Zoom lens

Abstract: A zoom lens includes at least two lens groups, i.e., a first lens group and a second lens group. The second lens group includes a first sub-group near to the first lens group and a second sub-group far from the first lens group, and the first lens group and the first sub-group in the second lens group together form a substantially afocal system in at least a portion of a zooming range. In the zoom lens, focusing is effected by the first sub-group in the second lens group being moved along the optical axis. Considering a case where this zoom lens is applied for auto focusing, it is preferable that the first lens group be disposed on that side in the lens group which is most adjacent to the object side.

Description: BACKGROUND OF THE INVENTION Field of the Invention This invention relates to a zoom lens. Related Background Art Generally in a zoom lens, focusing is effected by moving the foremost lens group thereof, i.e. the lens group which is most adjacent to the object side. This focusing method is still used in many zoom lenses because in a zooming range for objects on the same distance, focusing can be accomplished by a substantially constant amount of movement and moreover the structure of the lens barrel can be constructed relatively simply. However, the foremost lens group of a popular zoom lens requires the largest lens diameter and therefore, the zoom lens becomes heavy, and this leads to the disadvantage that in case of auto focusing, quick focusing becomes difficult. So, in recent years, the lighter weight of a lens group for focusing has been desired with the spread of auto focus cameras and various focusing systems have been proposed. Zoom lenses disclosed, for example, in JP-A-52-109952, JP-A-56-21112, JP-A-57-4018 and JP-A-1-204013 are known. In the zoom lens disclosed in the above-mentioned JP-A-52-109952, focusing is effected by moving a part of the foremost lens group thereof, and in a zooming range for objects on the same distance, focusing can be accomplished by a substantially constant amount of movement and the structure of the lens barrel can be constructed relatively simply. However, the full length of the foremost lens group is increased and a movable lens for focusing is disposed in the foremost lens group of a large lens diameter, and this leads to the disadvantage that a great decrease in the weight of the focusing group cannot be very much expected. In the zoom lens of JP-A-56-21112, focusing is effected by moving some of the lens groups behind the foremost lens group, and in a zooming range for objects on the same distance, focusing can be accomplished by a substantially constant amount of movement and the structure of the lens barrel can be made relatively simple. However, this zoom lens is restricted to a four-group afocal zoom lens type and is not popular. Also, in the focusing system disclosed in JP-A-57-4018, any other lens group than the foremost lens group is used as a focusing group. Therefore, the amount of movement differs depending on each vari-focused state for objects on the same distance. Specifically, focusing is effected by the use of a zooming cam and a focusing cam which are function-approximated to each other in the correction of the amount of movement. This method has the feature that a group of small fluctuation of a short distance or a group small in weight can be freely selected, but has the disadvantage that the structure of the lens barrel becomes complicated. A system for an integral lens type camera is disclosed in JP-A-1-204013. This is a system in which each vari-focused state is read by an electrical signal and an amount of movement conforming thereto is found. This system also has the feature that a group of small fluctuation of a short distance or a group of light weight can be freely selected, but has the disadvantage that it cannot be used as a zoom lens for a single-lens reflex camera of the manual focusing type. Further, in a lens exclusively for auto focusing or the like, when the correction of the amount of movement is effected in accordance with the focal length within the zooming range, it is preferable that the following condition be satisfied in the entire zooming range: β F > 1.8 The above-mentioned substantially afocal system refers to a lens system in a state in which the lateral magnification β F of a first sub-group in a second lens group in case of an infinity state is |β F | ≧ 100. When optical systems approximate to each other in small thickness are supposed, in succession from the object side, a foremost lens group which is not concerned in focusing is defined as (A), a focusing lens group concerned in focusing is defined as (F) and a lens group on the image side which is not concerned in focusing is defined as (B). The focal length of the foremost lens group (A) which is not concerned in focusing is defined as f A , the focal length of the focusing lens group (F) is defined as f F , the lateral magnification of the focusing lens group (F) when the photographing distance is infinity is defined as β F , the photographing distance (the distance between object images) is defined as R, and the amount of movement by which the focusing lens group (F) is moved to be focused on an object at the photographing distance R is defined as Δx (the movement from the object side to the image side is positive). Also, the length of the entire lens system is defined as TL (the length from the object side principal point to the image plane of the lens group (A) on the object side). When the distance from the object side principal point of the foremost lens group (A) to the object is D 0 , the amount of movement Δx for focusing is expressed by the following equation I as described in a publication Optics, Vol. 12, No. 5, October, 1983, pp. 359 - 366 ("The New Focusing System for Zoom Lens"). (R-TL-f A )Δx = (D 0 -f A )Δx = f A 2 (Δx + β F x f F ) Δx{Δx+(β F 2 -1) x (f F /β F )} A zoom lens of the kind defined by the precharacterizing features of Claim 1 is known from the DE-A-3 027 558. During zooming the first sub-group of the second lens group moves leading to a relatively complicated structure of the zoom lens. SUMMARY OF THE INVENTION Accordingly, it is the object of the present invention to eliminate the disadvantages peculiar to the focusing systems in the above-described zoom lenses according to the prior art and to provide a zoom lens of the kind defined by the precharacterizing features of claim 1 which is light in weight and can be used for auto focusing. This object is attained by the characterizing features of claim 1. Considering a case where this zoom lens is applied for auto focusing, it is preferable that the first lens group be disposed on that side in the lens group which is most adjacent to the object side. Further, to effect more effective focusing, it is preferable that the following condition be satisfied in the entire zooming range: β F > 3.3, where |β F | is the absolute value of the lateral magnification β F of the first sub-group in the second lens group in an infinity state. Further, equation (I) can be approximately rewritten into the following equation (II): (D 0 - f A )Δx ≃ f A 2 x β F 2 (β F 2 - 1) When β F is infinity or sufficiently great, equation (I) and equation (II) can be approximately rewritten into the following equation (III): (D 0 - f A )Δx = f A 2 A case where as in the present invention, the second lens group is divided into first and second sub-groups and in the vari-focused state of at least a portion in the zooming range from the wide angle end to the telephoto end, the first lens group and the first sub-group in the second lens group together form a substantially afocal system and the first sub-group in the second lens group is moved along the optical axis corresponds to a case where the lateral magnification β F of the first sub-group in the above-mentioned equation (I) or (II) is infinity or sufficiently great. Thus, in such case, equation (III) is established. In the present invention, the focal length f A of the lens group (A) on the object side is equal to an invariable value f 1 duirng vari-focusing, and equation (III) becomes (D 0 - f 1 )Δx = f 1 2 ≃ constant. Next, considering that the variation in the distance D 0 from the object side principal point of the lens group (A) on the object side to the object by vari-focusing at the same photographing distance is relatively small, equation (IV) can be approximated as follows: Δx = f 1 2 /(D 0 - f 1 ) ≃ constant. Thus, when the lateral magnification β F is sufficiently great in all the zooming range from the wide angle end to the telephoto end, equation (V) is established in all the zooming range. The amount of movement of the first sub-group in the second lens group can be made substantially constant in the entire zooming range. Therefore, even if the amount of movement is made constant, the amount of movement of the image plane in vari-focusing will pose no problem in practical use, and the hardware structure of the first lens group of the present invention can be made as simple as the hardware structure of the movement of the lens group on the object side in the prior-art zoom lens. Also, when the zoom lens of the present invention is used for auto focusing or the like, if the first lens group is disposed most adjacent to the object side, the weight of the focusing group can be made very light because the effective diameter of the second lens group is very small as compared with that of the first lens group and moreover the second lens group is divided into the first sub-group for focusing and the second sub-group for non-focusing, and this is very advantageous for focusing by auto focusing. When manual focusing is considered, it is desirable that the aforementioned CONDITION (1) be satisfied in the entire zooming range. If the range of CONDITION (1) is exceeded, the amount of movement of the image plane in the vari-focusing when the amount of movement is made constant will become too great and it will become necessary to effect cam correction or the like to thereby vary the amount of movement. Also, in case of a zoom lens for a manual focusing type single lens reflex camera, the structure of the hardware becomes complicated, and this is not preferable. However, if the correction of the amount of movement is possible even if CONDITION (1) is exceeded, the focusing group can be made very light in weight, and this is suitable as a focusing system for auto focusing. So, when the correction of the amount of movement is taken into account, it is desirable that the aforementioned CONDITION (2) be satisfied. If the range of CONDITION (2) is exceeded, it will be possible to vary the amount of movement by cam correction or the like, but the lens spacing necessary for focusing will further widen and the full length of the lens will become great, and this is not preferable. Further, it is desirable that the following condition be satisfied when the focusing according to the present invention is effected: 4 < f 1 (f 1 +d F,R )/(d F,R x f T ) < 15, where d F,R : the space between the first sub-group and the second sub-group in the second lens group during the infinity state; f 1 : the focal length of the first lens group; f T : the focal length of the entire system at the telephoto end. Conditional expression (3) is concerned with the focal length of the first lens group and the space between the first sub-group and the second sub-group in the second lens group during the infinity state. If the upper limit of conditional expression (3) is exceeded, the space necessary for focusing will be deficient and therefore, the close-up photographing distance will become long, and this is not preferable. Even if the space is secured, the refractive power of the first lens group will become weak and it will become difficult to assume a good zoom disposition and it will also become difficult to well balance the fluctuations of various aberrations during vari-focusing. If conversely, the lower limit of conditional expression (3) is exceeded, the space necessary for focusing can be sufficiently secured, but the full length will become great, and this is not preferable. If the increase in the full length is suppressed, the refractive power of the first lens group will become strong and it will become difficult to assume a preferable zoom disposition and it will also become difficult to well balance the fluctuations of various aberrations during vari-focusing. Embodiments of the present invention will hereinafter be described with reference to the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 shows the lens construction of a first embodiment of the zoom lens of the present invention. Figure 2 shows the lens construction of a second embodiment of the zoom lens of the present invention. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Figure 1 shows the lens construction of a first embodiment. The zoom lens of the first embodiment comprises, in succession from the object side, a first lens group G1 comprising a negative meniscus lens having its convex surface facing the object side, a biconcave lens, a biconvex lens and a positive meniscus lens having its convex surface facing the object side, and having negative refractive power as a whole, a second lens group G2 comprising a front group (hereinafter referred to as the focusing group G2F) comprising a cemented lens, and a rear group G2R comprising a positive meniscus lens having its convex surface facing the object side, and having positive refractive power as a whole, a stop S, a third lens group G3 comprising a cemented lens, and a fourth lens group G4 comprising a positive meniscus lens having its convex surface facing the object side, a negative meniscus lens having its convex surface facing the object side, a biconvex lens and a cemented lens. Figure 2 shows the lens construction of a second embodiment. The zoom lens of the second embodiment comprises, in succession from the object side, a first lens group G1 comprising a cemented lens and a positive meniscus lens having its convex surface facing the object side, and having positive refractive power as a whole, a second lens group G2 comprising a front group (hereinafter referred to as the focusing group G2F) comprising a cemented lens, and a rear group G2R comprising a cemented lens and a biconcave lens, and having negative refractive power as a whole, a third lens group G3 comprising a positive meniscus lens having its concave surface facing the object side and a cemented lens, and a fourth lens group G4 comprising a positive meniscus lens having its convex surface facing the object side, a positive meniscus lens having its convex surface facing the object side, a negative meniscus lens having its convex surface facing the object side, a biconvex lens and a negative meniscus lens having its concave surface facing the object side. From each embodiment, it is seen that the arrangement of the refractive powers of the first lens group G1 and the second lens group G2 may be negative and positive, or positive and negative. The numerical data of the respective embodiments of the present invention will be shown in Tables 1 and 2 below. In these tables, the numbers at the left end represent the order from the object side, r represents the radius of curvature of each lens surface, d represents the spacing between adjacent lens surfaces, the refractive index n and Abbe number ν are values for d-line (λ = 587.6 nm). FN represents F number, 2ω represents the angle of view, d 0 represents the distance from the object to the lens surface which is most adjacent to the object side, Bf represents the back focal length, and β is a value for the photographing magnification. Also, the shape of the aspherical surface is expressed by the following equation: where h : the height from the optical axis; X(h) : the distance in the direction of the optical axis to the tangential plane of the aspherical surface at the height h from the optical axis; r : the paraxial radius of curvature; k : cone constant; C 2i : the 2ith order aspherical surface coefficient. (Numerical Data of First Embodiment) f = 20.5 - 34.0, FN = 2.89, 2ω = 95.2° - 64.6° r d ν n 1 49.529 2.50 49.4 1.77279 2 19.409 13.00 3 -82.454 2.00 47.5 1.78797 4 38.992 2.80 5 153.969 4.00 31.6 1.75692 6 -153.969 0.20 7 34.815 3.50 31.6 1.75692 8 51.692 (d8 = variable) 9 43.020 1.20 29.5 1.71736 10 22.359 5.50 69.9 1.51860 11 -56.755 (d11 = variable) 12 48.361 3.00 53.9 1.71300 13 436.187 (d13 = variable) 14 -63.760 1.20 52.3 1.74810 15 22.250 4.00 25.4 1.80518 16 76.693 (d16 = variable) 17 28.759 3.00 50.8 1.65844 18 68.431 1.50 19 67.908 2.00 26.1 1.78470 20 27.642 2.50 21 2058.323 4.00 45.4 1.79668 22 -50.144 0.20 23 105.997 8.00 57.0 1.62280 24 -20.350 1.70 23.0 1.86074 25 -44.631 (Bf = variable) (variable spacing for vari-focusing) f 20.5000 28.0000 34.0000 d 0 ∞ ∞ ∞ d 8 17.8289 6.3818 1.5051 d 11 3.3045 3.3045 3.3045 d 13 3.5982 8.1846 11.7305 d 16 9.1470 4.5606 1.0148 Bf 38.5995 45.1515 50.2170 β -0.0518 -0.0703 -0.0857 d 0 361.7220 366.6170 366.4282 d 8 19.8364 8.3602 3.5272 d 11 1.2969 1.3261 1.2824 d 13 3.5982 8.1846 11.7305 d 16 9.1470 4.5606 1.0148 Bf 38.5995 45.1515 50.2170 (the aspherical surface coefficient of the first surface) cone constant : k = 0.1000 x 10 aspherical surface constant : C 2 = 0.0000 C 4 = 0.4780 x 10 -5 C 6 = 0.4468 x 10 -8 C 8 = -0.7609 x 10 -11 C 10 = 0.1215 x 10 -13 (condition-corresponding numerical values) (1) |β F | Min = 5.859 (3) f 1 (f 1 + d F,R )/(d F,R x f T ) = 7.796 (Numerical Data of Second Embodiment) f = 82.0 - 196.0, FN = 2.89, 2ω = 30.1° - 12.2° r d ν n 1 102.933 3.00 25.4 1.80518 2 72.817 10.30 82.6 1.49782 3 -1208.506 0.20 4 107.315 7.20 82.6 1.49782 5 1107.838 (d5 = variable) 6 -427.809 3.90 35.7 1.62588 7 -82.554 1.60 60.1 1.62041 8 63.036 (d8 = variable) 9 -120.975 1.50 64.1 1.51680 10 38.555 4.50 25.5 1.80458 11 129.984 3.50 12 -94.774 1.60 53.9 1.71300 13 122.725 (d13 = variable) 14 -496.023 4.50 60.3 1.51835 15 -57.366 0.20 16 78.171 8.50 60.7 1.56384 17 -50.040 1.70 31.6 1.75692 18 -1381.323 (d18 = variable) 19 42.137 6.00 82.6 1.49782 20 155.005 0.22 21 32.919 6.00 59.7 1.53996 22 41.016 1.00 23 39.546 3.27 25.5 1.80458 24 27.620 21.95 25 115.322 6.00 40.3 1.60717 26 -46.951 2.63 27 -33.211 3.27 45.0 1.74400 28 -139.379 (Bf = variable) (variable spacing for vari-focusing) f 81.9953 134.9969 195.9952 d 0 ∞ ∞ ∞ d 5 3.1983 28.3818 40.5070 d 8 16.6627 16.6627 16.6627 d 13 24.5540 14.8062 3.5877 d 18 18.5793 3.1436 2.2369 Bf 59.4549 59.4548 59.4546 β -0.0507 -0.0809 -0.1157 d 0 1775.0088 1775.0089 1775.0091 d 5 12.8409 37.6425 50.1466 d 8 7.0201 7.4020 7.0231 d 13 24.5540 14.8062 3.5877 d 18 18.5793 3.1436 2.2369 Bf 59.4549 59.4548 59.4546 (condition-corresponding numerical values) (1) |β F | Min = 4.688 (3) f 1 (f 1 + d F,R )/(d F,R x f T ) = 5.300 From each embodiment, it is apparent that the focusing group G2F is compact and the amount of movement of the focusing group G2F at the same photographing distance is substantially constant irrespective of each vari-focused position.

Claims: A zoom lens, including, as seen from the object side in the indicated order: a first lens group (G1), a second lens group (G2) including a first sub-group (G2F) near to said first lens group (G1) and a second sub-group (G2R) far from said first lens group (G1), a third lens group (G3) which is movable upon zooming, disposed on the image side of the second lens group (G2) and a fourth lens group (G4); and further comprising cam means for driving the lens groups (G1, G2, G3); wherein an air gap between said first lens group (G1) and said second lens group (G2) is varied when zooming is effected; and wherein said cam means are adapted to move at least the second and the third lens groups (G2, G3) with respect to the image plane to effect zooming, and the first and the fourth lens groups (G1, G4) are also moved by said cam means if the first lens group (G1) has negative refractive power; characterized in that said first lens group (G1) and said first sub-group (G2F) in said second lens group (G2) together form a substantially afocal system in at least a portion of a zooming range and only said first sub-group (G2F) in said second lens group (G2) is moved with respect to the image plane along the optical axis to effect focusing. A zoom lens according to Claim 1, satisfying the following condition in the whole of the zooming range: |β F | > 1.8, where |β F | represents the absolute value of the lateral magnification β F of the first sub-group (G2F) in said second lens group (G2) in an infinity state. A zoom lens according to Claim 2, satisfying the following condition in the whole of the zooming range: |β F | > 3.3. A zoom lens according to Claim 3, satisfying the following condition: 4 < f 1 (f 1 + d F,R )/(d F,R x f T ) < 15, where d F,R : the spacing between the first sub-group (G2F) and the second sub-group (G2R) in the second lens group (G2) during an infinity state; fl: the focal length of the first lens group (G1); fT: the focal length of the entire optical system at the telephoto end.

Inventors: NAKATSUJI MASAHIRO, TATSUNO WATARU, NAKATSUJI, MASAHIRO, TATSUNO, WATARU
Applicants: NIPPON KOGAKU KK, NIKON CORPORATION
Application year: 1992
Main classification: G02B15
IPC codes: G02B15, G02B13