JP2000221404A5 - Imaging optical system, optical system using the same, optical apparatus - Google Patents
Imaging optical system, optical system using the same, optical apparatus Download PDFInfo
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- JP2000221404A5 JP2000221404A5 JP1999019282A JP1928299A JP2000221404A5 JP 2000221404 A5 JP2000221404 A5 JP 2000221404A5 JP 1999019282 A JP1999019282 A JP 1999019282A JP 1928299 A JP1928299 A JP 1928299A JP 2000221404 A5 JP2000221404 A5 JP 2000221404A5
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- prism
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- imaging optical
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- 230000003287 optical Effects 0.000 title claims description 77
- 238000003384 imaging method Methods 0.000 title claims description 43
- 230000004907 flux Effects 0.000 claims 11
- 238000005286 illumination Methods 0.000 claims 4
- 230000004075 alteration Effects 0.000 claims 2
- 230000005540 biological transmission Effects 0.000 claims 2
Description
【0001】
【発明の属する技術分野】
本発明は、結像光学系及びそれを用いた光学系、光学装置に関し、その中でも特に、ビデオカメラやデジタルスチルカメラ、フィルムスキャナー、内視鏡等、小型の撮像素子を用いた光学装置用の反射面にパワーを有する偏心光学系に関するものである。
[0001]
Field of the Invention
The present invention relates to an imaging optical system, an optical system using the same, and an optical apparatus, and in particular, for an optical apparatus using a small imaging device such as a video camera, a digital still camera, a film scanner, or an endoscope. The present invention relates to a decentered optical system having a power on a reflecting surface.
本発明は従来技術のこのような問題点に鑑みてなされたものであり、その目的は、少ない光学素子の構成枚数で高性能、低コストな結像光学系とそれを用いた光学系、光学装置を提供することである。 The present invention has been made in view of such problems in the prior art, and its object is to provide a high-performance, low-cost imaging optical system with a small number of optical elements, an optical system using the same, and an optical system It is providing a device.
また、本発明のもう1つの目的は、少ない反射回数の反射面を用いて光路を折り畳むことにより小型化された高性能な結像光学系とそれを用いた光学系、光学装置を提供することである。 In addition, another object of the present invention is to provide a high-performance imaging optical system miniaturized by folding an optical path using a reflection surface with a small number of reflections, and an optical system and an optical apparatus using the same. It is.
本発明のもう1つの目的は、絞り近傍に位相型ローパスフィルターを配置し、各プリズムが適切なパワー配置をとることにより、小型でより高性能な結像光学系とそれを用いた光学系、光学装置を提供することである。 Another object of the present invention is to arrange a phase type low pass filter in the vicinity of a stop, and to make each prism an appropriate power arrangement, to thereby form a compact and higher performance imaging optical system and an optical system using the same. An optical device is provided.
Claims (27)
22°<|θs3|<45° ・・・(1)
ここで、θs3は、物点中心を通り、絞り中心を通過して像面中心に到達する光線を軸上主光線とするとき、第1プリズムの第3面での軸上主光線の反射角度、つまり、軸上主光線と第1プリズムの第3面との交わる点における反射面の偏心方向の法線と軸上主光線のなす角である。A first prism and a second prism are provided across the stop, and the first prism is a first surface for entering a light flux into the prism, and a second surface and a third surface for reflecting the light flux inside the prism, It has a fourth surface for emitting the light flux out of the prism, and at least one of the second and third reflecting surfaces has a rotationally asymmetric surface shape with power, and the second prism has at least three. Having three optical element surfaces, at least one of which has a rotationally asymmetric surface shape with power, and the reflection angle of the axial chief ray at the third surface of the first prism is as follows: An imaging optical system characterized by satisfying the condition, making an angle between an axial chief ray emitted from the final surface of the optical system and an off-axis chief ray small and not forming an intermediate image.
22 ° <| θs3 | <45 ° (1)
Here, θs3 is the reflection angle of the axial chief ray at the third surface of the first prism, assuming that the ray passing through the center of the object point and passing through the center of the aperture to reach the image plane center is the axial chief ray. That is, it is the angle between the normal of the decentered direction of the reflecting surface and the axial chief ray at the intersection of the axial chief ray and the third surface of the first prism.
0.6f<FB<2.0f ・・・(2)
ここで、FBは、物点中心を通り、絞り中心を通過して像面中心に到達する光線を軸上主光線とするとき、第2プリズムの最も像側に位置する光学作用面から像面までの軸上主光線に沿った長さを示し、媒質の屈折率を1.0(空気)としたときの長さであり、fは、結像光学系の総合焦点距離である。A first prism and a second prism are provided across the stop, and the first prism is a first surface for entering a light flux into the prism, and a second surface and a third surface for reflecting the light flux inside the prism, It has a fourth surface for emitting the light flux out of the prism, and at least one of the second and third reflecting surfaces has a rotationally asymmetric surface shape with power, and the second prism has at least three. Having two optical element surfaces, at least one of which has a rotationally asymmetric surface shape with power, and an axial main surface from the optical surface at the most image side of the second prism to the image surface An imaging optical system characterized in that the distance between light rays satisfies the following condition, the angle between the axial chief ray emitted from the final surface of the optical system and the off-axis chief ray is small, and an intermediate image is not formed.
0.6 f <FB <2.0 f (2)
Here, when the light passing through the center of the object point and passing through the center of the stop and reaching the center of the image plane is the axial chief ray, the optical action surface located closest to the image side of the second prism to the image plane Represents the length along the axial chief ray up to the point where the refractive index of the medium is 1.0 (air), and f is the total focal length of the imaging optical system.
2.5f<DR<5.5f ・・・(3)
ここで、DRは、物点中心を通り、絞り中心を通過して像面中心に到達する光線を軸上主光線とするとき、第2プリズムの最も物体側に位置する光学作用面から像面までの軸上主光線に沿った長さを示し、媒質の屈折率を1.0(空気)としたときの長さである。3. The image forming optical system according to claim 2, wherein a distance of an axial chief ray from an optical action surface closest to the object side of the second prism to an image plane satisfies the following condition.
2.5f <DR <5.5f (3)
Here, DR denotes an optical action surface located on the most object side of the second prism when a ray passing through the object center and passing through the aperture center and reaching the image plane center is the on-axis chief ray. Shows the length along the axial chief ray up to the point where the refractive index of the medium is 1.0 (air).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11019282A JP2000221404A (en) | 1999-01-28 | 1999-01-28 | Image forming optical system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11019282A JP2000221404A (en) | 1999-01-28 | 1999-01-28 | Image forming optical system |
Publications (2)
Publication Number | Publication Date |
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JP2000221404A JP2000221404A (en) | 2000-08-11 |
JP2000221404A5 true JP2000221404A5 (en) | 2005-05-19 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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JP11019282A Pending JP2000221404A (en) | 1999-01-28 | 1999-01-28 | Image forming optical system |
Country Status (1)
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JP (1) | JP2000221404A (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006113159A (en) | 2004-10-13 | 2006-04-27 | Konica Minolta Opto Inc | Imaging optical system |
CN116909076B (en) * | 2023-09-12 | 2024-01-05 | 江西联益光学有限公司 | Optical imaging system |
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1999
- 1999-01-28 JP JP11019282A patent/JP2000221404A/en active Pending
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