (1), where ri is the radius of curvature of the i-th surface and x and y are coordinates in each local coordinate system of the i-th surface.
また、各実施形態において自由曲面形状は以下の式(2)で表す。 In each embodiment, the free-form surface shape is expressed by the following equation (2).
なお、式(2)はxに関して偶数次の項のみであるため、式(2)により規定される自由曲面はyz面を対称面とする面対称な形状となる。 Since Equation (2) is only an even-order term with respect to x, the free-form surface defined by Equation (2) has a plane-symmetric shape with the yz plane as the symmetry plane.
[数値実施例1-第1の結像光学系]
画角は、X方向に±1.86°、Y方向に±2.48°である。
焦点距離はX方向に71.65mm、Y方向に71.65mmである。
像面サイズはx方向に4.65mm、y方向に6.20mmである。
第1面R10は円形であり、その直径は8.96mmである。
X軸方向のF値は8.00、Y軸方向のF値は8.00である。
[Numerical Example 1-First Imaging Optical System]
The angle of view is ± 1.86 ° in the X direction and ± 2.48 ° in the Y direction.
The focal length is 71.65 mm in the X direction and 71.65 mm in the Y direction.
The image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
The first surface R10 is circular and has a diameter of 8.96 mm.
The F value in the X axis direction is 8.00, and the F value in the Y axis direction is 8.00.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R10) 0.00 0.00 0.00 40.00 0.00 0.00
2(R11) 0.00 0.00 40.00 40.00 11.00 0.00 第1反射面
3(R12) 0.00 -14.98 2.91 36.00 -11.00 0.00 第2反射面
4(R13) 0.00 -14.98 38.91 45.00 -19.00 0.00 第3反射面
5(R14) 0.00 12.72 3.45 24.00 26.00 0.00 第4反射面
6(R15) 0.00 18.53 26.74 53.53 38.00 0.00 第5反射面
像面(IMG) 0.00 -35.00 26.74 0.00 0.00
自由曲面データ
第2面(R11) 第1反射面
C20 = -7.7219E-03 C02 = -4.2924E-03 C21 = 9.8995E-05
C03 = -7.7248E-06 C40 = -4.1351E-07 C22 = -1.0099E-06
C04 = 1.9032E-07 C41 = -1.3142E-10 C23 = 3.9926E-09
C05 = -3.0502E-09 C60 = 1.4870E-08 C42 = 5.9771E-10
C24 = -5.6596E-10 C06 = 7.5010E-11 C60 = 1.4516E-10
C43 = 1.8655E-10 C25 = 2.9739E-11 C07 = -1.2587E-11
C80 = -2.2747E-10 C62 = -1.6996E-11 C44 = -1.5602E-11
C26 = 2.6932E-12 C08 = -1.5064E-13
第3面(R12) 第2反射面
C20 = 6.7745E-03 C02 = -1.1708E-03 C21 = -2.3109E-04
C03 = 7.1582E-06 C40 = 1.8023E-06 C22 = -5.4476E-06
C04 = 1.3742E-06 C41 = -3.6639E-07 C23 = -6.2119E-08
C05 = -4.4260E-08 C60 = -4.5070E-07 C42 = -3.7793E-08
C24 = 1.3179E-08 C06 = -2.2325E-10 C60 = 2.8252E-07
C43 = -9.5435E-08 C25 = 3.4608E-09 C07 = -3.7969E-10
C80 = 5.1974E-08 C62 = 4.0008E-08 C44 = -1.6874E-08
C26 = 1.0054E-09 C08 = -7.9061E-11
第4面(R13) 第3反射面
C20 = -6.8875E-03 C02 = -4.9000E-03 C21 = -2.3094E-05
C03 = -3.5548E-05 C40 = 9.4480E-08 C22 = 4.8163E-07
C04 = 2.1256E-07 C41 = -2.5743E-08 C23 = -4.1325E-08
C05 = -5.4575E-09 C60 = -1.3763E-09 C42 = 4.1999E-10
C24 = 1.1998E-10 C06 = -1.2844E-10 C60 = 8.8422E-12
C43 = 2.1369E-10 C25 = -6.7900E-11 C07 = -2.2668E-11
C80 = 2.0387E-11 C62 = 3.4046E-12 C44 = -8.4044E-12
C26 = 2.2069E-11 C08 = 9.3176E-13
第5面(R14) 第4反射面
C20 = 9.6880E-04 C02 = 3.0495E-03 C21 = -1.0450E-04
C03 = -7.0174E-05 C40 = -1.0598E-06 C22 = -2.9722E-06
C04 = -3.1156E-06 C41 = -3.1277E-08 C23 = -1.4166E-07
C05 = -1.3498E-07 C60 = 2.4905E-08 C42 = -4.1160E-09
C24 = -7.1603E-09 C06 = -5.6986E-09 C60 = -8.2893E-11
C43 = 4.1124E-10 C25 = -6.5948E-11 C07 = -3.0828E-10
C80 = -4.1903E-10 C62 = 3.7535E-11 C44 = 7.5462E-11
C26 = 1.4310E-11 C08 = -1.7744E-11
第6面(R15) 第5反射面
C20 = -2.8637E-03 C02 = -3.7440E-03 C21 = 1.2838E-05
C03 = -4.3225E-05 C40 = -3.4750E-07 C22 = -2.6506E-06
C04 = -1.3963E-06 C41 = -1.2464E-08 C23 = -2.6233E-08
C05 = -2.4544E-08 C60 = 1.0694E-08 C42 = -3.7640E-09
C24 = -1.5270E-10 C06 = -1.0056E-09 C60 = 1.0694E-10
C43 = 6.8000E-10 C25 = 1.3447E-11 C07 = -1.2174E-10
C80 = -2.0423E-10 C62 = 8.4051E-11 C44 = 6.8613E-11
C26 = -4.1729E-11 C08 = -7.3438E-13
各反射面における軸上光束に対する焦点距離データ
(fixは第i反射面のx方向の焦点距離、fiyは第i反射面のy方向の焦点距離である。以下の数値実施例においても同様。)
f1x = 32.982 mm f1y = 57.172 mm
f2x = 37.594 mm f2y = -209.606 mm
f3x = 38.389 mm f3y = 48.241 mm
f4x = 287.108 mm f4y = 73.684 mm
f5x = 110.786 mm f5y = 52.618 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R10) 0.00 0.00 0.00 40.00 0.00 0.00
2 (R11) 0.00 0.00 40.00 40.00 11.00 0.00 First reflective surface 3 (R12) 0.00 -14.98 2.91 36.00 -11.00 0.00 Second reflective surface 4 (R13) 0.00 -14.98 38.91 45.00 -19.00 0.00 Third reflective surface 5 (R14) 0.00 12.72 3.45 24.00 26.00 0.00 Fourth reflective surface 6 (R15) 0.00 18.53 26.74 53.53 38.00 0.00 Fifth reflective surface image surface (IMG) 0.00 -35.00 26.74 0.00 0.00
Free-form data 2nd surface (R11) 1st reflective surface
C20 = -7.7219E-03 C02 = -4.2924E-03 C21 = 9.8995E-05
C03 = -7.7248E-06 C40 = -4.1351E-07 C22 = -1.0099E-06
C04 = 1.9032E-07 C41 = -1.3142E-10 C23 = 3.9926E-09
C05 = -3.0502E-09 C60 = 1.4870E-08 C42 = 5.9771E-10
C24 = -5.6596E-10 C06 = 7.5010E-11 C60 = 1.4516E-10
C43 = 1.8655E-10 C25 = 2.9739E-11 C07 = -1.2587E-11
C80 = -2.2747E-10 C62 = -1.6996E-11 C44 = -1.5602E-11
C26 = 2.6932E-12 C08 = -1.5064E-13
3rd surface (R12) 2nd reflective surface
C20 = 6.7745E-03 C02 = -1.1708E-03 C21 = -2.3109E-04
C03 = 7.1582E-06 C40 = 1.8023E-06 C22 = -5.4476E-06
C04 = 1.3742E-06 C41 = -3.6639E-07 C23 = -6.2119E-08
C05 = -4.4260E-08 C60 = -4.5070E-07 C42 = -3.7793E-08
C24 = 1.3179E-08 C06 = -2.2325E-10 C60 = 2.8252E-07
C43 = -9.5435E-08 C25 = 3.4608E-09 C07 = -3.7969E-10
C80 = 5.1974E-08 C62 = 4.0008E-08 C44 = -1.6874E-08
C26 = 1.0054E-09 C08 = -7.9061E-11
4th surface (R13) 3rd reflective surface
C20 = -6.8875E-03 C02 = -4.9000E-03 C21 = -2.3094E-05
C03 = -3.5548E-05 C40 = 9.4480E-08 C22 = 4.8163E-07
C04 = 2.1256E-07 C41 = -2.5743E-08 C23 = -4.1325E-08
C05 = -5.4575E-09 C60 = -1.3763E-09 C42 = 4.1999E-10
C24 = 1.1998E-10 C06 = -1.2844E-10 C60 = 8.8422E-12
C43 = 2.1369E-10 C25 = -6.7900E-11 C07 = -2.2668E-11
C80 = 2.0387E-11 C62 = 3.4046E-12 C44 = -8.4044E-12
C26 = 2.2069E-11 C08 = 9.3176E-13
5th surface (R14) 4th reflective surface
C20 = 9.6880E-04 C02 = 3.0495E-03 C21 = -1.0450E-04
C03 = -7.0174E-05 C40 = -1.0598E-06 C22 = -2.9722E-06
C04 = -3.1156E-06 C41 = -3.1277E-08 C23 = -1.4166E-07
C05 = -1.3498E-07 C60 = 2.4905E-08 C42 = -4.1160E-09
C24 = -7.1603E-09 C06 = -5.6986E-09 C60 = -8.2893E-11
C43 = 4.1124E-10 C25 = -6.5948E-11 C07 = -3.0828E-10
C80 = -4.1903E-10 C62 = 3.7535E-11 C44 = 7.5462E-11
C26 = 1.4310E-11 C08 = -1.7744E-11
6th surface (R15) 5th reflective surface
C20 = -2.8637E-03 C02 = -3.7440E-03 C21 = 1.2838E-05
C03 = -4.3225E-05 C40 = -3.4750E-07 C22 = -2.6506E-06
C04 = -1.3963E-06 C41 = -1.2464E-08 C23 = -2.6233E-08
C05 = -2.4544E-08 C60 = 1.0694E-08 C42 = -3.7640E-09
C24 = -1.5270E-10 C06 = -1.0056E-09 C60 = 1.0694E-10
C43 = 6.8000E-10 C25 = 1.3447E-11 C07 = -1.2174E-10
C80 = -2.0423E-10 C62 = 8.4051E-11 C44 = 6.8613E-11
C26 = -4.1729E-11 C08 = -7.3438E-13
Focal length data for the axial light flux on each reflecting surface (fix is the focal length of the i-th reflecting surface in the x direction, and fiy is the focal length of the i-th reflecting surface in the y direction. The same applies to the following numerical examples).
f1x = 32.982 mm f1y = 57.172 mm
f2x = 37.594 mm f2y = -209.606 mm
f3x = 38.389 mm f3y = 48.241 mm
f4x = 287.108 mm f4y = 73.684 mm
f5x = 110.786 mm f5y = 52.618 mm
[数値実施例1-第2の結像光学系]
画角は、X方向に±7.40°、Y方向に±9.82°である。
焦点距離はX方向に17.91mm、Y方向に17.91mmである。
像面サイズはx方向に4.65mm、y方向に6.20mmである。
第1面R20は円形であり、その直径は2.24mmである。
X軸方向のF値は8.00、Y軸方向のF値は8.00である。
[Numerical Example 1—Second Imaging Optical System]
The angle of view is ± 7.40 ° in the X direction and ± 9.82 ° in the Y direction.
The focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
The image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
The first surface R20 is circular and has a diameter of 2.24 mm.
The F value in the X axis direction is 8.00, and the F value in the Y axis direction is 8.00.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R20) 0.00 0.00 0.00 30.00 0.00 0.00
2(R21) 0.00 0.00 30.00 28.00 10.00 0.00 第1反射面
3(R22) 0.00 -9.58 3.69 25.00 -13.00 0.00 第2反射面
4(R23) 0.00 -12.19 28.55 32.00 -19.00 0.00 第3反射面
5(R24) 0.00 10.04 5.53 17.00 26.00 0.00 第4反射面
6(R25) 0.00 12.41 22.37 47.41 41.00 0.00 第5反射面
像面(IMG) 0.00 -35.00 22.37 0.00 0.00
自由曲面データ
第2面(R21) 第1反射面
C20 = -1.3006E-02 C02 = -1.1409E-02 C21 = -2.2986E-04
C03 = 1.2070E-05 C40 = -3.7621E-06 C22 = -1.0194E-05
C04 = 1.0296E-06 C41 = -2.6648E-07 C23 = 4.9447E-08
C05 = -2.9010E-08 C60 = -4.7813E-09 C42 = 1.1215E-08
C24 = 3.5840E-10 C06 = -4.5631E-09 C60 = 5.1317E-09
C43 = 2.2967E-09 C25 = -1.3047E-09 C07 = 2.7855E-10
C80 = 2.5363E-10 C62 = 6.5924E-10 C44 = -1.5322E-10
C26 = 7.2553E-11 C08 = 4.0316E-11
第3面(R22) 第2反射面
C20 = 2.9667E-03 C02 = 1.4595E-03 C21 = 1.5246E-03
C03 = -1.0807E-04 C40 = -6.9320E-06 C22 = -6.8515E-05
C04 = -2.7921E-06 C41 = 1.3563E-06 C23 = 3.1874E-06
C05 = 8.8318E-08 C60 = 9.2595E-07 C42 = -3.5347E-07
C24 = 4.0001E-07 C06 = -4.5950E-08 C60 = -4.6989E-08
C43 = 9.1490E-08 C25 = 6.5183E-08 C07 = -2.2248E-08
C80 = -7.9873E-08 C62 = 2.4536E-08 C44 = -2.3377E-08
C26 = -2.6562E-08 C08 = 3.2125E-09
第4面(R23) 第3反射面
C20 = -1.3393E-03 C02 = 5.5393E-04 C21 = 4.4302E-04
C03 = -6.3472E-05 C40 = 4.1455E-06 C22 = -6.3673E-06
C04 = -2.0399E-07 C41 = 1.0384E-06 C23 = -8.8449E-07
C05 = -1.1335E-07 C60 = -4.9241E-08 C42 = 2.5551E-07
C24 = 6.0826E-07 C06 = -2.1658E-08 C60 = -5.9467E-08
C43 = 9.4023E-08 C25 = 2.6562E-08 C07 = 4.7888E-09
C80 = -6.3428E-10 C62 = -1.1471E-09 C44 = -1.5733E-08
C26 = -2.2921E-08 C08 = 8.9385E-10
第5面(R24) 第4反射面
C20 = 4.7321E-03 C02 = 4.9841E-03 C21 = 6.9652E-05
C03 = -3.9378E-05 C40 = 6.1954E-07 C22 = 1.2448E-06
C04 = -1.6757E-06 C41 = 1.6652E-07 C23 = 1.1462E-07
C05 = -9.2172E-08 C60 = -4.0244E-09 C42 = -2.4076E-08
C24 = 1.1632E-08 C06 = -2.9886E-09 C60 = 7.8085E-10
C43 = 1.1763E-09 C25 = -1.1734E-09 C07 = -8.6470E-11
C80 = -1.1153E-11 C62 = 3.2793E-10 C44 = -5.9399E-11
C26 = -2.1541E-10 C08 = 5.2901E-12
第6面(R25) 第5反射面
C20 = -5.7783E-03 C02 = -2.7383E-03 C21 = 4.6744E-05
C03 = 2.0108E-06 C40 = 4.6547E-07 C22 = 2.8448E-06
C04 = -1.3642E-06 C41 = 1.2274E-07 C23 = 7.3930E-08
C05 = -3.2422E-08 C60 = -3.5765E-09 C42 = -1.3784E-08
C24 = 2.5123E-09 C06 = -1.8232E-09 C60 = 1.3342E-09
C43 = 2.5511E-10 C25 = -7.9154E-10 C07 = 7.9806E-12
C80 = -1.0800E-11 C62 = 1.9625E-10 C44 = -4.9972E-11
C26 = -3.7395E-11 C08 = 4.8805E-12
各反射面の軸上光束における焦点距離データ
f1x = 19.519 mm f1y = 21.579 mm
f2x = 86.485 mm f2y = 166.902 mm
f3x = 197.419 mm f3y = -426.732 mm
f4x = 58.779 mm f4y = 45.083 mm
f5x = 57.327 mm f5y = 68.904 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R20) 0.00 0.00 0.00 30.00 0.00 0.00
2 (R21) 0.00 0.00 30.00 28.00 10.00 0.00 First reflective surface 3 (R22) 0.00 -9.58 3.69 25.00 -13.00 0.00 Second reflective surface 4 (R23) 0.00 -12.19 28.55 32.00 -19.00 0.00 Third reflective surface 5 (R24) 0.00 10.04 5.53 17.00 26.00 0.00 4th reflective surface 6 (R25) 0.00 12.41 22.37 47.41 41.00 0.00 5th reflective surface image surface (IMG) 0.00 -35.00 22.37 0.00 0.00
Free-form data 2nd surface (R21) 1st reflective surface
C20 = -1.3006E-02 C02 = -1.1409E-02 C21 = -2.2986E-04
C03 = 1.2070E-05 C40 = -3.7621E-06 C22 = -1.0194E-05
C04 = 1.0296E-06 C41 = -2.6648E-07 C23 = 4.9447E-08
C05 = -2.9010E-08 C60 = -4.7813E-09 C42 = 1.1215E-08
C24 = 3.5840E-10 C06 = -4.5631E-09 C60 = 5.1317E-09
C43 = 2.2967E-09 C25 = -1.3047E-09 C07 = 2.7855E-10
C80 = 2.5363E-10 C62 = 6.5924E-10 C44 = -1.5322E-10
C26 = 7.2553E-11 C08 = 4.0316E-11
3rd surface (R22) 2nd reflective surface
C20 = 2.9667E-03 C02 = 1.4595E-03 C21 = 1.5246E-03
C03 = -1.0807E-04 C40 = -6.9320E-06 C22 = -6.8515E-05
C04 = -2.7921E-06 C41 = 1.3563E-06 C23 = 3.1874E-06
C05 = 8.8318E-08 C60 = 9.2595E-07 C42 = -3.5347E-07
C24 = 4.0001E-07 C06 = -4.5950E-08 C60 = -4.6989E-08
C43 = 9.1490E-08 C25 = 6.5183E-08 C07 = -2.2248E-08
C80 = -7.9873E-08 C62 = 2.4536E-08 C44 = -2.3377E-08
C26 = -2.6562E-08 C08 = 3.2125E-09
4th surface (R23) 3rd reflective surface
C20 = -1.3393E-03 C02 = 5.5393E-04 C21 = 4.4302E-04
C03 = -6.3472E-05 C40 = 4.1455E-06 C22 = -6.3673E-06
C04 = -2.0399E-07 C41 = 1.0384E-06 C23 = -8.8449E-07
C05 = -1.1335E-07 C60 = -4.9241E-08 C42 = 2.5551E-07
C24 = 6.0826E-07 C06 = -2.1658E-08 C60 = -5.9467E-08
C43 = 9.4023E-08 C25 = 2.6562E-08 C07 = 4.7888E-09
C80 = -6.3428E-10 C62 = -1.1471E-09 C44 = -1.5733E-08
C26 = -2.2921E-08 C08 = 8.9385E-10
5th surface (R24) 4th reflective surface
C20 = 4.7321E-03 C02 = 4.9841E-03 C21 = 6.9652E-05
C03 = -3.9378E-05 C40 = 6.1954E-07 C22 = 1.2448E-06
C04 = -1.6757E-06 C41 = 1.6652E-07 C23 = 1.1462E-07
C05 = -9.2172E-08 C60 = -4.0244E-09 C42 = -2.4076E-08
C24 = 1.1632E-08 C06 = -2.9886E-09 C60 = 7.8085E-10
C43 = 1.1763E-09 C25 = -1.1734E-09 C07 = -8.6470E-11
C80 = -1.1153E-11 C62 = 3.2793E-10 C44 = -5.9399E-11
C26 = -2.1541E-10 C08 = 5.2901E-12
6th surface (R25) 5th reflective surface
C20 = -5.7783E-03 C02 = -2.7383E-03 C21 = 4.6744E-05
C03 = 2.0108E-06 C40 = 4.6547E-07 C22 = 2.8448E-06
C04 = -1.3642E-06 C41 = 1.2274E-07 C23 = 7.3930E-08
C05 = -3.2422E-08 C60 = -3.5765E-09 C42 = -1.3784E-08
C24 = 2.5123E-09 C06 = -1.8232E-09 C60 = 1.3342E-09
C43 = 2.5511E-10 C25 = -7.9154E-10 C07 = 7.9806E-12
C80 = -1.0800E-11 C62 = 1.9625E-10 C44 = -4.9972E-11
C26 = -3.7395E-11 C08 = 4.8805E-12
Focal length data for on-axis luminous flux of each reflecting surface
f1x = 19.519 mm f1y = 21.579 mm
f2x = 86.485 mm f2y = 166.902 mm
f3x = 197.419 mm f3y = -426.732 mm
f4x = 58.779 mm f4y = 45.083 mm
f5x = 57.327 mm f5y = 68.904 mm
[数値実施例2-第3の結像光学系]
画角は、X方向に±0.62°、Y方向に±0.83°である。
焦点距離はX方向に214.98mm、Y方向に214.95mmである。
像面サイズはx方向に4.65mm、y方向に6.20mmである。
第1面R30は円形であり、その直径は19.5mmである。
X軸方向のF値は11.02、Y軸方向のF値は11.02である。
[Numerical Example 2—Third Imaging Optical System]
The angle of view is ± 0.62 ° in the X direction and ± 0.83 ° in the Y direction.
The focal length is 214.98 mm in the X direction and 214.95 mm in the Y direction.
The image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
The first surface R30 is circular and has a diameter of 19.5 mm.
The F value in the X-axis direction is 11.02, and the F value in the Y-axis direction is 11.02.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R30) 0.00 0.00 0.00 57.00 0.00 0.00
2(R31) 0.00 0.00 57.00 57.00 10.00 0.00 第1反射面
3(R32) 0.00 -19.50 3.44 53.00 -11.00 0.00 第2反射面
4(R33) 0.00 -21.34 56.41 65.00 -17.00 0.00 第3反射面
5(R34) 0.00 16.86 3.82 31.00 26.00 0.00 第4反射面
6(R35) 0.00 25.41 33.62 60.41 37.00 0.00 第5反射面
像面(IMG) 0.00 -35.00 33.62 0.00 0.00
自由曲面データ
第2面(R31) 第1反射面
C20 = -8.6661E-03 C02 = -1.4567E-03 C21 = 1.5768E-05
C03 = -1.3125E-06 C40 = -1.8162E-07 C22 = -5.8632E-08
C04 = 1.1225E-07 C41 = -5.8654E-10 C23 = -1.0201E-09
C05 = -1.1671E-09 C60 = -5.3529E-10 C42 = -6.0898E-12
C24 = 1.1026E-11 C06 = 3.2614E-11 C60 = -3.3531E-13
C43 = -1.4877E-12 C25 = -9.5755E-13 C07 = 5.9142E-13
C80 = -2.0141E-13 C62 = -5.1356E-14 C44 = -4.7674E-13
C26 = -2.9488E-13 C08 = 4.5537E-14
第3面(R32) 第2反射面
C20 = 9.1712E-03 C02 = -1.4331E-03 C21 = 1.6261E-05
C03 = 3.2265E-05 C40 = 1.3861E-07 C22 = 3.3164E-07
C04 = 7.8851E-07 C41 = -1.7816E-09 C23 = 1.8317E-08
C05 = -9.7241E-09 C60 = 9.6172E-11 C42 = -1.7200E-11
C24 = -1.7071E-11 C06 = 7.2551E-10 C60 = -7.2382E-12
C43 = -1.1213E-11 C25 = -1.3765E-11 C07 = 6.7281E-12
C80 = 2.3994E-13 C62 = 9.6441E-13 C44 = 3.8422E-13
C26 = -4.2216E-14 C08 = -4.7923E-13
第4面(R33) 第3反射面
C20 = -2.0668E-03 C02 = -3.9068E-03 C21 = -4.0773E-07
C03 = -1.3303E-05 C40 = 3.9215E-07 C22 = 1.3735E-07
C04 = -9.4971E-07 C41 = 2.7216E-09 C23 = 1.3040E-08
C05 = -5.6551E-08 C60 = 7.9108E-10 C42 = 4.0658E-11
C24 = 2.3380E-10 C06 = -3.2568E-09 C60 = 7.7110E-12
C43 = -1.3356E-12 C25 = 1.5744E-11 C07 = -8.8218E-11
C80 = 5.4983E-13 C62 = 8.3570E-13 C44 = 1.9553E-12
C26 = 2.4717E-12 C08 = -1.2961E-12
第5面(R34) 第4反射面
C20 = -8.5973E-04 C02 = 9.9833E-03 C21 = -4.1178E-05
C03 = 4.9253E-05 C40 = 1.2855E-06 C22 = -1.1201E-07
C04 = 1.3989E-06 C41 = 2.6698E-08 C23 = -7.4543E-08
C05 = 3.0287E-09 C60 = -2.2360E-09 C42 = -2.6779E-08
C24 = -6.1557E-08 C06 = 1.0160E-08 C60 = -2.2211E-11
C43 = 4.0368E-10 C25 = 3.8460E-09 C07 = 3.1813E-09
C80 = 7.0740E-12 C62 = 4.6634E-10 C44 = 2.2528E-09
C26 = 3.4047E-09 C08 = 1.5920E-10
第6面(R35) 第5反射面
C20 = 1.4913E-03 C02 = -5.9072E-03 C21 = 1.3644E-05
C03 = -2.7893E-04 C40 = 5.2068E-07 C22 = 5.5143E-07
C04 = 6.5678E-06 C41 = -7.1779E-09 C23 = 9.6909E-09
C05 = -2.5290E-07 C60 = -5.9621E-09 C42 = 1.0785E-08
C24 = 2.5574E-08 C06 = 3.6792E-08 C60 = 5.7367E-10
C43 = -1.2131E-10 C25 = -1.1832E-09 C07 = 5.3316E-09
C80 = 1.0446E-10 C62 = -1.9725E-10 C44 = -7.8369E-10
C26 = -5.2472E-10 C08 = 5.2491E-11
各反射面の軸上光束における焦点距離データ
f1x = 29.293 mm f1y = 169.010 mm
f2x = 27.770 mm f2y = -171.240 mm
f3x = 126.488 mm f3y = 61.195 mm
f4x = -323.534 mm f4y = 22.508 mm
f5x = -209.904 mm f5y = 33.800 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R30) 0.00 0.00 0.00 57.00 0.00 0.00
2 (R31) 0.00 0.00 57.00 57.00 10.00 0.00 First reflective surface 3 (R32) 0.00 -19.50 3.44 53.00 -11.00 0.00 Second reflective surface 4 (R33) 0.00 -21.34 56.41 65.00 -17.00 0.00 Third reflective surface 5 (R34) 0.00 16.86 3.82 31.00 26.00 0.00 4th reflective surface 6 (R35) 0.00 25.41 33.62 60.41 37.00 0.00 5th reflective surface image surface (IMG) 0.00 -35.00 33.62 0.00 0.00
Free-form data 2nd surface (R31) 1st reflective surface
C20 = -8.6661E-03 C02 = -1.4567E-03 C21 = 1.5768E-05
C03 = -1.3125E-06 C40 = -1.8162E-07 C22 = -5.8632E-08
C04 = 1.1225E-07 C41 = -5.8654E-10 C23 = -1.0201E-09
C05 = -1.1671E-09 C60 = -5.3529E-10 C42 = -6.0898E-12
C24 = 1.1026E-11 C06 = 3.2614E-11 C60 = -3.3531E-13
C43 = -1.4877E-12 C25 = -9.5755E-13 C07 = 5.9142E-13
C80 = -2.0141E-13 C62 = -5.1356E-14 C44 = -4.7674E-13
C26 = -2.9488E-13 C08 = 4.5537E-14
3rd surface (R32) 2nd reflective surface
C20 = 9.1712E-03 C02 = -1.4331E-03 C21 = 1.6261E-05
C03 = 3.2265E-05 C40 = 1.3861E-07 C22 = 3.3164E-07
C04 = 7.8851E-07 C41 = -1.7816E-09 C23 = 1.8317E-08
C05 = -9.7241E-09 C60 = 9.6172E-11 C42 = -1.7200E-11
C24 = -1.7071E-11 C06 = 7.2551E-10 C60 = -7.2382E-12
C43 = -1.1213E-11 C25 = -1.3765E-11 C07 = 6.7281E-12
C80 = 2.3994E-13 C62 = 9.6441E-13 C44 = 3.8422E-13
C26 = -4.2216E-14 C08 = -4.7923E-13
4th surface (R33) 3rd reflective surface
C20 = -2.0668E-03 C02 = -3.9068E-03 C21 = -4.0773E-07
C03 = -1.3303E-05 C40 = 3.9215E-07 C22 = 1.3735E-07
C04 = -9.4971E-07 C41 = 2.7216E-09 C23 = 1.3040E-08
C05 = -5.6551E-08 C60 = 7.9108E-10 C42 = 4.0658E-11
C24 = 2.3380E-10 C06 = -3.2568E-09 C60 = 7.7110E-12
C43 = -1.3356E-12 C25 = 1.5744E-11 C07 = -8.8218E-11
C80 = 5.4983E-13 C62 = 8.3570E-13 C44 = 1.9553E-12
C26 = 2.4717E-12 C08 = -1.2961E-12
5th surface (R34) 4th reflective surface
C20 = -8.5973E-04 C02 = 9.9833E-03 C21 = -4.1178E-05
C03 = 4.9253E-05 C40 = 1.2855E-06 C22 = -1.1201E-07
C04 = 1.3989E-06 C41 = 2.6698E-08 C23 = -7.4543E-08
C05 = 3.0287E-09 C60 = -2.2360E-09 C42 = -2.6779E-08
C24 = -6.1557E-08 C06 = 1.0160E-08 C60 = -2.2211E-11
C43 = 4.0368E-10 C25 = 3.8460E-09 C07 = 3.1813E-09
C80 = 7.0740E-12 C62 = 4.6634E-10 C44 = 2.2528E-09
C26 = 3.4047E-09 C08 = 1.5920E-10
6th surface (R35) 5th reflective surface
C20 = 1.4913E-03 C02 = -5.9072E-03 C21 = 1.3644E-05
C03 = -2.7893E-04 C40 = 5.2068E-07 C22 = 5.5143E-07
C04 = 6.5678E-06 C41 = -7.1779E-09 C23 = 9.6909E-09
C05 = -2.5290E-07 C60 = -5.9621E-09 C42 = 1.0785E-08
C24 = 2.5574E-08 C06 = 3.6792E-08 C60 = 5.7367E-10
C43 = -1.2131E-10 C25 = -1.1832E-09 C07 = 5.3316E-09
C80 = 1.0446E-10 C62 = -1.9725E-10 C44 = -7.8369E-10
C26 = -5.2472E-10 C08 = 5.2491E-11
Focal length data for on-axis luminous flux of each reflecting surface
f1x = 29.293 mm f1y = 169.010 mm
f2x = 27.770 mm f2y = -171.240 mm
f3x = 126.488 mm f3y = 61.195 mm
f4x = -323.534 mm f4y = 22.508 mm
f5x = -209.904 mm f5y = 33.800 mm
[数値実施例3-第1の結像光学系]
画角は、X方向に±2.48°、Y方向に±1.86°である。
焦点距離はX方向に71.63mm、Y方向に71.65mmである。
像面サイズはx方向に6.20mm、y方向に4.65mmである。
第1面R40は円形であり、その直径は8.96mmである。
X軸方向のF値は8.00、Y軸方向のF値は8.00である。
[Numerical Example 3—First Imaging Optical System]
The angle of view is ± 2.48 ° in the X direction and ± 1.86 ° in the Y direction.
The focal length is 71.63 mm in the X direction and 71.65 mm in the Y direction.
The image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
The first surface R40 is circular and has a diameter of 8.96 mm.
The F value in the X axis direction is 8.00, and the F value in the Y axis direction is 8.00.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R40) 0.00 0.00 0.00 25.00 0.00 0.00
2(R41) 0.00 0.00 25.00 21.00 -15.00 0.00 第1反射面
3(R42) 0.00 10.50 6.81 19.00 -28.00 0.00 第2反射面
4(R43) 0.00 -8.45 8.14 25.00 -15.00 0.00 第3反射面
5(R44) 0.00 14.02 19.10 28.00 13.00 0.00 第4反射面
像面(IMG) 0.00 -13.98 19.10 0.00 0.00
自由曲面データ
第2面(R41) 第1反射面
C20 = -9.6851E-04 C02 = -1.6382E-03 C21 = -2.7563E-07
C03 = -7.3475E-06 C40 = 3.2467E-07 C22 = 1.2440E-06
C04 = 2.7910E-07 C41 = 2.3177E-09 C23 = 3.9548E-08
C05 = 1.0987E-08 C60 = 5.3591E-09 C42 = 1.5138E-08
C24 = 6.8213E-09 C06 = 1.1146E-09 C60 = 6.1860E-10
C43 = 4.3260E-10 C25 = -4.2188E-10 C07 = 3.3197E-11
C80 = -1.8682E-10 C62 = -5.6301E-10 C44 = -7.0291E-10
C26 = -1.8045E-10 C08 = -9.8203E-12
第3面(R42) 第2反射面
C20 = 1.4351E-03 C02 = 1.9088E-04 C21 = -2.5020E-06
C03 = -5.9554E-06 C40 = 5.4545E-07 C22 = 2.9345E-06
C04 = 5.8877E-07 C41 = 4.9083E-09 C23 = 1.6095E-08
C05 = 1.1321E-08 C60 = 6.2234E-09 C42 = 2.1551E-08
C24 = 9.3795E-09 C06 = 1.8957E-09 C60 = 8.3730E-10
C43 = 7.0942E-10 C25 = -8.7024E-10 C07 = -1.4456E-11
C80 = -2.9646E-10 C62 = -5.9367E-10 C44 = -1.0606E-09
C26 = -1.1098E-10 C08 = 4.7549E-12
第4面(R43) 第3反射面
C20 = -2.1823E-03 C02 = -1.8353E-03 C21 = -7.0071E-06
C03 = -2.8755E-06 C40 = 2.0059E-08 C22 = 2.5511E-06
C04 = 4.3568E-07 C41 = 9.9815E-10 C23 = -9.0890E-09
C05 = 1.9388E-08 C60 = 6.9399E-09 C42 = 3.1789E-08
C24 = 1.7870E-08 C06 = 3.3869E-09 C60 = 5.6110E-10
C43 = 1.2049E-09 C25 = -1.3043E-09 C07 = -1.8523E-10
C80 = -3.4212E-10 C62 = -5.6930E-10 C44 = -1.7893E-09
C26 = -7.6135E-12 C08 = 6.3786E-11
第5面(R44) 第4反射面
C20 = -5.7370E-04 C02 = 6.2396E-04 C21 = -3.6500E-06
C03 = -3.0502E-06 C40 = -1.0155E-06 C22 = 4.3797E-07
C04 = -4.2621E-07 C41 = 5.8787E-08 C23 = 3.2461E-08
C05 = 3.5229E-08 C60 = 1.8499E-08 C42 = 5.2158E-08
C24 = 2.5269E-08 C06 = 7.4259E-11 C60 = -1.8883E-09
C43 = -1.0764E-09 C25 = 2.7881E-09 C07 = -7.3263E-10
C80 = -1.3321E-09 C62 = 1.4928E-10 C44 = -5.7184E-09
C26 = 1.8445E-09 C08 = 5.6683E-10
各反射面の軸上光束における焦点距離データ
f1x = 267.235 mm f1y = 147.405 mm
f2x = 197.296 mm f2y = 1156.430 mm
f3x = 118.600 mm f3y = 131.578 mm
f4x = -447.230 mm f4y = 390.399 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R40) 0.00 0.00 0.00 25.00 0.00 0.00
2 (R41) 0.00 0.00 25.00 21.00 -15.00 0.00 First reflective surface 3 (R42) 0.00 10.50 6.81 19.00 -28.00 0.00 Second reflective surface 4 (R43) 0.00 -8.45 8.14 25.00 -15.00 0.00 Third reflective surface 5 (R44) 0.00 14.02 19.10 28.00 13.00 0.00 4th reflective image plane (IMG) 0.00 -13.98 19.10 0.00 0.00
Free-form surface data 2nd surface (R41) 1st reflective surface
C20 = -9.6851E-04 C02 = -1.6382E-03 C21 = -2.7563E-07
C03 = -7.3475E-06 C40 = 3.2467E-07 C22 = 1.2440E-06
C04 = 2.7910E-07 C41 = 2.3177E-09 C23 = 3.9548E-08
C05 = 1.0987E-08 C60 = 5.3591E-09 C42 = 1.5138E-08
C24 = 6.8213E-09 C06 = 1.1146E-09 C60 = 6.1860E-10
C43 = 4.3260E-10 C25 = -4.2188E-10 C07 = 3.3197E-11
C80 = -1.8682E-10 C62 = -5.6301E-10 C44 = -7.0291E-10
C26 = -1.8045E-10 C08 = -9.8203E-12
3rd surface (R42) 2nd reflective surface
C20 = 1.4351E-03 C02 = 1.9088E-04 C21 = -2.5020E-06
C03 = -5.9554E-06 C40 = 5.4545E-07 C22 = 2.9345E-06
C04 = 5.8877E-07 C41 = 4.9083E-09 C23 = 1.6095E-08
C05 = 1.1321E-08 C60 = 6.2234E-09 C42 = 2.1551E-08
C24 = 9.3795E-09 C06 = 1.8957E-09 C60 = 8.3730E-10
C43 = 7.0942E-10 C25 = -8.7024E-10 C07 = -1.4456E-11
C80 = -2.9646E-10 C62 = -5.9367E-10 C44 = -1.0606E-09
C26 = -1.1098E-10 C08 = 4.7549E-12
4th surface (R43) 3rd reflective surface
C20 = -2.1823E-03 C02 = -1.8353E-03 C21 = -7.0071E-06
C03 = -2.8755E-06 C40 = 2.0059E-08 C22 = 2.5511E-06
C04 = 4.3568E-07 C41 = 9.9815E-10 C23 = -9.0890E-09
C05 = 1.9388E-08 C60 = 6.9399E-09 C42 = 3.1789E-08
C24 = 1.7870E-08 C06 = 3.3869E-09 C60 = 5.6110E-10
C43 = 1.2049E-09 C25 = -1.3043E-09 C07 = -1.8523E-10
C80 = -3.4212E-10 C62 = -5.6930E-10 C44 = -1.7893E-09
C26 = -7.6135E-12 C08 = 6.3786E-11
5th surface (R44) 4th reflective surface
C20 = -5.7370E-04 C02 = 6.2396E-04 C21 = -3.6500E-06
C03 = -3.0502E-06 C40 = -1.0155E-06 C22 = 4.3797E-07
C04 = -4.2621E-07 C41 = 5.8787E-08 C23 = 3.2461E-08
C05 = 3.5229E-08 C60 = 1.8499E-08 C42 = 5.2158E-08
C24 = 2.5269E-08 C06 = 7.4259E-11 C60 = -1.8883E-09
C43 = -1.0764E-09 C25 = 2.7881E-09 C07 = -7.3263E-10
C80 = -1.3321E-09 C62 = 1.4928E-10 C44 = -5.7184E-09
C26 = 1.8445E-09 C08 = 5.6683E-10
Focal length data for on-axis luminous flux of each reflecting surface
f1x = 267.235 mm f1y = 147.405 mm
f2x = 197.296 mm f2y = 1156.430 mm
f3x = 118.600 mm f3y = 131.578 mm
f4x = -447.230 mm f4y = 390.399 mm
[数値実施例3-第2の結像光学系]
画角は、X方向に±9.82°、Y方向に±7.40°である。
焦点距離はX方向に17.91mm、Y方向に17.91mmである。
像面サイズはx方向に6.20mm、y方向に4.65mmである。
第1面R50は円形であり、その直径は2.24mmである。
X軸方向のF値は8.00、Y軸方向のF値は8.00である。
[Numerical Example 3—Second Imaging Optical System]
The angle of view is ± 9.82 ° in the X direction and ± 7.40 ° in the Y direction.
The focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
The image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
The first surface R50 is circular and has a diameter of 2.24 mm.
The F value in the X axis direction is 8.00, and the F value in the Y axis direction is 8.00.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R50) 0.00 0.00 0.00 11.50 0.00 0.00 第1屈折面
2(R51) 0.00 0.00 11.50 9.50 -11.00 0.00 第1反射面
3(R52) 0.00 3.56 2.69 7.00 -26.00 0.00 第2反射面
4(R53) 0.00 -3.17 4.62 9.00 -20.00 0.00 第3反射面
5(R54) 0.00 5.05 8.28 10.00 12.00 0.00 第4反射面
6(R55) 0.00 -4.95 8.28 9.04 0.00 0.00 第2屈折面
像面(IMG) 0.00 -13.98 8.28 0.00 0.00 IMG
プリズムを構成する媒質の屈折率データ
d線:1.5311
g線:1.5432
C線:1.5283
F線:1.5378
自由曲面データ
第1面(R50) 第1屈折面
C20 = -7.3094E-04 C02 = 1.1885E-03 C21 = -3.7160E-04
C03 = -6.6290E-04 C40 = -2.8983E-04 C22 = 2.5951E-04
C04 = -5.6954E-05 C41 = 0 C23 = 0
C05 = 0 C60 = 0 C42 = 0
C24 = 0 C06 = 0 C60 = 0
C43 = 0 C25 = 0 C07 = 0
C80 = 0 C62 = 0 C44 = 0
C26 = 0 C08 = 0
第2面(R51) 第1反射面
C20 = -4.1874E-02 C02 = -1.0943E-02 C21 = -3.5200E-03
C03 = -4.0978E-04 C40 = 4.2519E-06 C22 = -4.4827E-04
C04 = -7.0714E-05 C41 = 2.8973E-05 C23 = -4.3018E-05
C05 = 5.8079E-07 C60 = -2.3453E-07 C42 = 8.3925E-06
C24 = 1.0622E-06 C06 = 8.6058E-07 C60 = -7.5231E-07
C43 = -5.3690E-08 C25 = -4.7292E-07 C07 = -1.3345E-06
C80 = 1.1281E-09 C62 = -1.8161E-07 C44 = -9.7343E-08
C26 = -3.9920E-07 C08 = 2.5430E-07
第3面(R52) 第2反射面
C20 = 6.0622E-02 C02 = 2.2535E-02 C21 = 6.2664E-03
C03 = -6.7830E-04 C40 = 2.4556E-04 C22 = 9.1413E-04
C04 = 1.2966E-04 C41 = 1.1081E-04 C23 = 9.3169E-05
C05 = -3.0783E-05 C60 = 2.2444E-05 C42 = -1.1711E-05
C24 = 1.7149E-05 C06 = 6.6828E-06 C60 = -1.5236E-06
C43 = -6.0915E-07 C25 = -3.0053E-06 C07 = -1.5883E-08
C80 = -1.7996E-05 C62 = 2.3150E-05 C44 = -5.4819E-07
C26 = 8.1042E-08 C08 = -1.1805E-07
第4面(R53) 第3反射面
C20 = -6.2209E-03 C02 = -5.3092E-03 C21 = 2.3491E-04
C03 = 2.9430E-03 C40 = 4.9852E-05 C22 = 4.4870E-04
C04 = 3.6794E-04 C41 = -3.7843E-05 C23 = -6.4350E-05
C05 = -7.3309E-05 C60 = -1.7424E-07 C42 = -2.2383E-05
C24 = -1.9852E-05 C06 = -4.5558E-05 C60 = 1.8400E-06
C43 = -8.0132E-06 C25 = 4.9915E-05 C07 = -4.8562E-05
C80 = 4.0315E-08 C62 = 8.6824E-09 C44 = 3.6764E-05
C26 = -5.7012E-05 C08 = 1.2704E-04
第5面(R54) 第4反射面
C20 = 1.8875E-02 C02 = 3.5771E-02 C21 = 1.2774E-03
C03 = 7.7340E-05 C40 = 1.1798E-05 C22 = -6.2301E-05
C04 = 1.2409E-05 C41 = -4.5093E-06 C23 = 9.1678E-06
C05 = 6.6219E-06 C60 = 1.5324E-07 C42 = 8.3399E-07
C24 = -5.3917E-07 C06 = 5.6967E-06 C60 = 6.0363E-08
C43 = -1.4358E-07 C25 = 1.6014E-07 C07 = 5.2628E-07
C80 = 5.8874E-10 C62 = -5.0843E-09 C44 = 6.4886E-08
C26 = 3.0201E-08 C08 = -5.4287E-07
第6面(R55) 第2屈折面
C20 = 5.5511E-02 C02 = 4.6073E-02 C21 = -8.8590E-04
C03 = -4.5594E-03 C40 = -6.2276E-05 C22 = -1.0073E-04
C04 = 5.6478E-03 C41 = 1.9518E-05 C23 = 9.7473E-04
C05 = 3.8139E-04 C60 = 2.7276E-06 C42 = 6.1233E-05
C24 = -1.1971E-04 C06 = -1.1853E-05 C60 = 1.2066E-06
C43 = -2.0750E-05 C25 = 4.2182E-05 C07 = -2.9605E-05
C80 = 1.8368E-07 C62 = -2.1166E-06 C44 = 9.4032E-06
C26 = 1.3091E-05 C08 = 2.4689E-05
各反射面の軸上光束における焦点距離データ
第1透過面 f1x = -1287.99 mm f1y = 792.133 mm
第1反射面 f2x = 3.972 mm f2y = 14.646 mm
第2反射面 f3x = 2.997 mm f3y = 6.512 mm
第3反射面 f4x = 27.932 mm f4y = 28.900 mm
第4反射面 f5x = 8.844 mm f5y = 4.465 mm
第2透過面 f6x = -16.960 mm f6y = -20.434 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R50) 0.00 0.00 0.00 11.50 0.00 0.00 First refracting surface 2 (R51) 0.00 0.00 11.50 9.50 -11.00 0.00 First reflecting surface 3 (R52) 0.00 3.56 2.69 7.00 -26.00 0.00 Second reflecting surface 4 (R53) 0.00- 3.17 4.62 9.00 -20.00 0.00 Third reflective surface 5 (R54) 0.00 5.05 8.28 10.00 12.00 0.00 Fourth reflective surface 6 (R55) 0.00 -4.95 8.28 9.04 0.00 0.00 Second refractive surface image surface (IMG) 0.00 -13.98 8.28 0.00 0.00 IMG
Refractive index data d-line of the medium constituting the prism: 1.5311
g line: 1.5432
C line: 1.5283
F line: 1.5378
Free-form surface data 1st surface (R50) 1st refractive surface
C20 = -7.3094E-04 C02 = 1.1885E-03 C21 = -3.7160E-04
C03 = -6.6290E-04 C40 = -2.8983E-04 C22 = 2.5951E-04
C04 = -5.6954E-05 C41 = 0 C23 = 0
C05 = 0 C60 = 0 C42 = 0
C24 = 0 C06 = 0 C60 = 0
C43 = 0 C25 = 0 C07 = 0
C80 = 0 C62 = 0 C44 = 0
C26 = 0 C08 = 0
Second surface (R51) First reflective surface
C20 = -4.1874E-02 C02 = -1.0943E-02 C21 = -3.5200E-03
C03 = -4.0978E-04 C40 = 4.2519E-06 C22 = -4.4827E-04
C04 = -7.0714E-05 C41 = 2.8973E-05 C23 = -4.3018E-05
C05 = 5.8079E-07 C60 = -2.3453E-07 C42 = 8.3925E-06
C24 = 1.0622E-06 C06 = 8.6058E-07 C60 = -7.5231E-07
C43 = -5.3690E-08 C25 = -4.7292E-07 C07 = -1.3345E-06
C80 = 1.1281E-09 C62 = -1.8161E-07 C44 = -9.7343E-08
C26 = -3.9920E-07 C08 = 2.5430E-07
3rd surface (R52) 2nd reflective surface
C20 = 6.0622E-02 C02 = 2.2535E-02 C21 = 6.2664E-03
C03 = -6.7830E-04 C40 = 2.4556E-04 C22 = 9.1413E-04
C04 = 1.2966E-04 C41 = 1.1081E-04 C23 = 9.3169E-05
C05 = -3.0783E-05 C60 = 2.2444E-05 C42 = -1.1711E-05
C24 = 1.7149E-05 C06 = 6.6828E-06 C60 = -1.5236E-06
C43 = -6.0915E-07 C25 = -3.0053E-06 C07 = -1.5883E-08
C80 = -1.7996E-05 C62 = 2.3150E-05 C44 = -5.4819E-07
C26 = 8.1042E-08 C08 = -1.1805E-07
4th surface (R53) 3rd reflective surface
C20 = -6.2209E-03 C02 = -5.3092E-03 C21 = 2.3491E-04
C03 = 2.9430E-03 C40 = 4.9852E-05 C22 = 4.4870E-04
C04 = 3.6794E-04 C41 = -3.7843E-05 C23 = -6.4350E-05
C05 = -7.3309E-05 C60 = -1.7424E-07 C42 = -2.2383E-05
C24 = -1.9852E-05 C06 = -4.5558E-05 C60 = 1.8400E-06
C43 = -8.0132E-06 C25 = 4.9915E-05 C07 = -4.8562E-05
C80 = 4.0315E-08 C62 = 8.6824E-09 C44 = 3.6764E-05
C26 = -5.7012E-05 C08 = 1.2704E-04
5th surface (R54) 4th reflective surface
C20 = 1.8875E-02 C02 = 3.5771E-02 C21 = 1.2774E-03
C03 = 7.7340E-05 C40 = 1.1798E-05 C22 = -6.2301E-05
C04 = 1.2409E-05 C41 = -4.5093E-06 C23 = 9.1678E-06
C05 = 6.6219E-06 C60 = 1.5324E-07 C42 = 8.3399E-07
C24 = -5.3917E-07 C06 = 5.6967E-06 C60 = 6.0363E-08
C43 = -1.4358E-07 C25 = 1.6014E-07 C07 = 5.2628E-07
C80 = 5.8874E-10 C62 = -5.0843E-09 C44 = 6.4886E-08
C26 = 3.0201E-08 C08 = -5.4287E-07
6th surface (R55) 2nd refractive surface
C20 = 5.5511E-02 C02 = 4.6073E-02 C21 = -8.8590E-04
C03 = -4.5594E-03 C40 = -6.2276E-05 C22 = -1.0073E-04
C04 = 5.6478E-03 C41 = 1.9518E-05 C23 = 9.7473E-04
C05 = 3.8139E-04 C60 = 2.7276E-06 C42 = 6.1233E-05
C24 = -1.1971E-04 C06 = -1.1853E-05 C60 = 1.2066E-06
C43 = -2.0750E-05 C25 = 4.2182E-05 C07 = -2.9605E-05
C80 = 1.8368E-07 C62 = -2.1166E-06 C44 = 9.4032E-06
C26 = 1.3091E-05 C08 = 2.4689E-05
Focal length data for the light flux on the axis of each reflecting surface First transmitting surface f1x = -1287.99 mm f1y = 792.133 mm
First reflective surface f2x = 3.972 mm f2y = 14.646 mm
Second reflecting surface f3x = 2.997 mm f3y = 6.512 mm
Third reflective surface f4x = 27.932 mm f4y = 28.900 mm
Fourth reflective surface f5x = 8.844 mm f5y = 4.465 mm
Second transmission surface f6x = -16.960 mm f6y = -20.434 mm
[数値実施例4-第1の結像光学系]
画角は、X方向に±7.40°、Y方向に±9.82°である。
焦点距離はX方向に17.91mm、Y方向に17.91mmである。
像面サイズはx方向に4.65mm、y方向に6.20mmである。
第1面R60は円形であり、その直径は3.00mmである。
X軸方向のF値は5.97、Y軸方向のF値は5.97である。
[Numerical Example 4—First Imaging Optical System]
The angle of view is ± 7.40 ° in the X direction and ± 9.82 ° in the Y direction.
The focal length is 17.91 mm in the X direction and 17.91 mm in the Y direction.
The image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
The first surface R60 is circular and has a diameter of 3.00 mm.
The F value in the X axis direction is 5.97, and the F value in the Y axis direction is 5.97.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R60) 0.00 0.00 0.00 30.00 0.00 0.00
2(R61) 0.00 0.00 30.00 30.00 12.00 0.00 第1反射面
3(R62) 0.00 -12.20 2.59 27.00 -14.00 0.00 第2反射面
4(R63) 0.00 -14.09 29.53 36.00 -21.00 0.00 第3反射面
5(R64) 0.00 11.81 4.52 14.00 26.00 0.00 第4反射面
6(R65) 0.00 13.27 18.44 36.27 42.00 0.00 第5反射面
像面(IMG) 0.00 -23.00 18.44 0.00 0.00
自由曲面データ
第2面(R61) 第1反射面
C20 = -1.1849E-02 C02 = -1.0607E-02 C21 = -2.3977E-04
C03 = -1.2754E-05 C40 = -5.2728E-06 C22 = -1.4164E-05
C04 = 1.2196E-06 C41 = -8.2631E-07 C23 = -5.8287E-08
C05 = -2.0877E-09 C60 = 2.6555E-09 C42 = -8.8692E-09
C24 = 1.5123E-08 C06 = -1.8240E-09 C60 = 1.5733E-08
C43 = 4.4639E-09 C25 = -9.4563E-10 C07 = 2.8419E-10
C80 = 4.9141E-10 C62 = 1.7490E-09 C44 = -2.0239E-10
C26 = -4.3355E-11 C08 = 1.4602E-11
第3面(R62) 第2反射面
C20 = 4.8732E-03 C02 = 6.5515E-04 C21 = 1.3543E-03
C03 = -3.0394E-05 C40 = -3.5345E-06 C22 = -7.8867E-05
C04 = 1.3671E-07 C41 = 2.5025E-06 C23 = 3.3914E-06
C05 = 1.1651E-07 C60 = 2.3263E-07 C42 = -2.9986E-07
C24 = -5.1449E-08 C06 = -1.7020E-07 C60 = -8.1769E-08
C43 = 8.0296E-08 C25 = 6.3623E-08 C07 = -1.0593E-08
C80 = -1.4984E-08 C62 = 7.7631E-09 C44 = -1.4488E-08
C26 = -8.0964E-09 C08 = 5.2661E-09
第4面(R63) 第3反射面
C20 = -3.3709E-03 C02 = -3.2783E-03 C21 = 3.4993E-04
C03 = -4.2014E-05 C40 = 2.6432E-06 C22 = -6.6985E-06
C04 = -1.2922E-07 C41 = 5.2885E-07 C23 = -2.1170E-07
C05 = -1.1845E-07 C60 = -1.6295E-08 C42 = 1.5114E-07
C24 = 1.3110E-07 C06 = -1.9142E-08 C60 = -3.2961E-08
C43 = 3.0118E-08 C25 = 7.8137E-09 C07 = 2.8597E-09
C80 = -1.0802E-09 C62 = -3.9826E-09 C44 = 7.2686E-10
C26 = -1.2989E-09 C08 = 4.5982E-10
第5面(R64) 第4反射面
C20 = 4.1462E-03 C02 = 3.8137E-03 C21 = 1.3681E-04
C03 = -1.1395E-04 C40 = 3.6354E-07 C22 = 1.9179E-06
C04 = -7.7444E-06 C41 = 2.2568E-07 C23 = 2.0398E-07
C05 = -5.1116E-07 C60 = -1.3020E-08 C42 = -5.5838E-08
C24 = 1.3111E-08 C06 = -3.2016E-08 C60 = 1.7461E-09
C43 = 2.1222E-09 C25 = -4.7752E-10 C07 = -1.4142E-09
C80 = 3.1691E-11 C62 = 6.5187E-10 C44 = 2.7977E-11
C26 = -1.8006E-10 C08 = 2.6990E-12
第6面(R65) 第5反射面
C20 = -7.3010E-03 C02 = -3.6550E-03 C21 = 1.1180E-04
C03 = -4.9306E-05 C40 = 3.3023E-07 C22 = 5.3654E-06
C04 = -3.9064E-06 C41 = 1.0809E-07 C23 = 7.4197E-08
C05 = -1.2426E-07 C60 = -1.8337E-08 C42 = -3.1374E-08
C24 = -4.3353E-09 C06 = -9.0699E-09 C60 = 3.1742E-09
C43 = -1.3700E-10 C25 = -1.3583E-09 C07 = -1.6529E-10
C80 = 4.1803E-11 C62 = 3.1765E-10 C44 = -8.4932E-11
C26 = -2.1445E-11 C08 = 5.6011E-12
各反射面の軸上光束における焦点距離データ
f1x = 21.570 mm f1y = 23.053 mm
f2x = 52.872 mm f2y = 370.258 mm
f3x = 79.441 mm f3y = 71.194 mm
f4x = 67.086 mm f4y = 58.919 mm
f5x = 46.077 mm f5y = 50.831 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R60) 0.00 0.00 0.00 30.00 0.00 0.00
2 (R61) 0.00 0.00 30.00 30.00 12.00 0.00 First reflective surface 3 (R62) 0.00 -12.20 2.59 27.00 -14.00 0.00 Second reflective surface 4 (R63) 0.00 -14.09 29.53 36.00 -21.00 0.00 Third reflective surface 5 (R64) 0.00 11.81 4.52 14.00 26.00 0.00 4th reflective surface 6 (R65) 0.00 13.27 18.44 36.27 42.00 0.00 5th reflective surface image surface (IMG) 0.00 -23.00 18.44 0.00 0.00
Free-form surface data 2nd surface (R61) 1st reflective surface
C20 = -1.1849E-02 C02 = -1.0607E-02 C21 = -2.3977E-04
C03 = -1.2754E-05 C40 = -5.2728E-06 C22 = -1.4164E-05
C04 = 1.2196E-06 C41 = -8.2631E-07 C23 = -5.8287E-08
C05 = -2.0877E-09 C60 = 2.6555E-09 C42 = -8.8692E-09
C24 = 1.5123E-08 C06 = -1.8240E-09 C60 = 1.5733E-08
C43 = 4.4639E-09 C25 = -9.4563E-10 C07 = 2.8419E-10
C80 = 4.9141E-10 C62 = 1.7490E-09 C44 = -2.0239E-10
C26 = -4.3355E-11 C08 = 1.4602E-11
3rd surface (R62) 2nd reflective surface
C20 = 4.8732E-03 C02 = 6.5515E-04 C21 = 1.3543E-03
C03 = -3.0394E-05 C40 = -3.5345E-06 C22 = -7.8867E-05
C04 = 1.3671E-07 C41 = 2.5025E-06 C23 = 3.3914E-06
C05 = 1.1651E-07 C60 = 2.3263E-07 C42 = -2.9986E-07
C24 = -5.1449E-08 C06 = -1.7020E-07 C60 = -8.1769E-08
C43 = 8.0296E-08 C25 = 6.3623E-08 C07 = -1.0593E-08
C80 = -1.4984E-08 C62 = 7.7631E-09 C44 = -1.4488E-08
C26 = -8.0964E-09 C08 = 5.2661E-09
4th surface (R63) 3rd reflective surface
C20 = -3.3709E-03 C02 = -3.2783E-03 C21 = 3.4993E-04
C03 = -4.2014E-05 C40 = 2.6432E-06 C22 = -6.6985E-06
C04 = -1.2922E-07 C41 = 5.2885E-07 C23 = -2.1170E-07
C05 = -1.1845E-07 C60 = -1.6295E-08 C42 = 1.5114E-07
C24 = 1.3110E-07 C06 = -1.9142E-08 C60 = -3.2961E-08
C43 = 3.0118E-08 C25 = 7.8137E-09 C07 = 2.8597E-09
C80 = -1.0802E-09 C62 = -3.9826E-09 C44 = 7.2686E-10
C26 = -1.2989E-09 C08 = 4.5982E-10
5th surface (R64) 4th reflective surface
C20 = 4.1462E-03 C02 = 3.8137E-03 C21 = 1.3681E-04
C03 = -1.1395E-04 C40 = 3.6354E-07 C22 = 1.9179E-06
C04 = -7.7444E-06 C41 = 2.2568E-07 C23 = 2.0398E-07
C05 = -5.1116E-07 C60 = -1.3020E-08 C42 = -5.5838E-08
C24 = 1.3111E-08 C06 = -3.2016E-08 C60 = 1.7461E-09
C43 = 2.1222E-09 C25 = -4.7752E-10 C07 = -1.4142E-09
C80 = 3.1691E-11 C62 = 6.5187E-10 C44 = 2.7977E-11
C26 = -1.8006E-10 C08 = 2.6990E-12
6th surface (R65) 5th reflective surface
C20 = -7.3010E-03 C02 = -3.6550E-03 C21 = 1.1180E-04
C03 = -4.9306E-05 C40 = 3.3023E-07 C22 = 5.3654E-06
C04 = -3.9064E-06 C41 = 1.0809E-07 C23 = 7.4197E-08
C05 = -1.2426E-07 C60 = -1.8337E-08 C42 = -3.1374E-08
C24 = -4.3353E-09 C06 = -9.0699E-09 C60 = 3.1742E-09
C43 = -1.3700E-10 C25 = -1.3583E-09 C07 = -1.6529E-10
C80 = 4.1803E-11 C62 = 3.1765E-10 C44 = -8.4932E-11
C26 = -2.1445E-11 C08 = 5.6011E-12
Focal length data for on-axis luminous flux of each reflecting surface
f1x = 21.570 mm f1y = 23.053 mm
f2x = 52.872 mm f2y = 370.258 mm
f3x = 79.441 mm f3y = 71.194 mm
f4x = 67.086 mm f4y = 58.919 mm
f5x = 46.077 mm f5y = 50.831 mm
[数値実施例4-第2の結像光学系]
画角は、X方向に±1.86°、Y方向に±2.48°である。
焦点距離はX方向に71.65mm、Y方向に71.65mmである。
像面サイズはx方向に4.65mm、y方向に6.20mmである。
第1面R70は円形であり、その直径は8.96mmである。
X軸方向のF値は7.99、Y軸方向のF値は7.99である。
[Numerical Example 4—Second Imaging Optical System]
The angle of view is ± 1.86 ° in the X direction and ± 2.48 ° in the Y direction.
The focal length is 71.65 mm in the X direction and 71.65 mm in the Y direction.
The image plane size is 4.65 mm in the x direction and 6.20 mm in the y direction.
The first surface R70 is circular and has a diameter of 8.96 mm.
The F value in the X axis direction is 7.9, and the F value in the Y axis direction is 7.9.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R70) 0.00 0.00 0.00 21.00 0.00 0.00
2(R71) 0.00 0.00 21.00 22.00 13.00 0.00 第1反射面
3(R72) 0.00 -9.64 1.23 19.00 -15.00 0.00 第2反射面
4(R73) 0.00 -10.97 20.18 26.00 -21.00 0.00 第3反射面
5(R74) 0.00 7.73 2.12 11.00 27.00 0.00 第4反射面
6(R75) 0.00 9.26 13.01 32.26 41.00 0.00 第5反射面
像面(IMG) 0.00 -23.00 13.01 0.00 0.00
自由曲面データ
第2面(R71) 第1反射面
C20 = -1.3097E-02 C02 = -6.5662E-03 C21 = 4.0277E-04
C03 = -4.5591E-05 C40 = 2.0463E-06 C22 = -2.5201E-06
C04 = -8.2150E-07 C41 = -3.1869E-08 C23 = 1.0790E-08
C05 = 7.1138E-08 C60 = 3.4528E-09 C42 = -1.3542E-09
C24 = 5.6874E-09 C06 = -1.0687E-08 C60 = -2.5661E-10
C43 = 8.4152E-10 C25 = -1.5245E-09 C07 = 1.2188E-09
C80 = -6.8661E-11 C62 = 8.0214E-11 C44 = -2.1675E-11
C26 = 4.5006E-10 C08 = -4.8284E-11
第3面(R72) 第2反射面
C20 = 1.0214E-02 C02 = -1.0926E-02 C21 = 4.9822E-06
C03 = 3.4616E-04 C40 = -6.1899E-05 C22 = -5.3191E-05
C04 = -8.3220E-06 C41 = -5.7063E-06 C23 = 4.4775E-06
C05 = 3.7873E-06 C60 = 1.3021E-05 C42 = 6.1850E-06
C24 = 7.3067E-07 C06 = -2.6194E-07 C60 = 1.3438E-06
C43 = -8.8786E-07 C25 = -8.2660E-07 C07 = -3.2418E-08
C80 = -1.9257E-06 C62 = -1.3107E-06 C44 = -6.0038E-07
C26 = -8.1111E-08 C08 = 4.1425E-09
第4面(R73) 第3反射面
C20 = -1.6793E-02 C02 = -1.5250E-02 C21 = 6.8184E-05
C03 = 3.8297E-05 C40 = -4.6483E-06 C22 = -1.0220E-05
C04 = -5.8580E-06 C41 = 8.0382E-08 C23 = 2.5410E-07
C05 = 1.0292E-07 C60 = -5.0842E-09 C42 = -1.2848E-08
C24 = -5.1362E-10 C06 = -2.0783E-08 C60 = 4.0373E-10
C43 = -1.8448E-09 C25 = 1.2830E-11 C07 = -3.2549E-09
C80 = 4.5851E-11 C62 = -7.2414E-11 C44 = -1.3814E-10
C26 = 9.8425E-10 C08 = -7.4979E-11
第5面(R74) 第4反射面
C20 = -2.7919E-03 C02 = 1.0948E-02 C21 = -1.8137E-03
C03 = 3.8375E-04 C40 = -1.5087E-05 C22 = -1.3172E-05
C04 = -2.3843E-05 C41 = -3.6027E-07 C23 = -1.3487E-06
C05 = -3.9800E-06 C60 = 6.7006E-08 C42 = -3.0649E-07
C24 = 2.1746E-07 C06 = -5.7690E-07 C60 = 4.4161E-09
C43 = -6.1052E-08 C25 = 6.1649E-08 C07 = -1.2750E-07
C80 = -4.1923E-09 C62 = 1.3662E-08 C44 = 2.7702E-08
C26 = 1.6826E-08 C08 = -3.2237E-08
第6面(R75) 第5反射面
C20 = -2.2621E-03 C02 = -8.0290E-03 C21 = -3.5769E-04
C03 = -1.6503E-04 C40 = 1.6452E-06 C22 = -3.3962E-05
C04 = 1.1040E-05 C41 = 8.8354E-07 C23 = -2.5143E-06
C05 = 7.1143E-07 C60 = 1.2133E-07 C42 = -1.3257E-07
C24 = 4.8156E-09 C06 = 6.3194E-08 C60 = 1.5081E-08
C43 = 4.9038E-08 C25 = 2.1104E-09 C07 = 1.0194E-08
C80 = -6.5378E-09 C62 = -1.6927E-09 C44 = 8.2618E-10
C26 = -1.4545E-08 C08 = -1.4402E-10
各反射面の軸上光束における焦点距離データ
f1x = 19.591 mm f1y = 37.098 mm
f2x = 25.341 mm f2y = -22.101 mm
f3x = 15.947 mm f3y = 15.304 mm
f4x = -100.498 mm f4y = 20.346 mm
f5x = 146.434 mm f5y = 23.499 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R70) 0.00 0.00 0.00 21.00 0.00 0.00
2 (R71) 0.00 0.00 21.00 22.00 13.00 0.00 First reflective surface 3 (R72) 0.00 -9.64 1.23 19.00 -15.00 0.00 Second reflective surface 4 (R73) 0.00 -10.97 20.18 26.00 -21.00 0.00 Third reflective surface 5 (R74) 0.00 7.73 2.12 11.00 27.00 0.00 4th reflective surface 6 (R75) 0.00 9.26 13.01 32.26 41.00 0.00 5th reflective surface image surface (IMG) 0.00 -23.00 13.01 0.00 0.00
Free-form data 2nd surface (R71) 1st reflective surface
C20 = -1.3097E-02 C02 = -6.5662E-03 C21 = 4.0277E-04
C03 = -4.5591E-05 C40 = 2.0463E-06 C22 = -2.5201E-06
C04 = -8.2150E-07 C41 = -3.1869E-08 C23 = 1.0790E-08
C05 = 7.1138E-08 C60 = 3.4528E-09 C42 = -1.3542E-09
C24 = 5.6874E-09 C06 = -1.0687E-08 C60 = -2.5661E-10
C43 = 8.4152E-10 C25 = -1.5245E-09 C07 = 1.2188E-09
C80 = -6.8661E-11 C62 = 8.0214E-11 C44 = -2.1675E-11
C26 = 4.5006E-10 C08 = -4.8284E-11
3rd surface (R72) 2nd reflective surface
C20 = 1.0214E-02 C02 = -1.0926E-02 C21 = 4.9822E-06
C03 = 3.4616E-04 C40 = -6.1899E-05 C22 = -5.3191E-05
C04 = -8.3220E-06 C41 = -5.7063E-06 C23 = 4.4775E-06
C05 = 3.7873E-06 C60 = 1.3021E-05 C42 = 6.1850E-06
C24 = 7.3067E-07 C06 = -2.6194E-07 C60 = 1.3438E-06
C43 = -8.8786E-07 C25 = -8.2660E-07 C07 = -3.2418E-08
C80 = -1.9257E-06 C62 = -1.3107E-06 C44 = -6.0038E-07
C26 = -8.1111E-08 C08 = 4.1425E-09
4th surface (R73) 3rd reflective surface
C20 = -1.6793E-02 C02 = -1.5250E-02 C21 = 6.8184E-05
C03 = 3.8297E-05 C40 = -4.6483E-06 C22 = -1.0220E-05
C04 = -5.8580E-06 C41 = 8.0382E-08 C23 = 2.5410E-07
C05 = 1.0292E-07 C60 = -5.0842E-09 C42 = -1.2848E-08
C24 = -5.1362E-10 C06 = -2.0783E-08 C60 = 4.0373E-10
C43 = -1.8448E-09 C25 = 1.2830E-11 C07 = -3.2549E-09
C80 = 4.5851E-11 C62 = -7.2414E-11 C44 = -1.3814E-10
C26 = 9.8425E-10 C08 = -7.4979E-11
5th surface (R74) 4th reflective surface
C20 = -2.7919E-03 C02 = 1.0948E-02 C21 = -1.8137E-03
C03 = 3.8375E-04 C40 = -1.5087E-05 C22 = -1.3172E-05
C04 = -2.3843E-05 C41 = -3.6027E-07 C23 = -1.3487E-06
C05 = -3.9800E-06 C60 = 6.7006E-08 C42 = -3.0649E-07
C24 = 2.1746E-07 C06 = -5.7690E-07 C60 = 4.4161E-09
C43 = -6.1052E-08 C25 = 6.1649E-08 C07 = -1.2750E-07
C80 = -4.1923E-09 C62 = 1.3662E-08 C44 = 2.7702E-08
C26 = 1.6826E-08 C08 = -3.2237E-08
6th surface (R75) 5th reflective surface
C20 = -2.2621E-03 C02 = -8.0290E-03 C21 = -3.5769E-04
C03 = -1.6503E-04 C40 = 1.6452E-06 C22 = -3.3962E-05
C04 = 1.1040E-05 C41 = 8.8354E-07 C23 = -2.5143E-06
C05 = 7.1143E-07 C60 = 1.2133E-07 C42 = -1.3257E-07
C24 = 4.8156E-09 C06 = 6.3194E-08 C60 = 1.5081E-08
C43 = 4.9038E-08 C25 = 2.1104E-09 C07 = 1.0194E-08
C80 = -6.5378E-09 C62 = -1.6927E-09 C44 = 8.2618E-10
C26 = -1.4545E-08 C08 = -1.4402E-10
Focal length data for on-axis luminous flux of each reflecting surface
f1x = 19.591 mm f1y = 37.098 mm
f2x = 25.341 mm f2y = -22.101 mm
f3x = 15.947 mm f3y = 15.304 mm
f4x = -100.498 mm f4y = 20.346 mm
f5x = 146.434 mm f5y = 23.499 mm
[数値実施例5-第1の結像光学系]
画角は、X方向に±2.48°、Y方向に±1.86°である。
焦点距離はX方向に71.63mm、Y方向に71.65mmである。
像面サイズはx方向に6.20mm、y方向に4.65mmである。
第1面R80は円形であり、その直径は8.96mmである。
X軸方向のF値は7.99、Y軸方向のF値は8.00である。
[Numerical Example 5—First Imaging Optical System]
The angle of view is ± 2.48 ° in the X direction and ± 1.86 ° in the Y direction.
The focal length is 71.63 mm in the X direction and 71.65 mm in the Y direction.
The image plane size is 6.20 mm in the x direction and 4.65 mm in the y direction.
The first surface R80 is circular and has a diameter of 8.96 mm.
The F value in the X-axis direction is 7.99, and the F value in the Y-axis direction is 8.00.
面データ
面番号 Xi Yi Zi Di θxi θyi
1(R80) 0.00 0.00 0.00 30.00 0.00 0.00
2(R81) 0.00 0.00 30.00 27.00 -15.00 0.00 第1反射面
3(R82) 0.00 13.50 6.62 24.00 -28.00 0.00 第2反射面
4(R83) 0.00 -10.44 8.29 30.00 -15.00 0.00 第3反射面
5(R84) 0.00 16.52 21.44 37.32 13.00 0.00 第4反射面
像面(IMG) 0.00 -20.80 21.44 0.00 0.00
自由曲面データ
第2面(R81) 第1反射面
C20 = 1.6573E-03 C02 = -4.9492E-04 C21 = 5.7515E-06
C03 = -8.4053E-06 C40 = -1.1915E-07 C22 = -2.5296E-08
C04 = -2.2552E-07 C41 = 9.7021E-08 C23 = 4.1303E-08
C05 = -1.3955E-09 C60 = 1.3621E-08 C42 = 5.3892E-08
C24 = 2.3890E-08 C06 = 2.9568E-09 C60 = -1.9392E-09
C43 = -1.1327E-10 C25 = -4.1682E-10 C07 = 1.3528E-10
C80 = -1.7405E-10 C62 = -1.0536E-09 C44 = -8.7215E-10
C26 = -2.2739E-10 C08 = 8.6178E-12
第3面(R82) 第2反射面
C20 = 1.2986E-03 C02 = 1.7238E-04 C21 = 1.5345E-05
C03 = -1.6647E-05 C40 = -6.9248E-07 C22 = -3.1052E-07
C04 = -4.7187E-07 C41 = 1.2671E-07 C23 = 9.2417E-08
C05 = 1.6648E-08 C60 = 7.5234E-09 C42 = 3.8913E-08
C24 = 2.1299E-08 C06 = 6.5888E-09 C60 = -1.4243E-09
C43 = -8.9807E-10 C25 = -1.0820E-09 C07 = -2.9560E-11
C80 = -4.5870E-11 C62 = -3.6597E-10 C44 = -3.9172E-10
C26 = -1.6850E-10 C08 = -2.6644E-11
第4面(R83) 第3反射面
C20 = -5.0948E-03 C02 = -2.5056E-03 C21 = -6.3293E-06
C03 = -2.2971E-05 C40 = -7.4058E-07 C22 = -8.4193E-07
C04 = -6.4218E-07 C41 = 7.6108E-08 C23 = 6.0598E-08
C05 = 2.8273E-08 C60 = 3.5155E-09 C42 = 2.1456E-08
C24 = 1.3892E-08 C06 = 1.0271E-08 C60 = -6.5060E-10
C43 = -5.3615E-10 C25 = -9.5256E-10 C07 = -1.6459E-10
C80 = -1.6210E-11 C62 = -1.3117E-10 C44 = -2.0857E-10
C26 = -1.1243E-10 C08 = -7.5599E-11
第5面(R84) 第4反射面
C20 = -4.2285E-03 C02 = 9.6427E-04 C21 = -1.6362E-05
C03 = -2.1208E-05 C40 = -2.7846E-06 C22 = -1.8770E-06
C04 = -1.4132E-06 C41 = 3.0886E-07 C23 = 1.4701E-07
C05 = 4.9844E-08 C60 = 3.4521E-08 C42 = 1.0056E-07
C24 = 2.4949E-08 C06 = 3.3659E-08 C60 = -8.3751E-09
C43 = -3.9621E-09 C25 = -3.9225E-09 C07 = -7.6975E-10
C80 = -5.0435E-10 C62 = -1.3276E-09 C44 = -1.3957E-09
C26 = -3.7318E-10 C08 = -5.9170E-10
各反射面の軸上光束における焦点距離データ
f1x = -156.167 mm f1y = 487.918 mm
f2x = 218.037 mm f2y = 1280.540 mm
f3x = 50.801 mm f3y = 96.3785 mm
f4x = - 60.678 mm f4y = 252.619 mm
Surface data surface number Xi Yi Zi Di θxi θyi
1 (R80) 0.00 0.00 0.00 30.00 0.00 0.00
2 (R81) 0.00 0.00 30.00 27.00 -15.00 0.00 First reflective surface 3 (R82) 0.00 13.50 6.62 24.00 -28.00 0.00 Second reflective surface 4 (R83) 0.00 -10.44 8.29 30.00 -15.00 0.00 Third reflective surface 5 (R84) 0.00 16.52 21.44 37.32.
Free-form surface data 2nd surface (R81) 1st reflective surface
C20 = 1.6573E-03 C02 = -4.9492E-04 C21 = 5.7515E-06
C03 = -8.4053E-06 C40 = -1.1915E-07 C22 = -2.5296E-08
C04 = -2.2552E-07 C41 = 9.7021E-08 C23 = 4.1303E-08
C05 = -1.3955E-09 C60 = 1.3621E-08 C42 = 5.3892E-08
C24 = 2.3890E-08 C06 = 2.9568E-09 C60 = -1.9392E-09
C43 = -1.1327E-10 C25 = -4.1682E-10 C07 = 1.3528E-10
C80 = -1.7405E-10 C62 = -1.0536E-09 C44 = -8.7215E-10
C26 = -2.2739E-10 C08 = 8.6178E-12
3rd surface (R82) 2nd reflective surface
C20 = 1.2986E-03 C02 = 1.7238E-04 C21 = 1.5345E-05
C03 = -1.6647E-05 C40 = -6.9248E-07 C22 = -3.1052E-07
C04 = -4.7187E-07 C41 = 1.2671E-07 C23 = 9.2417E-08
C05 = 1.6648E-08 C60 = 7.5234E-09 C42 = 3.8913E-08
C24 = 2.1299E-08 C06 = 6.5888E-09 C60 = -1.4243E-09
C43 = -8.9807E-10 C25 = -1.0820E-09 C07 = -2.9560E-11
C80 = -4.5870E-11 C62 = -3.6597E-10 C44 = -3.9172E-10
C26 = -1.6850E-10 C08 = -2.6644E-11
4th surface (R83) 3rd reflective surface
C20 = -5.0948E-03 C02 = -2.5056E-03 C21 = -6.3293E-06
C03 = -2.2971E-05 C40 = -7.4058E-07 C22 = -8.4193E-07
C04 = -6.4218E-07 C41 = 7.6108E-08 C23 = 6.0598E-08
C05 = 2.8273E-08 C60 = 3.5155E-09 C42 = 2.1456E-08
C24 = 1.3892E-08 C06 = 1.0271E-08 C60 = -6.5060E-10
C43 = -5.3615E-10 C25 = -9.5256E-10 C07 = -1.6459E-10
C80 = -1.6210E-11 C62 = -1.3117E-10 C44 = -2.0857E-10
C26 = -1.1243E-10 C08 = -7.5599E-11
5th surface (R84) 4th reflective surface
C20 = -4.2285E-03 C02 = 9.6427E-04 C21 = -1.6362E-05
C03 = -2.1208E-05 C40 = -2.7846E-06 C22 = -1.8770E-06
C04 = -1.4132E-06 C41 = 3.0886E-07 C23 = 1.4701E-07
C05 = 4.9844E-08 C60 = 3.4521E-08 C42 = 1.0056E-07
C24 = 2.4949E-08 C06 = 3.3659E-08 C60 = -8.3751E-09
C43 = -3.9621E-09 C25 = -3.9225E-09 C07 = -7.6975E-10
C80 = -5.0435E-10 C62 = -1.3276E-09 C44 = -1.3957E-09
C26 = -3.7318E-10 C08 = -5.9170E-10
Focal length data for on-axis luminous flux of each reflecting surface
f1x = -156.167 mm f1y = 487.918 mm
f2x = 218.037 mm f2y = 1280.540 mm
f3x = 50.801 mm f3y = 96.3785 mm
f4x =-60.678 mm f4y = 252.619 mm
[数値実施例5-第2の結像光学系]
面番号 ri di ndi vdi 有効径
R90,R91 -10.441 1.00 1.60311 60.6 2.24
R92 -3.948 0.20 2.49
R93 -3.315 2.00 1.75520 27.5 2.50
R94 -5.048 2.00 3.30
R95 0.000 3.00 1.69680 55.5 3.74 プリズム入射面
R96 0.000 3.00 1.69680 55.5 5.46 プリズム反射面
R97 0.000 7.50 4.42 プリズム射出面
R98 18.126 1.50 1.51633 64.1 5.93
R99 -8.330 1.90 5.94
R100 -6.707 1.00 1.71736 29.5 5.18
R101 -403.187 5.90 5.38
像面(IMG) 0.000
各種データ
焦点距離 17.91
Fナンバー 8.01
半画角(°) 12.22
像高 3.875
レンズ全長 29.000
BF 5.900
入射瞳位置 0.000
射出瞳位置 -13.79
前側主点位置 1.62
後側主点位置 -12.01
単レンズデータ
レンズ 始面 焦点距離
1 1 9.95
2 3 -25.40
3 8 11.27
4 10 -9.52
[Numerical Example 5—Second Imaging Optical System]
Surface number ri di ndi vdi Effective diameter
R90, R91 -10.441 1.00 1.60311 60.6 2.24
R92 -3.948 0.20 2.49
R93 -3.315 2.00 1.75520 27.5 2.50
R94 -5.048 2.00 3.30
R95 0.000 3.00 1.69680 55.5 3.74 Prism entrance surface
R96 0.000 3.00 1.69680 55.5 5.46 Prism reflecting surface
R97 0.000 7.50 4.42 Prism exit surface
R98 18.126 1.50 1.51633 64.1 5.93
R99 -8.330 1.90 5.94
R100 -6.707 1.00 1.71736 29.5 5.18
R101 -403.187 5.90 5.38
Image plane (IMG) 0.000
Various data focal length 17.91
F number 8.01
Half angle of view (°) 12.22
Statue height 3.875
Total lens length 29.000
BF 5.900
Entrance pupil position 0.000
Exit pupil position -13.79
Front principal point position 1.62
Rear principal point position -12.01
Single lens data lens Start surface
2 3 -25.40
3 8 11.27
4 10 -9.52
以上、本発明の好ましい実施形態及び実施例について説明したが、本発明はこれらの実施形態及び実施例に限定されず、その要旨の範囲内で種々の組合せ、変形及び変更が可能である。例えば、上述した各実施例では第1の結像光学系L1に対して第2の結像光学系L2を移動させる例について述べたが、第1の結像光学系L1を第2の結像光学系L2に対して移動させても良い。従って、本発明の範囲を公にするために以下の請求項を添付する。 The preferred embodiments and examples of the present invention have been described above, but the present invention is not limited to these embodiments and examples, and various combinations, modifications, and changes are possible within the scope of the gist. For example, in each of the above-described embodiments, the example in which the second imaging optical system L2 is moved with respect to the first imaging optical system L1 has been described, but the first imaging optical system L1 is used as the second imaging optical system L1. You may move with respect to the optical system L2. Therefore, in order to make the scope of the present invention public, the following claims are attached.
本願は、2018年3月30日提出の日本国特許出願特願2018-069293を基礎として優先権を主張するものであり、その記載内容の全てをここに援用する。 This application claims priority on the basis of Japanese Patent Application No. 2018-069293 filed on Mar. 30, 2018, the entire contents of which are incorporated herein by reference.
L1 第1の結像光学系
L2 第2の結像光学系
100 撮像装置(光学装置)
L1 First imaging optical system L2 Second imaging
Claims (19)
前記第1の結像光学系が使用される状態において、前記第2の結像光学系は前記第1の結像光学系の光路を遮らない位置に配置され、
前記第2の結像光学系が使用される状態において、前記第2の結像光学系は前記光路を遮る位置に配置されることを特徴とする光学装置。 An optical apparatus having first and second imaging optical systems, wherein the first and second imaging optical systems can be switched and used.
In a state where the first imaging optical system is used, the second imaging optical system is disposed at a position that does not block the optical path of the first imaging optical system,
The optical apparatus, wherein the second imaging optical system is disposed at a position that blocks the optical path when the second imaging optical system is used.
前記第1の結像光学系と前記第2の結像光学系のいずれが使用される場合であっても、前記撮像素子を用いて画像を取得することを特徴とする請求項1に記載の光学装置。 The optical device has an image sensor,
2. The image according to claim 1, wherein an image is acquired by using the imaging element regardless of which of the first imaging optical system and the second imaging optical system is used. Optical device.
前記第1の結像光学系と前記第2の結像光学系のいずれが使用される場合であっても、前記撮像素子を用いて画像が取得され、
前記切り替えは、前記第1及び第2の結像光学系の相対位置関係を、前記第1の結像光学系によって結像される光線が通る空間から前記第2の結像光学系が退避された状態と、前記空間内に前記第2の結像光学系が挿入された状態との間で変化させることによって行われ、
前記切り替えの前後で、前記第1の結像光学系と前記撮像素子の相対位置関係は変化しないことを特徴とする光学装置。 An optical apparatus having first and second imaging optical systems and an image sensor, wherein the first and second imaging optical systems can be switched and used.
Regardless of which of the first imaging optical system and the second imaging optical system is used, an image is acquired using the imaging element,
In the switching, the relative position relationship between the first and second imaging optical systems is such that the second imaging optical system is withdrawn from a space through which light rays imaged by the first imaging optical system pass. And a state in which the second imaging optical system is inserted into the space, and
The optical apparatus according to claim 1, wherein a relative positional relationship between the first imaging optical system and the imaging element does not change before and after the switching.
前記第2の結像光学系が使用される状態において、物体からの光は前記開口部の少なくとも一部の領域を通って前記第2の結像光学系に入射することを特徴とする請求項1乃至15のいずれか一項に記載の光学装置。 An opening through which light from an object is incident when the first imaging optical system is used;
The light from the object is incident on the second imaging optical system through at least a partial region of the opening in a state where the second imaging optical system is used. The optical device according to any one of 1 to 15.
前記光学装置は、前記第3の結像光学系を使用する際には、前記第1の結像光学系及び前記第2の結像光学系を、前記第3の結像光学系によって結像される光線が通る空間から退避させるように前記第1乃至第3の結像光学系の相対位置関係を変化させ、
前記第1の結像光学系または前記第2の結像光学系を使用する際には、使用する結像光学系が前記第3の結像光学系によって結像される光線が通る空間に挿入されるように前記第1乃至第3の結像光学系の相対位置関係を変化させることを特徴とする請求項1乃至16のいずれか一項に記載の光学装置。 A third imaging optical system;
When the optical device uses the third imaging optical system, the first imaging optical system and the second imaging optical system are imaged by the third imaging optical system. Changing the relative positional relationship of the first to third imaging optical systems so as to be retracted from the space through which the light beam passes,
When using the first imaging optical system or the second imaging optical system, the imaging optical system to be used is inserted into a space through which the light beam imaged by the third imaging optical system passes. The optical device according to any one of claims 1 to 16, wherein the relative positional relationship of the first to third imaging optical systems is changed as described above.
The optical apparatus according to claim 1, wherein the second imaging optical system includes a plurality of lenses and a prism having a reflecting surface.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2018-069293 | 2018-03-30 | ||
| JP2018069293A JP2019179189A (en) | 2018-03-30 | 2018-03-30 | Optical device |
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| Publication Number | Publication Date |
|---|---|
| WO2019189289A1 true WO2019189289A1 (en) | 2019-10-03 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2019/013059 Ceased WO2019189289A1 (en) | 2018-03-30 | 2019-03-27 | Optical apparatus |
Country Status (2)
| Country | Link |
|---|---|
| JP (1) | JP2019179189A (en) |
| WO (1) | WO2019189289A1 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN113126235A (en) * | 2021-04-12 | 2021-07-16 | 中国电子科技集团公司第十一研究所 | Visual field switching mechanism of infrared optical system and infrared optical system |
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|---|---|---|---|---|
| JPH1195108A (en) * | 1997-09-22 | 1999-04-09 | Canon Inc | Optical element and imaging system using the same |
| JP2000098476A (en) * | 1998-09-28 | 2000-04-07 | Canon Inc | Optical system |
| JP2002300438A (en) * | 2001-03-29 | 2002-10-11 | Fuji Photo Film Co Ltd | Digital camera |
| JP2012226205A (en) * | 2011-04-21 | 2012-11-15 | Olympus Imaging Corp | Driving device and imaging apparatus using the same |
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2018
- 2018-03-30 JP JP2018069293A patent/JP2019179189A/en active Pending
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH1195108A (en) * | 1997-09-22 | 1999-04-09 | Canon Inc | Optical element and imaging system using the same |
| JP2000098476A (en) * | 1998-09-28 | 2000-04-07 | Canon Inc | Optical system |
| JP2002300438A (en) * | 2001-03-29 | 2002-10-11 | Fuji Photo Film Co Ltd | Digital camera |
| JP2012226205A (en) * | 2011-04-21 | 2012-11-15 | Olympus Imaging Corp | Driving device and imaging apparatus using the same |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN113126235A (en) * | 2021-04-12 | 2021-07-16 | 中国电子科技集团公司第十一研究所 | Visual field switching mechanism of infrared optical system and infrared optical system |
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| JP2019179189A (en) | 2019-10-17 |
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