WO2016013302A1 - 広角光学系および内視鏡 - Google Patents
広角光学系および内視鏡 Download PDFInfo
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- WO2016013302A1 WO2016013302A1 PCT/JP2015/065990 JP2015065990W WO2016013302A1 WO 2016013302 A1 WO2016013302 A1 WO 2016013302A1 JP 2015065990 W JP2015065990 W JP 2015065990W WO 2016013302 A1 WO2016013302 A1 WO 2016013302A1
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/06—Panoramic objectives; So-called "sky lenses" including panoramic objectives having reflecting surfaces
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
- A61B1/00064—Constructional details of the endoscope body
- A61B1/00071—Insertion part of the endoscope body
- A61B1/0008—Insertion part of the endoscope body characterised by distal tip features
- A61B1/00096—Optical elements
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
- A61B1/00163—Optical arrangements
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
- A61B1/00163—Optical arrangements
- A61B1/00174—Optical arrangements characterised by the viewing angles
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/04—Reversed telephoto objectives
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/18—Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
- G02B17/08—Catadioptric systems
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
- G02B17/08—Catadioptric systems
- G02B17/0856—Catadioptric systems comprising a refractive element with a reflective surface, the reflection taking place inside the element, e.g. Mangin mirrors
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
- G02B17/08—Catadioptric systems
- G02B17/0896—Catadioptric systems with variable magnification or multiple imaging planes, including multispectral systems
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B23/00—Telescopes, e.g. binoculars; Periscopes; Instruments for viewing the inside of hollow bodies; Viewfinders; Optical aiming or sighting devices
- G02B23/24—Instruments or systems for viewing the inside of hollow bodies, e.g. fibrescopes
- G02B23/2407—Optical details
- G02B23/2423—Optical details of the distal end
- G02B23/243—Objectives for endoscopes
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B23/00—Telescopes, e.g. binoculars; Periscopes; Instruments for viewing the inside of hollow bodies; Viewfinders; Optical aiming or sighting devices
- G02B23/24—Instruments or systems for viewing the inside of hollow bodies, e.g. fibrescopes
- G02B23/26—Instruments or systems for viewing the inside of hollow bodies, e.g. fibrescopes using light guides
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0025—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration
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- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
- A61B1/00163—Optical arrangements
- A61B1/00174—Optical arrangements characterised by the viewing angles
- A61B1/00183—Optical arrangements characterised by the viewing angles for variable viewing angles
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B1/00—Instruments for performing medical examinations of the interior of cavities or tubes of the body by visual or photographical inspection, e.g. endoscopes; Illuminating arrangements therefor
- A61B1/00163—Optical arrangements
- A61B1/00195—Optical arrangements with eyepieces
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0055—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras employing a special optical element
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
- G02B17/02—Catoptric systems, e.g. image erecting and reversing system
- G02B17/06—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror
- G02B17/0605—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror using two curved mirrors
- G02B17/061—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror using two curved mirrors on-axis systems with at least one of the mirrors having a central aperture
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
- G02B27/0938—Using specific optical elements
- G02B27/0977—Reflective elements
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/001—Axicons, waxicons, reflaxicons
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B9/00—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or -
- G02B9/12—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or - having three components only
Definitions
- the present invention relates to a wide-angle optical system and an endoscope.
- An observable optical system is known (for example, see Patent Documents 1 and 2).
- the optical system of Patent Document 1 is incident on the cylindrical surface from the object side with respect to the normal direction of the cylindrical surface, that is, from the narrow angle side, and incident on the cylindrical surface from the image side with respect to the normal direction, that is, from the wide angle side. Since the direction of refraction with respect to the light beam is different from each other, it is difficult to correct lateral chromatic aberration with a common optical element at a later stage.
- the optical system of Patent Document 2 does not cause a problem of correcting the lateral chromatic aberration, but the first optical element has only one reflection of light from the side. The image is inverted upside down.
- the present invention has been made in view of the above-described circumstances, and a wide-angle optical system capable of sufficiently correcting lateral chromatic aberration by a common optical element in the subsequent stage while aligning the directions of the images of all the fields of view and the endoscope. Provide a mirror.
- An aspect of the present invention includes a first group having a negative lens having a negative refractive power and a positive lens having a positive refractive power, a second group having a catadioptric optical element disposed on the image side of the first group, A catadioptric optical element disposed on the image side of the second group and having a positive refractive power, the catadioptric optical element having an optical axis at the center and an annular shape around the first transmission surface
- a second reflecting surface that reflects light from the object side, a second surface disposed on the image side, and a conical surface disposed between the first surface and the second surface and having an apex angle on the object side
- a wide-angle optical system that satisfies the following expressions (1), (2), and (3).
- ⁇ n is the Abbe number of the negative lens
- ⁇ p is the Abbe number of the positive lens
- ⁇ n is the refractive power of the negative lens
- ⁇ p is the refractive power of the positive lens
- ⁇ is the angle of the apex angle of the third surface.
- ⁇ k is the half field angle of the principal ray with the smallest field angle in the side field of view, and 0 ⁇ k ⁇ 90 °.
- the light when light from a front object enters the first group, the light passes through a negative lens having a large Abbe number and a positive lens having a small Abbe number. Increasing the Abbe number of the negative lens that easily causes lateral chromatic aberration can suppress the occurrence of lateral chromatic aberration in light passing through the first group. And the light which passed the 1st group is condensed by the 3rd group, after passing the 1st transmission surface of the 2nd group, and the 2nd transmission surface.
- the light from the side object is incident on the third surface of the second group without entering the first group.
- the light incident on the third surface satisfies the expression (3)
- all of the principal rays are incident from the image side with respect to the normal of the third surface and refracted on the image side.
- the sign of the chromatic aberration of magnification occurring in all the light from the side object can be aligned with the sign of the chromatic aberration of magnification occurring in the light from the front object.
- the light from the side refracted to the image side on the third surface is reflected once in the order of the second reflecting surface of the second surface and the first reflecting surface of the first surface, and then the second surface. And is condensed by the third group through the second transmission surface.
- the chromatic aberration of magnification of all the lights can be sufficiently corrected by the common third group. . Since the light from the side object is reflected twice in the catadioptric optical element, the side field image is prevented from being inverted upside down. Thereby, the direction of the image of all the visual fields can be made uniform.
- the negative lens and the positive lens of the first group may satisfy the following expression (4). (4) ⁇ n>35> ⁇ p
- Another aspect of the present invention is an endoscope including any one of the above wide-angle optical systems. According to this aspect, it is possible to acquire a wide-angle endoscopic image in which the lateral chromatic aberration is sufficiently corrected.
- the lateral chromatic aberration can be sufficiently corrected by the common optical element in the subsequent stage while aligning the directions of the images of all the visual fields.
- FIG. 1 is an overall view of an endoscope according to an embodiment of the present invention. It is a block diagram of the wide angle optical system which concerns on one Embodiment of this invention.
- FIG. 3 is a diagram illustrating a lens arrangement of a first example of the wide-angle optical system in FIG. 2.
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 113 °.
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 104 °.
- FIG. 3 is a diagram illustrating a lens arrangement of a first example of the wide-angle optical system in FIG. 2.
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 95 °.
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 86 °.
- FIG. 4A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 77 °.
- FIG. 4A is an aberration diagram of light from a front object in the wide-angle optical system in FIG.
- FIG. 4A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 60 °.
- FIG. 4A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 4A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 4A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 3 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °.
- FIG. 4 is a diagram illustrating a lens arrangement of a second example of the wide-angle optical system in FIG. 2.
- FIG. 7A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 115 °.
- FIG. 7A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 7A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 95 °.
- FIG. 7A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 85 °.
- FIG. 7A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 7A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 74 °.
- FIG. 7A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 60 °.
- FIG. 7A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 7A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 7A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 6 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °.
- FIG. 6 is a diagram illustrating a lens arrangement of a third example of the wide-angle optical system in FIG. 2.
- FIG. 10A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 10A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 105 °.
- FIG. 10A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 95 °.
- FIG. 10A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 10A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 75 °.
- FIG. 10A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 73 °.
- FIG. 10A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 60 °.
- FIG. 10A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 10A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 10A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 9 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °. It is a figure which shows the lens arrangement
- FIG. 13A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 116 °.
- FIG. 13A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 106 °.
- FIG. 13A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 96 °.
- FIG. 13A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 86 °.
- FIG. 13A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 76 °.
- FIG. 13A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 74 °.
- FIG. 13A is an aberration diagram of light from a front object in the wide-angle optical system in FIG.
- FIG. 13A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 13A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 13A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 12 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °.
- FIG. 10 is a diagram illustrating a lens arrangement of a fifth example of the wide-angle optical system in FIG. 2.
- FIG. 16A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 116 °.
- FIG. 16A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 107 °.
- FIG. 16A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 16A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 89 °.
- FIG. 16A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 80 °.
- FIG. 16A is an aberration diagram of light from a front object in the wide-angle optical system in FIG.
- FIG. 16A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 60 °.
- FIG. 16A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 16A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 16A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 15 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °. It is a figure which shows the lens arrangement
- FIG. 19A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 115 °.
- FIG. 19A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 19A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 95 °.
- FIG. 19A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 85 °.
- FIG. 19A is an aberration diagram of light from a lateral object in the wide-angle optical system in FIG.
- FIG. 19A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 73 °.
- FIG. 19A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 60 °.
- FIG. 19A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 45 °.
- FIG. 19A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 30 °.
- FIG. 19A is an aberration diagram of light from a front object in the wide-angle optical system in FIG. 18 and illustrates a case where the half field angle of a principal ray at the minimum field angle is 0 °.
- an endoscope 1 and a wide-angle optical system 3 according to a first embodiment of the present invention will be described below with reference to the drawings.
- an endoscope 1 according to this embodiment includes an elongated and flexible insertion portion 2 that is inserted into a body, and front and side objects P and S that are provided at the distal end of the insertion portion 2. And a wide-angle optical system 3 for acquiring the first image.
- the wide-angle optical system 3 is focused by the first group 6 that collects light from the front and the first group 6 in order from the front object P side.
- the first group 6 includes a negative lens 4 that is disposed on the object P side and has a negative refractive power, and a positive lens 5 that is disposed closer to the image side than the negative lens 4 and has a positive refractive power.
- the negative lens 4 is a plano-concave lens having a concave surface on the image side
- the positive lens 5 is a plano-convex lens having a convex surface on the image side.
- the negative lens 4 and the positive lens 5 satisfy the conditions of the following expressions (1) and (2).
- ⁇ n is the Abbe number of the negative lens 4
- ⁇ p is the Abbe number of the positive lens 5
- ⁇ n is the refractive power of the negative lens 4
- ⁇ p is the refractive power of the positive lens 5.
- the second group 7 includes a first surface 11 disposed on the object P side, a second surface 12 disposed on the image side, and a third surface disposed between the first surface 11 and the second surface 12. 13, a catadioptric optical element 14, a parallel plate 15, an aperture stop 16 disposed on the image side of the parallel plate 15, and a biconvex lens 17.
- the first surface 11 is disposed in a substantially annular shape around the first transmission surface 11a, and a substantially circular first transmission surface 11a that transmits light from the first group 6 with the optical axis disposed in the center. And a first reflecting surface 11b that internally reflects light from the image side.
- the second surface 12 has a substantially circular second transmission surface 12a that transmits the light that has been transmitted through the first transmission surface 11a and the light that has been internally reflected at the first reflection surface 11b, with the optical axis disposed at the center.
- a second reflecting surface 12b is provided around the second transmitting surface 12a so as to have a substantially annular shape and reflect light internally.
- the internal reflection at the second reflection surface 12b is total reflection.
- the third surface 13 is formed in a conical surface shape having an apex angle on the front object P side, and transmits light from the side.
- the vertex angle of the third surface 13 satisfies the condition of the expression (3).
- ⁇ is the apex angle of the third surface 13
- ⁇ k is the half field angle of the principal ray with the smallest field angle in the side field of view
- the light from the side object S that has passed through the third surface 13 is refracted by the third surface 13, then internally reflected by the second reflecting surface 12 b of the second surface 12, and further by the first reflection of the first surface 11.
- the portion that is internally reflected at the surface 11 b, passes through the second transmission surface 12 a of the second surface 12, and passes through the parallel plate 15 and the aperture stop 16 is condensed by the biconvex lens 17 and enters the third group 8. It has become.
- the third group 8 is a lens group that includes a cemented lens 18 on which light that has passed through the aperture stop 16 enters and has positive refractive power.
- Reference numeral 19 denotes another lens constituting the third group 8.
- the cemented lens 18 is obtained by cementing a biconvex lens 20 disposed on the object P side and a meniscus lens 21.
- the distal end of the insertion portion 2 is disposed to face the front object P.
- the first group 6 since the Abbe number of the negative lens 4 is set to be larger than the Abbe number of the positive lens 5 as shown in Expression (1), the occurrence of lateral chromatic aberration in the negative lens 4 can be suppressed. Since the first group 6 has a negative refractive power as a whole as shown in Expression (2), it can collect light from a wide range in front.
- the light from the side is incident on the third surface 13 of the catadioptric optical element 14 of the second group 7. Since the light from the side satisfies the expression (3), all the principal rays are incident from the image side with respect to the normal of the third surface 13 when entering the third surface 13.
- the two lights from the front and the side are passed through the second group 7 and then passed through the common third group 8 and photographed by the image sensor 10.
- the signs of the lateral chromatic aberration are aligned when the two lights from the front and the side are emitted from the second group 7, so
- the third group 8 can sufficiently correct the lateral chromatic aberration of all light. Since the light from the side object S is internally reflected twice in the catadioptric optical element 14, the image is prevented from being inverted upside down. Accordingly, there is an advantage that the directions of the images of all the visual fields can be made uniform.
- the first group 6 is illustrated in which the negative lens 4 and the positive lens 5 are arranged in order from the object P side, but instead, the order of the positive lens 5 and the negative lens 4 is changed. May be.
- the wide-angle optical system 3 preferably satisfies the following expression (4). (4) ⁇ n>35> ⁇ p According to this, the lateral chromatic aberration generated in the negative lens 4 can be more easily suppressed.
- the second reflecting surface 12b is exemplified as one that totally reflects the light from the side object S that has passed through the third surface 13, but instead, the inner surface of the second reflecting surface 12b.
- the side may be a mirror coat.
- FIG. 3 shows the lens arrangement of the wide-angle optical system 3 according to the present embodiment.
- 4A to 5E are aberration diagrams of the lens arrangement according to the present example, in which the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- r is the radius of curvature (mm)
- d is the surface separation (mm)
- ⁇ is the Abbe number
- Nd is the refractive index with respect to the d line
- OBJ the subject (front object P)
- IMG is the imaging surface 9. Is shown.
- the symbol * indicates an aspheric lens.
- fn represents the focal length (mm) of the negative lens 4
- fp represents the focal length (mm) of the positive lens. According to this, it is understood that the conditional expressions (1) to (4) are satisfied.
- / ⁇ n 0.026
- / ⁇ p 0.021 (
- the apex angle ⁇ is at a position away from the first surface 11 by 4.77 (mm) toward the front object P.
- the maximum half field angle of light from the front object P is 76 °
- the half field angle of principal rays from the side object S is 76 ° to 116 °
- the focal length (front light path) is 0.
- the F-number (front optical path) is 5.0
- the maximum image height is 1.0 mm
- the maximum front image height is 0.609 mm.
- FIG. 6 shows the lens arrangement of the wide-angle optical system 3 according to this embodiment.
- FIGS. 7A to 8E show aberration diagrams of the wide-angle optical system 3 according to the present example, in which the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- the maximum front half angle of view is 74 °
- the half angle of view of the principal ray from the side is 75 ° to 116 °
- the focal length (front light path) is 0.566 mm
- the F number front light path
- the maximum image height is 1.0 mm
- the maximum front image height is 0.607 mm.
- FIG. 9 shows the lens arrangement of the wide-angle optical system 3 according to this embodiment.
- 10A to 11E are aberration diagrams of the wide-angle optical system 3 according to the present example, in which the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- the specs in this embodiment are: the maximum front half angle of view is 73 °, the half angle of view of the principal ray from the side is 73 ° to 114 °, the focal length (front light path) is 0.574 mm, and the F number (front light path). Is 3.0, the maximum image height is 1.0 mm, and the maximum front image height is 0.612 mm.
- FIG. 12 shows the lens arrangement of the wide-angle optical system 3 according to the present embodiment.
- 13A to 14E are aberration diagrams of the wide-angle optical system 3 according to the present example, in which the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- the maximum front half angle of view is 75 °
- the half angle of view of the principal ray from the side is 76 ° to 115 °
- the focal length (front light path) is 0.702 mm
- the maximum image height is 1.0 mm
- the maximum front image height is 0.646 mm.
- FIG. 15 shows the lens arrangement of the wide-angle optical system 3 according to the present embodiment.
- FIGS. 16A to 17E show aberration diagrams of the wide-angle optical system 3 according to the present example.
- the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- / ⁇ n 0.026
- / ⁇ p 0.015 (
- the apex angle ⁇ is located 4.71 mm away from the first surface 11 toward the front object P.
- the maximum front half angle of view is 80 °
- the half angle of view of the principal ray from the side is 80 ° to 116 °
- the focal length (front light path) is 0.547 mm
- the maximum image height is 1.0 mm
- the maximum front image height is 0.620 mm.
- FIG. 18 shows a lens arrangement of the wide-angle optical system 3 according to the present embodiment.
- 19A to 20E are aberration diagrams of the wide-angle optical system 3 according to the present example, in which the X direction indicates lateral chromatic aberration and the Y direction indicates coma aberration.
- the maximum front half angle of view is 73.5 °
- the half angle of view of the principal ray from the side is 74 ° to 116 °
- the focal length (front light path) is 0.588 mm
- the F number (front) The optical path) is 3.0
- the maximum image height is 1.0 mm
- the maximum front image height is 0.623 mm.
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Abstract
Description
特許文献2では、第1の光学素子の像側の反射面で1回だけ反射された側方からの光と、物体側から入射して屈折し、像側の透過面を透過した前方からの光とが正の光学素子に入射するようになっている。
特許文献2の光学系は、倍率色収差の補正の問題は生じないが、第1の光学素子における側方からの光の反射回数が1回のみであるため、前方視野の像と側方視野の像とが上下反転してしまう。
(1) νn>νp
(2) |φn|>|φp|
(3) α/2>90°-θk
ここで、νnは前記負レンズのアッベ数、νpは前記正レンズのアッベ数、φnは前記負レンズの屈折力、φpは前記正レンズの屈折力、αは前記第3面の頂角の角度、θkは側方視野内の最小画角の主光線の半画角であり、0<θk<90°である。
側方の物体からの光は反射屈折光学素子内において2回反射されるため、側方視野の像が上下反転することが防止される。これにより、全ての視野の像の方向を揃えることができる。
(4) νn>35>νp
本態様によれば、倍率色収差を十分に補正した広角の内視鏡画像を取得することができる。
本実施形態に係る内視鏡1は、図1に示されるように、体内に挿入される細長く柔軟な挿入部2と、該挿入部2の先端に設けられ前方および側方の物体P,Sの画像を取得する広角光学系3とを備えている。
負レンズ4は、像側に凹面を配置した平凹レンズであり、正レンズ5は、像側に凸面を有する平凸レンズである。
(1) νn>νp
(2) |φn|>|φp|
ここで、νnは負レンズ4のアッベ数、νpは正レンズ5のアッベ数、φnは負レンズ4の屈折力であり、φpは正レンズ5の屈折力である。
第3面13は、前方の物体P側に頂角を有する円錐面状に形成され、側方からの光を透過するようになっている。
(3) α/2>90°-θk
ここで、αは第3面13の頂角の角度、θkは側方視野内の最小画角の主光線の半画角であり、0<θk<90°である。
接合レンズ18は、物体P側に配置される両凸レンズ20と、メニスカスレンズ21とを接合したものである。
本実施形態に係る内視鏡1を用いて前方および側方の物体P,Sを観察するには、挿入部2の先端を前方の物体Pに対向させて配置する。
第1群6は、式(1)に示すように負レンズ4のアッベ数が正レンズ5のアッベ数より大きく設定されているので、負レンズ4における倍率色収差の発生を抑制することができる。第1群6は、式(2)に示すように全体として負の屈折力を有しているので、前方の広い範囲からの光を集光することができる。
このように、本実施形態に係る広角光学系3によれば、前方および側方からの2つの光は第2群7から射出された時点で倍率色収差の符号が揃えられているので、共通の第3群8によって全ての光の倍率色収差を十分に補正することができるという利点がある。
側方の物体Sからの光は反射屈折光学素子14内において2回内面反射されるため、像が上下反転することが防止される。これにより、全ての視野の像の方向を揃えることができるという利点がある。
(4) νn>35>νp
これによれば、負レンズ4において発生する倍率色収差をより抑制し易くすることができる。
図3は本実施例に係る広角光学系3のレンズ配列を示している。図4Aから図5Eは本実施例に係るレンズ配列の収差図を示し、X方向が倍率色収差、Y方向がコマ収差を示している。
以下のレンズデータにおいて、rは曲率半径(mm)、dは面間隔(mm)、νはアッベ数、Ndはd線に対する屈折率、OBJは被写体(前方の物体P)、IMGは撮像面9を示している。レンズデータ中、記号*は非球面レンズであることを示している。
OBJ ∞ 4.878144
1 ∞ 0.286885 40.8 1.8830
2 0.82194 0.483607
3 ∞ 0.475288 17.4 1.9591
4 -2.70744 0.081967
5* -7.77656 0.803279 64.1 1.5163
6* 1.53360 0.327869
7 ∞ 0.491803 46.6 1.8160
8 ∞ 0.024590
STO ∞ 0.000000
10 12.29508 0.948401 46.6 1.8160
11 -4.56082 0.081967
12 2.62295 1.270492 54.7 1.7292
13 -1.77686 0.327869 17.4 1.9591
14 -4.72357 0.183674
15 4.29340 1.024590 40.9 1.8061
16* -4.64897 0.491803
17 ∞ 0.737705 64.1 1.5163
18 ∞ 0.573770 64.1 1.5163
19 ∞ 0.000000
IMG ∞ 0.000000
非球面デ-タ
第5面
K=0.000000,A4=0.181585E+00,A6=-0.170990E+00,A8=0.292551E-01,A10=0.350339E-01
第6面
K=-0.484012,A4=0.356447E-01,A6=0.300682E-01,A8=-0.261528E-01,A10=0.609574E-02
第16面
K=0.000000,A4=0.413814E-01,A6=0.353986E-02,A8=0.553823E-01,A10=-0.364465E-01
fn=-0.925
fp=2.786
φn=-1.801
φp=0.359
νn=40.8
νp=17.4
|φn|/νn=0.026
|φp|/νp=0.021
(|φn|/νn)/(|φp|/νp)=1.284
α=46°
となる。頂角αは第1面11から前方の物体P側に4.77(mm)離れた位置にある。
図6は本実施例に係る広角光学系3のレンズ配列を示している。図7Aから図8Eは本実施例に係る広角光学系3の収差図を示し、X方向が倍率色収差、Y方向がコマ収差を示している。
OBJ ∞ 4.066102
1 ∞ 0.286885 40.8 1.8830
2 0.79205 0.467213
3 ∞ 0.468048 18.9 1.9343
4 -2.84888 0.081967
5* -21.31148 0.870556 64.1 1.5163
6* 1.12433 0.567778
7 ∞ 0.491803 64.1 1.5163
8 ∞ 0.024590
STO ∞ 0.087009
10 12.29508 0.948401 46.6 1.8160
11 -4.49367 0.170697
12 2.32825 1.270492 54.7 1.7292
13 -2.73661 0.327869 18.9 1.9343
14 -28.22847 0.233287
15 ∞ 0.327869 64.1 1.5163
16 ∞ 0.118685
17 2.87047 1.147541 64.1 1.5163
18* -2.86885 0.532787
19 ∞ 0.737705 64.1 1.5163
20 ∞ 0.573770 64.1 1.5163
21 ∞ 0.000000
IMG ∞ 0.000000
非球面データ
第5面
K=0.000000,A4=0.177750E-01,A6=0.514143E-01,A8=-0.146876E+00,A10=0.966753E-01
第6面
K=-10.486544,A4=0.181585E+00,A6=-0.961834E-01,A8=0.249683E-01,A10=-0.257298E-02
第18面
K=0.000000,A4=0.177810E+00,A6=-0.137418E+00,A8=0.137236E+00,A10=-0.190231E-01
fn=-0.892
fp=3.049
φn=-1.121
φp=0.328
νn=40.8
νp=18.9
|φn|/νn=0.027
|φp|/νp=0.017
(|φn|/νn)/(|φp|/νp)=1.584
α=45.2°
となる。頂角αは第1面11から前方の物体P側に5.03mm離れた位置にある。
OBJ ∞ 11.681544
1 ∞ 0.515625 18.9 1.9343
2 -4.91864 0.250000 71.8 1.7682
3 0.80388 0.741094
4* -3.88773 1.333333 64.1 1.5163
5* 2.57540 0.250420
6 ∞ 0.625000 64.1 1.5163
7 ∞ 0.050000
STO ∞ 0.310778
9 786.25122 1.015625 46.6 1.8160
10 -3.62923 0.166667
11 3.00000 1.406250 46.6 1.8160
12 -2.98777 0.390625 18.9 1.9343
13 -65.80744 0.477509
14 4.87920 1.326240 64.1 1.5163
15* -3.58578 0.616667
16 ∞ 0.833333 64.1 1.5163
17 ∞ 0.833333 64.1 1.5163
18 ∞ 0.000000
IMG ∞ 0.000000
非球面データ
第4面
K=0.000000,A4=0.808060E-01,A6=-0.622080E-01,A8=0.978987E-02,A10=0.806216E-02
第5面
K=0.000000,A4=-0.615673E-03,A6=-0.860821E-02,A8=0.184745E-02,A10=-0.168134E-03
第15面
K=0.000000,A4=0.575488E-01,A6=0.184501E-01,A8=-0.143676E-01,A10=0.806216E-02
fn=-0.880
fp=5.265
φn=-1.137
φp=0.190
νn=71.8
νp=18.9
|φn|/νn=0.016
|φp|/νp=0.010
(|φn|/νn)/(|φp|/νp)=1.575
α=50.5°
となる。頂角αは第1面11から前方の物体P側に7mm離れた位置にある。
OBJ ∞ 8.379325
1 ∞ 0.335196 40.8 1.8830
2 1.00847 0.469274
3 1.73184 0.470085 17.4 1.9591
4 2.91464 0.351955
5* -11.88457 1.005587 64.1 1.5163
6* 1.82961 0.525140
7 -1.64469 0.883901 46.6 1.8160
8 -1.81306 0.111732
STO ∞ 0.209578
10 14.52514 0.782119 46.6 1.8160
11 -5.00980 0.111732
12 4.00733 1.428177 46.6 1.8160
13 -2.27022 0.391061 17.4 1.9591
14 -12.63447 0.111732
15 ∞ 0.670391 64.1 1.5163
16 ∞ 0.111732
17 8.45282 1.184413 40.9 1.8061
18* -21.83998 0.525140
19 ∞ 0.636872 64.1 1.5163
20 ∞ 0.558659 64.1 1.5163
21 ∞ 0.000000
IMG ∞ 0.000000
非球面データ
第5面
K=0.000000,A4=0.716898E-01,A6=-0.689122E-01,A8=0.574472E-02,A10=0.204598E-01
第6面
K=-0.130259,A4=0.531045E-01,A6=-0.689122E-01,A8=0.212911E-01,A10=-0.279626E-02
第18面
K=0.000000,A4=-0.409946E-02,A6=0.610747E-01,A8=-0.368003E-01,A10=0.796250E-03
fn=-1.135
fp=3.672
φn=-0.881
φp=0.272
νn=40.8
νp=17.4
|φn|/νn=0.022
|φp|/νp=0.016
(|φn|/νn)/(|φp|/νp)=1.379
α=50°
となる。頂角αは第1面11から前方の物体P側に6.81mm離れた位置にある。
OBJ ∞ 6.292165
1 ∞ 0.294118 40.8 1.8830
2 0.84790 0.487395
3 ∞ 0.464607 18.9 1.9343
4 -3.36303 0.084034
5* -8.40336 0.840336 64.1 1.5163
6* 1.22079 0.533938
7 ∞ 0.504202 64.1 1.5163
8 ∞ 0.025210
STO ∞ 0.281827
10 5.09426 0.949580 47.4 1.7920
11 -5.09426 0.130195
12 2.79328 1.310924 54.7 1.7292
13 -2.79328 0.327731 18.9 1.9343
14 ∞ 0.084034
15 ∞ 0.336134 64.1 1.5163
16 ∞ 0.084034
17 2.89916 1.159664 64.1 1.5163
18* -2.43697 0.554439
19 ∞ 0.756303 64.1 1.5163
20 ∞ 0.588235 64.1 1.5163
21 ∞ 0.000000
IMG ∞ 0.000000
非球面データ
第5面
K=0.000000,A4=0.172083E+00,A6=-0.216060E+00,A8=0.971054E-01,A10=0.000000E+00
第6面
K=-5.101829,A4=0.770935E-01,A6=-0.124607E-01,A8=-0.617295E-02,A10=0.185243E-02
第18面
K=0.000000,A4=0.159629E+00,A6=-0.124019E+00,A8=0.142429E+00,A10=-0.489314E-01
fn=-0.955
fp=3.600
φn=-1.047
φp=0.278
νn=40.8
νp=18.9
|φn|/νn=0.026
|φp|/νp=0.015
(|φn|/νn)/(|φp|/νp)=1.747
α=48°
となる。頂角αは第1面11から前方の物体P側に4.71mm離れた位置にある。
OBJ ∞ 19.917502
1 ∞ 0.416667 71.8 1.7682
2 1.12833 0.716667
3 -3.66667 0.458333 18.9 1.9343
4 -3.13864 0.083333
5* -6.14499 1.500000 64.1 1.5163
6* 2.88252 1.143789
7 ∞ 0.666667 64.1 1.5163
8 ∞ 0.050000
STO ∞ 0.166667
10 10.50000 1.133333 46.6 1.8160
11 -6.47879 0.166667
12 3.75000 1.681428 46.6 1.8160
13 -3.22553 0.416667 18.9 1.9343
14 22.71414 0.166667
15 3.33333 1.350000 64.1 1.5163
16* -3.14155 0.583333
17 ∞ 0.833333 64.1 1.5163
18 ∞ 0.833333 64.1 1.5163
19 ∞ 0.000000
IMG ∞ 0.000000
非球面データ
第5面
K=0.000000,A4=0.488513E-01,A6=-0.232544E-01,A8=0.396655E-02,A10=0.134335E-03
第6面
K=0.000000,A4=0.210465E-02,A6=-0.518526E-02,A8=0.848642E-03,A10=-0.604811E-04
第18面
K=0.000000,A4=0.428587E-01,A6=0.308236E-01,A8=-0.279936E-01,A10=0.868532E-02
fn=-1.464
fp=16.437
φn=-0.683
φp=0.061
νn=71.8
νp=18.9
|φn|/νn=0.010
|φp|/νp=0.003
(|φn|/νn)/(|φp|/νp)=2.955
α=50.5°
となる。頂角αは第1面11から前方の物体P側に7.33mm離れた位置にある。
3 広角光学系
4 負レンズ
5 正レンズ
6 第1群
7 第2群
8 第3群
11 第1面
11a 第1透過面
11b 第1反射面
12 第2面
12a 第2透過面
12b 第2反射面
13 第3面
14 反射屈折光学素子
Claims (3)
- 負の屈折力の負レンズおよび正の屈折力の正レンズを有する第1群と、
該第1群の像側に配置され反射屈折光学素子を有する第2群と、
該第2群の像側に配置され正の屈折力の第3群とを備え、
前記反射屈折光学素子が、中心に光軸を備える第1透過面および該第1透過面の周囲に環状に配置され像側からの光を反射する第1反射面を備え、物体側に配置された第1面と、中心に光軸を備える第2透過面および該第2透過面の周囲に環状に配置され物体側からの光を反射する第2反射面を備え、像側に配置された第2面と、前記第1面および前記第2面の間に配置され物体側に頂角を有する円錐面状の透過面である第3面とを備え、
次の式(1),(2),(3)を満足する広角光学系。
(1) νn>νp
(2) |φn|>|φp|
(3) α/2>90°-θk
ここで、νnは前記負レンズのアッベ数、νpは前記正レンズのアッベ数、φnは前記負レンズの屈折力、φpは前記正レンズの屈折力、αは前記第3面の頂角の角度、θkは側方視野内の最小画角の主光線の半画角であり、0<θk<90°である。 - 前記第1群の前記負レンズおよび前記正レンズが次の式(4)を満足する請求項1に記載の広角光学系。
(4) νn>35>νp - 請求項1または請求項2に記載の広角光学系を備える内視鏡。
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2016500842A JP5905180B1 (ja) | 2014-07-23 | 2015-06-03 | 広角光学系および内視鏡 |
EP15824993.8A EP3173836A4 (en) | 2014-07-23 | 2015-06-03 | Wide angle optical system and endoscope |
CN201580003030.0A CN105814471B (zh) | 2014-07-23 | 2015-06-03 | 广角光学系统和内窥镜 |
US15/173,040 US9563040B2 (en) | 2014-07-23 | 2016-06-03 | Wide-angle optical system and endoscope |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2014149683 | 2014-07-23 | ||
JP2014-149683 | 2014-07-23 |
Related Child Applications (1)
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US15/173,040 Continuation US9563040B2 (en) | 2014-07-23 | 2016-06-03 | Wide-angle optical system and endoscope |
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EP (1) | EP3173836A4 (ja) |
JP (1) | JP5905180B1 (ja) |
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WO (1) | WO2016013302A1 (ja) |
Families Citing this family (6)
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EP3312655A4 (en) * | 2015-06-16 | 2019-02-20 | Olympus Corporation | OPTICAL WIDE ANGLE SYSTEM |
JP6109461B1 (ja) * | 2015-06-18 | 2017-04-05 | オリンパス株式会社 | 内視鏡用対物光学系 |
DE102017113274A1 (de) * | 2017-06-16 | 2018-12-20 | avateramedical GmBH | Kameraobjektiv für ein Endoskop und Endoskop |
US10678060B2 (en) * | 2017-10-26 | 2020-06-09 | Fluke Corporation | Laser line generation device having combination aspheric lens and axicon |
US11793397B2 (en) * | 2020-03-09 | 2023-10-24 | Omniscient Imaging, Inc. | Encapsulated opto-electronic system for co-directional imaging in multiple fields of view |
CN111323900A (zh) * | 2020-04-20 | 2020-06-23 | 华中科技大学 | 一种用于高温窑炉内部成像的内窥镜装置 |
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- 2015-06-03 WO PCT/JP2015/065990 patent/WO2016013302A1/ja active Application Filing
- 2015-06-03 JP JP2016500842A patent/JP5905180B1/ja active Active
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Also Published As
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JPWO2016013302A1 (ja) | 2017-04-27 |
EP3173836A1 (en) | 2017-05-31 |
EP3173836A4 (en) | 2018-03-21 |
CN105814471B (zh) | 2019-04-02 |
US9563040B2 (en) | 2017-02-07 |
CN105814471A (zh) | 2016-07-27 |
JP5905180B1 (ja) | 2016-04-20 |
US20160282591A1 (en) | 2016-09-29 |
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