Zoom lens

This application claims benefit of Japanese Application No. 2006-306587 filed in Japan on Nov. 13, 2006, the contents of which are incorporated by this reference.

BACKGROUND OF THE INVENTION

The present invention relates generally to a zoom lens, and more particularly to a zoom lens lending itself to a camera-specific taking lens.

In recent years, there have been growing demands for camera-specific zoom lenses capable of taking photographs both over an ever wider scene through zooming and at an ever wider range of subject distance from infinity to a short distance.

So far, focusing on subjects on short distances has generally been implemented by moving the whole or a part of one lens group among lens groups with the space between them varying at the time of zooming. However, this gives rise to large aberration fluctuations upon focusing that lead to degradations in association with short-distance photography, or is less than satisfactory in terms of much wider short-distance scenes. There has also been the so-called floating mechanism used with single-focus lenses, wherein multiple lens groups are independently moved upon focusing to make correction of aberration fluctuations at short distances, thereby achieving plenty of short-distance performance or the specifications for the shortest distance. For reasons of lens or mechanism size reductions, fast AF, and reductions in the shortest distance, the so-called inner focus mode wherein internal lens groups are driven for focusing goes mainstream for focusing with taking lenses. An example of the floating mechanism of the inner focus mode applied to zoom lenses is set forth in, for instance, Patent Publication 1.

Patent Publication 1

JP(A)2004-341060

A problem with the inner focus mode applied to a zoom lens is, however, that the floating mechanism combined with that gets a lot more complicated, because of changes depending on a zooming position in the amount of movement of a focusing lens group from infinity to a constant subject distance.

SUMMARY OF THE INVENTION

In view of that problem with the prior art as briefed above, an object of the invention is to provide a novel mechanism for a zoom lens designed to focus on a short distance subject by moving a focusing lens group a varying amount in the optical axis direction depending on a zooming position.

According to one aspect of the invention, the aforesaid object is achievable by the provision of a zoom lens adapted to focus on a short distance subject by moving a focusing lens group a varying amount in an optical axis direction depending on a zooming position while there is a change in the space between two lens groups adjacent to each other, characterized in that the space between said two lens groups stays constant at a constant subject distance wherever the zooming position lies.

According to another aspect of the invention, there is a zoom lens provided, which comprises, in order from its object side, a positive first lens group, a negative second lens group and a positive third lens group, wherein zooming is implemented with a change in the space between adjacent lens groups, and said negative second lens group is moved a varying amount in an optical axis direction depending on a zooming position thereby focusing on a short distance subject, and which is characterized in that said negative second lens group comprises a negative front unit and a negative rear unit wherein a space between said negative front unit and said rear unit is varied by a subject distance yet the space between said negative front unit and said negative rear unit stays constant wherever the zooming position lies.

Preferably in this case, at least one lens surface in said front unit is defined by an aspheric surface whose negative or positive power grows weak or strong with a distance from the optical axis, and said rear unit comprises, in order from its object side, a negative lens and a positive lens.

The advantages of, and the requirements for, the aforesaid arrangement are now explained.

To provide a solution to such a problem with the prior art zoom lens as mentioned above—the complexity of the mechanism engendered by the inner focus and floating mechanism combination, the invention provides a zoom lens adapted to focus on a short distance subject by allowing two adjoining lens groups to move a varying amount in the optical axis direction depending on the zooming position while there is a change in the space between them, wherein whatever the subject distance is, the space between the two lens groups stays constant.

Ordinarily, the application of the inner focus mode to a zoom lens requires a cooperating mechanism for moving a focusing lens group to a focusing position in association with zooming, because the amount of movement of the focusing lens group from an infinite position to a constant subject distance differs with focal lengths. Further, a combination of the inner focus mode with the floating mode requires a mechanism in cooperation with the zooming mechanism for each lens group that moves independently upon focusing, making the structure of the lens barrel much more complicated.

In the invention, therefore, the zoom lens is designed such that the space between two lens groups that move independently upon focusing is dependent on the subject distance alone, and two such lens groups move as one piece depending on the focal length, whereby improvements by floating in the short distance performance are achievable without making the mechanism in cooperation with the zooming mechanism complicated.

The invention also provides a zoom lens comprising, in order from its object side, a positive first lens group, a negative second lens group and a positive third lens group, with zooming being implemented while the space between adjacent lens group is varied, and focusing on a short distance subject being implemented by moving the negative second lens group an amount that differs in the optical axis direction depending on a zooming position, wherein the negative second lens group comprises a negative front unit and a negative rear unit, and the space between the negative front unit and the negative rear unit is changed depending on a subject distance while the space between the negative front unit and the negative rear unit stays constant wherever the zooming position lies. It is thus possible to make correction of astigmatism produced when focusing is implemented by the negative second lens group while the space between the front unit and the rear unit stays constant. It is also possible to reduce the size and cost of the whole lens barrel without making the lens barrel structure complicated.

Further, at least one lens surface in the front unit is configured as an aspheric surface having negative or positive power growing weak or strong with a distance from the optical axis so that distortion at the wide-angle end can be well corrected. Furthermore, the negative rear unit is made up of, in order from its object side, a negative lens and a positive lens so that fluctuations of astigmatism likely to occur in association with focusing can be well corrected.

And now, a zoom lens having an angle of view exceeding 70° at the wide-angle end is likely to produce chromatic aberration of magnification, and so chromatic aberration of g line or the like remaining at the time of correction of chromatic aberration near C line and F line in particular, i.e., the so-called secondary spectra are not easy to correct. As well known in the art, such chromatic aberration is corrected by use of fluorite having low dispersion and anomalous dispersion or optical glass having similar characteristics. Chromatic aberration Δ_CFof C line and F line produced at a thin single lens is represented by

Δ_CF=Φ/ν_d

Here Φ: the power of the single lens, and

ν_d=(n_d−1)/(n_F−n_C): the Abbe constant of the material.

The conditions for the achromatization of C line and F line with a doublet consisting of a combined positive and negative lens are

Φ=Φ₁+Φ₂, Φ₁>0, Φ₂<0 (1)

Δ_CF=Φ₁/ν_d1+Φ₂/ν_d2=0 (2)

Here Φ: the power of the whole,

Φ_i: the power of the i-th lens, and

ν_di: the Abbe constant of the i-th lens. That is,

Φ₁=ν_d1/(ν_d1−ν_d2)×Φ (3)

Φ₂=−ν_d2/(ν_d1−ν_d2)×Φ (4)

From equations (3) and (4), the then residual chromatic aberration Δ_Fgof g line with respect to F line is represented by

$\begin{matrix} \begin{matrix} Δ_{Fg} = Φ_{1} \times θ_{gF 1} / v_{d 1} + Φ_{2} \times θ_{gF 2} / v_{d 2} \\ = - (θ_{gF 1} - θ_{gF 2}) / (v_{d 1} - v_{d 2}) \times Φ \end{matrix} & (5) \end{matrix}$

θ_gFi=(n_gi−n_Fi)/(n_Fi−n_Ci): the partial dispersion ratio of g line of the i-th lens

Thus, it is well known that three wavelengths, C, F, g line, etc. can be achromatized with a combination of two positive and negative lenses having the same θ_gFbut varying Abbe constants.

However, the characteristics of most of currently existing glasses are such that θ_gFis almost proportional to ν_d, substantially existing near the straight line of the following equation:

θ_gF=−0.001781ν_d+0.6494 (6)

Therefore, when two glass materials differing in ν_dare selected, θ_gFcomes to differ in proportion to that, too; chromatic aberration of g line remaining in the case of the achromatization of C line and F line with a combination of glass materials existing on the straight line of equation (6) stays constant no matter how they are combined. In general, to correct such secondary spectra, glass materials having characteristics departing from equation (6) or the so-called anomalous dispersion, especially fluorite having low dispersion yet a high partial dispersion ratio or glass materials close in characteristic to it are used. These materials have ν_dOf as large as 80 to 95; when Φ>0, Φ₁>0 and Φ₂<0 in the aforesaid achromatism conditions (1) and (2), the perfect achromatization of C line, F line and g line could theoretically be expected if the material for Φ₁is used in combination with such a material as meeting equations (3) and (4) and θ_gF1=θ_gF2. However, actually available materials capable of meeting θ_gF1=θ_gF2have some limitations on both Abbe constant and refractive index, and with camera-specific taking lenses that must satisfy various specifications for aberration correction, size reductions and other considerations, perfect achromatization would indeed be difficult due to the need of using a material having much higher refractive index and dispersion.

As for a thin lens system made up of n lenses as in equations (2) and (5), the condition for the achromatization of C line and F line is

ΣΦ_i/ν_di=0 (7)

The then residual chromatic aberration of F line and g line is

Σθ_gFi×Φ_i/ν_di (8)

If it is made up of only the material existing on equation (6), from equations (6) and (7), (8) becomes

$\begin{matrix} \sum {(- 0 / 001781 v_{di} + 0.6494) \times Φ_{i} / v_{di}} = \sum {(- 0001781 + 06494 / v_{di}) \times Φ_{i}} = \sum (- 0.001781 \times Φ_{i}) = - 0.001781 \times Φ & (9) \end{matrix}$

It follows that condition (8) is determined by the power of the whole system alone. Consider here the case where the power Φ of the whole system is positive. Equation (9) becomes negative; so this value may be diminished by using for a lens of positive power a material with partial dispersion larger than given by equation (6). However, when only a material having low dispersion yet a high partial dispersion ratio, like fluorite, is used, θ_gFtakes a value of 0.53 to 0.54, and most glass materials on equation (6) have a θ_gFvalue of greater than 0.54; so from equations (7) and (8), it is noted that unless an optical system is mainly made up of a glass material that is on the equation (6) and has a value of up to 0.54, it is necessary to give large power to a lens made of an anomalous dispersion material so as to make correction of residual chromatic aberration.

Here take achromatization with three lenses as an example. When

Φ=Φ₁+Φ₂+Φ₂, Φ>0, Φ₁, Φ₃>0, Φ₂>0

the achromatism condition for C line and F line is

Φ₁/ν_d1+Φ₂/ν_d2+Φ₃/ν_d3=0

The then residual chromatic aberration of g line with respect to F line is

Δ_Fg=θ_gF1×Φ₁/ν₁/ν_d1+θ_gF2×Φ₂/ν_d2+θ_gF3×Φ₃/ν_d3

Here the conditions for Δ_Fg=0 are

Φ₁=(θ_gF2−θ_gF3)×ν_d1/k×Φ

Φ₂=(θ_gF3−θ_gF1)×ν_d2/k×Φ

Φ₃=(θ_gF1−θ_gF2)×ν_d3/k×Φ

k=(θ_gF2−θ_gF3)×ν_d1+(θ_gF3−θ_gF1)×ν_d2+(θ_gF1−θg_F2)×ν_d3

If the three materials are all on equation (6), k=0 or there is no solution. When any one of them is a material having a partial dispersion ratio greater than given by equation (6), for instance, when the material of the lens having power Φ₁is

θ_gF=−0.991781ν_d+0.6494+α, α>0

Φ₁=0.001781×ν_d1/α×Φ (10)

Φ₂=(θ_gF3−θ_gF1)×ν_d2/{(ν_d3−ν_d2)×α}×Φ

Φ₃=(θ_gF1−θ_gF2)×ν_d3/{(ν_d3−θ_d2)×α}×Φ

That is, the value of equation (10) is determined irrespective of the material of Φ₂, Φ₃. For the glass material having low dispersion and anomalous dispersion as expressed by a large θ_gFand used relatively often in view of productivity, cost, etc., for instance, the materials having such characteristics as given by

(1) n_d=1.497, ν_d=81.5, θ_gF=0.537

(2) n_d=1.439, ν_d=95, θ_gF=0.534

are generally used.

When these are used as the material for Φ₁, the value of Φ₁(equation (10)) for implementing achromatization at three wavelengths becomes

(1) 4.37Φ

(2) 3.15Φ

That is, to make sure perfect achromatization at three wavelengths, it is required to give a power about 3 to 4.5 times as large to the material having lower dispersion and a higher partial dispersion ratio. However, this is often unachievable, because of providing some considerable restrictions on recent camera-specific taking lenses for which higher performance, and further size and cost reductions are needed. Further, for a wide-angle zoom lens or a single lens reflex camera-specific interchangeable zoom lens required to have a long back focus, it is required to apply a high-refractive-index material to a negative lens so as to make correction of a negative Petzval's sum. However, most high-refractive-index materials have high dispersion; so it is difficult to make a sensible tradeoff between achromatization and correction of the Petzval's sum by use of the aforesaid material combination.

On the other hand, it is known that the material having a large θ_gFexceeding the value given by equation (6) includes, in addition to the aforesaid low-dispersion material, a high-dispersion material where ν_d≧30. The invention provides a method for implementing achromatization within an entire lens system or zoom lens by use of a combination of the material having such low dispersion yet high partial dispersion ratio as meeting the following condition (a), for instance, fluorite with the material having such high dispersion and high partial dispersion ratio as meeting the following condition (b).

ν_d≧80, θ_gF≧−0.001781ν_d+0.6494+0.02 (a)

ν_d≦30, θ_gF≧−0.001781ν_d+0.6494+0.01 (b)

For instance, when the material of the aforesaid (1) and (2) is used for Φ₁the material of n_d=1.85, ν_d=24 and θ_gF=0.62 is used for Φ₂and the material of ν_d=30 according to equation (6) is used for Φ₃, the values of Φ₁, Φ₂and Φ₃are

(1) Φ₁=2.23Φ, Φ₂=1.56Φ, Φ₃=−2.79

(2) Φ₁=1.93Φ, Φ₂=1.23Φ, Φ₃=−2.16

Also, when the material of n_d=1.92, ν_d=18.9 and θ_gF=0.65 is used for Φ₂, there are

(1) Φ₁=2.07Φ, Φ₂=0.53Φ, Φ₃=−1.60

(2) Φ₁=1.82Φ, Φ₂=0.42Φ, Φ₃=−1.24

That is, the value of Φ₁can be smaller than could be obtained with the combination of the aforesaid material of low dispersion and anomalous dispersion with only the material according to equation (6). Further, the material having low dispersion and high refractive index and having a proper negative power can be used for Φ₃, so that there can be a sensible tradeoff offered between achromatization and correction of the Petzval's sum.

While the achromatism conditions for the entire thin lens system have been described, it is understood that much the same principles may be applied to implementing achromatization for the respective groups of a zoom lens, and correction of the secondary spectra of chromatic aberration of magnification likely to occur at a wide-angle zoom lens as well.

Chromatic aberration of magnification is likely to occur with the asymmetric arrangement about an aperture stop of a zoom lens comprising, in order from its object side, a positive first lens group, a negative second lens group, the aperture stop and a lens group located on an image plane side with respect to that and having generally positive power, with zooming implemented while the space between adjacent lens groups is varied, wherein the combined power of the first and second lens groups located on the object side with respect to the aperture stop is negative, and the power of the lens group(s) on the image plane side with respect to the aperture stop is positive. In the invention, therefore, at least two positive lenses using the materials represented by the following conditions (a) and (b) are located in the lens group(s) on the image plane side with respect to the aperture stop so as to make correction of the secondary spectra of chromatic aberration of magnification.

ν_d≧80, θ_gF≧−0.001781ν_d+0.6494+0.02 (a)

ν_d≧30, θ_gF≧−0.001781ν_d+0.6494+0.01 (b)

Here, θ_gF=(n_g−n_F)/(n_F−n_C)

n_g: the g-line refractive index

n_F: the F-line refractive index

n_d: the d-line refractive index

n_C: the C-line refractive index

For the zoom lens of such construction as described above, it is necessary not only to implement independent achromatization within the positive lens group located on the image plane side with respect to the aperture stop but also to correct the secondary spectra produced at the negative lens group on the object side with respect to the aperture stop; so it is desired to produce the secondary spectra at the positive lens group located on the image plane side with respect to the aperture stop in the opposite direction to normal. In this case, such selection of glass materials as described above becomes much more effective.

That is to say, with the recent progress of digitalized photography, there is a growing demand for how to address image quality degradation engendered by chromatic aberrations. For a zoom lens having an angle of view exceeding 70° at the wide-angle end, there is an increasing demand for further reductions in the chromatic blurring of peripheral images caused by chromatic aberration of magnification in particular. So far, making correction of the secondary spectra using fluorite having low dispersion and anomalous dispersion or glass close to it has been well known; however, there is still a limit to that.

This problem is solved by the following embodiments.

[1] A zoom lens, comprising a plurality of lens groups in which the space between them is varied for zooming, characterized in that at least one of said plurality of lens groups comprises at least two lenses made of two materials that meet the two following conditions and having the same sign:

ν_d≧80, θ_gF≧−0.001781ν_d+0.6494+0.02 (a)

ν_d≧30, θ_gF≧−0.001781ν_d+0.6494+0.01 (b)

where:

θ_gF=(n_g−n_F)/(n_F−n_C),

n_g: the g-line refractive index,

n_F: the F-line refractive index,

n_d: the d-line refractive index, and

n_C: the C-line refractive index.

[2] A zoom lens having an angle of view of at least 70° at a wide-angle end, comprising, in order from its object side, a positive first lens group, a negative second lens group, an aperture stop, and a lens group having generally positive power on an image plane side with respect to that, in which zooming is implemented while the space between adjoining lens groups is varied, characterized by further comprising on an image plane side with respect to said aperture stop at least two lenses formed of two materials that meet two following conditions and having the same sign:

ν_d≧80, θ_gF≧−0.001781ν_d+0.6494+0.02 (a)

ν_d≧30, θ_gF≧−0.001781ν_d+0.6494+0.01 (b)

where:

θ_gF=(n_g−n_F)/(n_F−n_C),

n_g: the g-line refractive index,

n_F: the F-line refractive index,

n_d: the d-line refractive index, and

n_C: the C-line refractive index.

In the invention, the space between two independently moving lenses groups is made dependent on the subject distance alone, and two such lens groups move as one single piece depending on the focal length, so that improvements in the short-distance performance are achievable by floating without making a mechanism in cooperation with the zoom mechanism complicated.

Still objects and advantages of the invention will be in part be obvious and will in part be apparent from the specification.

The invention accordingly comprises the features of construction, combinations of elements, and arrangement of parts which will be exemplified in the construction hereinafter set forth, and the scope of the invention will be indicated in the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is illustrative in lens section of Example 1 of the zoom lens according to the invention at the wide-angle end (a), in the intermediate state (b) and at the telephoto end (c) upon focusing on an object point at infinity.

FIG. 2 is illustrative, as in FIG. 1, of Example 2 of the zoom lens according to the invention.

FIG. 3 is illustrative, as in FIG. 1, of Example 3 of the zoom lens according to the invention.

FIG. 4 is an aberration diagram for Example 1 upon focusing on an object point at infinity.

FIG. 5 is an aberration diagram for Example 1 upon focusing on a subject distance of 75 cm.

FIG. 6 is an aberration diagram for Example 2 upon focusing on an object point at infinity.

FIG. 7 is an aberration diagram for Example 2 upon focusing on an subject distance of 37 cm.

FIG. 8 is an aberration diagram for Example 3 upon focusing on an object point at infinity.

FIG. 9 is an aberration diagram for Example 3 upon focusing on a subject distance of 35 cm.

FIG. 10 is illustrative in section including the optical axis of one example of the lens barrel used with the zoom lens of the invention.

FIG. 11 is illustrative in section including the optical axis of the barrel portion for the second group at an angular position different from that in FIG. 10.

FIG. 12 is illustrative of relative positions of the cam groove, key groove and cam pin for controlling the front and rear units of the second group in the lens barrel in the example of FIG. 10.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The zoom lens of the invention is now explained with reference to Examples 1, 2 and 3. FIGS. 1, 2, and 3 is illustrative in lens section of Example 1, 2, and 3, respectively, at the wide-angle end (a), in the intermediate state (b), and at the telephoto end (c) upon focusing on an object point at infinity. In each drawing, G1 is indicative of the first lens group, G2F the front unit of the second lens group, G2R the rear unit of the second lens group, S an aperture stop, G3 the third lens group, and I the image plane.

EXAMPLE 1

As shown in FIG. 1, Example 1 is directed to a zoom lens made up of, in order from its object side, the first lens group G1 having positive power, the negative power front unit G2F of the second lens group having negative power, the negative power rear unit G2R of the second lens group having negative power, the aperture stop S and the third lens group G3 having positive power. Upon zooming from the wide-angle end to the telephoto end, the first lens group G1 moves on a concave locus toward the object side, and is positioned more on the object side at the telephoto end than at the wide-angle end, and the front G2F and rear unit G2R of the second lens group G2 move together toward the image side. The aperture stop S and the third lens group G3 move together toward the object side. It is here noted that the locus of movement upon zooming of the second lens group G2 made up of the front G2F and the rear unit G2R varies depending on the subject distance (the distance from the subject to the image plane I).

Upon focusing from infinity to a short distance, the front G2F and the rear unit G2R of the second lens group move in a direction of the space between them becoming narrow, and that space depends on the subject distance but does not on a zooming position (the focal length).

In order from the object side, the first lens group G1 is made up of a negative meniscus lens convex on its object side and two positive meniscus lenses, each convex on its object side; the front unit G2F of the second lens group G2 is made up of two negative meniscus lenses each convex on its object side, a negative meniscus lens convex on its image side and a double-convex positive lens; the rear unit G2R of the second lens group G2 is made up of a double-concave negative lens and a positive meniscus lens convex on its object side; and the third lens group G3 is made up of a positive meniscus lens convex on its object side, a double-convex positive lens, a negative meniscus lens convex on its image side, a double-convex positive lens, a cemented lens of a negative meniscus lens convex on its object side and a double-convex positive lens, a negative meniscus lens convex on its image side, a double-convex positive lens and a positive meniscus lens convex on its image side.

Four aspheric surfaces are used: two at both surfaces of the second negative meniscus lens in the front unit G2F of the second lens group G2, and two at both surfaces of the double-convex positive lens located in the third lens group G3 and nearest to its image side.

EXAMPLE 2

As shown in FIG. 2, Example 2 is directed to a zoom lens made up of, in order from its object side, the first lens group G1 having positive power, the negative power front unit G2F of the second lens group having negative power, the negative power rear unit G2R of the second lens group having negative power, the aperture stop S and the third lens group G3 having positive power. Upon zooming from the wide-angle end to the telephoto end, the first lens group G1 moves on a concave locus toward the object side, and is positioned more on the object side at the telephoto end than at the wide-angle end, and the front G2F and rear unit G2R of the second lens group G2 move together toward the image side. The aperture stop S and the third lens group G3 move together toward the object side. It is here noted that the locus of movement upon zooming of the second lens group G2 made up of the front. G2F and the rear unit G2R varies depending on the subject distance (the distance from the subject to the image plane I).

In order from the object side, the first lens group G1 is made up of a negative meniscus lens convex on its object side, a double-convex positive lens and a positive meniscus lenses convex on its object side; the front unit G2F of the second lens group G2 is made up of two negative meniscus lenses each convex on its object side, a negative meniscus lens convex on its image side and a double-convex positive lens; the rear unit G2R of the second lens group G2 is made up of a double-concave negative lens and a double-convex positive lens; and the third lens group G3 is made up of two positive meniscus lenses each convex on its object side, a negative meniscus lens convex on its image side, a cemented lens of a negative meniscus lens convex on its object side and a double-convex positive lens, a double-concave negative lens, a double-convex positive lens, and a positive meniscus lens convex on its image side.

EXAMPLE 3

As shown in FIG. 3, Example 3 is directed to a zoom lens made up of, in order from its object side, the first lens group G1 having positive power, the negative power front unit G2F of the second lens group having negative power, the negative power rear unit G2R of the second lens group having negative power, the aperture stop S and the third lens group G3 having positive power. Upon zooming from the wide-angle end to the telephoto end, the first lens group G1 moves on a concave locus toward the object side, and is positioned more on the object side at the telephoto end than at the wide-angle end, and the front G2F and rear unit G2R of the second lens group G2 move together toward the image side. The aperture stop S and the third lens group G3 move together toward the object side. It is here noted that the locus of movement upon zooming of the second lens group G2 made up of the front G2F and the rear unit G2R varies depending on the subject distance (the distance from the subject to the image plane I).

In order from the object side, the first lens group G1 is made up of a negative meniscus lens convex on its object side, a plano-convex positive lens and a positive meniscus lens convex on its object side; the front unit G2F of the second lens group G2 is made up of two negative meniscus lenses each convex on its object side, a negative meniscus lens convex on its image side and a double-convex positive lens; the rear unit G2R of the second lens group G2 is made up of a double-concave negative lens and a positive meniscus lens convex on its object side; and the third lens group G3 is made up of a positive meniscus lens convex on its object side, a double-convex positive lens, a negative meniscus lens convex on its image side, a double-convex positive lens, a cemented lens of a double-concave negative lens and a double-convex positive lens, a negative meniscus lens convex on its image side, a double-convex positive lens and a positive meniscus lens convex on its image side.

In what follows, numerical data about each example are enumerated below, but symbols used hereinafter but not hereinbefore have the following meanings.

- f: the focal length of the whole optical system,
- F: the F-number,
- ω: the half angle of view,
- WE: the wide-angle end,
- ST: the intermediate state,
- TE: the telephoto end,
- r₁, r₂, . . . : the radius of curvature of each lens surface,
- d₁, d₂, . . . : the space between the adjacent lens surface,
- n_d1, n_d2, . . . : the d-line refractive index of each lens, and
- ν_d1, ν_d2, . . . : the Abbe constant of each lens.
  
  The bracketed figures after WE, ST and TE are the subject distances (mm) as measured from the image plane. Here suppose x and y to be an optical axis provided that the direction of travel of light is taken as positive and a direction orthogonal to that optical axis. Then, aspheric surface shape is given by

$x = (y^{2} / r) / [1 + {1 - (K + 1) {(y / r)}^{2}}^{1 / 2}] + A_{4} y^{4} + A_{6} y^{6} + A_{8} y^{8} + A_{10} y^{10}$

Here r is the paraxial radius of curvature, K is the conical coefficient, and A₄, A₆, A₈and A₁₀are the 4^th-, 6^th-, 8^th-, and 10^th-order aspheric coefficients.
EXAMPLE 1

r₁= 387.355
d₁= 2.63
n_d1= 1.84666
ν_d1= 23.78

r₂= 111.767
d₂= 0.01

r₃= 111.356
d₃= 6.47
n_d2= 1.77250
ν_d2= 49.60

r₄= 3365.600
d₄= 0.20

r₅= 57.289
d₅= 5.97
n_d3= 1.77250
ν_d3= 49.60

r₆= 111.018
d₆= (Variable)

r₇= 58.091
d₇= 2.01
n_d4= 1.88300
ν_d4= 40.76

r₈= 15.990
d₈= 8.04

r₉= 102.838
d₉= 1.92
n_d5= 1.58313
ν_d5= 59.38

(Aspheric)

r₁₀= 26.644
d₁₀= 7.47

(Aspheric)

r₁₁= −22.460
d₁₁= 1.62
n_d6= 1.48749
ν_d6= 70.23

r₁₂= −36.701
d₁₂= 0.15

r₁₃= 100.700
d₁₃= 4.32
n_d7= 1.84666
ν_d7= 23.78

r₁₄= −50.637
d₁₄= (Variable)

r₁₅= −52.349
d₁₅= 1.61
n_d8= 1.59469
ν_d8= 32.36

r₁₆= 72.901
d₁₆= 0.15

r₁₇= 60.892
d₁₇= 2.70
n_d9= 1.81454
ν_d9= 38.95

r₁₈= 173.601
d₁₈= (Variable)

r₁₉= ∞ (Stop)
d₁₉= 1.70

r₂₀= 49.288
d₂₀= 3.09
n_d10= 1.60753
ν_d10= 34.16

r₂₁= 503.698
d₂₁= 0.15

r₂₂= 51.547
d₂₂= 3.21
n_d11= 1.60280
ν_d11= 47.85

r₂₃= −934.636
d₂₃= 8.85

r₂₄= −38.354
d₂₄= 1.78
n_d12= 1.52117
ν_d12= 45.51

r₂₅= −1291.613
d₂₅= 0.01

r₂₆= 54.193
d₂₆= 3.95
n_d13= 1.49700
ν_d13= 81.54

r₂₇= −95.019
d₂₇= 0.28

r₂₈= 170.410
d₂₈= 1.60
n_d14= 1.68893
ν_d14= 31.08

r₂₉= 20.026
d₂₉= 8.23
n_d15= 1.43875
ν_d15= 94.93

r₃₀= −44.268
d₃₀= 0.20

r₃₁= −37.935
d₃₁= 1.59
n_d16= 1.90366
ν_d18= 31.31

r₃₂= −300.910
d₃₂= 0.22

r₃₃= 50.668
d₃₃= 7.09
n_d17= 1.49700
ν_d17= 81.54

(Aspheric)

r₃₄= −36.662
d₃₄= 0.15

(Aspheric)

r₃₅= −125.640
d₃₅= 2.83
n_d18= 1.84666
ν_d18= 23.78

r₃₆= −53.971
d₃₆= (Variable)

r₃₇= ∞

(Imaging plane)

Aspherical Coefficients

9th surface

K = 0.000

A₄= 1.73390 × 10⁻⁵

A₆= −9.68245 × 10⁻⁸

A₈= 3.34280 × 10⁻¹⁰

A₁₀= −8.36705 × 10⁻¹³

10th surface

K = 0.000

A₄= 1.02609 × 10⁻⁶

A₆= −1.24880 × 10⁻⁷

A₈= 2.22314 × 10⁻¹⁰

A₁₀= −9.85649 × 10⁻¹³

33th surface

K = 0.000

A₄= −8.54265 × 10⁻⁶

A₆= 5.69449 × 10⁻⁹

A₈= 2.26533 × 10⁻¹¹

A₁₀= −3.21043 × 10⁻¹⁴

34th surface

K = 0.000

A₄= 6.17864 × 10⁻⁶

A₆= −8.70372 × 10⁻⁹

A₈= 4.10560 × 10⁻¹¹

A₁₀= −5.71444 × 10⁻¹⁴

Zooming Data

WE (∞)
ST (∞)
TE (∞)
WE (750)
ST (750)
TE (750)

f (mm)
14.21
22.09
34.25
14.26
21.89
32.70

F_NO
2.05
2.06
2.04
2.04
2.05
2.02

2ω (°)
77.41
53.55
35.77
77.10
53.83
37.04

d₆
0.60
8.71
29.13
1.36
9.27
28.77

d₁₄
5.78
5.78
5.78
3.27
3.27
3.27

d₁₈
33.16
11.13
1.84
34.91
13.08
4.72

d₃₆
33.77
41.85
46.61
33.78
41.85
46.63

θ_gF
θ_gF− formula (6)

n_d13, n_d17
0.537
0.033

n_d15
0.534
0.054

n_d18
0.620
0.013

EXAMPLE 2

r₁= 731.588
d₁= 2.63
n_d1= 1.84666
ν_d1= 23.78

r₂= 126.803
d₂= 0.20

r₃= 127.949
d₃= 5.82
n_d2= 1.77250
ν_d2= 49.60

r₄= −685.027
d₄= 0.20

r₅= 51.823
d₅= 5.21
n_d3= 1.77250
ν_d3= 49.60

r₆= 98.011
d₆= (Variable)

r₇= 52.780
d₇= 1.82
n_d4= 4.88300
ν_d4= 40.76

r₈= 15.474
d₈= 8.29

r₉= 300.548
d₉= 1.90
n_d5= 1.58313
ν_d5= 59.38

(Aspheric)

r₁₀= 25.874
d₁₀= 6.79

(Aspheric)

r₁₁= −21.402
d₁₁= 1.64
n_d6= 1.49700
ν_d6= 81.54

r₁₂= −31.787
d₁₂= 0.15

r₁₃= 97.342
d₁₃= 3.54
n_d7= 1.84666
ν_d7= 23.78

r₁₄= −57.944
d₁₄= (Variable)

r₁₅= −53.518
d₁₅= 1.68
n_d8= 1.88300
ν_d8= 40.76

r₁₆= 249.374
d₁₆= 0.15

r₁₇= 131.919
d₁₇= 2.57
n_d9= 1.78590
ν_d9= 44.20

r₁₈= −160.127
d₁₈= (Variable)

r₁₉= ∞ (Stop)
d₁₉= 1.50

r₂₀= 67.896
d₂₀= 2.89
n_d10= 1.88300
ν_d10= 40.76

r₂₁= 1475.243
d₂₁= 0.15

r₂₂= 37.278
d₂₂= 3.65
n_d11= 1.49700
ν_d11= 81.54

r₂₃= 150.000
d₂₃= 14.37

r₂₄= −34.316
d₂₄= 1.90
n_d12= 1.86099
ν_d12= 22.46

r₂₅= −44.544
d₂₅= 0.29

r₂₆= 47.997
d₂₆= 1.60
n_d13= 1.68893
ν_d13= 31.08

r₂₇= 18.729
d₂₇= 8.67
n_d14= 1.43875
ν_d14= 94.93

r₂₈= −58.800
d₂₈= 0.16

r₂₉= −54.295
d₂₉= 1.67
n_d15= 2.00330
ν_d15= 28.27

r₃₀= 250.000
d₃₀= 0.15

r₃₁= −38.844
d₃₁= 6.97
n_d16= 1.49700
ν_d16= 81.54

(Aspheric)

r₃₂= −38.588
d₃₂= 0.15

(Aspheric)

r₃₃= −105.622
d₃₃= 2.57
n_d17= 1.92286
ν_d17= 18.90

r₃₄= −52.369
d₃₄= (Variable)

r₃₅= ∞

(Imaging plane)

Aspherical Coefficients

9th surface

K = 0.000

A₄= 7.49104 × 10⁻⁶

A₆= −6.68652 × 10⁻⁸

A₈= 2.18412 × 10⁻¹⁰

A₁₀= −7.28168 × 10⁻¹³

10th surface

K = 0.000

A₄= −1.14035 × 10⁻⁵

A₆= −8.77809 × 10⁻⁸

A₈= 4.80848 × 10⁻¹¹

A₁₀= −4.71742 × 10⁻¹³

31th surface

K = 0.000

A₄= −1.11257 × 10⁻⁵

A₆= 1.23604 × 10⁻⁸

A₈= −3.55905 × 10⁻¹¹

A₁₀= 5.54826 × 10⁻¹⁴

32th surface

K = 0.000

A₄= 4.79552 × 10⁻⁶

A₆= −5.36425 × 10⁻⁹

A₈= −1.84054 × 10⁻¹²

A₁₀= −4.74223 × 10⁻¹⁴

Zooming Data

WE (∞)
ST (∞)
TE (∞)
WE (370)
ST (370)
TE (370)

f (mm)
14.25
22.16
34.01
14.30
21.74
31.13

F_NO
2.05
2.06
2.04
2.04
2.03
1.99

2ω (°)
77.36
53.53
35.97
76.90
54.07
38.27

d₆
0.56
7.37
25.87
1.56
8.18
25.02

d₁₄
6.41
6.41
6.41
0.63
0.63
0.63

d₁₈
31.67
10.07
1.59
36.43
15.05
8.22

d₃₄
33.72
43.08
48.15
33.73
43.12
48.14

θ_gF
θ_gF− formula (6)

n_d11
0.537
0.033

n_d14
0.534
0.054

n_d17
0.649
0.034

EXAMPLE 3

r₁= 388.432
d₁= 2.63
n_d1= 1.84666
ν_d1= 23.78

r₂= 116.328
d₂= 0.19

r₃= 120.478
d₃= 6.23
n_d2= 1.77250
ν_d2= 49.60

r₄= ∞
d₄= 0.20

r₅= 55.418
d₅= 6.31
n_d3= 1.77250
ν_d3= 49.60

r₆= 106.616
d₆= (Variable)

r₇= 58.092
d₇= 2.01
n_d4= 1.88300
ν_d4= 40.76

r₈= 15.659
d₈= 8.62

r₉= 499.999
d₉= 1.92
n_d5= 1.58253
ν_d5= 59.32

(Aspheric)

r₁₀= 31.329
d₁₀= 6.88

(Aspheric)

r₁₁= −22.540
d₁₁= 1.62
n_d6= 1.48749
ν_d6= 70.23

r₁₂= −34.382
d₁₂= 0.15

r₁₃= 109.408
d₁₃= 4.13
n_d7= 1.84666
ν_d7= 23.78

r₁₄= −52.304
d₁₄= (Variable)

r₁₅= −53.386
d₁₅= 1.61
n_d8= 1.62004
ν_d8= 36.26

r₁₆= 90.446
d₁₆= 0.15

r₁₇= 74.131
d₁₇= 2.68
n_d9= 1.78590
ν_d9= 44.20

r₁₈= 577.522
d₁₈= (Variable)

r₁₉= ∞ (Stop)
d₁₉= 1.70

r₂₀= 54.962
d₂₀= 2.98
n_d10= 1.63980
ν_d10= 34.46

r₂₁= 477.175
d₂₁= 0.15

r₂₂= 44.882
d₂₂= 3.94
n_d11= 1.62280
ν_d11= 57.05

r₂₃= −400.001
d₂₃= 9.25

r₂₄= −37.960
d₂₄= 1.79
n_d12= 1.57501
ν_d12= 41.50

r₂₅= −300.000
d₂₅= 0.15

r₂₆= 90.287
d₂₆= 3.53
n_d13= 1.49700
ν_d13= 81.54

r₂₇= −67.879
d₂₇= 0.29

r₂₈= −1026.371
d₂₈= 1.60
n_d14= 1.68893
ν_d14= 31.08

r₂₉= 21.042
d₂₉= 7.45
n_d15= 1.43875
ν_d15= 94.93

r₃₀= −44.725
d₃₀= 0.17

r₃₁= −40.315
d₃₁= 1.59
n_d16= 1.90366
ν_d16= 31.31

r₃₂= −1452.783
d₃₂= 0.15

r₃₃= 45.448
d₃₃= 7.46
n_d17= 1.49640
ν_d17= 81.24

(Aspheric)

r₃₄= −36.320
d₃₄= 0.15

(Aspheric)

r₃₅= −2245.818
d₃₅= 2.90
n_d18= 1.63494
ν_d18= 23.22

r₃₆= −56.553
d₃₆= (Variable)

r₃₇= ∞

(Imaging plane)

Aspherical Coefficients

9th surface

K = 0.000

A₄= 2.33955 × 10⁻⁵

A₆= −1.46412 × 10⁻⁷

A₈= 5.37937 × 10⁻¹⁰

A₁₀= −1.32462 × 10⁻¹²

10th surface

K = 0.000

A₄= 7.38718 × 10⁻⁶

A₆= −1.66142 × 10⁻⁷

A₈= 3.75503 × 10⁻¹⁰

A₁₀= −1.27423 × 10⁻¹²

33th surface

K = 0.000

A₄= −1.05652 × 10⁻⁵

A₆= 6.57981 × 10⁻¹⁰

A₈= 4.92273 × 10⁻¹¹

A₁₀= −8.47219 × 10⁻¹⁴

34th surface

K = 0.000

A₄= 4.57324 × 10⁻⁶

A₆= −1.30667 × 10⁻⁸

A₈= 5.78315 × 10⁻¹¹

A₁₀= −9.06114 × 10⁻¹⁴

Zooming Data

WE (∞)
ST (∞)
TE (∞)
WE (350)
ST (350)
TE (350)

f (mm)
14.22
22.08
34.28
13.95
21.04
30.04

F_NO
2.04
2.04
2.04
2.03
2.01
1.99

2ω (°)
77.45
53.63
35.87
78.51
55.55
39.57

d₆
0.60
9.28
28.72
0.76
9.09
26.50

d₁₄
6.20
6.20
6.20
0.85
0.85
0.85

d₁₈
33.99
11.81
1.99
39.19
17.36
9.57

d₃₆
33.77
41.71
46.62
33.78
41.76
46.60

θ_gF
θ_gF− formula (6)

n_d13, n_d17
0.537
0.033

n_d15
0.534
0.054

n_d18
0.668
0.060

FIGS. 4 and 5 are aberration diagrams for Example 1 upon focusing on an object point at infinity and a close-range object at a subject distance of 75 cm, respectively. Shown in these aberration diagrams are spherical aberration (SA), astigmatism (AS), distortion (DT) and chromatic aberration of magnification (CC) at the wide-angle end (a), in the intermediate state (b), and at the telephoto end (c), respectively, with “FIY” representing the maximum image height (mm). Similar aberration diagrams for Examples 2 and 3 are shown in FIGS. 6 and 7 (upon focusing on a close-range object at a subject distance of 37 cm) and FIGS. 8 and 9 (upon focusing on a close-range object at a subject distance of 35 cm), respectively.

One example of the lens barrel used with the inventive zoom lens is now explained. FIG. 10 is illustrative in section including the optical axis of the lens barrel here, and FIG. 11 is illustrative in section including the optical axis of a barrel portion for the second (lens) group at an angular position different from that of FIG. 10. It is here noted that this lens barrel comprises a zooming mechanism and a focusing mechanism for the zoom lens.

The lens barrel here embodies a zoom lens's zooming mechanism to be attached to cameras, digital cameras or the like. A fixed frame 11 is attached to an inner housing 10 forming a part of the barrel body, and a cam frame 12 rotatable about the optical axis is located around that. And as a zoom annulus 13 located near the rear end of the lens barrel and having a zoom rubber 14 wound around it is rotated, it causes rotation of a zoom pin 15 fixed inside of the zoom annulus 13. The end of the zoom pin 15 is planted in the cam frame 12, so that the cam frame 12 rotates together with the zoom annulus 13.

First, reference is made to the zooming mechanism for the third (lens) group that is implemented by the rotation of the zoom annulus 13.

The cam frame 12 is provided in it with a third group cam groove 16 for moving the third group, the fixed frame 11 positioned inside the cam frame 12 is provided in it with a third group key groove 17 running in the optical axis direction, and a third group cam pin 19 planted in a third group frame 18 in the fixed frame 11 is in engagement within the third group key groove 17 in the fixed frame 11 and the third group cam groove 16 in the cam frame 12.

Accordingly, as the zoom annulus 13 rotates, it permits the cam frame 12 to rotates so that the third group frame 18 moves along the locus of the third group cam groove 17 in the cam frame 12 in the optical axis direction.

Then, reference is made to the zooming mechanism for the first (lens) group that is implemented by the rotation of the zoom annulus 13.

The cam frame 12 is provided in it with a first cam groove 20 for moving the first group, and an inwardly extending first cam pin 11 is planted in a first group frame 21 with its end in engagement within the first cam groove 20 in the cam frame 12.

On the other hand, the fixed frame 11 is planted with a straightforward first group pin 23, and the end of that first group pin 23 is in engagement by way of the opening in the cam frame 12 within a first group key groove 24 provided in the first group frame 21 and running in the optical axis direction.

Accordingly, the first group frame 21 is kept against rotation by the engagement of the first straight-forward pin 23 within the first group key groove 24, but as the cam frame 13 rotates, it moves along the locus of the first group cam groove 20 in the cam frame 12 in the optical axis direction.

Then, reference is made to the zooming mechanism for the second (lens) group that is implemented by the rotation of the zoom annulus 13.

The fixed frame 11 is provided in it with a second group cam groove 25 for moving a second group zoom frame 26 in the optical axis direction while rotating it, the came frame 12 is provided in it with a second group key groove 27 that intersects that second group cam groove 25 and runs in the optical axis direction, the second group zoom frame 26 located inside the fixed frame 11 is planted with an outwardly extending second cam pin 28, and the end of the second group cam pin 28 is in engagement by way of the second group cam groove 25 in the fixed frame 11 within the second group key groove 27 provided in the cam frame 12 and running in the optical axis direction.

And a frame 29 for the second group's rear unit is located in the second group zoom frame 26, and an outwardly extending cam pin 30 for the second group's rear unit is planted in the frame 29 for the second group's rear unit, with its end in engagement within a cam groove 31 for the second group's rear unit that is located in the second group zoom frame 26.

A frame 32 for the second group's front unit is located within the frame 29 for the second group's rear unit, an outwardly extending cam pin 33 for the second group's front unit is planted in the frame 32 for the second group's front unit, and the cam pin 33 for the second group's front unit has its end in engagement within a key groove 35 located in the fixed frame 11 and running in the optical axis direction by way of a cam groove 34 for the second group's front unit located in the frame 29 for the second group's rear unit and the opening in the second group zoom frame 26.

A key groove 36 for the second group's rear unit running in the optical axis direction is located in the frame 29 for the second group's rear unit, and a distance lever 38 fixed to a distance frame 37 and extending in the optical axis direction is in engagement within that key groove 36 for the second group's rear unit so that the frame 29 for the second group's rear unit is movable only in the optical axis direction under the action of that distance lever 38.

Accordingly, as the cam frame 12 rotates, the second group zoom frame 26 rotates and moves along the locus of the second group cam groove 25 in the optical axis direction under the interaction between the second group key groove 28 provided in the cam frame 12, the second group cam pin 28 provided in the second group zoom frame 27 and the second group cam groove 25 provided in the fixed frame 11. As the second group zoom frame 26 rotates and moves, the frame 29 for the second group's rear unit kept against rotation by the distance lever 38 moves with respect to the second group zoom frame 26 in the optical axis direction under the interaction between the cam pin 30 planted therein for the second group's rear unit and the cam groove 31 for the second group's rear unit provided in the second group zoom frame 27. Consequently, the cam groove 31 for the second group's rear unit moves in the optical axis direction under the actions of both cam grooves, the second group cam groove 25 (provided in the fixed frame 11) and the cam groove 31 for the second group's rear unit (provided in the second group zoom frame 26).

In this case, the frame 32 for the second group's front unit is kept against rotation by the actions of the key groove 35 for the second group's front unit provided in the fixed frame 11 and the cam pin 33 for the second group's front unit planted in the frame 32 for the second group's front unit; there is neither the relative rotation of the frame 32 for the second group's front unit and the frame 29 for the second group's rear unit nor the relative movement of the frame 32 for the second group's front unit and the cam groove 34 for the second group's front unit, making sure the movement of the frame 32 for the second group's front unit together with the frame 29 for the second group's rear unit in the optical axis direction.

Next, reference is made to the focusing mechanism due to a spacing change between the second group's front and rear units implemented by the rotation of a distance annulus 40.

Upon the rotation of the distance annulus 40 located near the front end of the lens barrel and having a distance rubber 41 wound around it, a distance pin 42 fixed to the inside of the distance annulus 40 rotates. A distance pin 42 has its end planted in a distance frame 37 so that the distance frame 37 rotates in unison with the distance annulus 40. As the distance frame 37 rotates, the frame 29 for the second group's rear unit rotates under the actions of the distance lever 38 and the key groove 36 for the second group's rear unit, and the came pin 30 for the second group's rear unit rotates as well. The end of the cam pin. 30 for the second group's rear unit is in engagement within the cam groove 31 for the second group's rear unit in the second group zoom frame 26 so that the frame 29 for the second group's rear frame rotates and moves along the locus of the cam groove 31 for the second group's rear unit in the optical axis direction. The cam groove 34 for the second group's front unit is provided in the frame 29 for the second group's rear unit and the cam pin 33 for the second group's front unit, which is kept against rotation by the key groove 35 for the second group's front unit located in the fixed frame 11, extends through the cam groove 34 for the second group's front unit, so that by the rotation and movement of the frame 29 for the second group's rear unit, the cam pin 33 for the second group's front unit moves relative to the frame 29 for the second group's rear unit in the optical axis direction with the movement of the frame 32 for the second group's front unit relative to the frame 29 for the second group's rear unit.

FIG. 12 is illustrative of the relative positions of the cam grooves 25, 31, 34, the key grooves 27, 35 and the cam pins 28, 30, 33 all adapted to control the movement of the second group's front and rear units. The positions of the cam pin 33 for the second group's front unit and the cam pin 30 for the second group's rear unit in the directions of the key grooves 27 and 35 define the positions of the second group's front and rear units (the frames 32 and 29 for the second group's front and rear units) in the optical axis direction, respectively. And FIG. 12(a) is illustrative of a state controlled to an infinite distance at the wide-angle end; FIG. 12(b) is illustrative of a state controlled from the wide-angle end position of (a) to a short distance position; FIG. 12(c) is illustrative of a state controlled from the position of (a) to an infinite distance at the telephoto end; and FIG. 12(d) is illustrative of a state controlled from the telephoto end position of (c) to a short distance position at the telephoto end.

As, in the state of FIG. 12(a), the distance annulus 40 is rotated to rotate the distance frame 37, the frame 29 for the second group's rear unit rotates under the action of the distance lever 38, and the cam pin 30 for the second group's rear unit planted in the frame 29 for the second group's rear unit moves along the cam groove 31 for the second group's rear unit in the second group zoom frame 26, as depicted in FIG. 12(b) with the result that the frame 29 for the second group's rear unit rotates and moves. With this, the cam groove 34 for the second group's front unit provided in the frame 29 for the second group's rear unit, too, rotates and moves from a broken line position to a solid line position. Upon the rotation and movement of the cam groove 34 for the second group's front unit, the cam pin 33 for the second group's front unit located at the position of intersection of the key grooves 35 and 34 for the second group's front and rear units provided in the fixed frame 11 moves too. Accordingly, the second group's front and rear units (the frames 32 and 29 for the second group's front and rear units) move by a given distance in the optical axis direction while their spacing varies relatively.

On the other hand, as, in the state of FIG. 12(a), the zoom annulus 13 is rotated to rotate the cam frame 12, the second group key groove 27 rotates from a broken line position to a solid line position, as depicted in FIG. 12(c), and the second group cam pin 28 located at the position of intersection with the second group cam groove 25 provided in the fixed frame 11 rotates and moves, and the second group zoom frame 26 with the second group cam pin 28 planted in it rotates and moves too. With this, the cam groove 31 for the second group's rear unit provided in the second group zoom frame 26, too, rotates and moves from a broken line position to a solid line position. Upon the rotation and movement of the cam groove 31 for the second group's rear unit, the cam pin 30 for the second group's rear unit in engagement within it moves relatively along the cam groove 31 for the second group's rear unit because the distance lever 38 acts as a key, and the cam pin 30 for the second group's rear unit moves by a given distance along the optical axis direction under the action of both cam grooves, the second group cam groove 25 and the cam groove 31 for the second group's rear unit. As the cam pin 30 for the second group's rear unit moves in the optical axis direction, the frame 29 for the second group's rear unit planted in it moves together with the cam groove 34 for the second group's front unit from a broken line position to a solid line position. Thus, the cam pin 33 for the second group's front unit located at the position of intersection of the key groove 35 for the second group's front unit and the cam groove 34 for the second group's front unit provided in the fixed frame 11, too, moves the same distance in the same direction as the cam pin 30 for the second group's rear unit. Consequently, the front and rear units of the second group (the frames 32 and 29 for the second group's front and rear frames), while they are kept at a given distance, move by a given distance in the optical axis direction under the action of both cam grooves, the second groove cam groove 25 and the cam groove 31 for the second group's rear unit.

As, in the state of FIG. 12(c), the distance annulus 40 is rotated to rotate the distance frame 37, the frame 29 for the second group's rear unit rotates under the action of the distance lever 38, and the cam pin 30 for the second group's rear unit planted in the frame 29 for the second group's rear unit moves along the cam groove 31 for the second group's rear unit in the second group zoom frame 26, as depicted in FIG. 12(d), with the result that the frame 29 for the second group's rear unit rotates and moves. With this, the cam groove 34 for the second group's front unit provided in the frame 29 for the second group's rear unit, too, rotates and moves from a broken line position to a solid line position. Upon the rotation and movement of the cam groove 34 for the second group's front unit, the cam pin 33 located at the position of intersection of the key groove 35 and cam groove 34 for the second group's front unit provided in the fixed frame 11 moves too. Consequently, the second group's front and rear units (the frames 32 and 29 for the second group's front and rear units) move by a given distance in the optical axis direction while their spacing varies relatively.

While the inventive zoom lens and the lens barrel for it have been described with reference to the specific embodiments, it is contemplated that the invention is never limited to them, and so may be modified in various fashions.

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CPC

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Priority Claims (1)