# Patent

## Title
Zoom lens and apparatus using the same

## Abstract

A zoom lens according to the present invention includes, in order from the object side, a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, a third lens unit having a negative refractive power, and a fourth lens unit having a positive refractive power. During a magnification change from the wide-angle end through the telephoto end, the first lens unit and the fourth lens unit shift from the image-surface side toward the object side, a space between the first lens unit and the second lens unit increases, and spaces between individual lens units change. During a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit and the third lens unit individually shift independently.

## Background
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a zoom lens used in a silver-halide camera, a digital camera, a video camera or the like.
2. Description of the Related Art
Conventionally, in a zoom lens used in a silver-halide camera, a digital camera, a video camera or the like, it is known as a method for focusing from an object at the infinite distance to an object at a near distance to shift whole or a part of one unit out of lens units that change mutual spaces during a zooming operation (For example, refer to Japanese Patent Application Preliminary Publication (KOKAI) No. Hei 3-289612 or Japanese Patent Application Preliminary Publication (KOKAI) No. Hei 3-228008).
There is a type including four units having positive-negative-negative-positive power arrangement in order from the object side and performing focusing by shifting the positive first lens unit toward the object side, as in the method shown in KOKAI No. Hei 3-289612. Also, there is another type including three lens units having positive-negative-positive power arrangement in order from the object side and performing focusing by shifting forth the negative second lens unit toward the object side as in the method shown in KOKAI No. Hei 3-228008.
SUMMARY OF THE INVENTION
A zoom lens according to the present invention includes, in order from the object side, a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, a third lens unit having a negative refractive power, and a fourth lens unit having a positive refractive power, wherein, during a magnification change from the wide-angle end through the telephoto end, the first lens unit and the fourth lens unit shift from the image-surface side toward the object side, a space between the first lens unit and the second lens unit increases, and spaces between individual lens units change, and wherein, during a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit and the third lens unit individually shift independently.
Also, a zoom lens according to the present invention includes, in order from the object side, a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, a third lens unit having a negative refractive power, and a fourth lens unit having a positive refractive power, wherein, during a magnification change from the wide-angle end through the telephoto end, the first lens unit and the fourth lens unit shift from the image-surface side toward the object side, a space between the first lens unit and the second lens unit increases, and spaces between the individual lens units change, wherein, during a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit and the third lens unit individually shift independently, and wherein, for a focusing from an object at the infinite distance onto an object at any finite distance between the infinite distance and the proximate distance, amount of shift of the second lens unit and the third lens unit have predetermined values differing by zooming state.
Furthermore, a zoom lens according to the present invention includes, in order from the object side, a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, a third lens unit having a negative refractive power, and a fourth lens unit having a positive refractive power, wherein, during a magnification change from the wide-angle end through the telephoto end, the first lens unit and the fourth lens unit shift from the image-surface side toward the object side, a space between the first lens unit and the second lens unit increases, and spaces between individual lens units change, wherein, during a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit and the third lens unit individually shift independently, wherein, for a focusing from an object at the infinite distance onto an object at any finite distance between the infinite distance and the proximate distance, amount of shift of the second lens unit and the third lens unit have predetermined values differing by zooming state, and wherein the following condition is satisfied:

−2<X2w/X3W<0.5

where X2W is an amount of shift of the second lens unit and X3W is an amount of shift of the third lens unit for a focusing from the infinite distance to the proximate distance at the wide-angle end, upon a shift toward the image-surface side being given a positive value.

According to the present invention, it is possible to provide a zoom lens in which fluctuation of aberrations involved in focusing is stayed small and in which the proximate distance is designed sufficiently close without size increase of the lens system.
These features and advantages of the present invention will become apparent from the following detailed description of the preferred embodiments when taken in conjunction with the accompanying drawings.



BRIEF DESCRIPTION OF THE DRAWINGS
FIGS. 1A, 1B, and 1C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the first embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 2A, 2B and 2C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the second embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 3A, 3B and 3C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the third embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 4A, 4B and 4C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the fourth embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 5A–5D, 5E–5H, and 5I–5L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the first embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 6A–6D, 6E–6H, and 6I–6L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the second embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 7A–7D, 7E–7H, and 7I–7L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the third embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIGS. 8A–8D, 8E–8H, and 8I–8L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the fourth embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
FIG. 9 is a configuration diagram of a single-lens reflex camera in which the zoom lens according to the present invention is used as a photographing lens.



DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Preceding the explanation of the embodiments shown in the drawings, function and effect of the present invention are described below.
Regarding a zoom lens according to the present invention, it is possible to achieve small fluctuation of aberrations involved in focusing and to design the proximate distance to be sufficiently close without size increase of the lens system, by performing focusing by way of shifting each of the plurality of lens units in the zoom lens independently for an optimum amount in each zoom state. To be specific, in a zoom lens including a positive first lens unit, a negative second lens unit, a negative third lens unit, and a positive fourth lens unit with the first lens unit and the fourth lens unit shifting toward the object side and a space between the first lens unit and the second lens unit increasing during a magnification change from the wide-angle end through the telephoto end, configuration is made so that the second lens unit and the third lens unit individually shift independently during a focusing from an object at the infinite distance onto an object at a near distance.
If the focusing be made by shifting forth the second lens unit as stated above at the wide-angle end, it would be necessary, for the purpose of setting the proximate distance to be sufficiently close, to secure a wide space between the first lens unit and the second lens unit under the condition where the infinite distance is in focus. As a result, a lens diameter of the first lens unit would be rendered large. In addition, shift of the second lens unit would cause the problem of large fluctuation of astigmatism, distortion or the like. According to the present invention, the focusing is made by shifting forth mainly the third lens unit at the wide-angle end, to dispense with an extra space between the first lens unit and the second lens unit and to stay fluctuation of aberrations small. In addition, by shifting back the second lens unit toward the image-surface side by an amount smaller than the amount of shift of the third lens unit at the same time as the third lens unit is shifted forth toward the object side, fluctuation of aberrations involved in the shift of the third lens unit can cancel. Here, it is preferable to satisfy the following condition:

−2<X2w/X3W<0.5  (1)

where X2W is an amount of shift of the second lens unit and X3W is an amount of shift of the third lens unit for the focusing at the wide-angle end, with a shift toward the image-surface side being given a positive value.

Condition (1) specifies a ratio of the amount of shift of the second lens unit to the amount of shift of the third lens unit for the focusing. If the upper limit of Condition (1) is exceeded, the amount of shift of the second lens unit toward the object side is large, to result in a large lens diameter of the first lens unit and increase in fluctuation of aberrations during the focusing, as stated above. If the lower limit of Condition (1) is not reached, the amount of shift back toward the image-surface side of the second lens unit is large, to result in increase in amount of shift of the third lens unit, for a shift of the imaging position caused by the shift of the second lens unit is in the opposite direction to the focusing.
Here, the case where X2W/X3W=0 is explained. Upon designing focusing to be performed by shifting the second lens unit and the third lens unit for respectively independent amount at any position other than the wide-angle end, the configuration can be made so that the second lens unit is not shifted in a focusing at the wide-angle end.
It is much preferable to satisfy the following condition (1′):

−1<X2W/X3W<0.3  (1′)

Furthermore, if the following condition (1′′) is satisfied, good focusing operation can be achieved over the full zooming range while precluding a large lens diameter of the first lens unit.

−0.8<X2W/X3W<−0.01  (1′′)

Also, for a magnification change, a space between the first lens unit and the second lens unit should be sufficiently wide at the telephoto end. Thus, in order to achieve compact design of the length of the entire zoom lens, it is desirable that a space between the second lens unit and the third lens unit is small. In this case, it is desirable that the focusing is performed by shifting forth both of the second lens unit and the third lens unit. At the telephoto end, the space between the first lens unit and the second lens unit is large and the field angle is small. Thus, since fluctuation of aberrations involved in the shift of the second lens unit is small, the above-mentioned problem at the wide-angle end is not raised, and the proximate distance can be designed sufficiently small without degradation of performance.
In order to configure a system in which spaces for zooming are efficiently used and in which performance fluctuation caused by focusing is small, it is preferable that the second lens unit shifts toward the image side at the wide angle end and toward the object side at the telephoto end during a focusing from an object at the infinite distance onto an object at a finite distance.
In such an inner focus method, amount of shift of focusing lens unit(s) for a focusing onto a certain finite distance inevitably varies with zooming position, irrespective of whether a single lens unit or a plurality of lens units are used for focusing.
In a case where focusing is performed by a single lens unit, once the paraxial power arrangement of the entire system is determined, amount of shift of the focusing lens unit is uniquely determined by the object distance.
According to the present invention, in a case where focusing is performed by shifting a plurality of lens units independently, distribution ratio of amount of shift among the respective lens units may be arbitrarily selected. In this case, for realizing a smooth moving mechanism, it is desirable that, for a focusing from an object at the infinite distance onto an object at a certain finite distance, amount of shift of the second lens unit continuously changes as a zooming state changes from the wide-angle end through the telephoto end.
Also, it is desirable that, for a focusing from an object at the infinite distance onto an object at a certain finite distance, amount of shift of the third lens unit continuously changes as a zooming state changes from the wide-angle end through the telephoto end. In addition, if the configuration is made so that the third lens unit is shifted from the image side toward the object side during a focusing from an object at the infinite distance onto an object at a certain finite distance with its amount of shift increasing as a zooming state is changed from the wide-angle end through the telephoto end, a smooth moving mechanism can be much easily realized. In this configuration, effect of compensation for aberrations by shift of the second lens unit does not abruptly changes dependent on a zooming state, and thus a zoom lens in a good balance as a whole is achieved.
Also, upon expressing a shift of a focus lens by a function curve corresponding to f(Z)+g(L), which curve has a cam shape, where f(Z) and g(L) are cam rotation angle for zooming and cam rotation angle for focusing, respectively, upon taking zooming position Z and object distance L as parameters, it is desirable that distribution ratio of amount of shift for focusing between the respective lens units in each zooming position is set so that each of the second lens unit and the third lens unit can be expressed by an independent function curve corresponding to f(Z)+g(L).
Also, in a case where a focusing is performed by the second and third lens units in a zoom lens having positive-negative-negative-positive arrangement of refractive power with amount of shift of the second lens unit being small at the wide-angle end and increasing as a zooming state changes toward the telephoto side as set forth above, it is desirable that the cam curve of the second lens unit has an extreme value.
Also, it is much preferable to satisfy the following condition (2):

0.001<D12W/D12T<0.1  (2)

where D12W is a space between the first lens unit and the second lens unit at the wide-angle end under the condition where the infinite distance is in focus, and D12T is a space between the first lens unit and the second lens unit at the telephoto end under the condition where the infinite distance is in focus.

If the lower limit of Condition (2) is not reached, the space between the first lens unit and the second lens unit at the wide-angle end is so small that frames of the lens units are likely to interfere. On the other hand, if the upper limit is exceeded, the space between the first lens unit and the second lens unit at the wide-angle end is wide, to render the lens diameter of the first lens unit large.
It is much preferable to satisfy the following condition (2′):

0.005<D12W/D12T<0.07  (2′)

It is still much preferable to satisfy the following condition (2′′):

0.01<D12W/D12T<0.05  (2′′)

Also, it is preferable to satisfy the following condition (3)

3.0<D23w/D23T<20.0  (3)

where D23W is a space between the second lens unit and the third lens unit at the wide-angle end under the condition where the infinite distance is in focus, and D23T is a space between the second lens unit and the third lens unit at the telephoto end under the condition where the infinite distance is in focus.

Condition (3) specifies a ratio of the space between the second lens unit and the third lens unit at the wide-angle end to the space between the second lens unit and the third lens unit at the telephoto end. If the lower limit of Condition (3) is not reached, variation of the space between the second lens unit and the third lens unit in zooming is small, to less contribute to compensation, by change of the space between the second lens unit and the third lens unit, for fluctuation of aberrations. On the other hand, if the upper limit is exceeded, the space between the second lens unit and the third lens unit at the wide-angle end is large, to less contribute to compact design of the entire length at the wide-angle end.
It is much preferable to satisfy the following condition (3′):

4.0<D23W/D23T<10.0  (3′)

It is still much preferable to satisfy the following condition (3′′):

5.0<D23w/D23T<7.0  (3′′)

Also, it is preferable to satisfy the following condition (4):

0.7<X2T/X3T<1.5  (4)

where X2T is an amount of shift of the second lens unit for a focusing from the infinite distance onto the proximate distance at the telephoto end, and X3T is an amount of shift of the third lens unit for the focusing from the infinite distance onto the proximate distance at the telephoto end.

Condition (4) specifies a ratio of the amount of shift of the second lens unit to the amount of shift of the third lens unit for the focusing at the telephoto end. If the lower limit of Condition (4) is not reached, the amount of shift of the second lens unit in the focusing is small, and thus the second lens unit and the third lens unit are likely to interfere, to make it difficult to shorten the proximate distance. On the other hand, if the upper limited is exceeded, the amount of shift of the third lens unit in the focusing becomes small, and thus contribution of the third lens unit to the focusing is reduced.
It is much preferable to satisfy the following condition (4′):

0.8<X2T/X3T<1.3  (4′)

It is still much preferable to satisfy the following condition (4′′);

0.9<X2T/X3T<1.1  (4′)

In each of the examples above, the upper limit value alone or the lower limit value alone may be specified. Also, a plurality of the conditional expressions may be satisfied simultaneously.
In reference to the drawings and numerical data, the embodiments of the zoom lens according to the present invention are described below.
First Embodiment
FIGS. 1A, 1B, and 1C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the first embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively. FIGS. 5A–5D, 5E–5H, and 5I–5L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the first embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
As shown in FIG. 1, the zoom lens of the first embodiment includes, in order from the object side X toward an image-pickup element surface P, a first lens unit G11 having a positive refractive power, a second lens unit G12 having a negative refractive power, a third lens unit G13 having a negative refractive power, and a fourth lens unit G14 having a positive refractive power. During a magnification change from the wide-angle end (FIG. 1A) through the telephoto end (FIG. 1C), the first lens unit G11 and the fourth lens unit G14 are shifted from the image-surface side toward the object side. In this event, a space D1 between the first lens unit G11 and the second lens unit G12 increases, and spaces between individual lens units change. During a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit G12 and the third lens unit G13 individually shift independently. In FIG. 1, the reference symbol S denotes a stop, the reference symbol FL1 denotes an infrared absorption filter, the reference symbol FL3 denotes a lowpass filter, and the reference symbol FL4 denotes a cover glass of a CCD or CMOS sensor. The reference symbol P denotes an image pickup surface, which is disposed in the effective image-pickup diagonal direction of the CCD or CMOS sensor.
The first lens unit G11 is composed of, in order from the object side X, a negative first lens L11, a positive second lens L12, and a positive third lens L13. The first lens L11 and the second lens L12 form a cemented lens.
The second lens unit G12 is composed of, in order from the object side X, a negative fourth lens L14, a negative fifth lens L15 with its image-side concave surface being aspherical, a negative sixth lens L16, and a positive seventh lens L17.
The third lens unit G13 is composed of, in order from the object side X, a positive eighth lens L18, and a negative ninth lens L19 with its object-side concave surface being aspherical.
The fourth lens unit G14 is composed of, in order from the object side X, a positive tenth lens L110 with its image-side concave surface being aspherical, a positive eleventh lens L111, a negative twelfth lens L112, a positive thirteenth lens L113, and a negative fourteenth lens L114. Of these lenses, the twelfth lens, the thirteenth lens, and the fourteenth lens form a cemented lens.
The stop S is arranged between the third lens unit G13 and the fourth lens unit G14. The infrared absorption filter FL1, the lowpass filter FL2, and the cover glass FL3 of the CCD or CMOS sensor are arranged on the image side of the fourth lens unit G14 in this order toward the image pickup surface P.
The numerical data of the optical members constituting the zoom lens according to the first embodiment are shown below.
In the numerical data of the first embodiment, r1, r2, . . . denote radii of curvature of the respective lens surfaces, d1, d2, . . . denote thicknesses of or airspaces between the respective lenses, nd1, nd2, . . . are refractive indices of the respective lenses or airspaces ford-line rays, Vd1, vd2, . . . are Abbe's numbers of the respective lenses, Fno. denotes F-number, and f denotes a focal length of the entire system. Values of r, d, and f are in millimeters.
It is noted that an aspherical surface is expressed by the following equation:

z=(y2/r)/[1+{1−(1+K)(y/r)2}1/2]+A4y4+A6y6+A8y8+A10y10

where z is taken along the direction of the optical axis, y is taken along a direction intersecting the optical axis at right angles, a conical coefficient is denoted by K, and aspherical coefficients are denoted by A4, A6, A8, and A10.

These reference symbols are commonly used in the numerical data of the subsequent embodiments also.










Numerical data 1

















focal length f = 14.69~53.88 mm, Fno. = 2.85~3.55



2ω = 74.36°~23.36°











r1 = 92.1912





d1 = 2.5
nd1 = 1.84666
νd1 = 23.78



r2 = 50.9961



d2 = 5.84
nd2 = 1.6516
νd2 = 58.55



r3 = 193.066



d3 = 0.13
nd3 = 1



r4 = 47.0946



d4 = 4.36
nd4 = 1.7725
νd4 = 49.6



r5 = 104.1756



d5 = D1
nd5 = 1



r6 = 63.4707



d6 = 1.89
nd6 = 1.7725
νd6 = 49.6



r7 = 11.2012



d7 = 6.64
nd7 = 1



r8 = 311.5503



d8 = 1.8
nd8 = 1.58313
νd8 = 59.38



r9 = 17.622



d9 = 3.22
nd9 = 1



r10 = −49.2708



d10 = 1.5
nd10 = 1.57281
νd10 = 65.72



r11 = −135.9067



d11 = 0.17
nd11 = 1



r12 = 39.3696



d12 = 3.3
nd12 = 1.84666
νd12 = 23.78



r13 = −59.013



d13 = D2
nd13 = 1



r14 = 92.5004



d14 = 3.94
nd14 = 1.53609
νd14 = 60.92



r15 = −18.2971



d15 = 0.2
nd15 = 1



r16 = −17.4747



d16 = 1.8
nd16 = 1.8061
νd16 = 40.92



r17 = 116.0971



d17 = D3
nd17 = 1



r18 = ∞ (aperture stop)



d18 = 1.5
nd18 = 1



r19 = 19.9443



d19 = 4.98
nd19 = 1.51633
νd19 = 64.14



r20 = −154.1774



d20 = 1.1
nd20 = 1



r21 = 44.2951



d21 = 8.4
nd21 = 1.497
νd21 = 81.54



r22 = −24.6953



d22 = 0.19
nd22 = 1



r23 = −99.5386



d23 = 1.3
nd23 = 1.7725
νd23 = 49.6



r24 = 13.692



d24 = 8.82
nd24 = 1.48749
νd24 = 70.23



r25 = −12.0725



d25 = 1.3
nd25 = 1.62684
νd25 = 40.98



r26 = −23.8764



d26 = D4
nd26 = 1



r27 = ∞



d27 = 0.8
nd27 = 1.51633
νd27 = 64.14



r28 = ∞



d28 = 0.8
nd28 = 1



r29 = ∞



d29 = 2.8
nd29 = 1.54771
νd29 = 62.84



r30 = ∞



d30 = 0.5
nd30 = 1



r31 = ∞



d31 = 0.87
nd31 = 1.5231
νd31 = 54.49



r32 = ∞



d32 = 1.07
nd32 = 1










IMG = ∞ (image pickup surface)










aspherical coefficients













9th surface









K = 0




A2 = 0
A4 = −5.1635 × 10−5
A6 = −1.7186 × 10−7


A8 = −2.5602 × 10−9
A10 = 3.2674 × 10−11
A12 = −2.1983 × 10−13







16th surface









K = 0




A2 = 0
A4 = 1.3943 × 10−5
A6 = 4.9740 × 10−8


A8 = 1.0865 × 10−9
A10 = 6.4354 × 10−12







20th surface









K = 0




A2 = 0
A4 = 4.9366 × 10−5
A6 = 3.3833 × 10−8


A8 = 4.6617 × 10−10
A10 = −6.8786 × 10−12
A12 = 3.4557 × 10−14









(variable space in focusing)
















f = 14.67
f = 28.1
f = 53.88
















IO = ∞ (object distance (mm))












zooming space D1
1
16.21
30.51



D2
11.1
4.41
1.15



D3
12.62
6.11
1



D4
29.15
38.87
50.72







IO = 220 (object distance (mm))












zooming space D1
3.13
15.54
26.13



D2
5.92
1.41
0.99



D3
15.67
9.78
5.54



D4
29.15
38.87
50.72










Second Embodiment

FIGS. 2A, 2B, and 2C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the second embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively. FIGS. 6A–6D, 6E–6H, and 6I–6L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the second embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
As shown in FIG. 2, the zoom lens of the second embodiment includes, in order from the object side X toward an image-pickup element surface P, a first lens unit G21 having a positive refractive power, a second lens unit G22 having a negative refractive power, a third lens unit G23 having a negative refractive power, and a fourth lens unit G24 having a positive refractive power. During a magnification change from the wide-angle end (FIG. 2A) through the telephoto end (FIG. 2C), the first lens unit G21 and the fourth lens unit G24 are shifted from the image-surface side toward the object side. In this event, a space D1 between the first lens unit G21 and the second lens unit G22 increases, and spaces D2, D3, and D4 between individual lens units change. During a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit G22 and the third lens unit G23 individually shift independently. In FIG. 2, the reference symbol S denotes a stop. The reference symbol P denotes an image pickup surface, which is disposed in the effective image-pickup diagonal direction of a CCD or CMOS sensor.
The first lens unit G21 is composed of, in order from the object side X, a negative first lens L21, a positive second lens L22, and a positive third lens L23. The first lens L21 and the second lens L22 form a cemented lens.
The second lens unit G22 is composed of, in order from the object side X, a negative fourth lens L24, a negative fifth lens L25 with its image-side concave surface being aspherical, a negative sixth lens L26, and a positive seventh lens L27.
The third lens unit G23 is composed of, in order from the object side X, a negative eighth lens L28, a positive ninth lens L29 with its image-side convex surface being aspherical, and a negative tenth lens L210. The eighth lens L28 and the ninth lens L29 form a cemented lens.
The fourth lens unit G24 is composed of, in order from the object side X, a positive eleventh lens L211 with its image-side concave surface being aspherical, a negative twelfth lens L212, a negative thirteenth lens L213, a negative fourteenth lens L214, and a positive fifteenth lens L215. Each lens of the fourth lens unit G24 is constructed as a singlet lens. The stop S is arranged between the third lens unit G23 and the fourth lens unit G24. The image pickup surface P is arranged on the image side of the fourth lens unit G24.
This embodiment specifies a zoom lens having focal length of 14.71{tilde over ( )}53.88 mm, F-number of 2.85{tilde over ( )}3.75, and 2ω=74.58°{tilde over ( )}23.49°.










Numerical data 2

















focal length f = 14.71~53.88 mm, Fno. = 2.85~3.57



2ω = 74.58°~23.49°











r1 = 84.456





d1 = 2.27
nd1 = 1.84666
νd1 = 23.78



r2 = 51.995



d2 = 6.73
nd2 = 1.6968
νd2 = 55.53



r3 = 229.3



d3 = 0.13
nd3 = 1



r4 = 45.1147



d4 = 4.16
nd4 = 1.69213
νd4 = 55.37



r5 = 82.4423



d5 = D1
nd5 = 1



r6 = 70.9504



d6 = 1.18
nd6 = 1.804
νd6 = 46.57



r7 = 13.2517



d7 = 5.02
nd7 = 1



r8 = 48.8445



d8 = 0.99
nd8 = 1.65313
νd8 = 58.37



r9 = 18.6211



d9 = 4.42
nd9 = 1



r10 = −50.977



d10 = 1
nd10 = 1.61017
νd10 = 61.49



r11 = 67.7526



d11 = 2.44
nd11 = 1



r12 = 41.3578



d12 = 4.2
nd12 = 1.84666
νd12 = 23.78



r13 = −49.5698



d13 = D2
nd13 = 1



r14 = 429.3566



d14 = 1
nd14 = 1.79802
νd14 = 38.51



r15 = 18.4994



d15 = 4.77
nd15 = 1.51633
νd15 = 64.14



r16 = −31.5464



d16 = 0.31
nd16 = 1



r17 = −24.6047



d17 = 1
nd17 = 1.7994
νd17 = 45.15



r18 = −52.1062



d18 = D3
nd18 = 1



r19 = (S: stop)



d19 = D4
nd19 = 1



r20 = 30.2789



d20 = 3.11
nd20 = 1.56602
νd20 = 56



r21 = −139.0487



d21 = 2.25
nd21 = 1



r22 = 19.4216



d22 = 6.25
nd22 = 1.497
νd22 = 81.54



r23 = −32.3709



d23 = 0
nd23 = 1



r24 = 94.8037



d24 = 1
nd24 = 1.80123
νd24 = 44.49



r25 = 19.8715



d25 = 1.46
nd25 = 1



r26 = 119.9151



d26 = 0.94
nd26 = 1.80547
νd26 = 43.54



r27 = 13.8717



d27 = 0.02
nd27 = 1



r28 = 13.9681



d28 = 6.34
nd28 = 1.48749
νd28 = 70.23



r29 = −24.2991



d29 = D5
nd29 = 1



IMG = ∞










aspherical coefficients













9th surface









K = 0




A2 = 0
A4 = −1.2201 × 10−5
A6 = −8.3210 × 10−8


A8 = 2.9877E × 10−10
A10 = −3.5791 × 10−12







16th surface









K = 0




A2 = 0
A4 = −1.9830 × 10−5
A6 = −7.8377 × 10−8


A8 = 1.0328 × 10−9
A10 = −1.0396 × 10−11







21st surface









K = 0




A2 = 0
A4 = 3.8514 × 10−5
A6 = 6.4175 × 10−8


A8 = −2.1234 × 10−10
A10 = 3.8743E × 10−12









(variable space in focusing)
















f = 14.71
f = 29
f = 53.88
















IO = ∞ (object distance (mm))












zooming space D1
1
16.37
30.52



D2
9.29
4.37
1.32



D3
13.58
6.18
1.08



D4
7.82
3.25
1



D5
34.68
43.69
52.01







IO = 220 (object distance (mm))












zooming space D1
1.1
13.81
23.28



D2
4.77
1.21
0.99



D3
18
11.89
8.65



D4
7.82
3.25
1



D5
34.68
43.69
52.01










Third Embodiment

FIGS. 3A, 3B, and 3C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the third embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively. FIGS. 7A–7D, 7E–7H, and 7I–7L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the third embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
As shown in FIG. 3, the zoom lens of the third embodiment includes, in order from the object side X toward an image-pickup element surface P, a first lens unit G31 having a positive refractive power, a second lens unit G32 having a negative refractive power, a third lens unit G33 having a negative refractive power, and a fourth lens unit G34 having a positive refractive power. During a magnification change from the wide-angle end (FIG. 3A) through the telephoto end (FIG. 3C), the first lens unit G31 and the fourth lens unit G34 are shifted from the image-surface side toward the object side. In this event, a space D1 between the first lens unit G31 and the second lens unit G32 increases, and spaces D2, D3, D4, and D5 between individual lens units change. During a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit G32 and the third lens unit G33 individually shift independently. In FIG. 3, the reference symbol S denotes a stop, the reference symbol FL1 denotes an infrared absorption filter, the reference symbol FL2 denotes a filter (for instance, an ultraviolet absorption filter), the reference symbol FL3 denotes a lowpass filter, and the reference symbol FL4 denotes a cover glass of a CCD or CMOS sensor. The reference symbol P denotes an image pickup surface, which is disposed in the effective image-pickup diagonal direction of the CCD or CMOS sensor.
The first lens unit G31 is composed of, in order from the object side X, a negative first lens L31, a positive second lens L32, and a positive third lens L33. The first lens L31 and the second lens L32 form a cemented lens.
The second lens unit G32 is composed of, in order from the object side X, a negative fourth lens L34, a negative fifth lens L35, a negative sixth lens L36 with its image-side concave surface being aspherical, and a positive seventh lens L37.
The third lens unit G33 is composed of, in order from the object side X, a negative eighth lens L38, a positive ninth lens L39, and a negative tenth lens L310 with its object-side concave surface being aspherical. The eighth lens L38 and the ninth lens L39 form a cemented lens.
The fourth lens unit G34 is composed of, in order from the object side X, a positive eleventh lens L311 with its image-side concave surface being aspherical, a negative twelfth lens L312, a positive thirteenth lens L313, a negative fourteenth lens L314, and a positive fifteenth lens L315. Of these lenses of the fourth lens unit, each pair of the twelfth lens L312 and the thirteenth lens L313, and the fourteenth lens L314 and the fifteenth lens L315 form a cemented lens. The stop S is arranged between the third lens unit G33 and the fourth lens unit G34. The infrared absorption filter FL1, the filter FL2, and the lowpass filter FL3 are arranged behind the fourth lens unit G34. In addition, the cover glass FL4 is arranged on the image pickup surface P formed of a CCD or CMOS sensor.
This embodiment specifies a zoom lens having focal length of 14.69{tilde over ( )}53.09 mm, F-number of 2.85{tilde over ( )}3.57, and 2ω=74.34°{tilde over ( )}23.7°.










Numerical data 3

















focal length f = 14.69~53.09 mm, Fno. = 2.85~3.57



2ω = 74.34°~23.7°











r1 = 72.4777





d1 = 2.5
nd1 = 1.78472
νd1 = 25.68



r2 = 43.7011



d2 = 5.84
nd2 = 1.60311
νd2 = 60.64



r3 = 120.2886



d3 = 0.15
nd3 = 1



r4 = 50.8706



d4 = 4.15
nd4 = 1.7725
νd4 = 49.6



r5 = 116.5737



d5 = D1
nd5 = 1



r6 = 48.0592



d6 = 1.79
nd6 = 1.7725
νd6 = 49.6



r7 = 11.9943



d7 = 5.96
nd7 = 1



r8 = 402.0321



d8 = 1.30
nd8 = 1.72916
νd8 = 54.68



r9 = 22.3938



d9 = 2.08
nd9 = 1



r10 = 499.9999



d10 = 1.5
nd10 = 1.58213
νd10 = 59.38



r11 = 31.4025



d11 = 1.87
nd11 = 1



r12 = 32.5882



d12 = 3.64
nd12 = 1.84666
νd12 = 23.78



r13 = −56.5538



d13 = D2
nd13 = 1



r14 = 97.862



d14 = 1
nd14 = 1.68893
νd14 = 31.07



r15 = 14.9639



d15 = 4.48
nd15 = 1.51742
νd15 = 52.43



r16 = −77.7981



d16 = 0.71
nd16 = 1



r17 = −27.5251



d17 = 1.4
nd17 = 1.58213
νd17 = 59.38



r18 = −499.9997



d18 = D3
nd18 = 1



r19 = (aperture stop)



d19 = D4
nd19 = 1



r20 = 18.3735



d20 = 5.94
nd20 = 1.51533
νd20 = 64.14



r21 = −516.7792



d21 = 0.28
nd21 = 1



r22 = 38.9054



d22 = 1.45
nd22 = 1.741
νd22 = 52.64



r23 = 15.3846



d23 = 9.44
nd23 = 1.48749
νd23 = 70.23



r24 = −23.3077



d24 = 0.20
nd24 = 1



r25 = −278.1573



d25 = 1.15
nd25 = 1.8061
νd25 = 40.92



r26 = 17.639



d26 = 7
nd26 = 1.48749
νd26 = 70.23



r27 = −34.6815



d27 = D5
nd27 = 1



r28 = ∞



d28 = 0.7
nd28 = 1.51633
νd28 = 64.14



r29 = ∞



d29 = 0.4
nd29 = 1



r30 = ∞



d30 = 0.5
nd30 = 1.542
νd30 = 77.4



r31 = ∞



d31 = 2.8
nd31 = 1.54771
νd31 = 62.84



r32 = ∞



d32 = 0.5
nd32 = 1



r33 = ∞



d33 = 0.762
nd33 = 1.5231
νd33 = 54.49



r34 = ∞



d34 = 1.3189SZ
nd34 = 1



IMG = ∞










aspherical coefficients













11th surface









K = 0




A2 = 0
A4 = −1.5917 × 10−5
A6 = −4.1799 × 10−8


A8 = −6.0084 × 10−10
A10 = 9.0292 × 10−12
A12 = −5.9555 × 10−14







17th surface









K = 0




A2 = 0
A4 = 2.2092 × 10−5
A6 = 6.9507 × 10−8


A8 = −5.0225 × 10−10
A10 = 2.0146 × 10−12
A12 = 2.2283 × 10−15







21st surface









K = 0




A2 = 0
A4 = 5.7666 × 10−5
A6 = 1.9404 × 10−8


A8 = 4.2423 × 10−10
A10 = −5.5638 × 10−12
A12 = 1.9633 × 10−14









(variable space in focusing)
















f = 14.69
f = 28.1
f = 53.09
















IO = ∞ (object distance (mm))












zooming space D1
1
16.33
31.63



D2
7.94
3.7
1.46



D3
6.09
1.37
1.



D4
10.45
6.44
1



D5
29.21
39.43
51.02







IO = 229 (object distance (mm))












zooming space D1
1.65
14.99
27.44



D2
4.59
1.63
1.09



D3
8.78
4.79
5.56



D4
10.45
6.44
1



D5
29.28
39.58
51.45










Fourth Embodiment

FIGS. 4A, 4B, and 4C are sectional views taken along the optical axis that show the optical configuration of the zoom lens of the fourth embodiment according to the present invention, showing the states at the wide-angle end, the intermediate position, and the telephoto end, respectively. FIGS. 8A–8D, 8E–8H, and 8I–8L are diagrams that show spherical aberration, astigmatism, distortion, and chromatic aberration of magnification of the third embodiment at the wide-angle end, the intermediate position, and the telephoto end, respectively.
As shown in FIG. 4, the zoom lens of the fourth embodiment includes, in order from the object side X toward an image-pickup element surface P, a first lens unit G41 having a positive refractive power, a second lens unit G42 having a negative refractive power, a third lens unit G43 having a negative refractive power, and a fourth lens unit G44 having a positive refractive power. During a magnification change from the wide-angle end (FIG. 4A) through the telephoto end (FIG. 4C), the first lens unit G41 and the fourth lens unit G44 are shifted from the image-surface side toward the object side. In this event, a space D1 between the first lens unit G41 and the second lens unit G42 increases, and spaces D2, D3, D4 (, and D5) between individual lens units change. During a focusing from an object at the infinite distance onto an object at a near distance, the second lens unit G42 and the third lens unit G43 individually shift independently. In FIG. 4, the reference symbol S denotes a stop, the reference symbol S2 denotes a flare cut stop, the reference symbol FL1 denotes an infrared absorption filter, the reference symbol FL2 denotes a filter, the reference symbol FL3 denotes a lowpass filter, and the reference symbol FL4 denotes a cover glass of a CCD or CMOS sensor. The reference symbol P denotes an image pickup surface, which is disposed in the effective image-pickup diagonal direction of the CCD or CMOS sensor.
The first lens unit G41 is composed of, in order from the object side X, a negative first lens L41, a positive second lens L42, and a positive third lens L43. The first lens L41 and the second lens L42 form a cemented lens.
The second lens unit G42 is composed of, in order from the object side X, a negative fourth lens L44, a negative fifth lens L45, a negative sixth lens L46, and a positive seventh lens L47.
The third lens unit G43 is composed of, in order from the object side X, a negative eighth lens L48 with its object-side convex surface being aspherical, a positive ninth lens L49, and a negative tenth lens L410. The eighth lens L48 and the ninth lens L49 form a cemented lens.
The fourth lens unit G44 is composed of, in order from the object side X, a positive eleventh lens L411 with its object-side convex surface being aspherical, a negative twelfth lens L412, a positive thirteenth lens L413 with its object-side convex surface being aspherical, a negative fourteenth lens L414, and a positive fifteenth lens L415. Each pair of the twelfth lens L412 and the thirteenth lens L413, and the fourteenth lens L414 and the fifteenth lens L415 form a cemented lens. The stop S is arranged between the third lens unit G43 and the fourth lens unit G44. On the image side of the lens L415 of the fourth lens unit G44, arranged is the flare cut stop S2 that is shaped substantially as a rectangle, followed by the infrared absorption filter FL1, the filter FL2, the lowpass filter FL3, and the cover glass FL4 arranged in this order toward the image pickup surface P. Also, the image pickup surface P is formed of a CCD or CMOS sensor.
This embodiment specifies a zoom lens having focal length of 14.69{tilde over ( )}53.09 mm, F-number of 2.85{tilde over ( )}3.57, and 2ω=74.34°{tilde over ( )}23.70°.










Numerical data 4

















focal length f = 14.69~53.09 mm, Fno. = 2.85~3.57



2ω = 74.34°~23.70°











r1 = 72.48





d1 = 2.5
nd1 = 1.78472
νd1 = 25.68



r2 = 43.70



d2 = 5.84
nd2 = 1.60311
νd2 = 60.64



r3 = 120.29



d3 = 0.15
nd3 = 1



r4 = 50.87



d4 = 4.15
nd4 = 1.7725
νd4 = 49.6



r5 = 116.57



d5 = D1
nd5 = 1



r6 = 48.06



d6 = 1.79
nd6 = 1.7725
νd6 = 49.6



r7 = 11.99



d7 = 5.96
nd7 = 1



r8 = 402.03



d8 = 1.3
nd8 = 1.72916
νd8 = 54.68



r9 = 22.39



d9 = 2.08
nd9 = 1



r10 = 499.9999



d10 = 1.5
nd10 = 1.58213
νd10 = 59.38



r11 = 31.4025



d11 = 1.87
nd11 = 1



r12 = 32.59



d12 = 3.64
nd12 = 1.84666
νd12 = 23.78



r13 = −56.55



d13 = D2
nd13 = 1



r14 = 97.86



d14 = 1.01
nd14 = 1.68893
νd14 = 31.07



r15 = 14.96



d15 = 4.48
nd15 = 1.51742
νd15 = 52.43



r16 = −77.80



d16 = 0.71
nd16 = 1



r17 = −27.5251



d17 = 1.4
nd17 = 1.58213
νd17 = 59.38



r18 = −499.9997



d18 = D3
nd18 = 1



r19 = (aperture stop)



d19 = D4
nd19 = 1



r20 = 18.3735



d20 = 5.94
nd20 = 1.51533
νd20 = 64.14



r21 = −516.7792



d21 = 0.28
nd21 = 1



r22 = 38.91



d22 = 1.45
nd22 = 1.741
νd22 = 52.64



r23 = 15.38



d23 = 9.44
nd23 = 1.48749
νd23 = 70.23



r24 = −23.31



d24 = 0.20
nd24 = 1



r25 = −278.16



d25 = 1.15
nd25 = 1.8061
νd25 = 40.92



r26 = 17.64



d26 = 7
nd26 = 1.48749
νd26 = 70.23



r27 = −34.68



d27 = 0.14
nd27 = 1



r28 = ∞



d28 = D5
nd28 = 1



r29 = ∞



d29 = 0.7
nd29 = 1.516331
νd29 = 64.14



r30 = ∞



d30 = 0.4
nd30 = 1



r31 = ∞



d31 = 0.5
nd31 = 1.542
νd31 = 77.4



r32 = ∞



d32 = 2.8
nd32 = 1.54771
νd32 = 62.84



r33 = ∞



d33 = 0.5
nd33 = 1



r34 = ∞



d34 = 0.762
nd34 = 1.5231
νd34 = 54.49



r35 = ∞



d35 = 1.18
nd35 = 1



IMG = ∞










aspherical coefficients













14th surface









K = 0




A2 = 0
A4 = −1.5917 × 10−5
A6 = −4.1799 × 10−8


A8 = −6.0084 × 10−10
A10 = 9.0292 × 10−12
A12 = −5.9555 × 10−14







20th surface









K = 0




A2 = 0
A4 = 2.2092 × 10−5
A6 = 6.9507 × 10−8


A8 = −5.0225 × 10−10
A10 = 2.0146 × 10−12
A12 = 2.2283 × 10−15







24th surface









K = 0




A2 = 0
A4 = 5.7666 × 10−5
A6 = 1.9404 × 10−8


A8 = 4.2423 × 10−10
A10 =-5.5638 × 10−12
A12 = 1.9633 × 10−14









(variable space in focusing)
















f = 14.69
f = 28.1
f = 53.09
















IO = ∞ (object distance (mm))












zooming space D1
1
16.33
31.63



D2
7.94
3.7
1.46



D3
6.09
1.37
1.



D4
10.45
6.44
1



D5
29.21
39.43
51.02







IO = 235 (object distance (mm))












zooming space D1
1.65
14.99
27.44



D2
4.59
1.628
1.09



D3
8.78
4.79
5.56



D4
10.45
6.44
1



D5
29.23
39.43
51.12










The above-described zoom lenses according to the present invention are applicable to silver-halide or digital, single-lens reflex cameras. An application example of these is shown below.
FIG. 9 shows a single-lens reflex camera using a zoom lens of the present invention as the photographing lens and a compact CCD or C-MOS as the image-pickup element. In FIG. 9, the reference numeral 1 denotes a single-lens reflex camera, the reference numeral 2 denotes a photographing lens, the reference numeral 3 denotes a mount section, which achieves removable mount of the photographing lens 2 on the single-lens reflex camera 1. A screw type mount, a bayonet type mount and the like are applicable. In this example, a bayonet type mount is used. The reference numeral 4 denotes an image pickup surface of the image pickup element, the reference numeral 5 denotes a quick return mirror arranged between the lens system on the path of rays 6 of the photographing lens 2 and the image pickup surface 4, the reference numeral 7 denotes a finder screen disposed in a path of rays reflected from the quick return mirror, the reference numeral 8 denotes a penta prism, the reference numeral 9 denotes a finder, and the reference symbol E denotes an eye of an observer (eyepoint). A zoom lens of the present invention is used as the photographing lens 2 of the single-lens reflex camera 1 thus configured.

## Claims

1. A zoom lens comprising, in order from an object side:
a first lens unit having a positive refractive power;
a second lens unit having a negative refractive power;
a third lens unit having a negative refractive power; and
a fourth lens unit having a positive refractive power,
wherein, during a magnification change from a wide-angle end through a telephoto end, the first lens unit and the fourth lens unit shift from an image-surface side toward an object side, a space between the first lens unit and the second lens unit increases, and spaces between individual lens units change, and
wherein, during a focusing from an object at an infinite distance onto an object at a near distance, at least the second lens unit and the third lens unit individually shift independently.

2. A zoom lens according to claim 1, wherein an amount of shift of each of the second lens unit and the third lens unit for a focusing from an object at the infinite distance onto an object at any finite distance between the infinite distance and a proximate distance has a predetermined value differing by zooming position.

3. A zoom lens according to claim 1, satisfying the following condition:


−2<X2W/X3W<0.5


where X2W is an amount of shift of the second lens unit for a focusing from the infinite distance onto a proximate distance at the wide-angle end, and X3W is an amount of shift of the third lens unit for the focusing from the infinite distance onto the proximate distance at the wide-angle end, upon a shift toward the image-surface side being given a positive value.

4. A zoom lens according to claim 3, satisfying the following condition:


−1<X2W/X3W<0.3.

5. A zoom lens according to claim 3, satisfying the following condition:


−0.8<X2W/X3W<−0.01.

6. A zoom lens according to claim 1 or 2, wherein, during a focusing from an object at the infinite distance onto an object at a finite distance, the second lens unit shifts toward the image-surface side at the wide-angle end and shifts toward the object side at the telephoto end, and the third lens unit shifts toward the object side irrespective of zooming state.

7. A zoom lens according to claim 6, wherein an amount of shift of the second lens unit for a focusing from an object at the infinite distance onto an object at a particular finite distance continuously changes as a zooming state changes from the wide-angle end through the telephoto end.

8. A zoom lens according to claim 6, wherein an amount of shift of the third lens unit for a focusing from an object at the infinite distance onto an object at a particular finite distance continuously changes as a zooming state changes from the wide-angle end through the telephoto end.

9. A zoom lens according to claim 8, wherein, during the focusing from the object at the infinite distance onto the object at the particular finite distance, the third lens unit shifts towards the object side, with an amount of shift thereof increasing as a zooming state changes from the wide-angle end through the telephoto end.

10. A zoom lens according to claim 1 or 2, satisfying the following condition:


0.001<D12W/D12T<0.1


where D12W is a space between the first lens unit and the second lens unit at the wide-angle end under a condition where the infinite distance is in focus, and D12T is a space between the first lens unit and the second lens unit at the telephoto end under the condition where the infinite distance is in focus.

11. A zoom lens according to claim 10, satisfying the following condition:


0.005<D12W/D12T<0.07.

12. A zoom lens according to claim 10, satisfying the following condition:


0.01<D12W/D12T<0.05.

13. A zoom lens according to claim 1 or 2, satisfying the following condition:


3.0<D23W/D23T<20.0


where D23W is a space between the second lens unit and the third lens unit at the wide-angle end under a condition where the infinite distance is in focus, and D23T is a space between the second lens unit and the third lens unit at the telephoto end under the condition where the infinite distance is in focus.

14. A zoom lens according to claim 13, satisfying the following condition:


4.0<D23W/D23T<10.0

15. A zoom lens according to claim 13, satisfying the following condition:


5.0<D23W/D23T<7.0

16. A zoom lens according to claim 13, satisfying the following condition:


0.7<X2T/X3T<1.5


where X2T is an amount of shift of the second lens unit for a focusing from the infinite distance onto a proximate distance at the telephoto end, and X3T is an amount of shift of the third lens unit for the focusing from the infinite distance onto the proximate distance at the telephoto end.

17. A zoom lens according to claim 16, satisfying the following condition:


0.7<X2T/X3T<1.3.

18. A zoom lens according to claim 16, satisfying the following condition:


0.9<X2T/X3T<1.1.

19. A zoom lens device comprising:
a zoom lens according to claim 1; and
a lens mount section arranged on the image-surface side of the zoom lens, the lens mount section being connectable with a camera.

20. A zoom lens device comprising:
a zoom lens according to claim 2; and
a lens mount section arranged on the image-surface side of the zoom lens, the lens mount section being connectable with a camera.

21. A zoom lens device comprising:
a zoom lens according to claim 3; and
a lens mount section arranged on the image-surface side of the zoom lens, the lens mount section being connectable with a camera.