Optical system for rigid scope and rigid endoscope

Abstract

By suitably correcting a secondary spectrum, a clear, bright optical image is obtained. Provided is a rigid-scope optical system including: an objective optical system; and at least one relay optical systems that are formed of positive front groups, middle groups, and back groups in this order from an entrance side and that reimage an optical image imaged at imaging planes at the entrance side onto imaging planes at an exit side, wherein axial chromatic aberration between two wavelengths is corrected by an optical system other than the diffractive optical element, and axial chromatic aberration between the two wavelengths and another wavelength is corrected by the diffractive optical element.

Claims

The invention claimed is: 1. A rigid-scope optical system comprising: an objective optical system; and a plurality of relay optical systems that relay an optical image imaged at a primary imaging plane at the entrance side onto a secondary imaging plane at an exit side; wherein each of the plurality of relay optical systems is formed of a positive front group, a middle group, and a back group in this order from an entrance side, wherein the middle group of one of the relay optical systems that is disposed at an extreme exit side is provided with a diffractive optical element having a diffractive surface, and wherein the diffractive optical element receives an incident light beam, at the diffractive surface, whose axial chromatic aberration between at least two wavelengths has been corrected by an optical system other than the diffractive optical element, and the diffractive optical element corrects axial chromatic aberration related to another wavelength contained in the light beam. 2. The rigid-scope optical system according to claim 1 , wherein the relay optical system disposed at an extreme exit side satisfies the following expressions (1) and (2): 3 Lf<Lf doe  (1) 3 Lb<Lb doe  (2) where Lf is a distance from a primary imaging plane to a surface at the extreme entrance side of the front group of the relay optical system disposed at an extreme exit side, Lfdoe is a distance from the primary imaging plane to the diffractive surface of the relay optical system disposed at an extreme exit side, Lb is a distance from a surface at the extreme exit side of the back group to a secondary imaging plane of the relay optical system disposed at an extreme exit side, and Lbdoe is a distance from the diffractive surface to the secondary imaging plane of the relay optical system disposed at an extreme exit side. 3. The rigid-scope optical system according to claim 1 , wherein the relay optical system disposed at an extreme exit side satisfies the following expression (3): 0.5 <f doe/( ff+fm+fb )<10  (3) where fdoe is a focal distance of the diffractive optical element, ff is a focal distance of the front group of the relay optical system disposed at an extreme exit side, fm is a focal distance of the middle group of the relay optical system disposed at an extreme exit side, and fb is a focal distance of the back group of the relay optical system disposed at an extreme exit side. 4. The rigid-scope optical system according to claim 1 , wherein the relay optical system disposed at an extreme exit side or/and other relay optical systems comprises/comprise at least one combined optical system. 5. A rigid endoscope comprising the rigid-scope optical system according to claim 1 .
CROSS-REFERENCE TO RELATED APPLICATIONS This is a continuation of International Application PCT/JP2012/062590, with an international filing date of May 17, 2012, which is hereby incorporated by reference herein in its entirety. This application claims the benefit of Japanese Patent Application No. 2011-173074, the content of which is incorporated herein by reference. TECHNICAL FIELD The present invention relates to a rigid-scope optical system and a rigid endoscope. BACKGROUND ART In addition to common combined lenses, diffractive optical elements are conventionally used as means for correcting axial chromatic aberrations in optical systems provided in rigid endoscopes (see, for example, PTL 1). CITATION LIST Patent Literature {PTL 1} Japanese Unexamined Patent Application, Publication No. Hei 8-29678 SUMMARY OF INVENTION Technical Problem In the optical system described in PTL 1, although the axial chromatic aberration between two wavelengths is corrected by a diffractive optical element, axial chromatic aberration related to wavelengths other than these wavelengths is not corrected and remains as a so-called secondary spectrum. In addition, the optical performance is low because of a simple lens arrangement. In other words, a reduction in diffraction efficiency and flare occur because light beams are incident at an angle with respect to the diffractive surface, NA (numerical aperture) is not sufficient, and a negative secondary spectrum is produced due to over-correction of the secondary spectrum as a result of the inevitable increase in the power distribution of the diffractive surface. Solution to Problem A first aspect of the present invention is a rigid-scope optical system including: an objective optical system; and at least one relay optical system that is formed of a positive front group, a middle group, and a back group in this order from an entrance side and that reimages an optical image imaged at a primary imaging plane at the entrance side onto a secondary imaging plane at an exit side; wherein the middle group of one of the relay optical systems is provided with a diffractive optical element having a diffractive surface, and wherein axial chromatic aberration between two wavelengths is corrected by an optical system other than the diffractive optical element, and axial chromatic aberration between the two wavelengths and another wavelength is corrected by the diffractive optical element. A second aspect of the present invention is a rigid endoscope provided with the rigid-scope optical system mentioned above. BRIEF DESCRIPTION OF DRAWINGS FIG. 1 is an overall configuration diagram of a rigid-scope optical system according to an embodiment of the present invention. FIG. 2 is a lens diagram showing an objective optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 3 is a lens diagram showing a first relay optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 4 is a lens diagram showing a second relay optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 5 is a lens diagram showing a third relay optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 6 is a lens diagram showing a fourth relay optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 7 is a lens diagram showing a fifth relay optical system of a rigid-scope optical system according to Example 1 of the present invention. FIG. 8 is an axial chromatic aberration diagram of a rigid-scope optical system according to Example 1 of the present invention. FIG. 9 is a lens diagram showing an objective optical system of a rigid-scope optical system according to Example 2 of the present invention. FIG. 10 is a lens diagram showing a fifth relay optical system of a rigid-scope optical system according to Example 2 of the present invention. FIG. 11 is an axial chromatic aberration diagram of a rigid-scope optical system according to Example 2 of the present invention. FIG. 12 is a lens diagram showing a fifth relay optical system of a rigid-scope optical system according to Example 3 of the present invention. FIG. 13 is an axial chromatic aberration diagram of a rigid-scope optical system according to Example 3 of the present invention. FIG. 14 is a lens diagram showing a fifth relay optical system of a rigid-scope optical system according to Example 4 of the present invention. FIG. 15 is an axial chromatic aberration diagram of a rigid-scope optical system according to Example 4 of the present invention. DESCRIPTION OF EMBODIMENTS A rigid-scope optical system 100 according to an embodiment of the present invention will be described below with reference to FIG. 1 . As shown in FIG. 1 , the rigid-scope optical system 100 according to this embodiment is formed of an objective optical system 1 and first to fifth relay optical systems 10 , 20 , 30 , 40 , and 50 . The rigid-scope optical system 100 is accommodated in a rigid, straight, cylindrical lens barrel such that the objective optical system 1 faces the tip side, and the rigid-scope optical system 100 transmits an optical image of an object that has been collected and imaged by the objective optical system 1 by means of repeated image formation by the first to fifth relay optical systems 10 to 50 . The optical image that has been imaged by the fifth relay optical system 50 can be observed with an eyepiece optical system (not shown). Here, although the objective optical system 1 and the first to fifth relay optical systems 10 to 50 are arranged on the same straight optical axis, for the sake of illustration in FIG. 1 , the respective optical systems 1 , 10 , 20 , 30 , 40 , and 50 are arranged by dividing the optical axis at respective imaging planes P 1 to P 5 . The objective optical system 1 collects the light from the object (not shown) and images it at the first imaging plane P 1 . The first to fifth relay optical systems 10 , 20 , 30 , 40 , and 50 are respectively formed of positive front groups FG 1 to FG 5 , positive middle groups MG 1 to MG 5 , and positive back groups BG 1 to BG 5 , in this order from the entrance side. Specifically, the front groups FG 1 to FG 5 are formed of a single plano-convex lens whose convex surface faces the entrance side. The back groups BG 1 to BG 5 are formed of a single plano-convex lens whose convex surface faces the exit side. The middle groups MG 1 , MG 2 , MG 3 , and MG 4 in the respective first to fourth relay optical systems 10 , 20 , 30 , and 40 are each formed of a biconvex combined lens. The middle group MG 5 in the fifth relay optical system (one of the relay optical systems) 50 is formed of a diffractive optical element Ldoe and a biconvex combined lens L 51 , which are described later. The respective relay optical systems 10 , 20 , 30 , 40 , and 50 configured in this way relay the optical image on the first imaging plane P 1 to the sixth imaging plane P 6 at an optical magnification of substantially unity by imaging the optical images that have been imaged on the first to fifth imaging planes (primary imaging planes) P 1 to P 5 disposed at the immediately foregoing stages onto the second to sixth imaging planes (secondary imaging planes) P 2 to P 6 disposed at the immediately subsequent stages. Here, the combined lens (combined optical system) provided in the first to fourth relay optical systems 10 , 20 , 30 , and 40 is formed of a low-dispersion convex lens and a high-dispersion concave lens and corrects the axial chromatic aberration between two prescribed wavelengths, preferably between the C-line that corresponds to red (wavelength 656.3 nm) and the F-line that corresponds to blue (wavelength 486.1 nm), contained in the incident light beam. The diffractive optical element Ldoe provided in the fifth relay optical system 50 is of the multilayer type. In other words, the diffractive optical element Ldoe is formed by combining two optical elements, which are formed of glass materials having different refractive indices and Abbe numbers from each other and have diffractive surfaces Pdoe at one of their surfaces such that the diffractive surfaces Pdoe face each other. The diffractive optical element Ldoe corrects the axial chromatic aberration related to another wavelength, preferably the e-line, which corresponds to green (546.1 nm), between the C-line and the F-line, contained in the light beam whose axial chromatic aberration between two wavelengths has been corrected in the first to fourth relay optical systems 10 , 20 , 30 , and 40 . Here, the fifth relay optical system 50 satisfies the following expressions (1), (2), and (3): 3 Lf<Lf doe  (1) 3 Lb<Lb doe  (2) 0.5< f doe/( ff+fm+fb )<10  (3) where Lf is the distance from the fifth imaging plane (the primary imaging plane) to the surface at the extreme entrance side of the front group FG 5 , Lfdoe is the distance from the fifth imaging plane to the diffractive surface Pdoe, Lb is the distance from the surface at the extreme exit side of the back group BG 5 to the sixth imaging plane (the secondary imaging plane), Lbdoe is the distance from the diffractive surface Pdoe to the sixth imaging plane, fdoe is the focal distance of the diffractive optical element Ldoe, ff is the focal distance of the front group FG 5 , fm is the focal distance of the middle group MG 5 , and fb is the focal distance of the back group BG 5 . The expressions (1) and (2) define the position of the diffractive surface in the relay optical system. In other words, by positioning the diffractive surface sufficiently away from the front group surface at the extreme entrance side and back group surface at the extreme exit side, the light beam entering the diffractive surface becomes more collimated. Thus, it is possible to prevent the occurrence of flare at the diffractive surface with even higher reliability. When Lfdoe and Lbdoe are 3-times greater than Lf and LB, respectively, or less, it is difficult to sufficiently collimate the light beam entering the diffractive surface, and there is a risk of causing flare and a reduction in diffraction efficiency. Expression (3) defines the power of the diffractive optical element relative to the power of the one relay optical system as a whole. In other words, by suitably setting a range of the relative power of the diffractive optical element, it is possible to suitably correct the axial chromatic aberration and to make the pitch of the diffraction grating, which is formed on the diffractive surface, have a size suitable for processing. When the value of expression (3) is 0.5 or less, the power distribution in the diffractive surface is increased, producing a negative secondary spectrum, and the pitch of the diffraction grating becomes small, making processing thereof difficult. On the other hand, when the value of expression (3) is 10 or more, the secondary spectrum cannot be corrected sufficiently, and in addition, the pitch on the diffractive surface is increased, causing the number of diffraction grating rulings within the effective diameter to be reduced, thereby reducing the diffraction efficiency. With the thus-configured rigid-scope optical system 100 , the secondary spectrum remaining from the first to fourth relay optical systems 10 , 20 , 30 , and 40 is corrected by the diffractive optical element Ldoe that is provided in the fifth relay optical system 50 . By doing so, it is possible to obtain an optical image whose axial chromatic aberration has been suitably corrected over the entire visible region at the sixth imaging plane P 6 . In addition, in accordance with the expressions (1) and (2), the diffractive surface Pdoe is arranged at a position sufficiently away from the entrance side surface of the plano-convex lens in the front group FG 5 and the exit side surface of the plano-convex lens in the back group BG 5 in the fifth relay optical system 50 ; therefore, the light beam entering the diffractive surface Pdoe becomes a substantially collimated light beam. Thus, it is possible to achieve high diffraction efficiency at the diffractive surface Pdoe and to prevent the occurrence of flare. Furthermore, because the on-axis light beam and the off-axis light beam overlap at the position of the diffractive surface Pdoe, it is possible to prevent the occurrence of the magnification chromatic aberration and chromatic comatic aberration. In addition, by setting the relative power of the diffractive surface Pdoe in the fifth relay optical system 50 to the level defined by expression (3), it is possible to suitably correct the secondary spectrum with the diffractive optical element Ldoe and also to make the pitch of the diffraction grating formed on the diffractive surface Pdoe so as to have a preferable size in terms of processability and diffraction efficiency. In addition, by configuring the middle group MG 5 by combining the diffractive optical element Ldoe and the biconvex combined lens 51 , it is possible to make the power distribution of the diffractive optical element Ldoe small. EXAMPLE Examples 1 to 4 of the rigid-scope optical system according to the above-mentioned embodiment of the present invention will be explained below with reference to FIGS. 2 to 15 . In the lens data described in each Example, r denotes the radius of curvature, d denotes the intersurface distance, ne denotes the refractive index for the e-line, and vd denotes the Abbe number for the d-line. The surface number corresponding to the aperture is assigned S, and the surface number corresponding to the diffractive surface is assigned P. In addition, in the lens data and the attached lens diagram, IMG denotes an image plane. With respect to the aspheric surface, the surface number in the lens data is shown with *, and the radius of paraxial curvature r, the conic coefficient k, and the aspheric coefficients Ai (i=2, 4, 6, 8, 10) of the aspheric surface shape, which are defined by the following expressions, are shown in the aspheric surface data. In the following expressions, the optical axis direction is defined as z, and the direction orthogonal to the optical axis is defined as y. z = ( y 2 / r ) ⁢ / ⁡ [ 1 + { 1 - ( 1 + k ) ⁢ ( y ⁢ / ⁢ r ) 2 } 1 / 2 ] + A 2 ⁢ y 2 + A 4 ⁢ y 4 + A 6 ⁢ y 6 + A 8 ⁢ y 8 + A 10 ⁢ y 10 In addition, the diffractive surface is expressed as the aspheric surface shape of the equivalent ultra-high-index lens (refractive lens with very high refractive index) in accordance with the high-refractive-index method. The relationship according to the following expression, between the pitch d of the diffraction grating formed in the diffractive surface and the aspheric surface shape of the ultra-high-index lens; holds: d = m ⁢ ⁢ λ ⁢ / ⁡ [ ( n - 1 ) ⁢ { ch ⁢ / ⁢ ( 1 - c 2 ⁡ ( 1 + k ) ⁢ h 2 ) 1 / 2 + 2 ⁢ A 2 ⁢ h + 4 ⁢ A 4 ⁢ h 3 + 6 ⁢ A 6 ⁢ h 5 + 8 ⁢ A 8 ⁢ h 7 + 10 ⁢ A 10 ⁢ h 9 + … ⁢ } ] where h is the ray height, and m is the diffraction order. Example 1 As shown in FIGS. 2 to 7 , the rigid-scope optical system according to Example 1 of the present invention is provided with the objective optical system and the first to fifth relay optical systems, in this order from the object side. Each of the first to fourth relay optical systems is formed of the positive front group formed of the plano-convex lens whose convex surface faces the object side, the positive middle group formed of the combined lens, and the positive back group formed of the plano-convex lens whose convex surface faces the image side, in this order from the object side. The fifth relay optical system is formed of the positive front group formed of the plano-convex lens whose convex surface faces the object side, the positive middle group formed of the diffractive optical element and the combined lens, and the positive back group formed of the plano-convex lens whose convex surface faces the image side, in this order from the object side. The lens data for the rigid-scope optical system according to this Example is as follows. An axial chromatic aberration diagram of the thus-configured rigid-scope optical system is shown in FIG. 8 . With the rigid-scope optical system of this Example, the axial chromatic aberration between the C-line and the F-line can be corrected by the combined lenses provided in the first to fourth relay optical systems, and the remaining axial chromatic aberration related to the e-line can be corrected by the diffractive optical element provided in the fifth relay optical system. Lens Data Surface Number r d ne νd  1 ∞ 0.1886 1.77066 71.79  2 ∞ 0.0613  3* 22.2256 0.2358 1.79190 25.76  4 0.3320 0.1844  5 ∞ 1.9525 1.88814 40.78  6 ∞ 1.3205 1.88815 40.76  7 −2.0440 0.6791  8 71.5633 0.3631 1.83932 37.16  9 1.8963 1.0140 1.48915 70.23 10 −1.8963 0.3584 11 3.0373 1.3771 1.73234 54.68 12 −115.0826 1.3205 13 −0.9833 0.5565 1.85504 23.78 14 1.3960 0.9385 1.73234 54.68 15 −1.3960 0.8348 16 ∞ 2.4429 1.00000 17 4.9147 10.2057 1.59143 61.14 18 ∞ 0.9291 19 4.6600 0.6320 1.69661 53.21 20 −2.4665 0.0024 1.51203 60.00 21 −2.4625 0.8890 1.83945 42.72 22S ∞ 0.8890 1.83945 42.72 23 2.4625 0.0024 1.51203 60.00 24 2.4665 0.6320 1.69661 53.21 25 −4.6600 0.9291 26 ∞ 10.2057 1.59143 61.14 27 −4.9147 2.4429 28 ∞ 2.4429 29 4.9147 10.2057 1.59143 61.14 30 ∞ 0.9291 31 4.6600 0.6320 1.69661 53.21 32 −2.4665 0.0024 1.51203 60.00 33 −2.4625 0.8890 1.83945 42.72 34 ∞ 0.8890 1.83945 42.72 35 2.4625 0.0024 1.51203 60.00 36 2.4665 0.6320 1.69661 53.21 37 −4.6600 0.9291 38 ∞ 10.2057 1.59143 61.14 39 −4.9147 2.4429 40 ∞ 2.4429 41 4.9147 10.2057 1.59143 61.14 42 ∞ 0.9291 43 4.6600 0.6320 1.69661 53.21 44 −2.4665 0.0024 1.51203 60.00 45 −2.4625 0.8890 1.83945 42.72 46 ∞ 0.8890 1.83945 42.72 47 2.4625 0.0024 1.51203 60.00 48 2.4665 0.6320 1.69661 53.21 49 −4.6600 0.9291 50 ∞ 10.2057 1.59143 61.14 51 −4.9147 2.4429 52 ∞ 2.4429 53 4.9147 10.2057 1.59143 61.14 54 ∞ 0.9291 55 4.6600 0.6320 1.69661 53.21 56 −2.4665 0.0024 1.51203 60.00 57 −2.4625 0.8890 1.83945 42.72 58 ∞ 0.8890 1.83945 42.72 59 2.4625 0.0024 1.51203 60.00 60 2.4665 0.6320 1.69661 53.21 61 −4.6600 0.9291 62 ∞ 10.2057 1.59143 61.14 63 −4.9147 2.4429 64 ∞ 1.8534 65 3.3539 10.1396 1.59143 61.14 66 ∞ 0.6980 67 ∞ 0.4716 1.64640 23.40 68P 45347.1811 0.0000 930.00000 −3.45 69 ∞ 0.4716 1.70455 36.40 70 ∞ 0.3867 71 8.2956 1.2734 1.83945 42.71 72 ∞ 0.0141 73 ∞ 1.4620 1.83945 42.71 74 −10.6067 0.7499 75 ∞ 6.9044 1.48915 70.23 76 −11.0870 3.1636 IMG ∞ 0.0000 Aspheric Surface Data Surface 3 k = 0.0000 A 2 = 0 A 4 = 9.36E−01 A 6 = −1.84E+00 A 8 = 3.91E+00 A 10 = 0.00E+00 Surface 68 k = 24.0663 A 2 = 0 A 4 = −2.30E−06 A 6 = 5.64E−07 A 8 = 1.88E−06 A 10 = −7.55E−07 Miscellaneous Data Object Distance 14.1832 Focal Distance −1 Image Height 0.665 Fno. 5.76 Viewing Angle 70.71° Example 2 As shown in FIGS. 9 and 10 , a rigid-scope optical system according to Example 2 of the present invention differs from the rigid-scope optical system of Example 1 mainly in the lens arrangements of the objective optical system (surface numbers 1 to 15 ) and the fifth relay optical system (surface numbers 65 to 78 ). In the fifth relay optical system, the diffractive optical element is flanked by the two combined lenses in the optical axis direction. The lens arrangements of the first to fourth relay optical systems are substantially the same as that of the rigid-scope optical system of Example 1, and an illustration thereof shall be omitted. The lens data for the rigid-scope optical system according to this Example is as follows. An axial chromatic aberration diagram of the thus-configured rigid-scope optical system is shown in FIG. 11 . With the rigid-scope optical system of this Example, the axial chromatic aberration between the C-line and the F-line can be corrected by the combined lenses provided in the first to fourth relay optical systems, and the remaining axial chromatic aberration related to the e-line can be corrected by the diffractive optical element provided in the fifth relay optical system. Lens Data Surface Number r d ne νd  1 ∞ 0.1886 1.77066 71.79  2 ∞ 0.0613  3* 22.2258 0.2358 1.79190 25.76  4 0.3315 0.1844  5 ∞ 1.9525 1.88814 40.78  6 ∞ 1.1936 1.88815 40.76  7 −1.8699 0.2294  8 −20.4710 0.7292 1.83932 37.16  9 1.9505 1.0468 1.48915 70.23 10 −2.1435 0.4369 11 3.6510 1.2517 1.73234 54.68 12 −4.8434 1.2162 13 −1.1595 0.8772 1.85504 23.78 14 1.6194 1.1154 1.73234 54.68 15 −1.8369 1.0399 16 ∞ 2.4430 17 4.9147 10.2058 1.59143 61.14 18 ∞ 0.9291 19 4.6601 0.6320 1.69661 53.21 20 −2.4666 0.0024 1.51203 60.00 21 −2.4625 0.8890 1.83945 42.72 22S ∞ 0.8890 1.83945 42.72 23 2.4625 0.0024 1.51203 60.00 24 2.4666 0.6320 1.69661 53.21 25 −4.6601 0.9291 26 ∞ 10.2058 1.59143 61.14 27 −4.9147 2.4430 28 ∞ 2.4430 29 4.9147 10.2058 1.59143 61.14 30 ∞ 0.9291 31 4.6601 0.6320 1.69661 53.21 32 −2.4666 0.0024 1.51203 60.00 33 −2.4625 0.8890 1.83945 42.72 34 ∞ 0.8890 1.83945 42.72 35 2.4625 0.0024 1.51203 60.00 36 2.4666 0.6320 1.69661 53.21 37 −4.6601 0.9291 38 ∞ 10.2058 1.59143 61.14 39 −4.9147 2.4430 40 ∞ 2.4430 41 4.9147 10.2058 1.59143 61.14 42 ∞ 0.9291 43 4.6601 0.6320 1.69661 53.21 44 −2.4666 0.0024 1.51203 60.00 45 −2.4625 0.8890 1.83945 42.72 46 ∞ 0.8890 1.83945 42.72 47 2.4625 0.0024 1.51203 60.00 48 2.4666 0.6320 1.69661 53.21 49 −4.6601 0.9291 50 ∞ 10.2058 1.59143 61.14 51 −4.9147 2.4430 52 ∞ 2.4430 53 4.9147 10.2058 1.59143 61.14 54 ∞ 0.9291 55 4.6601 0.6320 1.69661 53.21 56 −2.4666 0.0024 1.51203 60.00 57 −2.4625 0.8890 1.83945 42.72 58 ∞ 0.8890 1.83945 42.72 59 2.4625 0.0024 1.51203 60.00 60 2.4666 0.6320 1.69661 53.21 61 −4.6601 0.9291 62 ∞ 10.2058 1.59143 61.14 63 −4.9147 2.4430 64 ∞ 1.8865 65 3.7190 9.4128 1.59143 61.14 66 ∞ 1.4353 67 8.8488 0.5666 1.69661 53.21 68 15.2761 0.7759 1.83945 42.71 69 ∞ 0.0141 70 ∞ 0.4716 1.64640 23.40 71P 56877.3621 0.0000 930.00000 −3.45 72 ∞ 0.4716 1.70455 36.40 73 ∞ 0.0141 74 ∞ 0.7759 1.83945 42.71 75 −15.2761 0.5666 1.69661 53.21 76 −8.8488 1.2100 77 ∞ 6.6026 1.48915 70.23 78 −7.9272 3.7871 IMG ∞ 0.0000 Aspheric Surface Data Surface 3 k = 0 A 2 = 0 A 4 = 9.36E−01 A 6 = −1.84E+00 A 8 = 3.91E+00 A 10 = 0.00E+00 Surface 71 k = 3.5108 A 2 = 0 A 4 = −2.95E−06 A 6 = 1.55E−06 A 8 = 0.00E+00 A 10 = 0.00E+00 Miscellaneous Data Object Distance 14.1485 Focal Distance −1 Image Height 0.665 Fno. 5.7568 Viewing Angle 70.1° Example 3 As shown in FIG. 12 , a rigid-scope optical system according to Example 3 of the present invention differs from the rigid-scope optical system of Example 2 mainly in the lens arrangement of the fifth relay optical system (surface numbers 65 to 78 ). The lens arrangements of the objective optical system and the first to fourth relay optical systems are substantially the same as that of the rigid-scope optical system of Example 2, and an illustration thereof shall be omitted. The lens data for the rigid-scope optical system according to this Example is as follows. An axial chromatic aberration diagram of the thus-configured rigid-scope optical system is shown in FIG. 13 . With the rigid-scope optical system of this Example, the axial chromatic aberration between the C-line and the F-line can be corrected by the combined lenses provided in the first to fourth relay optical systems, and the remaining axial chromatic aberration related to the e-line can be corrected by the diffractive optical element provided in the fifth relay optical system. Lens Data Surface Number r d ne νd  1 ∞ 0.1886 1.77066 71.79  2 ∞ 0.0613  3* 22.2258 0.2358 1.79190 25.76  4 0.3315 0.1844  5 ∞ 1.9525 1.88814 40.78  6 ∞ 1.1936 1.88815 40.76  7 −1.8699 0.2294  8 −20.4710 0.7292 1.83932 37.16  9 1.9505 1.0468 1.48915 70.23 10 −2.1435 0.4369 11 3.6510 1.2517 1.73234 54.68 12 −4.8434 1.2162 13 −1.1595 0.8772 1.85504 23.78 14 1.6194 1.1154 1.73234 54.68 15 −1.8369 1.0399 16 ∞ 2.4430 17 4.9147 10.2058 1.59143 61.14 18 ∞ 0.9291 19 4.6601 0.6320 1.69661 53.21 20 −2.4666 0.0024 1.51203 60.00 21 −2.4625 0.8890 1.83945 42.72 22S ∞ 0.8890 1.83945 42.72 23 2.4625 0.0024 1.51203 60.00 24 2.4666 0.6320 1.69661 53.21 25 −4.6601 0.9291 26 ∞ 10.2058 1.59143 61.14 27 −4.9147 2.4430 28 ∞ 2.4430 29 4.9147 10.2058 1.59143 61.14 30 ∞ 0.9291 31 4.6601 0.6320 1.69661 53.21 32 −2.4666 0.0024 1.51203 60.00 33 −2.4625 0.8890 1.83945 42.72 34 ∞ 0.8890 1.83945 42.72 35 2.4625 0.0024 1.51203 60.00 36 2.4666 0.6320 1.69661 53.21 37 −4.6601 0.9291 38 ∞ 10.2058 1.59143 61.14 39 −4.9147 2.4430 40 ∞ 2.4430 41 4.9147 10.2058 1.59143 61.14 42 ∞ 0.9291 43 4.6601 0.6320 1.69661 53.21 44 −2.4666 0.0024 1.51203 60.00 45 −2.4625 0.8890 1.83945 42.72 46 ∞ 0.8890 1.83945 42.72 47 2.4625 0.0024 1.51203 60.00 48 2.4666 0.6320 1.69661 53.21 49 −4.6601 0.9291 50 ∞ 10.2058 1.59143 61.14 51 −4.9147 2.4430 52 ∞ 2.4430 53 4.9147 10.2058 1.59143 61.14 54 ∞ 0.9291 55 4.6601 0.6320 1.69661 53.21 56 −2.4666 0.0024 1.51203 60.00 57 −2.4625 0.8890 1.83945 42.72 58 ∞ 0.8890 1.83945 42.72 59 2.4625 0.0024 1.51203 60.00 60 2.4666 0.6320 1.69661 53.21 61 −4.6601 0.9291 62 ∞ 10.2058 1.59143 61.14 63 −4.9147 2.4430 64 ∞ 1.8865 65 3.7190 9.4128 1.59143 61.14 66 ∞ 1.4135 67 4.7493 0.5333 1.69661 53.21 68 −2.6933 0.7447 1.83945 42.71 69 ∞ 0.0141 70 ∞ 0.4716 1.64640 23.40 71P 231984.5611 0.0000 930.00000 −3.45 72 ∞ 0.4716 1.70455 36.40 73 ∞ 0.0141 74 ∞ 0.7447 1.83945 42.71 75 2.6933 0.5333 1.69661 53.21 76 −4.7493 1.1610 77 ∞ 6.6026 1.48915 70.23 78 −7.9272 3.8241 IMG ∞ 0.0000 Aspheric Surface Data Surface 3 k = 0.0000 A 2 = 0 A 4 = 9.36E−01 A 6 = −1.84E+00 A 8 = 3.91E+00 A 10 = 0.00E+00 Surface 71 k = 3.5112 A 2 = 0 A 4 = −3.19E−06 A 6 = 2.50E−06 A 8 = 0.00E+00 A 10 = 0.00E+00 Miscellaneous Data Object Distance 14.1485 Focal Distance −1 Image Height 0.665 Fno. 5.7568 Viewing Angle 69.98° Example 4 As shown in FIG. 14 , a rigid-scope optical system according to Example 4 of the present invention differs from the rigid-scope optical system of Example 2 mainly in the lens arrangement of the fifth relay optical system (surface numbers 65 to 78 ). The arrangements of the objective optical system and the first to fourth relay optical systems are substantially the same as that of the rigid-scope optical system of Example 2, and an illustration thereof shall be omitted. The lens data for the rigid-scope optical system according to this Example is as follows. An axial chromatic aberration diagram of the thus-configures rigid-scope optical system is shown in FIG. 15 . With the rigid-scope optical system of this Example, the axial chromatic aberration between the C-line and the F-line can be corrected by the combined lenses provided in the first to fourth relay optical systems, and the remaining axial chromatic aberration related to the e-line can be corrected by the diffractive optical element provided in the fifth relay optical system. Lens Data Surface Number r d ne νd  1 ∞ 0.1886 1.77066 71.79  2 ∞ 0.0613  3* 22.2256 0.2358 1.79190 25.76  4 0.3315 0.1844  5 ∞ 1.9525 1.88814 40.78  6 ∞ 1.1936 1.88815 40.76  7 −1.8699 0.2294  8 −20.4708 0.7292 1.83932 37.16  9 1.9504 1.0468 1.48915 70.23 10 −2.1435 0.4369 11 3.6510 1.2517 1.73234 54.68 12 −4.8433 1.2162 13 −1.1595 0.8772 1.85504 23.78 14 1.6194 1.1154 1.73234 54.68 15 −1.8368 1.0399 16 ∞ 2.4429 17 4.9147 10.2057 1.59143 61.14 18 ∞ 0.9291 19 4.6600 0.6320 1.69661 53.21 20 −2.4665 0.0024 1.51203 60.00 21 −2.4625 0.8890 1.83945 42.72 22S ∞ 0.8890 1.83945 42.72 23 2.4625 0.0024 1.51203 60.00 24 2.4665 0.6320 1.69661 53.21 25 −4.6600 0.9291 26 ∞ 10.2057 1.59143 61.14 27 −4.9147 2.4429 28 ∞ 2.4429 29 4.9147 10.2057 1.59143 61.14 30 ∞ 0.9291 31 4.6600 0.6320 1.69661 53.21 32 −2.4665 0.0024 1.51203 60.00 33 −2.4625 0.8890 1.83945 42.72 34 ∞ 0.8890 1.83945 42.72 35 2.4625 0.0024 1.51203 60.00 36 2.4665 0.6320 1.69661 53.21 37 −4.6600 0.9291 38 ∞ 10.2057 1.59143 61.14 39 −4.9147 2.4429 40 ∞ 2.4429 41 4.9147 10.2057 1.59143 61.14 42 ∞ 0.9291 43 4.6600 0.6320 1.69661 53.21 44 −2.4665 0.0024 1.51203 60.00 45 −2.4625 0.8890 1.83945 42.72 46 ∞ 0.8890 1.83945 42.72 47 2.4625 0.0024 1.51203 60.00 48 2.4665 0.6320 1.69661 53.21 49 −4.6600 0.9291 50 ∞ 10.2057 1.59143 61.14 51 −4.9147 2.4429 52 ∞ 2.4429 53 4.9147 10.2057 1.59143 61.14 54 ∞ 0.9291 55 4.6600 0.6320 1.69661 53.21 56 −2.4665 0.0024 1.51203 60.00 57 −2.4625 0.8890 1.83945 42.72 58 ∞ 0.8890 1.83945 42.72 59 2.4625 0.0024 1.51203 60.00 60 2.4665 0.6320 1.69661 53.21 61 −4.6600 0.9291 62 ∞ 10.2057 1.59143 61.14 63 −4.9147 2.4429 64 ∞ 4.0000 65 3.1973 7.0000 1.59143 61.14 66 ∞ 1.6210 67 −6.9788 0.5202 1.69661 53.21 68 1.6001 0.9080 1.83945 42.71 69 ∞ 0.0141 70 ∞ 0.4716 1.64640 23.40 71P 12138.3807 0.0000 930.00000 −3.45 72 ∞ 0.4716 1.70455 36.40 73 ∞ 0.0141 74 ∞ 0.9039 1.83945 42.71 75 −1.4289 0.5190 1.69661 53.21 76 31.4292 1.3000 77 ∞ 4.9223 1.48915 70.23 78 −5.7900 3.1223 IMG ∞ 0.0000 Aspheric Surface Data Surface 3 k = 0.0000 A 2 = 0 A 4 = 9.36E−01 A 6 = −1.84E+00 A 8 = 3.91E+00 A 10 = 0.00E+00 Surface 71 k = 0.00E+00 A 2 = 0 A 4 = −3.64E−05 A 6 = 3.65E−06 A 8 = 0.00E+00 A 10 = 0.00E+00 Miscellaneous Data Object Distance 14.1483 Focal Distance −1 Image Height 0.665 Fno. 5.7568 Viewing Angle 69.51° Respective values of the parameters in the conditional expressions (1), (2), and (3) for the fifth relay optical system provided in the rigid-scope optical system according to above-mentioned Examples 1 to 4 are as shown in Table 1. TABLE 1 Conditional Expression Example 1 Example 2 Example 3 Example 4 (1) 3Lf 5.560 5.660 5.660 12.000 Lfdoe 13.163 14.563 14.476 14.535 (2) 3Lb 9.491 11.361 11.472 9.367 Lbdoe 14.426 13.428 13.351 11.253 (3) fdoe 48.827 61.241 249.784 13.070 ff 5.670 6.288 6.288 5.406 fm 5.433 5.763 5.763 6.712 fb 22.666 16.206 16.206 11.837 fdoe/ 1.446 2.167 8.840 0.546 (ff + fm + fb) {Reference Signs List} 1 objective optical system 10, 20, 30, 40, 50 relay optical system 100 rigid-scope optical system BG1, BG2, BG3, BG4, BG5 back group MG1, MG2, MG3, MG4, MG5 middle group FG1, FG2, FG3, FG4, FG5 front group Ldoe diffractive optical element P1, P2, P3, P4, P5, P6 imaging plane Pdoe diffractive surface

Description

Topics

Download Full PDF Version (Non-Commercial Use)

Patent Citations (6)

    Publication numberPublication dateAssigneeTitle
    JP-H0829678-AFebruary 02, 1996Olympus Optical Co Ltd, オリンパス光学工業株式会社硬性鏡観察光学系
    US-2002018305-A1February 14, 2002Minolta Co., Ltd.Fixed focal length lens system
    US-2004125445-A1July 01, 2004Jan HooglandIntegrated optical system for endoscopes and the like
    US-2008273247-A1November 06, 2008Yuri KazakevichColor-Corrected Optical System
    US-7511891-B2March 31, 2009Grintech GmbhMiniaturized optically imaging system with high lateral and axial resolution
    WO-0122866-A1April 05, 2001Visionscope, Inc.Endoscope system

NO-Patent Citations (2)

    Title
    E. Ezhov, et al., "Apochromatic Correction of the Rigid Grin Endoscope," Opoelectronics Instrumentation and Data Processing 43(1): 70-75 (2007).
    International Search Report, dated Jul. 24, 2012, issued in corresponding Japanese Patent Application No. PCT/JP2012/062590.

Cited By (1)

    Publication numberPublication dateAssigneeTitle
    US-9877654-B2January 30, 2018Novadaq Technologies Inc.Near infrared imaging