JP3144192B2 - Zoom lens - Google Patents

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a small zoom lens having a high zoom ratio and a wide angle of view suitable for a lens shutter camera, a video camera, and the like. The present invention relates to a zoom lens which is excellent in portability and has a reduced length (distance from one lens surface to an image surface).

[0002]

2. Description of the Related Art Recently, in a lens shutter camera, a video camera, and the like, a small zoom lens having a short overall lens length has been demanded with the downsizing of the camera. In particular, lens shutter cameras are becoming smaller and smaller due to the development of peripheral technology such as electric circuits for driving the zoom, and the photographic lenses provided with them are also required to have high zoom ratios and compact zoom lenses. I have.

Conventionally, as a zoom lens for a lens shutter, a so-called two-group zoom lens comprising two lens groups having positive and negative refractive powers has been mainly used. Since the two-unit zoom lens has a simple lens configuration and a moving mechanism at the time of zooming, it has advantages such as downsizing of the camera and relatively low cost. However, since the zooming operation must be performed by only one lens group, the zooming ratio is about 1.6 to 2 times. Forcibly increasing the zooming ratio requires an increase in the size of the lens system. At the same time, it becomes difficult to maintain high optical performance.

On the basis of a two-unit zoom lens, the first unit is divided into two lens units having a positive refractive power.
A three-unit zoom lens which aims at high zoom ratio as a three-unit configuration having positive and negative refractive powers is disclosed in, for example, JP-A-3-282409, JP-A-4-37810, and JP-A-4-7651.
No. 1 publication and the like.

However, if an attempt is made to achieve a wide-angle zoom lens system having a half-angle of view of 35 ° or more with this lens group configuration, the change in the position of the entrance pupil during zooming becomes large. For this reason, it is very difficult to suppress aberration fluctuations due to zooming when achieving high zooming.

In addition, a zoom lens having a wide angle of view and a high zoom ratio by increasing the half angle of view at the wide angle end to about 38 ° and the zoom ratio by about 3.5 times by grouping a plurality of lenses is known, for example. Kaihei 2-
No. 72316 and Japanese Patent Application Laid-Open No. 3-249614. However, these zoom lens systems both have a large front lens diameter and a large overall lens length, and are not always sufficient as a photographing lens of a compact camera.

In particular, when applied to a camera using an external finder, there is a problem that the lens barrel covers the field of view of the finder at the wide angle end. In addition, as a result, there arises a problem that the arrangement of the viewfinder and the form of the camera are restricted.

[0008]

Generally, in a zoom lens, if the refractive power of each lens unit is increased, the amount of movement of each lens unit for obtaining a predetermined zoom ratio is reduced, and the overall length of the lens is reduced. High magnification can be achieved. However, if the refractive power of each lens group is simply increased, the aberration variation accompanying zooming increases, and it is necessary to obtain good optical performance over the entire zoom range, especially when aiming for high zooming and a wide angle of view. There is a problem that it becomes difficult.

The present invention comprises five lens groups as a whole, and appropriately sets the moving conditions, refractive power and the like of each lens group during zooming, so that the angle of view at the wide-angle end is about 64 to 74 °,
It is an object of the present invention to provide a zoom lens having high optical performance over the entire zoom range with a zoom ratio of about 3.5.

[0010]

A zoom lens according to the present invention has a first group of negative refractive power and a second group of positive refractive power in order from the object side.
At the wide-angle end, the combined lens unit includes a front lens unit having a positive refractive power, a fourth lens unit having a positive refractive power, and a fifth lens unit having a negative refractive power. And a rear group consisting of two lens groups. In zooming from the wide-angle end to the telephoto end, the first, second, and third groups have a combined refracting power of the front group that is longer than that of the wide-angle end. The fourth and fifth lens units move so as to be weaker at the end, and the distances between the fourth and fifth lens units are reduced. The focal length of the i-th lens unit is fi, the focal length of the entire system at the wide-angle end is fW, The lateral magnification at the wide-angle end of the i-th lens unit is βiW, the combined refractive power of the front unit at the wide-angle end and the telephoto end is φ _123W ,
_Assuming that φ _123T and the zoom ratio are Z, 0.4 <| f5 / fW | <1.5 (1) 1.1 <β5W <1.9 (...) (2) 0.8 <| f1 / fW | <5.0 (5) 0.7 <f2 / fW <6.0 (6) 0.15 <( _Φ123W / _φ123T ) / Z <0.8 (7) 0.25 <β4W <1.2 (8) 0.1 <f5 · (1−β5W) /FW<0.7 (9) The following condition is satisfied.

[0011]

FIG. 1 is an explanatory view of a paraxial refractive power arrangement of zoom lenses according to embodiments 1 to 4 of the present invention. FIG. 2 is an explanatory diagram of a paraxial refractive power arrangement of zoom lenses according to Examples 5 to 7 of the present invention. 1 and 2, (A) is a wide-angle end,
(B) shows the telephoto end. 3 to 9 are lens cross-sectional views at the wide-angle end of Numerical Examples 1 to 7 of the present invention, respectively. 10 to 30 are graphs showing various aberrations of Numerical Examples 1 to 7 of the present invention.

In the drawing, LF denotes a front group having a positive refractive power, LR denotes a rear group, SP denotes an aperture, and IP denotes an image plane. Li (i = 1 to
5) is the i-th group. Arrows indicate the moving direction of each lens group when zooming from the wide-angle side to the telephoto side.

The front unit LF includes three lens units, a first unit L1, a second unit L2, and a third unit L3. The combined refractive power at the wide-angle end is positive. The rear unit LR includes two lens units, a fourth unit L4 having a positive refractive power and a fifth unit L5 having a negative refractive power.

At the time of zooming from the wide-angle end to the telephoto end, each of the first, second, and third units moves toward the object side with the second unit changing the relative positional relationship with the other lens units. The combined power of the front group moves so as to be weaker at the telephoto end than at the wide-angle end. In addition, the fourth and fifth units are moved toward the object side so that the distance between them is reduced. At this time, Examples 1 to
In 4, the distance between the third lens unit and the fourth lens unit is set to be larger at the telephoto end than at the wide-angle end. Thereby, the combined system of the third group and the fourth group, when viewed as an independent system, is multiplied with magnification.

On the other hand, in Examples 5 to 7, since the refractive power of the fourth lens unit is relatively weak, the fourth unit has an arbitrary moving trajectory during zooming so as to perform good aberration correction over the entire zooming range. It is good to do so. In Examples 5 to 7, the distance between the third lens unit and the fourth lens unit is made smaller at the telephoto end than at the wide-angle end in order to advantageously reduce the overall length of the lens at the telephoto end.

In the present invention, at the wide-angle end, a second lens unit having a positive refractive power and a third lens unit having a positive refractive power are arranged at a wide distance from the first lens unit having a negative refractive power. The focus type is set. As a result, the front principal point of the front group is located on the image plane side, and it is easy to widen the angle of view while preventing interference between the lens surfaces of the front group and the rear group. By making both the second and third units positive in refractive power, the strong positive refractive power of the retrofocus type in the front unit at the wide-angle end is shared by the second and third units, and a wide image is obtained. Easy keratinization. Then, the fourth lens unit is moved toward the object side to focus from an object at infinity to an object at a short distance.

In the zoom lens of the present invention, the focal length f of the whole lens system is expressed by the following equation.

F = fA · β4 · β5 (β4> 0, β5> 0) (a) where fA represents the composite focal length of the front group, and βi represents the lateral magnification of the i-th group. .

In the present invention, as can be understood from the equation (a), at the time of zooming from the wide-angle end to the telephoto end, the values of the lateral magnifications β4 and β5 are increased and, at the same time, the combined focal length fA of the front group is increased. By reducing the combined refracting power of the front group, a more efficient zooming effect is achieved. Also, the distance between the fourth lens unit having a positive refractive power and the fifth lens unit having a negative refractive power is made narrower (decreased) at the telephoto end than at the wide-angle end, thereby giving a zooming effect to the fifth lens unit. It facilitates high magnification. Also, the rear lens unit forms a telephoto type (telephoto type) together with the front lens unit having a positive refractive power by increasing the divergent (negative) refractive power at the telephoto end to reduce the size of the entire lens system. I have.

In particular, in the present invention, a paraxial refractive power arrangement as shown in FIG. 1 is employed to widen the photographing angle of view such that the focal length at the wide angle end becomes smaller than the screen diagonal length.

Specifically, the front group is a first group having a negative refractive power,
The second lens unit includes a second lens unit having a positive refractive power and a third lens unit having a positive refractive power.
Each lens group is moved such that the distance between the groups decreases and the distance between the second and third groups increases.

In the first to fourth embodiments of the present invention, the first and third units are moved integrally for simplification of the mechanism, but they may be moved independently. According to this, the degree of freedom of design can be increased.

In the present invention, in the above-described lens configuration, the above-mentioned conditional expressions (1), (2) and (5) to (9) are satisfied. This achieves high optical performance over the entire zoom range while further miniaturizing the entire lens system.

Next, the technical meaning of each of the above conditional expressions will be described.

The conditional expression (1) is mainly for effectively changing the magnification with respect to the negative refractive power of the fifth lens unit. If the negative refractive power of the fifth lens unit becomes weaker beyond the upper limit of conditional expression (1), the zooming effect of the lens unit becomes weaker during zooming, so that a constant zoom ratio is obtained. For this purpose, the amount of movement of each lens group must be increased, and the overall length of the lens increases.

If the lower limit of conditional expression (1) is exceeded, the combined refractive power of the first to fourth units is positive and the refractive power of the fifth unit is negative at the wide-angle end. The effect as a telephoto type will be too strong.

As a result, the back focus of the lens system becomes too short, which leads to an increase in the outer diameter of the lens of the fifth group in order to secure a constant peripheral light amount, and at the same time, the refractive power of the lens group becomes strong. Too much distortion causes higher-order field curvature and astigmatism, which makes it difficult to correct them.

Conditional expression (2) relates to the lateral magnification of the fifth lens unit at the wide-angle end.

Assuming that the back focus of the lens system at the wide-angle end is BfW, the following expression can be obtained: BfW = f5 · (1−β5W).

Therefore, in the present invention, the total length of the lens system and various aberrations are corrected in a well-balanced manner by appropriately setting the values of conditional expression (2) together with conditional expression (1).

When the imaging magnification is increased beyond the upper limit of the conditional expression (2), the back focus becomes longer, but the first to fourth focal lengths are increased.
The refracting power of the group becomes too strong, and the aberration variation increases. On the other hand, if the imaging magnification becomes smaller than the lower limit, it becomes difficult to obtain a predetermined back focus.
It is not good because the outer diameter of the lens of the group increases. Conditional expression (5) relates to the ratio between the refractive power of the first lens unit and that of the first lens unit at the wide-angle end.
The refractive power of the group becomes too weak, and the overall length of the lens increases. If the lower limit value is exceeded, the refractive power of the first lens unit becomes strong, so that it becomes difficult to secure a predetermined back focus at the wide-angle end. Conditional expression (6) relates to the ratio of the refractive power of the whole lens system to the second lens unit at the wide-angle end. In this case, the movement amount of the lens group becomes large, which leads to an increase in the lens system. If the lower limit is exceeded, the refractive power of the second lens unit becomes too strong, and the refractive power of the third lens unit also becomes strong, making it difficult to correct spherical aberration. Conditional expression (7) relates to the zoom ratio of the front group.
If the upper limit of conditional expression (7) is exceeded, the magnification change in the front group becomes too large, the refractive power of the lens group in the front group becomes strong, and the movement amount of each lens group during zooming increases. Come. On the other hand, if the lower limit value is exceeded, the variable power allocation in the rear lens unit becomes too large, and the amount of movement of each lens unit in the rear lens unit to secure a predetermined zoom ratio is not good. Conditional expression (8) relates to the lateral magnification of the fourth lens unit at the wide-angle end. When the value exceeds the upper limit of conditional expression (8), it becomes difficult to obtain a back focus at the wide-angle end, which results in an increase in the outer diameter of the fifth lens unit. If the lower limit value is exceeded, the refractive power of the other lens units will increase in order to obtain a constant focal length, making it difficult to correct aberration fluctuations during zooming. Further, the focal length of the front group must be made longer, which is not good because the overall length of the lens becomes longer. Conditional expression (9) is for appropriately setting the refractive power and the lateral magnification of the fifth lens unit and mainly for obtaining a predetermined back focus. When the value exceeds the upper limit of conditional expression (9), the back focus becomes unnecessarily long at the wide-angle end, and the overall length of the lens increases. On the other hand, if the lower limit is exceeded, it becomes difficult to obtain a predetermined back focus at the wide-angle end, and the outer shape of the fifth lens unit increases, which is not good.

In the present invention, in order to widen the angle of view while minimizing aberration fluctuations due to zooming, and to ensure high optical performance over the entire screen, it is preferable to configure each lens unit as follows.

(1) _Assuming that the combined refractive power of the front unit at the wide-angle end is _φ123W , 0.3 <fW · _φ123W <1.8 (3) 0.6 <f3 / fW <2.5 It is preferable that the following condition is satisfied.

Conditional expression (3) relates to the refractive power of the front lens group. When the value exceeds the upper limit of conditional expression (3), the refractive power of the front lens group becomes too strong at the wide-angle end, and the effect of the telephoto system becomes strong. It is difficult to obtain the back focus. or,
Exceeding the lower limit lowers the refractive power of the front group and increases the overall length of the lens.At the same time, the positive refractive power of the rear group must be increased to maintain the focal length at the wide-angle end. It becomes difficult to balance various aberrations.

Conditional expression (4) relates to the positive refractive power of the third lens unit.
Since the refracting power of the group is weak, the amount of movement of the lens group at the time of zooming is large, which leads to an increase in the lens system. If the lower limit is exceeded, high-order spherical aberration is strongly generated in the third lens unit, and it becomes difficult to correct this.

In the present invention, the upper and lower limits of the above-mentioned conditional expressions (3) and (4) must be satisfied in order to satisfactorily correct the optical performance while reducing the overall length of the lens particularly at the wide-angle end. 0.4 <fW · _φ123W <1.5 (3a) 0.9 <f3 / fW <2.0 (4a) Is good.

[0037]

[0038]

[0039]

[0040]

[0041]

[0042]

(2) In particular, when the refractive power of the third and fourth units is relatively strong, the lateral magnification β4W of the fourth unit is obtained.
However, when the value range of 0.25 <β4W <0.6 is satisfied, it is desirable that conditional expressions (3) and (6) be within the following numerical range in order to achieve a small and favorable optical system.

0.3 <fW · _φ123W / <0.9 (3b) 1.8 ≦ f2 / fW <6.0 (6b) When the refractive power of the third lens unit is relatively strong and the refractive power of the fourth lens unit is relatively weak, the lateral magnification β4
When W takes a value range of 0.6 ≦ β4W <1.2, it is desirable that conditional expressions (3) and (6) be within the following numerical ranges in order to achieve a small and favorable optical system.

0.9 ≦ fW · φ _123W <1.8 (3c) 0.7 <f2 / fW <1.8 (6c) (3) Negative Has a positive lens and a negative lens at least one by one, and the lens surface on the image side of the negative lens preferably has a lens configuration with the concave surface facing the image side. .

(4) When an aspherical surface is introduced into the zoom lens of the present invention, the positive refractive power decreases (the negative refractive power increases) as the distance from the optical axis increases, as the distance from the optical axis increases, on the lens surface closer to the object than the stop. If an aspherical surface is used, it is possible to easily correct the curvature of field and spherical aberration at the telephoto end, aberration fluctuations due to zooming, and aberration correction of the entire screen. In addition, if it is introduced into the fifth lens group, mainly off-axis aberration can be favorably corrected.

(5) The fifth group having a negative refractive power has at least 1
When there are a negative lens and a positive lens each having a concave surface facing the object side for each sheet, and the average values of Abbe numbers of the materials of the positive lens and the negative lens in the fifth group are ν5P and ν5N, respectively, 12 <ν5N −ν5P <35 (10) It is preferable to satisfy the following condition. If the upper limit or the lower limit of conditional expression (10) is not satisfied, chromatic aberration fluctuations during zooming often occur, and it becomes difficult to correct this with another lens group.

(6) The aperture should be placed in an air gap existing between the lens surface closest to the image plane of the second lens unit and the lens surface closest to the image surface of the fourth lens unit so that the entrance pupil is located at an appropriate position. Are preferable because aberration fluctuation due to zooming can be suppressed. The stop may be moved independently of the other lens groups when zooming, or may be moved integrally with the other lens groups. This makes it possible to arrange the stop position near the entrance pupil position that moves during zooming, which is advantageous for preventing a change in field curvature aberration at the time of a small stop.

When focusing is performed, if the focus group includes an aperture, moving the focus group with the aperture fixed on the optical axis reduces the driving torque for moving the aperture mechanism during focusing. It is preferable because it can be used.

(7) If the focus group is divided into two or more lens groups and the distance between the lens groups is changed at the time of focusing, aberration variation during zooming and focusing can be reduced. preferable.

(8) In the first to fourth embodiments of the present invention, the focus is moved by moving the fourth unit to the object side, and the focus in the fifth to seventh embodiments is moved by moving the third and fourth units together toward the object side. Although focusing is performed from an object at infinity to an object at a short distance, it may be performed by moving another lens group. For example, a method of moving the front group to the object side may be used.

When the back focus is sufficient at the wide-angle end, the fifth unit may be moved to the image plane side, and in this case, it is effective to reduce the outer diameter of the lens of the first unit. Becomes Alternatively, two or more lens groups in the first to fifth groups may be simultaneously moved.

Next, numerical examples of the present invention will be described. In the numerical examples, Ri is the radius of curvature of the i-th lens surface in order from the object side, Di is the i-th lens thickness and air spacing from the object side, and Ni and νi are the i-th lens surfaces in order from the object side. The refractive index and Abbe number of glass.

Table 1 shows the relationship between the above-mentioned conditional expressions and various numerical values in the numerical examples.

The aspherical shape has an X axis in the optical axis direction, an H axis in a direction perpendicular to the optical axis, a positive traveling direction of light, R is a paraxial radius of curvature,
When A, B, C, D, and E are aspheric coefficients, respectively,

[0056]

(Equation 1) It is represented by the following equation.

(Numerical Example 1) F = 29.25 to 101.00 fNO = 1: 3.6 to 8.2 2ω = 73.0 ° to 24.2 ° R 1 = -136.48 D 1 = 1.30 N 1 = 1.80400 ν 1 = 46.6 R 2 = 44.39 D 2 = 0.41 R 3 = 53.68 D 3 = 3.00 N 2 = 1.80518 ν 2 = 25.4 R 4 = -226.68 D 4 = 1.10 N 3 = 1.66998 ν 3 = 39.3 R 5 = 35.15 D 5 = Variable R 6 = 36.05 D 6 = 1.00 N 4 = 1.84666 ν 4 = 23.8 R 7 = 22.91 D 7 = 2.70 N 5 = 1.48749 ν 5 = 70.2 R 8 = -148.68 D 8 = Variable R 9 = 29.98 D 9 = 2.80 N 6 = 1.56873 ν 6 = 63.2 R10 = -61.97 D10 = Variable R11 = -20.25 D11 = 0.87 N 7 = 1.64769 ν 7 = 33.8 R12 = -96.09 D12 = 1.00 R13 = ∞ (Aperture) D13 = 1.00 R14 = -49.89 D14 = 0.78 N 8 = 1.48749 ν 8 = 70.2 R15 = 41.40 D15 = 2.10 N 9 = 1.84666 ν 9 = 23.8 R16 = -42.55 D16 = 5.60 R17 = 31.32 D17 = 1.10 N10 = 1.84666 ν10 = 23.8 R18 = 12.25 D18 = 5.50 N11 = 1.58313 ν11 = 59.4 R19 = -25.47 D19 = variable R20 = -31.70 D20 = 3.50 N12 = 1.84666 ν12 = 23.8 R21 = -17.94 D21 = 0.20 R22 = -22.10 D22 = 1.30 N13 = 1.80610 ν13 = 41.0 R23 = -317.84 D23 = 4.89 R24 = -18.10 D24 = 1.50 N14 = 1.78590 ν14 = 44.2 R25 = -63.65 aspheric coefficients R19 K = -1.81 × 10 ^{- 1} A = 0 B = 8.60 × 10 ^-6 C = 9.07 × 10 ^-8 D = -1.91 × 10 ^-9 E = 0

[0058]

[Table 1] (Numerical Example 2) F = 28.84 to 101.48 fNO = 1: 3.6 to 8.2 2ω = 73.8 ° to 24.1 ° R 1 = -107.63 D 1 = 1.30 N 1 = 1.80400 ν 1 = 46.6 R 2 = 29.11 D 2 = 3.50 N 2 = 1.80518 ν 2 = 25.4 R 3 = 188.37 D 3 = 0.38 R 4 = 248.08 D 4 = 1.10 N 3 = 1.60342 ν 3 = 38.0 R 5 = 33.55 D 5 = Variable R 6 = 33.40 D 6 = 1.00 N 4 = 1.84666 ν 4 = 23.8 R 7 = 19.67 D 7 = 2.70 N 5 = 1.48749 ν 5 = 70.2 R 8 = -176.19 D 8 = Variable R 9 = 29.75 D 9 = 2.80 N 6 = 1.56873 ν 6 = 63.2 R10 =- 53.64 D10 = variable R11 = -19.54 D11 = 0.87 N 7 = 1.64769 ν 7 = 33.8 R12 = -93.56 D12 = 1.00 R13 = ∞ (Aperture) D13 = 1.00 R14 = -57.06 D14 = 0.78 N 8 = 1.48749 ν 8 = 70.2 R15 = 36.54 D15 = 2.10 N 9 = 1.84666 ν 9 = 23.8 R16 = -45.52 D16 = 4.85 R17 = 34.65 D17 = 1.10 N10 = 1.84666 ν10 = 23.8 R18 = 12.82 D18 = 5.50 N11 = 1.58313 ν11 = 59.4 R19 = -23.25 D19 = Variable R20 = -33.52 D20 = 3.00 N12 = 1.84666 ν12 = 23.8 R21 = -17.94 D21 = 0.15 R22 = -20.79 D22 = 1.30 N13 = 1.83481 ν13 = 42.7 R23 = -171.17 D23 = 4.39 R24 = -17.91 D24 = 1.50 N14 = 1.78590 ν14 = 44.2 R25 = -73.32 Aspheric coefficient R19 K = -3.37 × 10 ^-1 A = 0 B = 1.15 × 10 ^-5 C = -2.60 × 10 ^-8 D = -2.60 × 10 ^-10 E = 0

[0059]

[Table 2] (Numerical Example 3) F = 35.00 to 110.12 fNO = 1: 3.7 to 8.2 2ω = 63.4 ° to 22.2 ° R 1 = -209.03 D 1 = 1.30 N 1 = 1.80400 ν 1 = 46.6 R 2 = 127.91 D 2 = 0.41 R 3 = 143.81 D 3 = 3.00 N 2 = 1.80518 ν 2 = 25.4 R 4 = -90.07 D 4 = 1.10 N 3 = 1.66998 ν 3 = 39.3 R 5 = 50.47 D 5 = Variable R 6 = 36.53 D 6 = 1.00 N 4 = 1.84666 ν 4 = 23.8 R 7 = 25.31 D 7 = 3.80 N 5 = 1.48749 ν 5 = 70.2 R 8 = -1105.62 D 8 = Variable R 9 = 36.04 D 9 = 3.20 N 6 = 1.56873 ν 6 = 63.2 R10 = -160.41 D10 = variable R11 = ∞ (aperture) D11 = 1.30 R12 = -21.36 D12 = 0.87 N 7 = 1.64769 ν 7 = 33.8 R13 = -289.38 D13 = 2.00 R14 = -78.97 D14 = 0.78 N 8 = 1.48749 ν 8 = 70.2 R15 = 46.97 D15 = 2.10 N 9 = 1.84666 ν 9 = 23.8 R16 = -48.67 D16 = 5.60 R17 = 32.95 D17 = 1.10 N10 = 1.84666 ν10 = 23.8 R18 = 14.36 D18 = 5.50 N11 = 1.58313 ν11 = 59.4 R19 = -27.03 D19 = variable R20 = -30.81 D20 = 3.50 N12 = 1.84666 ν12 = 23.8 R21 = -19.27 D21 = 0.20 R22 = -30.53 D22 = 1.30 N13 = 1.80610 ν13 = 41.0 R23 = -115.65 D23 = 4.89 R24 = -18.03 D24 = 1.50 N14 = 1.78590 ν14 = 44.2 R25 = -118.71 aspheric coefficients ^{R19 K = 3.77 × 10 -1 A} = 0 B = 1.57 ^{10 -5 C = 3.17 × 10 -8} D = -8.36 × 10 -10 E = 0

[0060]

[Table 3] (Numerical Example 4) F = 35.00-110.00 fNO = 1: 3.7-8.2 2ω = 63.4 ° -22.3 ° R 1 = -112.16 D 1 = 1.30 N 1 = 1.80400 ν 1 = 46.6 R 2 = 139.61 D 2 = 0.41 R 3 = 163.84 D 3 = 3.00 N 2 = 1.80518 ν 2 = 25.4 R 4 = -107.84 D 4 = 1.10 N 3 = 1.66998 ν 3 = 39.3 R 5 = 76.56 D 5 = variable R 6 = 36.05 D 6 = 1.00 N 4 = 1.84666 ν 4 = 23.8 R 7 = 25.55 D 7 = 3.80 N 5 = 1.48749 ν 5 = 70.2 R 8 = -389.95 D 8 = Variable R 9 = 45.54 D 9 = 3.20 N 6 = 1.56873 ν 6 = 63.2 R10 = -160.77 D10 = Variable R11 = ∞ (Aperture) D11 = 1.30 R12 = -20.88 D12 = 0.87 N 7 = 1.64769 ν 7 = 33.8 R13 = -233.98 D13 = 2.00 R14 = -159.29 D14 = 0.78 N 8 = 1.48749 ν 8 = 70.2 R15 = 46.64 D15 = 2.10 N 9 = 1.84666 ν 9 = 23.8 R16 = -49.54 D16 = 5.60 R17 = 35.02 D17 = 1.10 N10 = 1.84666 ν10 = 23.8 R18 = 14.70 D18 = 5.50 N11 = 1.58313 ν11 = 59.4 R19 = -28.48 D19 = variable R20 = -19.90 D20 = 3.50 N12 = 1.84666 ν12 = 23.8 R21 = -17.24 D21 = 4.50 R22 = -16.95 D22 = 1.50 N13 = 1.77250 ν13 = 49.6 R23 = 483.96 Aspheric coefficient R19 K = 8.88 × 10 ^-1 A = 0 B = 1.21 × 10 ^-5 C = 1.06 × 10 ^-7 D = -1.47 × 10 ^-9 E = 0 Aspheric coefficient R22 K = 0 A = 0 B = 8.13 × 10 ^-6 C = 2.25 × 10 ^-8 D = -1.09 × 10 ^-11 E = 0

[0061]

[Table 4] (Numerical Example 5) F = 28.8-10.96 fNO = 1: 4.30-9.00 2ω = 73.8 ° -24.0 ° R 1 = -4116.96 D 1 = 2.60 N 1 = 1.51741 ν 1 = 52.4 R 2 = -51.61 D 2 = 0.88 R 3 = -32.32 D 3 = 1.20 N 2 = 1.77249 ν 2 = 49.6 R 4 = 28.95 D 4 = 2.80 N 3 = 1.84665 ν 3 = 23.8 R 5 = 265.48 D 5 = variable R 6 = 18.85 D 6 = 1.00 N 4 = 1.84665 ν 4 = 23.8 R 7 = 13.87 D 7 = 4.00 N 5 = 1.48749 ν 5 = 70.2 R 8 = -21.28 D 8 = 1.00 N 6 = 1.84665 ν 6 = 23.8 R 9 = -27.55 D 9 = Variable R10 = ∞ (aperture) D10 = 3.00 R11 = -25.23 D11 = 1.36 N 7 = 1.80518 ν 7 = 25.4 R12 = -47.39 D12 = 0.14 R13 = -36.10 D13 = 6.85 N 8 = 1.67790 ν 8 = 55.3 R14 = -12.22 D14 = variable R15 = -19.48 D15 = 2.50 N 9 = 1.58312 ν 9 = 59.4 R16 = -16.04 D16 = variable R17 = -32.40 D17 = 3.00 N10 = 1.76181 ν10 = 26.6 R18 = -18.03 D18 = 0.17 R19 = -25.42 D19 = 1.30 N11 = 1.69679 ν11 = 55.5 R20 = -921.97 D20 = 4.59 R21 = -14.26 D21 = 1.50 N12 = 1.71299 ν12 = 53.8 R22 = 190.18 Aspherical coefficient R11 K = 4.91 A = 0 B = -1.20 × 10 ^-4 C = -6.48 × 10 ^-7 D = -1.53 × 10 ^-8 E = 0 Aspherical surface coefficient R15 K = 1.19 A = 0 B = 2.27 × 10 ^-5 C = 1.48 × 10 ^-7 D = 1.04 × 10 ^-9 E = 0

[0062]

[Table 5] (Numerical Example 6) F = 29.11 to 101.99 fNO = 1: 4.30 to 9.00 2ω = 73.2 ° to 23.9 ° R 1 = 95.83 D 1 = 3.20 N 1 = 1.51633 ν 1 = 64.2 R 2 = -53.56 D 2 = 0.61 R 3 = -35.06 D 3 = 1.20 N 2 = 1.80400 ν 2 = 46.6 R 4 = 17.05 D 4 = 3.28 N 3 = 1.84665 ν 3 = 23.8 R 5 = 74.99 D 5 = Variable R 6 = 15.96 D 6 = 1.00 N 4 = 1.84665 ν 4 = 23.8 R 7 = 11.49 D 7 = 4.30 N 5 = 1.48749 ν 5 = 70.2 R 8 = -19.95 D 8 = 1.00 N 6 = 1.84665 ν 6 = 23.8 R 9 = -27.33 D 9 = Variable R10 = ∞ (aperture) D10 = 3.50 R11 = -24.67 D11 = 2.30 N 7 = 1.80518 ν 7 = 25.4 R12 = -46.17 D12 = 0.19 R13 = -34.22 D13 = 1.20 N 8 = 1.65159 ν 8 = 58.5 R14 = 356.16 D14 = 5.50 N 9 = 1.74319 ν 9 = 49.3 R15 = -13.76 D15 = Variable R16 = -19.38 D16 = 2.50 N10 = 1.51633 ν10 = 64.2 R17 = -15.27 D17 = Variable R18 = -31.26 D18 = 2.30 N11 = 1.84665 ν11 = 23.8 R19 = -20.72 D19 = 0.71 R20 = -24.00 D20 = 1.30 N12 = 1.69679 ν12 = 55.5 R21 = 837.91 D21 = 3.73 R22 = -21.23 D22 = 1.50 N13 = 1.77249 ν13 = 49.6 R23 = 171.78 Aspheric coefficient R11 K = 4.71 A = 0 B = -8.41 × 10 ^-5 C = -1.40 × 10 ^-7 D = -8.96 × 10 ^-9 E = 0 Aspheric coefficient R15 K = -2.63 A = 0 B = -1.15 × 10 ^-4 C = 2.26 × 10 ^-7 D = -1.31 × 10 ^-9 E = 0

[0063]

[Table 6] (Numerical Example 7) F = 28.8 to 2.40 fNO = 1: 4.30 to 9.00 2ω = 73.8 ° to 23.9 ° R 1 = -357.21 D 1 = 2.50 N 1 = 1.51741 ν 1 = 52.4 R 2 = -55.11 D 2 = 0.70 R 3 = -36.84 D 3 = 1.20 N 2 = 1.77249 ν 2 = 49.6 R 4 = 32.93 D 4 = 2.80 N 3 = 1.84666 ν 3 = 23.8 R 5 = 400.74 D 5 = Variable R 6 = 19.18 D 6 = 1.00 N 4 = 1.84666 ν 4 = 23.8 R 7 = 12.66 D 7 = 3.70 N 5 = 1.48749 ν 5 = 70.2 R 8 = -31.67 D 8 = 0.80 R 9 = ∞ (aperture) D 9 = variable R10 = -23.72 D10 = 1.00 N 6 = 1.80518 ν 6 = 25.4 R11 = -48.78 D11 = 0.18 R12 = -33.17 D12 = 7.30 N 7 = 1.65844 ν 7 = 50.9 R13 = -11.89 D13 = Variable R14 = -19.99 D14 = 2.50 N 8 = 1.58312 ν 8 = 59.4 R15 = -15.94 D15 = variable R16 = -34.31 D16 = 2.90 N 9 = 1.76182 ν 9 = 26.5 R17 = -18.06 D17 = 0.39 R18 = -26.91 D18 = 1.30 N10 = 1.83480 ν10 = 42.7 R19 = -140.63 D19 = 4.84 R20 = -13.09 D20 = 1.50 N11 = 1.71299 ν11 = 53.8 R21 = 882.45 Aspheric coefficient R10 K = 4.60 A = 0 B = -1.07 × 10 ^-4 C = -8.17 × 10 ^-7 D = -1.35 × 10 ^-8 E = 0 Aspheric coefficient R14 K = 1.27 A = 0 B = 1.56 × 10 ^-5 C = 1.44 × 10 ^-7 D = 1.18 × 10 ^-9 E = 0

[0064]

[Table 7]

[0065]

As described above, according to the present invention, the wide-angle end photographing is performed by appropriately configuring the moving conditions and the refracting power of each lens unit during zooming by forming the lens system from five lens units as a whole. It is possible to achieve a zoom lens having high optical performance over the entire zoom range with an angle of view of about 64 to 74 degrees and a zoom ratio of about 3.5.

[Brief description of the drawings]

FIG. 1 is an explanatory diagram of a paraxial refractive power arrangement of a zoom lens according to the present invention.

FIG. 2 is another explanatory diagram of the paraxial refractive power arrangement of the zoom lens of the present invention.

FIG. 3 is a sectional view of a lens at a wide angle end according to Numerical Embodiment 1 of the present invention.

FIG. 4 is a sectional view of a lens at a wide angle end according to Numerical Example 2 of the present invention.

FIG. 5 is a sectional view of a lens at a wide angle end according to Numerical Embodiment 3 of the present invention.

FIG. 6 is a sectional view of a lens at a wide-angle end according to a fourth numerical embodiment of the present invention.

FIG. 7 is a sectional view of a lens at a wide angle end according to Numerical Example 5 of the present invention.

FIG. 8 is a lens cross-sectional view at a wide angle end according to Numerical Example 6 of the present invention.

FIG. 9 is a sectional view of a lens at a wide angle end according to Numerical Example 7 of the present invention.

FIG. 10 is an aberration diagram at a wide-angle end according to Numerical Embodiment 1 of the present invention.

FIG. 11 is an intermediate aberration diagram of the numerical example 1 of the present invention.

FIG. 12 is an aberration diagram at a telephoto end in Numerical Example 1 of the present invention;

FIG. 13 is an aberration diagram at a wide angle end according to Numerical Example 2 of the present invention.

FIG. 14 is an intermediate aberration diagram of the numerical example 2 of the present invention.

FIG. 15 is an aberration diagram at a telephoto end in Numerical Example 2 of the present invention;

FIG. 16 is an aberration diagram at a wide angle end according to Numerical Example 3 of the present invention.

FIG. 17 is an intermediate aberration diagram of the numerical example 3 of the present invention.

FIG. 18 is an aberration diagram at a telephoto end in Numerical Example 3 of the present invention.

FIG. 19 is an aberration diagram at a wide angle end according to Numerical Example 4 of the present invention.

FIG. 20 is an intermediate aberration diagram of the numerical example 4 of the present invention.

FIG. 21 is an aberration diagram at a telephoto end in Numerical Example 4 of the present invention.

FIG. 22 is an aberration diagram at a wide angle end according to Numerical Example 5 of the present invention.

FIG. 23 is an intermediate aberration diagram of the numerical example 5 of the present invention.

FIG. 24 is an aberration diagram at a telephoto end in Numerical Example 5 of the present invention;

FIG. 25 is an aberration diagram at a wide angle end according to Numerical Example 6 of the present invention.

FIG. 26 is an intermediate aberration diagram of the numerical example 6 of the present invention.

FIG. 27 is an aberration diagram at a telephoto end in Numerical Example 6 of the present invention.

FIG. 28 is an aberration diagram at a wide angle end according to Numerical Example 7 of the present invention.

FIG. 29 is an intermediate aberration diagram of the numerical example 7 of the present invention.

FIG. 30 is an aberration diagram at a telephoto end in Numerical Example 7 of the present invention.

[Explanation of symbols]

 L1 First group L2 Second group L3 Third group L4 Fourth group L5 Fifth group SP Aperture IP Image plane dd line gg line S. C Sine condition ΔS Sagittal image plane ΔM Meridional image plane

──────────────────────────────────────────────────続 き Continued on the front page (58) Fields surveyed (Int. Cl. ⁷ , DB name) G02B 9/00-17/08 G02B 21/02-21/04 G02B 25/00-25/04

Claims (4)

(57) [Claims] 1. A first lens unit having a negative refractive power, a second lens unit having a positive refractive power, and a third lens unit having a positive refractive power. Has a front lens unit having a positive refractive power, a rear lens unit including a fourth lens unit having a positive refractive power, and a fifth lens unit having a negative refractive power, and when zooming from the wide-angle end to the telephoto end. The first, second, and third units move so that the combined refractive power of the front unit becomes weaker at the telephoto end than at the wide-angle end, and the fourth and fifth units move so that the distance between them decreases. do it
And the focal length of the i-th lens unit is fi
The focal length of the system is fW, and the lateral magnification at the wide-angle end of the i-th lens unit is
βiW, combined refractive power of the front group at wide-angle end and telephoto end
_Where φ _123W , φ _123T and the zoom ratio are Z, 0.4 <| f5 / fW | <1.51.1 <β5W <1.90.8 <| f1 / fW | <5.0 0.7 <f2 / fW <6.0 0.15 <( _φ123W / _φ123T ) / Z <0.8 0.25 <β4W <1.20.1 <f5 · (1-β5W) / fW A zoom lens that satisfies the condition of <0.7 . 2. In zooming from the wide-angle end to the telephoto end, each lens group moves toward the object side such that the distance between the first and second groups decreases and the distance between the second and third groups increases. The zoom lens according to claim 1, wherein 3. When the combined refractive power of the front unit at the wide-angle end is _φ123W , the following condition is satisfied: 0.3 <fW · _φ123W <1.8 0.6 <f3 / fW <2.5. The zoom lens according to claim 1, wherein: 4. The fifth group includes at least one negative lens and a positive lens each having a concave surface facing the object side, and the average value of Abbe numbers of the materials of the positive lens and the negative lens in the fifth group. The zoom lens according to claim 1, wherein, when? 5P and? 5N are respectively satisfied, a condition of 12 <? 5N-? 5P <35 is satisfied.