JPWO2020157905A1 - Manufacturing method of variable magnification optical system, optical equipment and variable magnification optical system - Google Patents

Abstract

The variable magnification optical system (ZL) consists of a first lens group (G1) having a positive refractive force, a second lens group (G2) having a negative refractive force, and a positive refractive force arranged in order from the object side. It has a third lens group (G3), a fourth lens group (G4) having a positive refractive power, a fifth lens group (G5), and a sixth lens group (G6), and has a variable magnification. At that time, a plurality of lens groups in the variable magnification optical system (ZL) move, the distance between adjacent lens groups changes, and there is an aperture (S) that moves at the time of magnification change. Of the moving lens groups, the lens group on the image side and the aperture (S) move integrally at the time of scaling.

Description

The present invention relates to a variable magnification optical system, an optical device using the variable magnification optical system, and a method for manufacturing the variable magnification optical system.

Conventionally, variable magnification optical systems suitable for photographic cameras, electronic still cameras, video cameras and the like have been proposed (see, for example, Patent Document 1). When the variable magnification optical system is increased in magnification and the angle of view is widened, it is difficult to obtain good optical performance, and the variable magnification optical system tends to be large in size.

Japanese Unexamined Patent Publication No. 9-184981

The variable magnification optical system according to the first aspect includes a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a first lens group having a positive refractive power arranged in order from the object side. A variable magnification optical system having three lens groups, a fourth lens group having a positive refractive power, a fifth lens group, and a sixth lens group, and the variable magnification optical system at the time of magnification change. The plurality of lens groups in the above are moved, the distance between adjacent lens groups is changed, the lens group has an aperture that moves at the time of magnification change, and the lens group on the image side most of the lens groups that move at the time of magnification change. The aperture and the aperture move integrally at the time of scaling.

The variable magnification optical system according to the second aspect includes a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a second lens group having a positive refractive power arranged in order from the object side. A variable magnification optical system having three lens groups, a fourth lens group having a positive refractive power, a fifth lens group, and a sixth lens group, and the variable magnification optical system at the time of magnification change. The lens group on the image side and the third lens group among the lens groups that move at the time of magnification change due to the movement of a plurality of lens groups including the third lens group in And, move integrally when scaling.

The optical device according to the third aspect is configured to include the above-mentioned variable magnification optical system.

The method for manufacturing the variable magnification optical system according to the fourth aspect includes a first lens group having a positive refractive force, a second lens group having a negative refractive force, and a positive refractive force arranged in order from the object side. A method for manufacturing a variable magnification optical system having a third lens group having a positive refractive power, a fourth lens group having a positive refractive power, a fifth lens group, and a sixth lens group. , The plurality of lens groups in the variable magnification optical system move, the distance between adjacent lens groups changes, and the lens group that moves at the time of magnification change is the most among the lens groups that move at the time of magnification change. Each lens is arranged in the lens barrel so that the lens group on the image side and the aperture move integrally when the magnification is changed.

It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 1st Example. 2 (A) and 2 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the first embodiment, respectively. 3 (A) and 3 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the first embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 2nd Example. 5 (A) and 5 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the second embodiment, respectively. 6 (A) and 6 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the second embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 3rd Example. 8 (A) and 8 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the third embodiment, respectively. 9 (A) and 9 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the third embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 4th Example. 11 (A) and 11 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fourth embodiment, respectively. 12 (A) and 12 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fourth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 5th Example. 14 (A) and 14 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fifth embodiment, respectively. 15 (A) and 15 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fifth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 6th Example. 17 (A) and 17 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the sixth embodiment, respectively. 18 (A) and 18 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the sixth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 7th Example. 20 (A) and 20 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the seventh embodiment, respectively. 21 (A) and 21 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the seventh embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 8th Example. 23 (A) and 23 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eighth embodiment, respectively. 24 (A) and 24 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eighth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 9th Example. 26 (A) and 26 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the ninth embodiment, respectively. 27 (A) and 27 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the ninth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 10th Example. 29 (A) and 29 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the tenth embodiment, respectively. 30 (A) and 30 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the tenth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on eleventh embodiment. 32 (A) and 32 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eleventh embodiment, respectively. 33 (A) and 33 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eleventh embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on a twelfth embodiment. 35 (A) and 35 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the twelfth embodiment, respectively. 36 (A) and 36 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the twelfth embodiment, respectively. It is a lens block diagram at the time of infinity focusing in the wide-angle end state of the variable magnification optical system which concerns on 13th Example. 38 (A) and 38 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the thirteenth embodiment, respectively. 39 (A) and 39 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the thirteenth embodiment, respectively. It is a figure which shows the structure of the camera provided with the variable magnification optical system which concerns on 1st and 2nd Embodiment. It is a flowchart which shows the manufacturing method of the variable magnification optical system which concerns on 1st Embodiment.

Hereinafter, the variable magnification optical system and the optical device according to the first and second embodiments will be described with reference to the drawings. First, a camera (optical device) provided with a variable magnification optical system according to the first and second embodiments will be described with reference to FIG. 40. As shown in FIG. 40, the camera 1 is a digital camera provided with the variable magnification optical system according to the first and second embodiments as the photographing lens 2. In the camera 1, the light from an object (subject) (not shown) is collected by the photographing lens 2 and reaches the image sensor 3. As a result, the light from the subject is captured by the image sensor 3 and recorded as a subject image in a memory (not shown). In this way, the photographer can shoot the subject with the camera 1. This camera may be a mirrorless camera or a single-lens reflex type camera having a quick return mirror.

Next, the variable magnification optical system (photographing lens) according to the first embodiment will be described. As an example of the variable magnification optical system (zoom lens) ZL according to the first embodiment, the variable magnification optical system ZL (1) has a positive refractive power arranged in order from the object side as shown in FIG. 1 lens group G1, a second lens group G2 having a negative refractive power, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, and a fifth lens group G5. And a sixth lens group G6. At the time of scaling, a plurality of lens groups in the variable magnification optical system ZL (1) move, and the distance between adjacent lens groups changes. As a result, fluctuations in astigmatism and spherical aberration during scaling can be suppressed. Further, the variable magnification optical system ZL (1) has an aperture (aperture aperture S) that moves when the magnification is changed, and the lens group on the image side and the aperture are the most image-side lens groups among the lens groups that move when the magnification is changed. , Moves integrally when scaling. As a result, the diameter of the lens barrel including the mechanical mechanism can be reduced while ensuring good optical performance. As described above, according to the first embodiment, it is possible to obtain a variable magnification optical system having a high magnification ratio and good optical performance, and an optical device provided with the variable magnification optical system.

Next, the variable magnification optical system according to the second embodiment will be described. Since the variable magnification optical system according to the second embodiment has the same configuration as the variable magnification optical system ZL according to the first embodiment, it will be described with the same reference numerals as those of the first embodiment. As an example of the variable magnification optical system (zoom lens) ZL according to the second embodiment, the variable magnification optical system ZL (1) has a positive refractive power arranged in order from the object side as shown in FIG. 1 lens group G1, a second lens group G2 having a negative refractive power, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, and a fifth lens group G5. And a sixth lens group G6. At the time of scaling, a plurality of lens groups including the third lens group G3 in the variable magnification optical system ZL (1) move, and the distance between adjacent lens groups changes. As a result, fluctuations in astigmatism and spherical aberration during scaling can be suppressed. Further, among the lens groups that move at the time of magnification change, the lens group on the image side and the third lens group G3 move integrally at the time of magnification change. As a result, the diameter of the lens barrel including the mechanical mechanism can be reduced while ensuring good optical performance. As described above, according to the second embodiment, it is possible to obtain a variable magnification optical system having a high magnification ratio and good optical performance, and an optical device provided with the variable magnification optical system.

The variable magnification optical system ZL according to the first and second embodiments may be the variable magnification optical system ZL (2) shown in FIG. 4, the variable magnification optical system ZL (3) shown in FIG. 7, and is shown in FIG. The variable magnification optical system ZL (4) may be used, or the variable magnification optical system ZL (5) shown in FIG. 13 may be used. Further, the variable magnification optical system ZL according to the first and second embodiments may be the variable magnification optical system ZL (6) shown in FIG. 16, the variable magnification optical system ZL (7) shown in FIG. 19, and FIG. 22. The variable magnification optical system ZL (8) shown in FIG. 25 may be used, or the variable magnification optical system ZL (9) shown in FIG. 25 may be used. Further, the variable magnification optical system ZL according to the first and second embodiments may be the variable magnification optical system ZL (10) shown in FIG. 28, the variable magnification optical system ZL (11) shown in FIG. 31, and FIG. 37. The variable magnification optical system ZL (13) shown in the above may be used.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the sixth lens group G6 is composed of two or more lenses. As a result, it is possible to suppress the occurrence of curvature of field and chromatic aberration of magnification.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the sixth lens group G6 and the diaphragm move integrally at the time of magnification change. As a result, the diameter of the lens barrel including the mechanical mechanism can be reduced while ensuring good optical performance.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the sixth lens group G6 and the third lens group G3 move integrally at the time of magnification change. As a result, the diameter of the lens barrel including the mechanical mechanism can be reduced while ensuring good optical performance.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the aperture and the third lens group G3 move integrally at the time of magnification change. As a result, the diameter of the lens barrel including the mechanical mechanism can be reduced while ensuring good optical performance.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (1).

3.00 <ft / fw <30.00 ... (1)
However, ft: the focal length of the variable magnification optical system ZL in the telephoto end state fw: the focal length of the variable magnification optical system ZL in the wide-angle end state.

The conditional expression (1) defines the magnification ratio of the variable magnification optical system ZL. By satisfying the conditional expression (1), the effect of the present embodiment can be maximized at a high scaling ratio. By setting the lower limit value of the conditional expression (1) to 3.30, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the lower limit of the conditional expression (1) is set to 3.50, 4.00, 4.50, 5.00, 6.00, and further 7.00. You may set it. Further, by setting the upper limit value of the conditional expression (1) to 25.00, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (1) may be set to 20.00, 15.00, 10.00, 9.00, and further 8.00. good.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (2).

35.0 ° <ωw <75.0 ° ・ ・ ・ (2)
However, ωw: half angle of view of the variable magnification optical system ZL in the wide-angle end state

The conditional expression (2) defines the half angle of view of the variable magnification optical system ZL in the wide-angle end state. By satisfying the conditional expression (2), the curvature of field can be satisfactorily corrected. By setting the lower limit value of the conditional expression (2) to 38.0 °, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit value of the conditional expression (2) may be set to 40.0 °. Further, by setting the upper limit value of the conditional expression (2) to 70.0 °, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (2) may be set to 60.0 °, 50.0 °, and further 45.0 °.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (3).

2.5 ° <ωt <15.0 ° ・ ・ ・ (3)
However, ωt: half angle of view of the variable magnification optical system ZL in the telephoto end state

The conditional expression (3) defines the half angle of view of the variable magnification optical system ZL in the telephoto end state. By satisfying the conditional expression (3), the effect of the present embodiment can be maximized at a high scaling ratio. By setting the lower limit value of the conditional expression (3) to 4.0 °, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (3) may be set to 5.0 ° and further 5.5 °. Further, by setting the upper limit value of the conditional expression (3) to 13.0 °, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (3) may be set to 12.0 °, 11.0 °, 10.0 °, and further 9.0 °. good.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (4).

−0.30 <fw / f123w <0.60 ・ ・ ・ (4)
However, fw: focal length of the variable magnification optical system ZL in the wide-angle end state f123w: combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3 in the wide-angle end state.

Conditional expression (4) defines the ratio between the focal length of the variable magnification optical system ZL in the wide-angle end state and the combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3. It is a thing. The conditional expression (4) means that the first lens group G1, the second lens group G2, and the third lens group G3 are substantially afocal in the wide-angle end state. By satisfying the conditional expression (4), spherical aberration and curvature of field in the wide-angle end state can be satisfactorily corrected.

When the corresponding value of the conditional expression (4) is less than the lower limit value, it becomes difficult to correct the spherical aberration in the wide-angle end state. By setting the lower limit value of the conditional expression (4) to −0.28, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the lower limit of the conditional expression (4) may be set to -0.25, -0.20, -0.15, and further -0.12. good.

If the corresponding value of the conditional expression (4) exceeds the upper limit value, it becomes difficult to correct the spherical aberration in the wide-angle end state. By setting the upper limit value of the conditional expression (4) to 0.55, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the upper limit of the conditional expression (4) is set to 0.50, 0.45, 0.40, 0.35, 0.30, 0.25, 0. It may be set to .20, 0.15, 0.10, and further 0.05.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (5).

-1.50 <ft / f123t <1.00 ... (5)
However, ft: the focal length of the variable magnification optical system ZL in the telephoto end state f123t: the combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3 in the telephoto end state.

Conditional expression (5) defines the ratio between the focal length of the variable magnification optical system ZL in the telephoto end state and the combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3. It is a thing. The conditional expression (5) means that the first lens group G1, the second lens group G2, and the third lens group G3 are substantially afocal in the telephoto end state. By satisfying the conditional expression (5), spherical aberration and curvature of field in the telephoto end state can be satisfactorily corrected.

When the corresponding value of the conditional expression (5) is less than the lower limit value, it becomes difficult to correct the spherical aberration in the telephoto end state. By setting the lower limit value of the conditional expression (5) to −1.35, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (5) may be set to −1.00, −0.90, and further −0.80.

If the corresponding value of the conditional expression (5) exceeds the upper limit value, it becomes difficult to correct the spherical aberration in the telephoto end state. By setting the upper limit value of the conditional expression (5) to 0.50, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (5) may be set to 0.20, 0.10, −0.10, and further −0.20.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (6).

0.20 <BFw / fw <0.60 ... (6)
However, BFw: the distance from the lens surface to the image plane of the variable magnification optical system ZL in the wide-angle end state fw: the focal length of the variable magnification optical system ZL in the wide-angle end state.

Conditional expression (6) defines the ratio of the back focus of the variable magnification optical system ZL to the focal length of the variable magnification optical system ZL in the wide-angle end state. By satisfying the conditional expression (6), the curvature of field in the wide-angle end state can be efficiently corrected.

When the corresponding value of the conditional expression (6) is less than the lower limit value, it becomes difficult to correct the curvature of field in the wide-angle end state. By setting the lower limit value of the conditional expression (6) to 0.25, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (6) may be set to 0.30, 0.35, 0.37, and further 0.40.

If the corresponding value of the conditional expression (6) exceeds the upper limit value, the correction of curvature of field in the wide-angle end state becomes insufficient. By setting the upper limit value of the conditional expression (6) to 0.56, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (6) may be set to 0.54, 0.52, and further 0.50.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the fifth lens group G5 moves with respect to the image plane at the time of focusing. As a result, fluctuations in spherical aberration during focusing can be suppressed.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the fifth lens group G5 has at least one positive lens and at least one negative lens. As a result, fluctuations in curvature of field during focusing can be suppressed.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (7).

1.00 <(-f5) / fw <16.00 ... (7)
However, f5: focal length of the fifth lens group G5 fw: focal length of the variable magnification optical system ZL in the wide-angle end state.

The conditional equation (7) defines the ratio between the focal length of the fifth lens group G5 and the focal length of the variable magnification optical system ZL in the wide-angle end state. By satisfying the conditional expression (7), the curvature of field generated at the time of focusing can be satisfactorily corrected.

If the corresponding value of the conditional expression (7) is less than the lower limit value, it becomes difficult to suppress the curvature of field that occurs during focusing. By setting the lower limit value of the conditional expression (7) to 1.10, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (7) may be set to 1.20, 1.30, 1.40, and further 1.45.

If the corresponding value of the conditional expression (7) exceeds the upper limit value, the correction of the curvature of field generated at the time of focusing becomes insufficient. Further, since the amount of movement of the fifth lens group G5 during focusing becomes large, the lens barrel becomes large. By setting the upper limit value of the conditional expression (7) to 15.50, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the upper limit of the conditional expression (7) is set to 10.00, 8.00, 5.00, 4.00, 3.00, 2.45, 2 It may be set to .38, 2.33, 2.28, 2.25, and further 2.10.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (8).

1.00 <Mv5 / Mv6 <3.00 ... (8)
However, Mv5: the amount of movement of the fifth lens group G5 when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object is +).
Mv6: Amount of movement of the sixth lens group G6 when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object is +).

Conditional expression (8) defines the ratio of the amount of movement of the fifth lens group G5 to the amount of movement of the sixth lens group G6 when scaling from the wide-angle end state to the telephoto end state. By satisfying the conditional expression (8), the curvature of field can be satisfactorily corrected.

When the corresponding value of the conditional expression (8) is less than the lower limit value, it becomes difficult to suppress the curvature of field generated in the fifth lens group G5. By setting the lower limit value of the conditional expression (8) to 1.10, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (8) may be set to 1.20, 1.30, and further 1.40.

If the corresponding value of the conditional expression (8) exceeds the upper limit value, it becomes difficult to correct the curvature of field in the fifth lens group G5. By setting the upper limit value of the conditional expression (8) to 2.50, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (8) may be set to 2.00, 1.80, and further 1.60.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the first lens group G1 moves with respect to the image plane at the time of magnification change. This makes it possible to obtain a high scaling ratio.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the first lens group G1 is composed of three or more lenses. As a result, spherical aberration can be satisfactorily corrected, especially in the telephoto end state. Moreover, it becomes possible to obtain a high scaling ratio.

It is desirable that the variable magnification optical system ZL according to the first and second embodiments satisfies the following conditional expression (9).

0.30 <Mv1 / (ft-fw) <0.80 ... (9)
However, Mv1: the amount of movement of the first lens group G1 when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object is +).
ft: Focal length of the variable magnification optical system ZL in the telephoto end state fw: Focal length of the variable magnification optical system ZL in the wide-angle end state

The conditional expression (9) defines the amount of movement of the first lens group G1 with respect to the change in the focal length at the time of scaling from the wide-angle end state to the telephoto end state. By satisfying the conditional expression (9), spherical aberration and curvature of field in the telephoto end state can be satisfactorily corrected.

When the corresponding value of the conditional expression (9) is less than the lower limit value, it becomes difficult to correct the spherical aberration in the telephoto end state. By setting the lower limit value of the conditional expression (9) to 0.32, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the lower limit of the conditional expression (9) may be set to 0.33, 0.34, and further 0.35.

If the corresponding value of the conditional expression (9) exceeds the upper limit value, it becomes difficult to correct the curvature of field in the telephoto end state. In addition, the diameter of the first lens group G1 becomes large, and the weight of the lens barrel becomes large. By setting the upper limit value of the conditional expression (9) to 0.77, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the upper limit of the conditional expression (9) is set to 0.70, 0.65, 0.58, 0.50, 0.45, and further 0.40. It may be set.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that an air lens is provided in the sixth lens group G6 and the following conditional expression (10) is satisfied.

0.00 <(RAR2 + RAR1) / (RAR2-RAR1) <2.00
... (10)
However, RR1: radius of curvature of the lens surface on the object side in the air lens of the sixth lens group G6 RAr2: radius of curvature of the lens surface on the image side in the air lens of the sixth lens group G6.

The conditional expression (10) defines the shape factor of the air lens provided in the sixth lens group G6. By satisfying the conditional expression (10), the curvature of field can be satisfactorily corrected.

When the corresponding value of the conditional expression (10) is less than the lower limit value, it becomes difficult to correct the curvature of field. By setting the lower limit value of the conditional expression (18) to 0.01, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of this embodiment, the lower limit of the conditional expression (10) is set to 0.10, 0.20, 0.28, 0.30, 0.40, and further 0.45. It may be set.

If the corresponding value of the conditional expression (10) exceeds the upper limit value, it becomes difficult to correct the curvature of field. By setting the upper limit value of the conditional expression (10) to 1.90, the effect of the present embodiment can be made more reliable. In order to further ensure the effect of the present embodiment, the upper limit of the conditional expression (10) may be set to 1.70, 1.50, 1.20, and further 1.00.

In the variable magnification optical system ZL according to the first and second embodiments, at least the first lens group G1, the third lens group G3, the fourth lens group G4, and the fifth lens group G5 at the time of magnification change. And the sixth lens group G6 should move with respect to the image plane. This makes it possible to increase the magnification fluctuation of each lens group at the time of scaling. Further, the aberration generated in the third lens group G3 at the time of scaling can be corrected by the fourth lens group G4.

In the variable magnification optical system ZL according to the first and second embodiments, it is desirable that the lens group that moves at the time of magnification change moves to the object side at the time of magnification change from the wide-angle end state to the telephoto end state. As a result, it is possible to secure a sufficient scaling ratio that satisfies the performance of the present embodiment.

Subsequently, the manufacturing method of the variable magnification optical system ZL according to the first embodiment will be outlined with reference to FIG. 41. First, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, a third lens group G3 having a positive refractive power, and a positive refractive power. A fourth lens group G4, a fifth lens group G5, and a sixth lens group G6 are arranged (step ST1). Then, at the time of scaling, the plurality of lens groups in the variable magnification optical system ZL move, and the distance between the adjacent lens groups changes (step ST2). In addition, an aperture that moves when scaling is arranged. At this time, each lens is arranged in the lens barrel so that the lens group on the image side and the aperture of the lens groups that move at the time of magnification change move integrally at the time of magnification change (step). ST3). According to such a manufacturing method, it is possible to manufacture a variable magnification optical system having a high magnification ratio and good optical performance.

Hereinafter, the variable magnification optical system ZL according to the first and second embodiments will be described with reference to the drawings. 1, FIG. 4, FIG. 7, FIG. 10, FIG. 13, FIG. 16, FIG. 19, FIG. 22, FIG. 25, FIG. 28, FIG. 31, FIG. 34, FIG. 37 are modifications according to the first to thirteenth embodiments. It is sectional drawing which shows the structure and the refractive power distribution of the magnification optical system ZL {ZL (1) to ZL (13)}. The first to eleventh examples and the thirteenth embodiment are examples corresponding to the first and second embodiments, and the twelfth embodiment is a reference example. In each figure, the moving direction along the optical axis of the lens group that moves when the magnification is changed from the wide-angle end state to the telephoto end state is indicated by an arrow. Furthermore, the direction of movement when the focusing group focuses on a short-distance object from infinity is indicated by an arrow together with the letters "focusing". The moving direction when at least a part of the third lens group G3 acts as an anti-vibration group to correct image blur is indicated by an arrow together with the characters "anti-vibration".

In these figures (FIGS. 1, FIG. 4, FIG. 7, FIG. 10, FIG. 13, FIG. 16, FIG. 19, FIG. 22, FIG. 25, FIG. 28, FIG. 31, FIG. 34, FIG. 37), each lens group is referred to as a reference. Each lens is represented by a combination of G and a number, and each lens is represented by a combination of a code L and a number. In this case, in order to prevent the types and numbers of the symbols and numbers from becoming large and complicated, the lens group and the like are represented by independently using combinations of the symbols and numbers for each embodiment. Therefore, even if the same combination of reference numerals and numbers is used between the examples, it does not mean that they have the same configuration.

Tables 1 to 13 are shown below. Among them, Table 1 is the first embodiment, Table 2 is the second embodiment, Table 3 is the third embodiment, Table 4 is the fourth embodiment, and Table 5 is the first embodiment. 5 Examples, Table 6 is the 6th Example, Table 7 is the 7th Example, Table 8 is the 8th Example, Table 9 is the 9th Example, Table 10 is the 10th Example, and Table 11 is the 11th Example. Examples, Table 12 is a table showing each specification data in the twelfth embodiment, and Table 13 is a table showing each specification data in the thirteenth embodiment. In each embodiment, the d-line (wavelength λ = 587.6 nm) and the g-line (wavelength λ = 435.8 nm) are selected as the calculation targets of the aberration characteristics.

In the [Overall specifications] table, FNO is the F number, ω is the half angle of view (unit is ° (degrees)), and Y is the image height. TL indicates the distance from the frontmost surface of the lens to the final surface of the lens on the optical axis at infinity, plus BF, and BF is the image from the final surface of the lens on the optical axis at infinity. The air conversion distance (back focus) to the surface I is shown. These values are shown for each of the wide-angle end (W), the first intermediate focal length (M1), the second intermediate focal length (M2), and the telephoto end (T) in each variable magnification state. Further, in the [Overall specifications] table, f3b indicates the focal length of the anti-vibration group. f3c indicates the focal length of the 3c group. βT3r indicates the magnification of a lens group consisting of lenses arranged on the image side of the anti-vibration group in the telephoto end state. βT3b indicates the magnification of the anti-vibration group in the telephoto end state. f123w indicates the combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3 in the wide-angle end state. f123t indicates the combined focal length of the first lens group G1, the second lens group G2, and the third lens group G3 in the telephoto end state.

In the [Lens Specifications] table, the surface numbers indicate the order of the optical surfaces from the object side along the direction in which the light beam travels, and R is the radius of curvature of each optical surface (the surface whose center of curvature is located on the image side). (Positive value), D is the distance on the optical axis from each optical surface to the next optical surface (or image surface), nd is the refractive index of the material of the optical member with respect to the d line, and νd is optical. The Abbe number based on the d-line of the material of the member is shown. The radius of curvature "∞" indicates a plane or an aperture, and (aperture S) indicates an aperture stop. The description of the refractive index nd of air = 1.00000 is omitted. When the lens surface is aspherical, the surface number is marked with * and the radius of curvature R indicates the paraxial radius of curvature.

In the table of [Aspherical surface data], the shape of the aspherical surface shown in [Lens specifications] is shown by the following equation (A). X (y) is the distance (zag amount) along the optical axis direction from the tangent plane at the apex of the aspherical surface to the position on the aspherical surface at the height y, and R is the radius of curvature of the reference sphere (near axis radius of curvature). , Kappa is the conical constant, and Ai is the i-th order aspherical coefficient. "E-n" indicates " ^{x10 -n".} For example, 1.234E-05 = 1.234 × 10 ^-5 . The second-order aspherical coefficient A2 is 0, and the description thereof is omitted.

X (y) = (y ² / R) / {1 + (1-κ × y ² / R ² ) ^1/2 } + A4 × y ⁴ + A6 × y ⁶ + A8 × y ⁸ + A10 × y ¹⁰ + A12 × y ¹²・・ ・ (A)

The [lens group data] table shows the starting surface (the surface closest to the object) and the focal length of each lens group.

The table of [variable spacing data] shows the surface spacing with the plane number in which the surface spacing is "variable" in the table showing [lens specifications]. Here, the wide-angle end (W), the first intermediate focal length (M1), the second intermediate focal length (M2), and the telephoto end (T) are scaled for each when focused at infinity and short distance. Indicates the surface spacing in the state. In [variable interval data], f indicates the focal length of the entire lens system, and β indicates the photographing magnification.

The table of [Conditional expression corresponding values] shows the values corresponding to each conditional expression.

Hereinafter, in all the specification values, "mm" is generally used for the focal length f, the radius of curvature R, the plane spacing D, other lengths, etc., unless otherwise specified, but the optical system is expanded proportionally. Alternatively, it is not limited to this because the same optical performance can be obtained even if the proportional reduction is performed.

The description of the table so far is common to all the examples, and the duplicate description below is omitted.

(First Example)
The first embodiment will be described with reference to FIGS. 1 to 3 and Table 1. FIG. 1 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the first embodiment. The variable magnification optical system ZL (1) according to the first embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 1, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally. The symbol (+) or (-) attached to each lens group symbol indicates the refractive power of each lens group, and this also applies to all the following examples.

The first lens group G1 is composed of a negative meniscus lens L11 having a convex surface facing the object side, a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side, which are arranged in order from the object side. Will be done.

The second lens group G2 includes a negative meniscus lens L21 having a convex surface facing the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a biconcave negative lens arranged in order from the object side. It is composed of a lens L24.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and an object side. It is composed of a negative meniscus lens L34 with a concave surface facing.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens with a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The negative meniscus lens L61 has an aspherical lens surface on the image plane I side. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 1 below lists the specifications of the variable magnification optical system according to the first embodiment.

(Table 1)
[Overall specifications]
Variable ratio 7.848
f123w = -217.63848
f123t = -267.32298
W M1 M2 T
FNO 4.12109 5.58779 6.39998 6.50002
ω 42.58698 22.66696 11.13686 6.13014
Y 20.50 21.70 21.70 21.70
TL 126.45486 144.98844 168.50373 188.4741
[Lens specifications]
Surface number RD νd nd
1 185.7354 2.0000 31.27 1.903660
2 75.9813 1.0263
3 81.5981 6.4204 67.90 1.593190
4-494.4016 0.1000
5 59.1320 6.1300 67.90 1.593190
6 390.1369 D1 (variable)
7 236.0277 1.2500 32.33 1.953750
8 19.0394 5.0675
9 -46.6700 1.1000 52.33 1.755000
10 68.1612 0.4169
11 37.1210 3.3840 20.88 1.922860
12 -52.5580 0.5124
13 -32.9357 1.0000 46.59 1.816000
14 416.8076 D2 (variable)
15 ∞ 2.0000 (Aperture S)
16 39.8204 2.5136 35.72 1.902650
17 -292.5261 0.5000
18 36.7161 1.0000 29.12 2.001000
19 20.9452 3.3404 53.74 1.579570
20 -76.0620 1.4447
21 -35.5626 1.0000 32.33 1.953750
22 -290.1606 D3 (variable)
23 37.1374 4.6344 42.73 1.834810
24 -37.1374 1.0000 31.27 1.903660
25 -308.9768 0.1000
26 31.6449 2.7756 32.33 1.953750
27 15.2741 8.7030 81.49 1.497100
28 * -40.3095 D4 (variable)
29 1365.4927 3.0634 23.80 1.846660
30 -35.3251 1.0000 40.13 1.851350
31 * 32.6144 D5 (variable)
32 -16.9998 1.4000 42.51 1.820800
33 * -22.5398 0.1000
34 626.7496 3.5530 37.57 1.683760
35 -77.6296 BF
[Aspherical data]
Side 28 κ = 1.0000, A4 = 3.13017E-05, A6 = -1.03090E-07
A8 = 6.53525E-10, A10 = -2.57830E-12, A12 = 0.32673E-14
Side 31 κ = 1.0000, A4 = -6.666636E-06, A6 = 5.10546E-08
A8 = 1.72567E-11, A10 = -2.40595E-12, A12 = 0.98445E-14
Side 33 κ = 1.0000, A4 = -1.93366E-06, A6 = -2.05750E-08
A8 = 8.81224E-11, A10 = -2.90421E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 98.9899
G2 7 -16.5057
G3 16 48.48369
G4 23 28.91747
G5 29 -39.0895
G6 32 -15588.34
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72001 49.99999 105.05133 193.99063
D0 ∞ ∞ ∞ ∞
D1 1.50000 17.29645 38.92328 54.52847
D2 18.83905 10.91446 4.55495 1.10018
D3 12.23175 6.39417 3.18615 1.47844
D4 5.54311 4.42699 5.70823 2.00068
D5 10.05055 17.00460 18.93085 24.34574
BF 11.75486 22.41624 30.66474 38.48515
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06221 -0.11053 -0.17918 -0.28386
D0 365.9340 397.4004 473.8851 503.9147
D1 1.50000 17.29645 38.92328 54.52847
D2 18.83905 10.91446 4.55495 1.10018
D3 12.23175 6.39417 3.18615 1.47844
D4 6.43705 6.05192 10.02051 11.69839
D5 9.15661 15.37967 14.61857 14.64803
BF 11.78171 22.50112 30.88824 39.04500
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 42.587
Conditional expression (3) ωt = 6.130
Conditional expression (4) fw / f123w = -0.114
Conditional expression (5) ft / f123t = -0.726
Conditional expression (6) BFw / fw = 0.476
Conditional expression (7) (-f5) / fw = 1.581
Conditional expression (8) Mv5 / Mv6 = 1.535
Conditional expression (9) Mv1 / (ft-fw) = 0.366
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.931

2 (A) and 2 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the first embodiment, respectively. 3 (A) and 3 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the first embodiment, respectively. In each aberration diagram of FIGS. 2 (A) and 2 (B), FNO indicates an F number and Y indicates an image height. The spherical aberration diagram shows the value of the F number corresponding to the maximum aperture, the astigmatism diagram and the distortion diagram show the maximum value of the image height, and the coma aberration diagram shows the value of each image height. The coma aberration diagrams of FIGS. 3 (A) and 3 (B) show the values of each image height. Further, in each aberration diagram, d indicates the d line (wavelength λ = 587.6 nm), and g indicates the g line (wavelength λ = 435.8 nm). In the astigmatism diagram, the solid line shows the sagittal image plane and the broken line shows the meridional image plane. In the aberration diagrams of each of the following examples, the same reference numerals as those of the present embodiment will be used, and duplicate description will be omitted.

From each aberration diagram, it can be seen that the variable magnification optical system according to the first embodiment has various aberrations satisfactorily corrected and has excellent imaging performance.

(Second Example)
The second embodiment will be described with reference to FIGS. 4 to 6 and Table 2. FIG. 4 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the second embodiment. The variable magnification optical system ZL (2) according to the second embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. A third lens group G3 having a positive refractive power provided with an aperture S, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a negative refractive power. It is composed of a sixth lens group G6 having a lens. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the third lens group G3 provided with the aperture stop S, the fourth lens group G4, and the fifth lens group G5 , And the sixth lens group G6 move along the optical axis in the direction indicated by the arrow in FIG. 4, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is composed of a negative meniscus lens L11 having a convex surface facing the object side, a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side, which are arranged in order from the object side. Will be done.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed.

The third lens group G3 is a combination of a biconvex positive lens L31, an aperture diaphragm S, a negative meniscus lens L32 having a convex surface facing the object side, and a biconvex positive lens L33 arranged in order from the object side. It is composed of a lens and a negative meniscus lens L34 with a concave surface facing the object side.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens with a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The negative meniscus lens L61 has an aspherical lens surface on the image plane I side. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 2 below lists the specifications of the variable magnification optical system according to the second embodiment.

(Table 2)
[Overall specifications]
Variable ratio 7.848
f123w = -377.733
f123t = -288.19144
W M1 M2 T
FNO 4.12000 5.60000 6.20000 6.49999
ω 43.04718 22.53540 10.65017 6.13829
Y 20.91 21.70 21.70 21.70
TL 125.95528 142.51715 167.85323 186.8435
[Lens specifications]
Surface number RD νd nd
1 188.64525 2.00000 31.27 1.903660
2 77.80524 0.84780
3 80.41425 6.51915 67.90 1.593190
4-471.30377 0.10000
5 62.30684 5.66572 67.90 1.593190
6 358.24871 D1 (variable)
7 230.01286 1.25000 43.79 1.848500
8 18.45421 5.50336
9 -40.33983 1.10000 52.34 1.755000
10 79.65336 0.38546
11 39.14822 3.37749 23.80 1.846660
12 -47.38891 0.46523
13 -31.94449 1.00000 46.59 1.816000
14 -2729.77760 D2 (variable)
15 41.64137 2.51154 35.73 1.902650
16 -289.39118 0.40000
17 ∞ 0.10000 (Aperture S)
18 38.12143 1.00000 29.12 2.001000
19 21.49924 3.26023 53.74 1.579570
20 -73.20919 1.47119
21 -34.94662 1.00000 32.33 1.953750
22 -165.99888 D3 (variable)
23 37.20805 4.18411 42.73 1.834810
24-43.17368 1.00003 31.27 1.903660
25 -659.56023 1.54931
26 28.71779 1.32801 32.33 1.953750
27 14.76801 9.10325 81.49 1.497100
28 * -42.86465 D4 (variable)
29 255.99237 3.36761 23.80 1.846660
30 -33.68693 1.00000 40.13 1.851350
31 * 31.06431 D5 (variable)
32 -23.57856 1.40000 45.21 1.794457
33 * -50.21699 0.10000
34 91.45040 3.78568 29.84 1.800000
35 -197.78095 BF
[Aspherical data]
Side 28 κ = 1.0000, A4 = 2.56920E-05, A6 = -9.38399E-08
A8 = 4.71077E-10, A10 = -1.70196E-12, A12 = 0.00000E + 00
Side 31 κ = 1.0000, A4 = -6.78111E-06, A6 = 6.47335E-08
A8 = -3.28125E-10, A10 = 2.56418E-13, A12 = 0.00000E + 00
Side 33 κ = 1.0000, A4 = 3.30419E-06, A6 = -1.76274E-09
A8 = 1.66657E-12, A10 = 1.80471E-14, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 102.16195
G2 7 -16.76640
G3 15 47.83089
G4 23 29.71748
G5 29 -41.62356
G6 32 -236.16863
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72031 50.00094 110.00281 194.00483
D0 ∞ ∞ ∞ ∞
D1 1.50000 17.23398 38.86323 55.71214
D2 19.13452 10.77832 3.90279 1.10000
D3 12.16022 5.90688 2.59619 1.47832
D4 5.12094 4.32200 5.90770 2.00000
D5 10.00915 17.06861 18.78383 23.80987
BF 11.25528 20.43218 31.02431 35.96804
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06086 -0.10794 -0.18504 -0.27368
D0 374.0451 407.4838 482.1484 513.1582
D1 1.50000 17.23398 38.86323 55.71214
D2 19.13452 10.77832 3.90279 1.10000
D3 12.16022 5.90688 2.59619 1.47832
D4 6.06949 6.02341 10.42761 11.59738
D5 9.06059 15.36720 14.26392 14.21249
BF 11.25529 20.4322 31.02445 35.96847
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 43.047
Conditional expression (3) ωt = 6.138
Conditional expression (4) fw / f123w = -0.112
Conditional expression (5) ft / f123t = -0.783
Conditional expression (6) BFw / fw = 0.455
Conditional expression (7) (-f5) / fw = 1.684
Conditional expression (8) Mv5 / Mv6 = 1.558
Conditional expression (9) Mv1 / (ft-fw) = 0.360
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.291

5 (A) and 5 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the second embodiment, respectively. 6 (A) and 6 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the second embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the second embodiment has various aberrations corrected well and has excellent imaging performance.

(Third Example)
The third embodiment will be described with reference to FIGS. 7 to 9 and Table 3. FIG. 7 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the third embodiment. The variable magnification optical system ZL (3) according to the third embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 7, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 includes a negative meniscus lens L21 having a convex surface facing the object side, a negative meniscus lens L22 having a convex surface facing the object side, and a positive meniscus lens L22 having a convex surface facing the object side, arranged in order from the object side. It is composed of L23, a positive meniscus lens L24 having a concave surface facing the object side, and a junction lens L25 having a negative meniscus lens L25 having a concave surface facing the object side. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L25 has an aspherical lens surface on the image plane I side.

The third lens group G3 is composed of a positive meniscus lens L31 having a convex surface facing the object side. The positive meniscus lens L31 has an aspherical lens surface on the object side.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side, a negative meniscus lens L42 having a convex surface facing the object side, and a positive meniscus lens L43 having a convex surface facing the object side. And a junction lens of a biconvex positive lens L44 and a negative meniscus lens L45 with a concave surface facing the object side. The negative meniscus lens L45 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a positive meniscus lens L51 with a concave surface facing the object side and a negative lens L52 having a biconcave shape. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a positive meniscus lens L62 having a concave surface facing the object side, which are arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive meniscus lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the positive meniscus lens L31 in the third lens group G3 constitutes a vibration-proof group having a positive refractive power that can move in a direction perpendicular to the optical axis, and the image formation position due to camera shake or the like is formed. The displacement (image blur on the image plane I) is corrected.

Table 3 below lists the specifications of the variable magnification optical system according to the third embodiment.

(Table 3)
[Overall specifications]
Variable ratio 7.850
f123w = -526.69259
f123t = -297.45559
W M1 M2 T
FNO 4.12000 5.00001 6.14000 6.50003
ω 41.94830 22.05780 10.36801 5.96172
Y 21.34 21.70 21.70 21.70
TL 118.25612 134.48400 163.70742 182.4804
[Lens specifications]
Surface number RD νd nd
1 151.3952 2.0000 23.80 1.846660
2 87.2806 5.9280 67.90 1.593190
3 -1349.8590 0.1000
4 76.7487 4.4238 67.90 1.593190
5 320.3570 D1 (variable)
6 * 395.1403 1.2500 40.66 1.883000
7 17.9444 4.0881
8 172.0131 1.0000 27.15 1.944421
9 41.2622 0.6317
10 28.0910 3.7608 20.88 1.922860
11 282.0417 1.6588
12 -43.9082 1.6452 25.64 1.784720
13 -19.4929 1.1000 43.36 1.839318
14 * -367.3130 D2 (variable)
15 ∞ 1.8230 (Aperture S)
16 * 25.2025 2.7754 59.33 1.609605
17 116.8971 D3 (variable)
18 27.7315 3.2255 67.90 1.593190
19 -829.3049 0.7234
20 31.9256 2.0849 32.32 1.953747
21 14.4283 4.6386 70.32 1.487490
22 87.2035 0.7730
23 61.3969 5.2420 82.57 1.497820
24 -18.0219 4.1197 37.22 1.882023
25 * -25.6911 D4 (variable)
26 -1678.9249 3.0141 25.26 1.902000
27 -33.6869 1.0000 40.12 1.851080
28 * 40.9152 D5 (variable)
29 -15.4450 1.2500 46.59 1.816000
30 -29.1017 0.1000
31 -162.7939 2.9649 29.37 1.950000
32 -61.0034 BF
[Aspherical data]
Side 6 κ = 1.9193, A4 = 5.26888E-06, A6 = -1.61582E-08
A8 = 5.37910E-11, A10 = -9.15512E-14, A12 = 0.00000E + 00
14th page κ = 6.000, A4 = 8.64764E-07, A6 = -1.04249E-08
A8 = -8.45595E-12, A10 = 4.36832E-13, A12 = 0.00000E + 00
16th surface κ = -0.0411, A4 = -5.82687E-06, A6 = 1.89727E-08
A8 = -3.04157E-10, A10 = 1.94188E-12, A12 = 0.00000E + 00
Side 25 κ = 1.0633, A4 = 1.55522E-05, A6 = -4.66061E-08
A8 = 2.01166E-10, A10 = -8.69226E-13, A12 = 0.00000E + 00
Side 28 κ = 0.000, A4 = -8.62706E-06, A6 = 9.53672E-08
A8 = -5.21848E-10, A10 = 1.74761E-12, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 111.43064
G2 6 -17.83112
G3 16 52.10796
G4 18 30.96133
G5 26 -50.42308
G6 29 -77.20586
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72028 50.00010 110.02145 194.04302
D0 ∞ ∞ ∞ ∞
D1 1.56355 16.96393 42.92481 58.95782
D2 18.90672 9.77960 3.82294 0.50000
D3 10.22026 5.92276 2.94135 1.20000
D4 6.49920 5.70254 5.42574 2.50000
D5 10.45535 15.54950 18.80771 23.47480
BF 9.29011 19.24474 28.46394 34.52694
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06124 -0.12203 -0.24452 -0.38142
D0 373.1327 356.9049 327.6814 308.9084
D1 1.56355 16.96393 42.92481 58.95782
D2 18.90672 9.77960 3.82294 0.50000
D3 10.22026 5.92276 2.94135 1.20000
D4 7.63429 7.89257 11.92314 16.79614
D5 9.32026 13.35947 12.31031 9.17866
BF 9.31670 19.34984 28.88441 35.54307
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.850
Conditional expression (2) ωw = 41.948
Conditional expression (3) ωt = 5.962
Conditional expression (4) fw / f123w = -0.047
Conditional expression (5) ft / f123t = -0.652
Conditional expression (6) BFw / fw = 0.376
Conditional expression (7) (-f5) / fw = 2.040
Conditional expression (8) Mv5 / Mv6 = 1.516
Conditional expression (9) Mv1 / (ft-fw) = 0.379
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 1.435

8 (A) and 8 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the third embodiment, respectively. 9 (A) and 9 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the third embodiment, respectively. From each of the various aberration diagrams, it can be seen that the variable magnification optical system according to the third embodiment has various aberrations corrected well and has excellent imaging performance.

(Fourth Example)
A fourth embodiment will be described with reference to FIGS. 10 to 12 and Table 4. FIG. 10 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the fourth embodiment. The variable magnification optical system ZL (4) according to the fourth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 10, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 includes a negative meniscus lens L21 having a convex surface facing the object side, a negative meniscus lens L22 having a convex surface facing the object side, a biconvex positive lens L23, and an object arranged in order from the object side. It is composed of a junction lens of a positive meniscus lens L24 having a concave surface facing the side and a negative meniscus lens L25 having a concave surface facing the object side. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L25 has an aspherical lens surface on the image plane I side.

The third lens group G3 is a junction lens of a positive meniscus lens L31 having a convex surface facing the object side, a biconvex positive lens L32, and a negative meniscus lens L33 having a concave surface facing the object side, arranged in order from the object side. It is composed of and. The positive meniscus lens L31 has an aspherical lens surface on the object side.

The fourth lens group G4 consists of a positive meniscus lens L41 having a convex surface facing the object side, a negative meniscus lens L42 having a convex surface facing the object side, and a positive meniscus lens L43 having a convex surface facing the object side, which are arranged in order from the object side. The lens is composed of a positive meniscus lens L44 having a concave surface facing the object side and a negative meniscus lens L45 having a concave surface facing the object side. The negative meniscus lens L45 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a plano-convex positive lens L62 having a plane facing the image plane I side, which are arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the positive lens L32 and the negative meniscus lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 4 below lists the specifications of the variable magnification optical system according to the fourth embodiment.

(Table 4)
[Overall specifications]
Variable ratio 7.848
f123w = 102.18699
f123t = -1535.17561
W M1 M2 T
FNO 4.12000 5.00001 6.14000 6.50003
ω 41.94830 22.05780 10.36801 5.96172
Y 21.65 21.70 21.70 21.70
TL 122.11284 138.25648 173.12226 195.4602
[Lens specifications]
Surface number RD νd nd
1 157.9423 2.0000 23.80 1.846660
2 81.8879 5.9036 67.90 1.593190
3 -2013.3747 0.1000
4 63.5017 4.6636 63.34 1.618000
5 210.8809 D1 (variable)
6 * 318.1018 1.2500 40.66 1.883000
7 16.7008 4.7201
8 704.9777 1.3500 25.79 1.940573
9 35.9277 0.1354
10 25.6246 4.3288 20.88 1.922860
11 -84.8316 1.1878
12 -26.8353 2.5514 26.72 1.759928
13 -14.0619 1.1000 40.66 1.883000
14 * -120.1155 D2 (variable)
15 ∞ 1.7168 (Aperture S)
16 * 25.0707 2.5492 56.42 1.650119
17 50.5707 1.8201
18 2141.2793 3.9646 47.10 1.718816
19 -19.4561 1.2000 29.37 1.950000
20 -40.3974 D3 (variable)
21 33.1155 2.7430 58.12 1.622989
22 102.1338 0.1000
23 26.3197 4.3495 29.37 1.950000
24 14.1783 4.4212 70.32 1.487490
25 72.5822 1.6811
26 -306.2709 4.3812 82.57 1.497820
27 -18.7373 1.2500 37.22 1.882023
28 * -24.4766 D4 (variable)
29 119.2349 3.5589 25.92 1.805628
30 -33.6869 1.0000 40.12 1.851080
31 * 32.8619 D5 (variable)
32 -22.4629 1.2500 40.66 1.883000
33 -43.8572 0.1000
34 61.5070 4.1976 33.02 1.689260
35 ∞ BF
[Aspherical data]
Side 6 κ = 6.000, A4 = 9.24936E-06, A6 = 4.48621E-09
A8 = -4.48203E-11, A10 = 1.6501E-13, A12 = 0.00000E + 00
14th page κ = 5.8635, A4 = -1.80704E-06, A6 = 1.46957E-08
A8 = -7.35664E-11, A10 = -5.50824E-13, A12 = 0.00000E + 00
16th surface κ = 0.0729, A4 = -4.52720E-06, A6 = 2.52623E-08
A8 = -1.11420E-10, A10 = 1.41519E-13, A12 = 0.00000E + 00
Side 28 κ = 1.0568, A4 = 1.62692E-05, A6 = -9.59061E-09
A8 = -6.35322E-11, A10 = 1.732247E-13, A12 = 0.00000E + 00
Side 31 κ = 1.0365, A4 = -5.49985E-06, A6 = 5.29125E-08
A8 = -9.39998E-11, A10 = 1.17057E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 106.62052
G2 6 -16.22739
G3 16 41.04090
G4 21 40.60874
G5 29 -49.86905
G6 32 -140.23760
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.71999 49.99999 109.99995 193.99988
D0 ∞ ∞ ∞ ∞
D1 1.50000 18.53350 35.68354 55.45436
D2 17.47125 8.41504 3.49296 0.78316
D3 8.24386 2.43196 1.40000 1.44036
D4 6.00186 7.14502 5.60349 2.49999
D5 10.03309 14.70182 17.27531 20.33845
BF 9.28884 17.45519 40.09303 45.36996
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06195 -0.10885 -0.20280 -0.28444
D0 369.2759 403.0933 448.2665 495.9287
D1 1.50000 18.53350 35.68354 55.45436
D2 17.47125 8.41504 3.49296 0.78316
D3 8.24386 2.43196 1.40000 1.44036
D4 7.29302 9.64626 10.19294 12.30143
D5 8.74193 12.20058 12.68586 10.53701
BF 9.31603 17.53910 40.38407 45.94189
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 41.948
Conditional expression (3) ωt = 5.962
Conditional expression (4) fw / f123w = 0.242
Conditional expression (5) ft / f123t = -0.126
Conditional expression (6) BFw / fw = 0.376
Conditional expression (7) (-f5) /fw=2.017
Conditional expression (8) Mv5 / Mv6 = 1.286
Conditional expression (9) Mv1 / (ft-fw) = 0.433
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.168

11 (A) and 11 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fourth embodiment, respectively. 12 (A) and 12 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fourth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the fourth embodiment has various aberrations corrected well and has excellent imaging performance.

(Fifth Example)
A fifth embodiment will be described with reference to FIGS. 13 to 15 and Table 5. FIG. 13 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the fifth embodiment. The variable magnification optical system ZL (5) according to the fifth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a positive refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 13, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L24 has an aspherical lens surface on the image plane I side.

The third lens group G3 is a junction lens of a positive meniscus lens L31 having a convex surface facing the object side, a negative meniscus lens L32 having a convex surface facing the object side, and a biconvex positive lens L33 arranged in order from the object side. It is composed of and. The positive meniscus lens L31 has an aspherical lens surface on the object side.

The fourth lens group G4 is a junction lens of a positive meniscus lens L41 having a convex surface facing the object side, a negative meniscus lens L42 having a convex surface facing the object side, and a biconvex positive lens L43 arranged in order from the object side. And a junction lens of a biconvex positive lens L44 and a biconcave negative lens L45. The negative lens L45 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 5 below lists the specifications of the variable magnification optical system according to the fifth embodiment.

(Table 5)
[Overall specifications]
Variable ratio 7.848
f123w = 148.33142
f123t = -861.38789
W M1 M2 T
FNO 4.12000 5.60000 6.20000 6.49999
ω 42.61146 22.53540 10.65017 6.13829
Y 20.68 21.70 21.70 21.70
TL 122.11284 137.15660 162.89036 188.0553
[Lens specifications]
Surface number RD νd nd
1 120.0314 2.0000 23.80 1.846660
2 75.2829 6.2421 82.57 1.497820
3 -2364.7242 0.1000
4 64.4734 5.0111 64.74 1.607834
5 308.6603 D1 (variable)
6 * 221.2774 1.2500 40.66 1.883000
7 17.1630 5.2789
8 -38.7201 1.1000 33.32 1.903162
9 95.9763 0.1000
10 40.1060 4.3656 20.88 1.922860
11 -33.5026 0.9492
12 -22.3899 1.1000 40.67 1.882762
13 * -102.6938 D2 (variable)
14 ∞ 0.8341 (Aperture S)
15 * 31.3299 2.7567 63.86 1.517039
16 394.2979 1.0000
17 76.9690 1.1000 25.78 1.906571
18 30.3656 2.9449 45.71 1.623046
19 -89.6818 D3 (variable)
20 23.7528 3.8095 41.66 1.659437
21 83.0826 2.6863
22 52.1032 1.8385 32.25 1.954620
23 15.4393 5.4045 70.32 1.487490
24 -39.4485 0.1000
25 37.0327 3.3978 67.89 1.593103
26 -838.1647 1.2500 43.15 1.810385
27 * 82.5521 D4 (variable)
28 623.8813 3.1385 22.74 1.808090
29 -33.6869 1.0000 41.21 1.836497
30 * 32.8807 D5 (variable)
31 -21.3174 1.2500 27.35 1.663819
32 -31.8044 0.1043
33 92.9303 3.5471 28.93 1.727721
34 -394.1540 BF
[Aspherical data]
Side 6 κ = 5.7341, A4 = 1.16802E-06, A6 = 2.03518E-09
A8 = 1.81447E-11, A10 = 8.58869E-14, A12 = 0.00000E + 00
Page 13 κ = 3.2914, A4 = -1.11111E-06, A6 = 1.49282E-09
A8 = -3.72110E-11, A10 = 6.45032E-13, A12 = 0.00000E + 00
Surface 15 κ = 0.0277, A4 = -8.27654E-06, A6 = 1.77158E-08
A8 = -1.81439E-10, A10 = 1.08193E-12, A12 = 0.00000E + 00
Page 27 κ = 1.9922, A4 = 1.24262E-05, A6 = -1.46784E-08
A8 = 3.73707E-10, A10 = -2.02655E-12, A12 = 0.00000E + 00
Side 30 κ = 1.9072, A4 = -8.91746E-06, A6 = 3.65180E-08
A8 = -5.04265E-10, A10 = 1.78607E-12, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 99.41971
G2 6 -15.74038
G3 15 41.65192
G4 20 37.63548
G5 28 -40.12367
G6 31 7119.59107
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.71999 49.99997 109.99986 193.99963
D0 ∞ ∞ ∞ ∞
D1 1.50000 16.60455 37.99399 53.23975
D2 18.36307 10.15010 3.58234 1.66590
D3 13.02129 4.83611 1.75831 1.47831
D4 6.45265 6.28920 8.47335 2.50000
D5 9.82549 18.17413 19.06777 25.32113
BF 9.29124 17.44341 28.35549 40.19113
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06170 -0.10941 -0.19455 -0.28776
D0 370.3154 405.3261 459.3561 504.3260
D1 1.50000 16.60455 37.99399 53.23975
D2 18.36307 10.15010 3.58234 1.66590
D3 13.02129 4.83611 1.75831 1.47831
D4 7.54590 8.23070 14.07758 12.27653
D5 8.73225 16.23263 13.46354 15.54460
BF 9.31427 17.51651 28.58674 40.69673
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 42.611
Conditional expression (3) ωt = 6.138
Conditional expression (4) fw / f123w = 0.167
Conditional expression (5) ft / f123t = -0.225
Conditional expression (6) BFw / fw = 0.376
Conditional expression (7) (-f5) / fw = 1.623
Conditional expression (8) Mv5 / Mv6 = 1.501
Conditional expression (9) Mv1 / (ft-fw) = 0.390
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.490

14 (A) and 14 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fifth embodiment, respectively. 15 (A) and 15 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the fifth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the fifth embodiment has various aberrations corrected well and has excellent imaging performance.

(6th Example)
The sixth embodiment will be described with reference to FIGS. 16 to 18 and Table 6. FIG. 16 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the sixth embodiment. The variable magnification optical system ZL (6) according to the sixth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a positive refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 16, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L24 has an aspherical lens surface on the image plane I side.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and an object side. It is composed of a negative meniscus lens L34 with a concave surface facing.

The fourth lens group G4 includes a biconvex positive lens L41 arranged in order from the object side, a junction lens of a negative meniscus lens L42 with a convex surface facing the object side, and a biconvex positive lens L43, and an object side. It is composed of a junction lens of a positive meniscus lens L44 having a convex surface facing the surface and a negative meniscus lens L45 having a concave surface facing the object side. The positive lens L41 has an aspherical lens surface on the object side. The negative meniscus lens L45 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 6 below lists the specifications of the variable magnification optical system according to the sixth embodiment.

(Table 6)
[Overall specifications]
Variable ratio 7.848
f123w = -136.43292
f123t = -215.16315
W M1 M2 T
FNO 4.12001 5.60001 6.20000 6.50003
ω 42.67959 22.59339 10.65052 6.14768
Y 20.58 21.70 21.70 21.70
TL 122.11285 136.30769 162.04178 189.3093
[Lens specifications]
Surface number RD νd nd
1 152.2083 2.0000 23.80 1.846660
2 89.2068 6.1884 82.57 1.497820
3-413.2934 0.1000
4 63.3220 4.8830 67.90 1.593190
5 253.0230 D1 (variable)
6 * 137.9264 1.2500 40.66 1.882996
7 17.8991 4.7805
8 -47.3363 1.1000 36.88 1.897432
9 75.2485 0.1000
10 39.7397 4.1374 21.58 1.918850
11 -39.0575 0.7197
12 -24.5868 1.1000 47.49 1.802013
13 * -591.6627 D2 (variable)
14 ∞ 0.7464 (Aperture S)
15 46.9722 2.7552 48.04 1.768500
16 -93.2395 0.5000
17 51.8617 1.1000 29.95 1.987022
18 25.2907 2.9021 45.71 1.623046
19 -73.0708 1.4973
20 -29.7887 1.0273 35.73 1.902641
21 -85.6917 D3 (variable)
22 * 28.7123 3.8190 45.24 1.768369
23 -400.5317 2.3100
24 68.0478 1.0008 32.32 1.953752
25 17.9627 5.9680 78.66 1.495797
26 -34.0844 0.1000
27 42.3850 3.2656 67.90 1.593190
28 754.0925 1.2500 44.96 1.790885
29 * 73.7905 D4 (variable)
30 256.5317 3.3327 22.74 1.808090
31 -33.6869 1.0000 40.27 1.839964
32 * 28.6240 D5 (variable)
33 -20.9675 1.2500 27.35 1.663819
34 -40.3074 0.1000
35 173.3096 4.5044 31.21 1.841022
36 -72.4610 BF
[Aspherical data]
Side 6 κ = 0.0442, A4 = -4.01520E-06, A6 = 2.02052E-08
A8 = -1.03759E-10, A10 = 3.37776E-13, A12 = 0.00000E + 00
Page 13 κ = 1.0000, A4 = -6.36415E-06, A6 = 2.72142E-08
A8 = -2.64695E-10, A10 = 8.53046E-13, A12 = 0.00000E + 00
Side 22 κ = 1.0000, A4 = -4.72982E-06, A6 = 7.21651E-09
A8 = -1.20147E-10, A10 = 3.75555E-13, A12 = 0.00000E + 00
Side 29 κ = 1.0000, A4 = 1.553597E-05, A6 = -6.12529E-09
A8 = 2.59000E-10, A10 = -2.05818E-12, A12 = 0.00000E + 00
Side 32 κ = 1.0000, A4 = -5.888848E-06, A6 = 4.28279E-08
A8 = -4.85291E-10, A10 = 2.28998E-12, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 101.19406
G2 6 -16.04849
G3 15 49.36913
G4 22 29.13636
G5 30 -37.13373
G6 33 424.58679
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72000 50.00001 109.99999 194.00003
D0 ∞ ∞ ∞ ∞
D1 1.50000 15.59832 37.20427 54.26539
D2 17.63580 9.34111 2.87140 1.75361
D3 12.53679 5.46459 2.24074 1.47831
D4 6.27123 7.05298 10.12752 2.50000
D5 9.72366 16.01381 16.16341 24.55336
BF 9.65757 18.04908 28.64666 39.97093
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06163 -0.10967 -0.19523 -0.28795
D0 370.3333 405.5358 460.2499 503.0996
D1 1.50000 15.59832 37.20427 54.26539
D2 17.63580 9.34111 2.87140 1.75361
D3 12.53679 5.46459 2.24074 1.47831
D4 7.24735 8.97695 15.97733 12.28747
D5 8.74755 14.08984 10.31360 14.76589
BF 9.68397 18.12250 28.87954 40.47730
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 42.680
Conditional expression (3) ωt = 6.148
Conditional expression (4) fw / f123w = -0.181
Conditional expression (5) ft / f123t = -0.902
Conditional expression (6) BFw / fw = 0.391
Conditional expression (7) (-f5) /fw=1.502
Conditional expression (8) Mv5 / Mv6 = 1.489
Conditional expression (9) Mv1 / (ft-fw) = 0.397
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.623

17 (A) and 17 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the sixth embodiment, respectively. 18 (A) and 18 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the sixth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the sixth embodiment has various aberrations corrected well and has excellent imaging performance.

(7th Example)
A seventh embodiment will be described with reference to FIGS. 19 to 21 and Table 7. FIG. 19 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the seventh embodiment. The variable magnification optical system ZL (7) according to the seventh embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 19, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L24 has an aspherical lens surface on the image plane I side.

The third lens group G3 is a junction lens of a positive meniscus lens L31 having a convex surface facing the object side, a negative meniscus lens L32 having a convex surface facing the object side, and a biconvex positive lens L33 arranged in order from the object side. And a flat concave negative lens L34 with a plane facing the image plane I side. The positive meniscus lens L31 has an aspherical lens surface on the object side.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens with a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a positive meniscus lens L62 having a concave surface facing the object side, which are arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive meniscus lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 7 below lists the specifications of the variable magnification optical system according to the seventh embodiment.

(Table 7)
[Overall specifications]
Variable ratio 7.854
f123w = 108.15193
f123t = -1180.72115
W M1 M2 T
FNO 4.11505 5.74532 6.36855 6.68279
ω 42.27184 21.88249 10.96245 6.04244
Y 20.89 21.70 21.70 21.70
TL 120.45755 140.80075 169.77272 195.4575
[Lens specifications]
Surface number RD νd nd
1 164.3654 2.0000 23.80 1.846660
2 73.5155 5.9893 67.90 1.593190
3 -2353.2843 0.1000
4 72.1741 4.8721 46.03 1.721059
5 384.7599 D1 (variable)
6 * 168.2036 1.5000 40.66 1.883000
7 15.8326 4.3451
8 -82.6447 1.5000 40.66 1.883000
9 46.2086 0.1000
10 30.2898 4.8789 23.29 1.872769
11 -32.6789 0.7547
12 -24.9555 1.5000 40.66 1.883000
13 * -2867.4336 D2 (variable)
14 ∞ 1.5000 (Aperture S)
15 * 24.1510 3.7103 57.75 1.633994
16 594.5882 1.0000
17 70.2793 1.5000 35.28 1.801392
18 17.4502 4.9253 46.90 1.702987
19 -111.3896 1.2478
20 -65.1233 1.5000 44.85 1.743972
21 ∞ D3 (variable)
22 132.6869 3.6334 82.57 1.497820
23 -33.2203 1.5000 23.99 1.871866
24 -81.5274 0.1000
25 26.2321 1.5000 40.98 1.869660
26 16.8448 7.0033 57.83 1.512954
27 * -36.7178 D4 (variable)
28 100.0646 3.3139 24.26 1.791180
29 -60.0000 1.5000 40.12 1.851080
30 * 35.0435 D5 (variable)
31 -19.8065 1.5000 40.79 1.877404
32 -36.0179 0.1000
33 -118.6453 3.6033 27.58 1.755201
34 -51.9780 BF
[Aspherical data]
Side 6 κ = 2.000, A4 = -3.54713E-06, A6 = 8.39421E-09
A8 = 5.74900E-12, A10 = -2.30186E-14, A12 = 0.00000E + 00
Side 13 κ = 1.0000, A4 = -8.88610E-06, A6 = 8.60054E-10
A8 = 9.35296E-11, A10 = -8.32892E-13, A12 = 0.00000E + 00
Surface 15 κ = 1.0000, A4 = -1.25166E-05, A6 = 2.21212E-08
A8 = -2.03902E-10, A10 = 7.07567E-13, A12 = 0.00000E + 00
Side 27 κ = 1.0000, A4 = 2.74577E-05, A6 = -5.57744E-08
A8 = 3.60461E-10, A10 = -1.20456E-12, A12 = 0.00000E + 00
Side 30 κ = 1.0000, A4 = -6.49026E-06, A6 = 5.84808E-08
A8 = -3.26107E-10, A10 = 9.49542E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 99.48878
G2 6 -15.91549
G3 15 36.81358
G4 22 35.33722
G5 28 -59.27007
G6 31 -101.60759
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.70000 50.00001 105.00002 194.00004
D0 ∞ ∞ ∞ ∞
D1 1.50000 16.10146 35.16750 51.29406
D2 17.11600 9.70503 4.20600 1.50000
D3 7.94167 4.05851 2.07803 1.50000
D4 8.59873 5.64789 5.81781 1.50000
D5 9.32368 17.20284 18.29639 22.86408
BF 9.30000 21.40756 37.52953 50.12197
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06152 -0.11064 -0.19039 -0.28955
D0 370.9313 400.5881 451.6162 495.9313
D1 1.50000 16.10146 35.16750 51.29406
D2 17.11600 9.70503 4.20600 1.50000
D3 7.94167 4.05851 2.07803 1.50000
D4 10.20432 7.93636 10.79923 11.04504
D5 7.71809 14.91438 13.31498 13.31904
BF 9.32674 21.49415 37.78613 50.71489
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.890
Conditional expression (2) ωw = 42.272
Conditional expression (3) ωt = 6.042
Conditional expression (4) fw / f123w = 0.227
Conditional expression (5) ft / f123t = -0.171
Conditional expression (6) BFw / fw = 0.375
Conditional expression (7) (-f5) / fw = 2.392
Conditional expression (8) Mv5 / Mv6 = 1.332
Conditional expression (9) Mv1 / (ft-fw) = 0.439
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 1.872

20 (A) and 20 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the seventh embodiment, respectively. 21 (A) and 21 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the seventh embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the seventh embodiment has various aberrations corrected well and has excellent imaging performance.

(8th Example)
The eighth embodiment will be described with reference to FIGS. 22 to 24 and Table 8. FIG. 22 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the eighth embodiment. The variable magnification optical system ZL (8) according to the eighth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 22, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12 arranged in order from the object side, and a positive meniscus lens L13 having a convex surface facing the object side. It is composed of and.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed. The negative meniscus lens L21 has an aspherical lens surface on the object side.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and an object side. It is composed of a negative meniscus lens L34 with a concave surface facing.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side, a positive meniscus lens L42 with a concave surface facing the object side, and a negative meniscus lens L43 with a concave surface facing the object side. And a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 8 below lists the specifications of the variable magnification optical system according to the eighth embodiment.

(Table 8)
[Overall specifications]
Variable ratio 7.854
f123w = -440.44611
f123t = -323.78995
W M1 M2 T
FNO 4.12083 5.77298 6.33626 6.49162
ω 42.50455 22.44807 11.22387 6.10280
Y 20.61 21.70 21.70 21.70
TL 120.46149 143.33661 170.26168 190.2487
[Lens specifications]
Surface number RD νd nd
1 119.2532 2.0000 25.26 1.902000
2 75.4740 6.1889 82.57 1.497820
3 -685.9404 0.1000
4 62.0223 5.1009 67.90 1.593190
5 237.4793 D1 (variable)
6 * 153.6662 1.5000 46.59 1.816000
7 15.5464 4.2474
8 -40.2333 1.5002 43.79 1.848500
9 79.6309 0.1006
10 32.2669 3.5980 22.74 1.808090
11 -38.3529 0.7346
12 -22.0127 1.5000 43.79 1.848500
13 -91.6465 D2 (variable)
14 ∞ 1.5000 (Aperture S)
15 44.5290 2.6559 44.85 1.743972
16 -81.3774 0.7000
17 33.2106 3.4046 30.99 1.940752
18 19.5338 3.9016 59.70 1.508752
19 -65.3422 1.3372
20 -26.7545 1.5000 29.68 1.730111
21 -101.6153 D3 (variable)
22 33.1030 6.1030 70.40 1.487502
23 -28.7765 0.1000
24 -116.0123 3.4598 68.30 1.507497
25 -28.0491 1.5000 32.03 1.910214
26 -237.5876 0.2542
27 95.5133 3.1295 59.13 1.611115
28 * -51.7400 D4 (variable)
29 333.8201 3.4464 22.74 1.808090
30 -49.9705 1.5000 44.82 1.743986
31 * 31.2247 D5 (variable)
32 -27.4502 1.5000 66.16 1.531180
33 -59.8926 0.1000
34 164.9552 2.6581 27.80 1.749763
35 -519.6427 BF
[Aspherical data]
Side 6 κ = 1.0000, A4 = 2.54661E-06, A6 = 1.57681E-08
A8 = -1.62633E-10, A10 = 6.99665E-13, A12 = 0.00000E + 00
Side 28 κ = 1.0000, A4 = 2.83706E-05, A6 = -3.41484E-08
A8 = 2.83345E-10, A10 = -4.50609E-13, A12 = 0.00000E + 00
Side 31 κ = 1.0000, A4 = -4.24770E-06, A6 = 6.21761E-08
A8 = -2.709037E-10, A10 = 4.34156E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 99.94559
G2 6 -15.36108
G3 15 40.04464
G4 22 30.83594
G5 29 -50.14179
G6 32 -238.46610
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.69999 49.99998 104.99995 193.99998
D0 ∞ ∞ ∞ ∞
D1 1.50000 18.29170 34.70486 54.28408
D2 15.49680 10.23739 4.55937 1.50000
D3 10.63532 4.97092 1.81398 1.50000
D4 8.89670 4.43383 5.19646 1.51052
D5 9.31183 19.43911 21.83341 25.83333
BF 9.29998 20.64280 36.83273 40.29998
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06119 -0.09874 -0.16976 -0.27724
D0 371.9273 449.0522 522.1271 502.1400
D1 1.50000 18.29170 34.70486 54.28408
D2 15.49680 10.23739 4.55937 1.50000
D3 10.63532 4.97092 1.81398 1.50000
D4 10.32916 6.26965 9.16937 12.36360
D5 7.87937 17.60328 17.86051 14.98025
BF 9.32282 20.70243 37.00914 40.76930
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.854
Conditional expression (2) ωw = 42.505
Conditional expression (3) ωt = 6.103
Conditional expression (4) fw / f123w = -0.056
Conditional expression (5) ft / f123t = -0.599
Conditional expression (6) BFw / fw = 0.377
Conditional expression (7) (-f5) /fw=2.030
Conditional expression (8) Mv5 / Mv6 = 1.533
Conditional expression (9) Mv1 / (ft-fw) = 0.412
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.467

23 (A) and 23 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eighth embodiment, respectively. 24 (A) and 24 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eighth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the eighth embodiment has various aberrations corrected well and has excellent imaging performance.

(9th Example)
A ninth embodiment will be described with reference to FIGS. 25 to 27 and Table 9. FIG. 25 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the ninth embodiment. The variable magnification optical system ZL (9) according to the ninth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 25, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 is a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a plano-convex positive lens L12 having a plane facing the image plane I side, which are arranged in order from the object side, and the object side. It is composed of a positive meniscus lens L13 having a convex surface facing the surface.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed. The negative meniscus lens L21 has an aspherical lens surface on the object side. The negative meniscus lens L24 has an aspherical lens surface on the image plane I side.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of the biconvex positive lens L32 and a negative meniscus lens L33 with a concave surface facing the object side, and both concaves. It is composed of a junction lens of a negative lens L34 having a shape and a positive meniscus lens L35 having a convex surface facing the object side. The positive lens L31 has an aspherical lens surface on the object side. The negative lens L34 has an aspherical lens surface on the object side.

The fourth lens group G4 is composed of a junction lens of a negative meniscus lens L41 having a convex surface facing the object side, a biconvex positive lens L42, and a biconvex positive lens L43 arranged in order from the object side. NS. In the positive lens L43, the lens surface on the image plane I side is an aspherical surface.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative lens L34 and the positive meniscus lens L35 in the third lens group G3 constitutes an anti-vibration group having a negative refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 9 below lists the specifications of the variable magnification optical system according to the ninth embodiment.

(Table 9)
[Overall specifications]
Variable ratio 7.854
f123w = 46.29531
f123t = 1060.13724
W M1 M2 T
FNO 4.11505 5.74532 6.36855 6.68279
ω 42.27184 21.88249 10.96245 6.04244
Y 21.03 21.70 21.70 21.70
TL 121.00241 139.79338 169.47903 195.5079
[Lens specifications]
Surface number RD νd nd
1 215.1564 1.5000 23.80 1.846660
2 73.5337 7.2326 67.90 1.593190
3 ∞ 0.1000
4 75.0074 5.6048 40.66 1.883000
5 344.8006 D1 (variable)
6 * 43.3708 1.5000 40.66 1.883000
7 13.2343 4.8088
8 -47.4291 1.5052 40.66 1.883000
9 43.0037 0.1000
10 28.6036 4.0197 20.88 1.922860
11 -55.9891 1.1418
12 -23.0332 1.5000 40.66 1.883000
13 * -75.5957 D2 (variable)
14 ∞ 1.5000 (Aperture S)
15 * 28.4224 4.3742 52.85 1.598604
16 -48.8993 0.1504
17 30.2173 5.4129 70.40 1.487490
18 -31.5840 1.5000 21.23 1.903627
19 -130.7132 1.2693
20 * -107.8541 1.5000 41.09 1.854203
21 30.6579 3.0466 26.18 1.822542
22 165.6444 D3 (variable)
23 33.3486 1.5007 40.66 1.883000
24 13.1929 6.5567 65.07 1.544771
25 -190.2474 0.7289
26 37.5609 4.7319 62.98 1.574225
27 * -76.3130 D4 (variable)
28 80.1779 3.4856 27.58 1.755201
29 -127.8937 1.5007 45.13 1.740338
30 26.5334 D5 (variable)
31 -26.2026 1.5000 60.35 1.619799
32 -54.6221 0.1000
33 586.6701 2.5595 28.29 1.738351
34 -391.8753 BF
[Aspherical data]
Side 6 κ = 1.0000, A4 = -6.29772E-06, A6 = -1.23182E-08
A8 = 7.321161E-11, A10 = -3.10876E-13, A12 = 0.00000E + 00
Page 13 κ = 1.0000, A4 = -8.92953E-06, A6 = -3.71644E-08
A8 = 8.09196E-10, A10 = -5.73691E-12, A12 = 0.00000E + 00
Surface 15 κ = 1.0000, A4 = -1.00000E-05, A6 = 2.20240E-08
A8 = -1.02146E-10, A10 = 0.00000E + 00, A12 = 0.00000E + 00
Side 20 κ = 1.0000, A4 = 3.32815E-06, A6 = 1.66254E-09
A8 = 0.00000E + 00, A10 = 0.00000E + 00, A12 = 0.00000E + 00
Side 27 κ = 1.0000, A4 = 1.00000E-05, A6 = -3.83755E-08
A8 = -1.30773E-10, A10 = -1.22891E-12, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 102.37710
G2 6 -14.98474
G3 15 29.62517
G4 23 38.66055
G5 28 -56.76096
G6 31 -113.46417
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.70007 50.00020 105.00052 194.00105
D0 ∞ ∞ ∞ ∞
D1 1.50000 18.30775 37.76411 54.05443
D2 18.03389 8.85777 3.84960 1.50000
D3 6.37316 1.62225 1.50000 1.64117
D4 2.43986 3.20131 6.09526 1.50000
D5 9.22531 23.30380 13.81143 17.88006
BF 13.00010 14.07041 36.02852 48.50219
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.08175 -0.12239 -0.19581 -0.27905
D0 272.2777 353.4868 423.8013 497.7725
D1 1.50000 18.30775 37.76411 54.05443
D2 18.03389 8.85777 3.84960 1.50000
D3 6.37316 1.62225 1.50000 1.64117
D4 4.23169 6.02328 12.47110 12.78692
D5 7.43347 20.48182 7.43559 6.59314
BF 13.03743 14.15445 36.24396 48.93981
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.887
Conditional expression (2) ωw = 42.272
Conditional expression (3) ωt = 6.042
Conditional expression (4) fw / f123w = 0.534
Conditional expression (5) ft / f123t = 0.179
Conditional expression (6) BFw / fw = 0.526
Conditional expression (7) (-f5) / fw = 2.298
Conditional expression (8) Mv5 / Mv6 = 1.244
Conditional expression (9) Mv1 / (ft-fw) = 0.438
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.830

26 (A) and 26 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the ninth embodiment, respectively. 27 (A) and 27 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the ninth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the ninth embodiment has various aberrations corrected well and has excellent imaging performance.

(10th Example)
The tenth embodiment will be described with reference to FIGS. 28 to 30 and Table 10. FIG. 28 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the tenth embodiment. The variable magnification optical system ZL (10) according to the tenth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 28, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 includes a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a positive meniscus lens L12 having a convex surface facing the object side, which are arranged in order from the object side, and a convex surface facing the object side. It is composed of a positive meniscus lens L13.

The second lens group G2 includes a negative meniscus lens L21 having a convex surface facing the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a biconcave negative lens arranged in order from the object side. It is composed of a lens L24.

The third lens group G3 is a junction lens of a positive meniscus lens L31 having a convex surface facing the object side, a negative meniscus lens L32 having a convex surface facing the object side, and a biconvex positive lens L33 arranged in order from the object side. And a negative meniscus lens L34 with a concave surface facing the object side.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens with a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 10 below lists the specifications of the variable magnification optical system according to the tenth embodiment.

(Table 10)
[Overall specifications]
Variable ratio 4.692
f123w = -96.28619
f123t = -88.05735
W M1 M2 T
FNO 3.66063 4.51062 5.00831 5.83006
ω 42.43419 22.44766 13.66195 10.17394
Y 20.54 21.70 21.70 21.70
TL 116.50601 138.64669 160.34507 171.5048
[Lens specifications]
Surface number RD νd nd
1 200.0000 2.0000 23.80 1.846660
2 108.2337 4.6568 70.32 1.487490
3 1133.5711 0.1000
4 68.7807 5.7029 70.32 1.487490
5 816.5190 D1 (variable)
6 102.0974 1.2000 46.59 1.816000
7 17.6075 4.9760
8 -59.3363 1.1000 51.28 1.659368
9 81.2225 0.1000
10 29.1388 3.9898 23.80 1.846660
11 -107.8110 0.8213
12 -38.4600 1.0000 46.59 1.816000
13 157.0586 D2 (variable)
14 ∞ 2.0000 (Aperture S)
15 41.9442 2.5619 35.72 1.902650
16 552.5411 0.5000
17 41.0223 0.9000 29.12 2.001000
18 23.0700 4.0200 53.74 1.579570
19 -69.7834 1.5452
20 -27.7457 1.0000 32.33 1.953750
21 -68.0384 D3 (variable)
22 33.5256 5.9460 46.59 1.816000
23 -23.9703 1.0000 32.35 1.850260
24-83.2531 0.1000
25 30.5301 1.1000 32.35 1.850260
26 14.8810 10.3852 70.32 1.487490
27 * -119.0936 D4 (variable)
28 81.3890 3.7144 23.80 1.846660
29 -48.0181 1.0000 42.73 1.834810
30 * 23.7254 D5 (variable)
31 -24.5058 1.4000 46.59 1.816000
32 -48.4638 0.1000
33 142.4943 3.2707 37.57 1.683760
34 -160.0000 BF
[Aspherical data]
Page 27 κ = 1.0000, A4 = 4.35979E-05, A6 = -4.15837E-09
A8 = 6.65149E-10, A10 = 0.00000E + 00, A12 = 0.00000E + 00
Side 30 κ = 1.0000, A4 = -2.71688E-06, A6 = 1.79186E-08
A8 = -3.84607E-10, A10 = 0.00000E + 00, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 143.63567
G2 6 -20.08403
G3 15 60.03586
G4 22 25.77538
G5 28 -42.36974
G6 31 -151.12346
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72617 50.01050 85.01086 116.00340
D0 ∞ ∞ ∞ ∞
D1 1.50000 23.91054 40.85381 47.19819
D2 17.00636 9.20443 4.57783 1.50000
D3 9.28353 3.49337 1.15783 0.30000
D4 2.84012 1.14718 1.49326 3.00287
D5 7.97989 15.46299 17.45245 16.80067
BF 11.70601 19.23807 28.61979 36.51305
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06049 -0.09676 -0.16160 -0.22064
D0 377.2840 455.1463 433.4475 422.2840
D1 1.50000 23.91054 40.85381 47.19819
D2 17.00636 9.20443 4.57783 1.50000
D3 9.28353 3.49337 1.15783 0.30000
D4 3.90798 2.82710 4.74497 7.99347
D5 6.91203 13.78307 14.20074 11.81007
BF 11.72550 19.28822 28.75888 36.77070
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 4.692
Conditional expression (2) ωw = 42.434
Conditional expression (3) ωt = 10.174
Conditional expression (4) fw / f123w = -0.257
Conditional expression (5) ft / f123t = -1.323
Conditional expression (6) BFw / fw = 0.473
Conditional expression (7) (-f5) / fw = 1.714
Conditional expression (8) Mv5 / Mv6 = 1.356
Conditional expression (9) Mv1 / (ft-fw) = 0.603
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.492

29 (A) and 29 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the tenth embodiment, respectively. 30 (A) and 30 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the tenth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the tenth embodiment has various aberrations satisfactorily corrected and has excellent imaging performance.

(11th Example)
The eleventh embodiment will be described with reference to FIGS. 31 to 33 and Table 11. FIG. 31 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the eleventh embodiment. The variable magnification optical system ZL (11) according to the eleventh embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of 6 lens groups G6. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 31, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally.

The first lens group G1 includes a junction lens of a negative meniscus lens L11 having a convex surface facing the object side and a positive meniscus lens L12 having a convex surface facing the object side, which are arranged in order from the object side, and a convex surface facing the object side. It is composed of a positive meniscus lens L13.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and an object side. It is composed of a negative meniscus lens L34 with a concave surface facing.

The fourth lens group G4 includes a junction lens of a biconvex positive lens L41 and a biconcave negative lens L42 arranged in order from the object side, and a negative meniscus lens L43 with a convex surface facing the object side and a biconvex shape. It is composed of a junction lens with the positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a positive meniscus lens L51 with a concave surface facing the object side and a negative lens L52 having a biconcave shape. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62. The image plane I is arranged on the image side of the sixth lens group G6.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 11 below lists the specifications of the variable magnification optical system according to the eleventh embodiment.

(Table 11)
[Overall specifications]
Variable ratio 3.438
f123w = 2466.12612
f123t = -146.93338
W M1 M2 T
FNO 3.65039 4.00020 ― 4.50024
ω 43.52469 -22.45389 ― 13.66502
Y 21.27 21.70-21.70
TL 116.50677 138.27327 ― 161.50351
[Lens specifications]
Surface number RD νd nd
1 200.0000 2.0000 23.80 1.846660
2 112.4996 4.3442 70.32 1.487490
3 642.3642 0.1000
4 64.3082 6.0839 70.32 1.487490
5 1033.4518 D1 (variable)
6 91.5822 1.2000 46.59 1.816000
7 16.7434 5.0969
8 -135.4549 1.1000 50.66 1.670176
9 31.8729 0.1000
10 24.8799 4.1715 23.80 1.846660
11 -336.6794 1.4309
12 -32.2164 1.0000 46.59 1.816000
13 -277.8484 D2 (variable)
14 ∞ 2.0000 (Aperture S)
15 41.4933 2.7587 43.79 1.848500
16 -1372.9949 0.5000
17 55.1173 0.9000 34.87 1.847939
18 24.3945 4.0805 56.69 1.586546
19 -76.2325 1.8582
20 -25.5665 1.0000 34.04 1.847872
21 -37.7016 D3 (variable)
22 46.4011 6.1027 46.59 1.816000
23 -43.4919 1.0000 26.59 1.847083
24 397.5382 0.1000
25 28.7499 1.1000 32.35 1.850260
26 18.0000 11.1086 70.32 1.487490
27 * -25.6478 D4 (variable)
28 -713.8966 3.6653 23.80 1.846660
29 -42.0000 1.0000 45.28 1.796882
30 * 31.7158 D5 (variable)
31 -19.7135 1.4000 62.26 1.536206
32 -42.7591 0.1000
33 217.1940 3.3164 37.57 1.683760
34 -160.0000 BF
[Aspherical data]
Side 27 κ = 1.0000, A4 = 6.15332E-05, A6 = -2.11407E-07
A8 = 7.47121E-10, A10 = -1.12141E-12, A12 = 0.00000E + 00
Side 30 κ = 1.0000, A4 = -1.68999E-05, A6 = 1.65258E-07
A8 = -4.68439E-10, A10 = 7.74341E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 135.65910
G2 6 -17.91192
G3 15 42.22744
G4 22 26.33888
G5 28 -39.70963
G6 31 -150.62287
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity Point at infinity f 24.72587 50.00755 ― 85.00361
D0 ∞ ∞ ― ∞
D1 1.50000 24.03902 ― 40.38368
D2 13.72037 5.30562 ― 1.50000
D3 8.95150 2.76337 ― 0.30000
D4 1.97894 1.51459 ― 1.15589
D5 10.03133 16.68380 ― 19.50588
BF 11.70677 19.34900 ― 30.04020
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06066 -0.11959 ― -0.19908
D0 377.2840 355.5169 ― 332.2840
D1 1.50000 24.03902 ― 40.38368
D2 13.72037 5.30562 ― 1.50000
D3 8.95150 2.76337 ― 0.30000
D4 2.78309 3.22774 ― 4.28073
D5 9.22718 14.97065 ― 16.38104
BF 11.72684 19.42705 ― 30.25539
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 3.438
Conditional expression (2) ωw = 43.525
Conditional expression (3) ωt = 13.665
Conditional expression (4) fw / f123w = 0.010
Conditional expression (5) ft / f123t = -0.579
Conditional expression (6) BFw / fw = 0.473
Conditional expression (7) (-f5) / fw = 1.616
Conditional expression (8) Mv5 / Mv6 = 1.517
Conditional expression (9) Mv1 / (ft-fw) = 0.746
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1) = 0.671

32 (A) and 32 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eleventh embodiment, respectively. 33 (A) and 33 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the eleventh embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the eleventh embodiment has various aberrations satisfactorily corrected and has excellent imaging performance.

(12th Example)
A twelfth embodiment will be described with reference to FIGS. 34 to 36 and Table 12. FIG. 34 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the twelfth embodiment. The variable magnification optical system ZL (12) according to the twelfth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. It is composed of an aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, and a fifth lens group G5 having a negative refractive power. When scaling from the wide-angle end state to the telephoto end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, and the fifth lens group G5 It moves along the optical axis in the direction indicated by the arrow in FIG. 34, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the fifth lens group G5 move integrally.

The first lens group G1 is composed of a negative meniscus lens L11 having a convex surface facing the object side, a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side, which are arranged in order from the object side. Will be done.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and both concaves. It is composed of a negative lens L34 having a shape.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens of a biconvex positive lens L44 and a junction lens of a biconvex positive lens L45 and a biconcave negative lens L46. The positive lens L44 has an aspherical lens surface on the image plane I side. The negative lens L46 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a negative meniscus lens L51 having a concave surface facing the object side and a biconvex positive lens L52 arranged in order from the object side. The negative meniscus lens L51 has an aspherical lens surface on the image plane I side. The image plane I is arranged on the image side of the fifth lens group G5.

In this embodiment, by moving the junction lens of the positive lens L45 and the negative lens L46 in the fourth lens group G4 to the image plane I side, from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Is focused. When the magnification is changed during focusing on a short-range object, the focusing lens of the positive lens L41 and the negative meniscus lens L42 and the junction lens of the negative meniscus lens L43 and the positive lens L44 in the fourth lens group are in focus. The junction lens between the positive lens L45 and the negative lens L46 moves with different amounts of movement. When the magnification is changed when the infinity object is in focus, all the lenses of the fourth lens group G4 move integrally. Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 12 below lists the specifications of the variable magnification optical system according to the twelfth embodiment.

(Table 12)
[Overall specifications]
Variable ratio 7.848
f123w = -297.77158
f123t = -199.23081
W M1 M2 T
FNO 4.12000 5.69956 6.30000 6.50003
ω 42.96973 22.56096 11.03929 6.08825
Y 21.29 21.70 21.70 21.70
TL 129.0507 143.6432 173.1936 191.4323
[Lens specifications]
Surface number RD νd nd
1 181.0189 2.0855 31.27 1.90366
2 74.7364 0.8982
3 78.3131 6.0267 67.90 1.59319
4-878.3490 0.1429
5 65.0716 4.8340 67.90 1.59319
6 661.4054 D1 (variable)
7 171.3932 1.1000 35.72 1.90265
8 18.9469 5.2527
9 -57.6716 1.0000 52.33 1.75500
10 53.7286 0.4722
11 34.8478 3.1650 20.88 1.92286
12 -81.2943 1.3566
13 -31.9419 0.9000 46.59 1.81600
14 -487.1030 D2 (variable)
15 ∞ 2.0101 (Aperture S)
16 45.9039 2.3316 35.72 1.90265
17 -163.4046 0.5000
18 33.6170 1.1581 29.12 2.00100
19 19.7670 3.5655 53.74 1.57957
20 -85.9122 1.3700
21 -41.3606 1.0329 32.33 1.95375
22 1717.1475 D3 (variable)
23 37.7633 4.9751 42.73 1.83481
24 -38.9447 1.0000 31.27 1.90366
25 -804.1582 0.1000
26 29.7427 3.0986 32.33 1.95375
27 15.4408 8.8739 81.49 1.49710
28 * -39.9876 D4 (variable)
29 10338.5730 3.6738 23.80 1.84666
30 -27.6080 1.0000 40.13 1.85135
31 * 31.8891 D5 (variable)
32 -29.8624 1.4000 40.13 1.85135
33 * -63.8559 0.1000
34 66.4034 4.5715 37.57 1.68376
35 -424.4531 BF
[Aspherical data]
Side 28 κ = 1.0000, A4 = 2.91470E-05, A6 = -1.17772E-07
A8 = 9.21285E-10, A10 = -5.994865E-12, A12 = 0.14842E-13
Side 31 κ = 1.0000, A4 = -5.83910E-06, A6 = 1.34714E-07
A8 = -1.32747E-09, A10 = 8.60735E-12, A12 = -0.22325E-13
Side 33 κ = 1.0000, A4 = 4.26328E-06, A6 = -4.06929E-09
A8 = 4.06528E-11, A10 = -1.22140E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 105.7291
G2 7 -16.8196
G3 16 48.27007
G4 23 44.51528
G5 32 -372.043
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72000 49.99999 104.99993 194.00004
D0 ∞ ∞ ∞ ∞
D1 1.73220 15.73205 40.41864 55.46338
D2 20.01315 10.99318 5.91904 1.09143
D3 13.56296 6.37783 3.44003 1.69135
D4 4.09147 4.09147 4.09147 4.09147
D5 9.90112 17.08625 20.02405 21.77273
BF 11.75486 21.36749 31.30545 39.32701
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06144 -0.10950 -0.17803 -0.26497
D0 370.94930 406.35680 476.80640 558.56770
D1 1.73220 15.73205 40.41864 55.46338
D2 20.01315 10.99318 5.91904 1.09143
D3 13.56296 6.37783 3.44003 1.69135
D4 4.89647 5.55202 7.55497 11.91843
D5 9.09612 15.62570 16.56055 13.94577
BF 11.75486 21.36749 31.30545 39.32701
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.884
Conditional expression (2) ωw = 42.970
Conditional expression (3) ωt = 6.088
Conditional expression (4) fw / f123w = -0.083
Conditional expression (5) ft / f123t = -0.974
Conditional expression (6) BFw / fw = 0.476
Conditional expression (7) (-f5) / fw = 15.051
Conditional expression (9) Mv1 / (ft-fw) = 0.369

35 (A) and 35 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the twelfth embodiment, respectively. 36 (A) and 36 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the twelfth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the twelfth embodiment has various aberrations satisfactorily corrected and has excellent imaging performance.

(13th Example)
The thirteenth embodiment will be described with reference to FIGS. 37 to 39 and Table 13. FIG. 37 is a lens configuration diagram at infinity focusing in the wide-angle end state of the variable magnification optical system according to the thirteenth embodiment. The variable magnification optical system ZL (13) according to the thirteenth embodiment has a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, and an aperture arranged in order from the object side. Aperture S, a third lens group G3 having a positive refractive power, a fourth lens group G4 having a positive refractive power, a fifth lens group G5 having a negative refractive power, and a third lens group having a negative refractive power. It is composed of a 6-lens group G6 and a 7th lens group G7 having a positive refractive power. When scaling from the wide-angle end state to the telescopic end state, the first lens group G1, the second lens group G2, the aperture stop S, the third lens group G3, the fourth lens group G4, the fifth lens group G5, and the third lens group. The 6 lens group G6 moves along the optical axis in the direction indicated by the arrow in FIG. 37, and the distance between adjacent lens groups changes. At the time of scaling, the aperture diaphragm S, the third lens group G3, and the sixth lens group G6 move integrally. Further, at the time of scaling, the seventh lens group G7 is fixed with respect to the image plane I.

The first lens group G1 is composed of a negative meniscus lens L11 having a convex surface facing the object side, a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side, which are arranged in order from the object side. Will be done.

The second lens group G2 has a negative meniscus lens L21 having a convex surface facing the object side, a negative lens L22 having a biconcave shape, a positive lens L23 having a biconvex shape, and a concave surface on the object side, which are arranged in order from the object side. It is composed of a negative meniscus lens L24 that is directed.

The third lens group G3 includes a biconvex positive lens L31 arranged in order from the object side, a junction lens of a negative meniscus lens L32 with a convex surface facing the object side, and a biconvex positive lens L33, and an object side. It is composed of a negative meniscus lens L34 with a concave surface facing.

The fourth lens group G4 is a junction lens of a biconvex positive lens L41 arranged in order from the object side and a negative meniscus lens L42 having a concave surface facing the object side, and a negative meniscus lens L43 having a convex surface facing the object side. It is composed of a junction lens with a biconvex positive lens L44. The positive lens L44 has an aspherical lens surface on the image plane I side.

The fifth lens group G5 is composed of a junction lens of a biconvex positive lens L51 and a biconcave negative lens L52. The negative lens L52 has an aspherical lens surface on the image plane I side.

The sixth lens group G6 is composed of a negative meniscus lens L61 having a concave surface facing the object side and a biconvex positive lens L62 arranged in order from the object side. An air lens is formed between the negative meniscus lens L61 and the positive lens L62.

The seventh lens group G7 is composed of a positive meniscus lens L71 with a concave surface facing the object side. The image plane I is arranged on the image side of the seventh lens group G7.

In this embodiment, by moving the fifth lens group G5 to the image plane I side, focusing is performed from a long-distance object to a short-distance object (from an infinity object to a finite-distance object). Further, in this embodiment, the junction lens of the negative meniscus lens L32 and the positive lens L33 in the third lens group G3 constitutes an anti-vibration group having a positive refractive power that can move in a direction perpendicular to the optical axis. The displacement of the imaging position due to camera shake or the like (image blur on the image plane I) is corrected.

Table 13 below lists the specifications of the variable magnification optical system according to the thirteenth embodiment.

(Table 13)
[Overall specifications]
Variable ratio 7.852
f123w = -242.5247
f123t = -265.90409
W M1 M2 T
FNO 4.12000 5.69956 6.30000 6.50003
ω 42.96973 22.56096 11.03929 6.08825
Y 20.93 21.70 21.70 21.70
TL 127.52968 144.84356 169.66796 191.04949
[Lens specifications]
Surface number RD νd nd
1 183.1489 1.7000 31.27 1.90366
2 76.2993 0.8845
3 78.7954 6.1936 67.90 1.59319
4-594.6799 0.1000
5 61.9988 5.6077 67.90 1.59319
6 371.0839 D1 (variable)
7 190.1957 1.1000 35.72 1.90265
8 19.1266 5.1112
9 -52.1202 1.0000 52.33 1.75500
10 58.1840 0.5132
11 36.9591 3.1252 20.88 1.92286
12 -69.4993 0.6909
13 -34.0835 0.9000 46.59 1.81600
14 -15713.5710 D2 (variable)
15 ∞ 2.0000 (Aperture S)
16 40.7989 2.3289 35.72 1.90265
17 -299.8253 0.5000
18 38.9427 1.0000 29.12 2.00100
19 21.5486 3.5304 53.74 1.57957
20 -63.7114 1.3676
21 -35.4002 1.0000 32.33 1.95375
22 -265.5862 D3 (variable)
23 37.7375 4.7476 42.73 1.83481
24 -37.5607 1.0000 31.27 1.90366
25 -325.9958 0.1000
26 31.4406 3.1004 32.33 1.95375
27 15.3849 8.5803 81.49 1.49710
28 * -42.3410 D4 (variable)
29 572.4423 3.1728 23.80 1.84666
30 -34.5910 1.0000 40.13 1.85135
31 * 31.5461 D5 (variable)
32 -19.9700 1.4000 40.13 1.85135
33 * -28.8707 0.1000
34 136.4370 3.5760 37.57 1.68376
35 -114.7970 D6 (variable)
36 -118.5432 2.3370 63.88 1.51680
37 -70.3002 BF
[Aspherical data]
Side 28 κ = 1.0000, A4 = 3.787774E-05, A6 = -4.14498E-07
A8 = 6.80734E-09, A10 = -6.10728E-11, A12 = 0.20806E-12
Side 31 κ = 1.0000, A4 = -1.36815E-05, A6 = 2.49099E-07
A8 = -3.33308E-09, A10 = 2.73107E-11, A12 = -0.88099E-13
Side 33 κ = 1.0000, A4 = 1.98989E-06, A6 = -1.03153E-08
A8 = 4.34935E-11, A10 = -1.04756E-13, A12 = 0.00000E + 00
[Lens group data]
Focal length
G1 1 103.06116
G2 7 -17.00821
G3 16 49.18043
G4 23 29.23287
G5 29 -39.13048
G6 32 -1300.48544
G7 36 328.82617
[Variable interval data]
W M1 M2 T
Point at infinity Point at infinity Point at infinity point at infinity f 24.72000 50.00000 104.99999 194.09403
D0 ∞ ∞ ∞ ∞
D1 1.50000 17.37231 39.57659 56.44287
D2 19.29037 11.03703 4.56142 1.16368
D3 12.96315 6.13632 3.05308 1.47831
D4 4.87593 4.10851 5.56324 1.90252
D5 9.73283 17.32708 18.95559 24.19108
D6 0.80000 10.49492 19.59067 27.50369
BF 10.60000 10.59999 10.59998 10.59995
W M1 M2 T
Short Distance Short Distance Short Distance Short Distance β -0.06123 -0.10885 -0.17758 -0.28031
D0 372.47030 405.15640 480.33200 508.95050
D1 1.50000 17.37231 39.57659 56.44287
D2 19.29037 11.03703 4.56142 1.16368
D3 12.96315 6.13632 3.05308 1.47831
D4 5.77372 5.76435 9.89727 11.65975
D5 8.83504 15.67124 14.62157 14.43385
D6 0.80000 10.49492 19.59067 27.50369
BF 11.75486 21.36749 31.30545 39.32701
[Conditional expression correspondence value]
Conditional expression (1) ft / fw = 7.852
Conditional expression (2) ωw = 42.970
Conditional expression (3) ωt = 6.088
Conditional expression (4) fw / f123w = -0.102
Conditional expression (5) ft / f123t = -0.730
Conditional expression (6) BFw / fw = 0.429
Conditional expression (7) (-f5) / fw = 1.583
Conditional expression (8) Mv5 / Mv6 = 1.541
Conditional expression (9) Mv1 / (ft-fw) = 0.375
Conditional expression (10) (RAR2 + RAR1) / (RAR2-RAR1)
=-0.651

38 (A) and 38 (B) are aberration diagrams at infinity focusing in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the thirteenth embodiment, respectively. 39 (A) and 39 (B) are coma aberration diagrams when blur correction is performed in the wide-angle end state and the telephoto end state of the variable magnification optical system according to the thirteenth embodiment, respectively. From each aberration diagram, it can be seen that the variable magnification optical system according to the thirteenth embodiment has various aberrations satisfactorily corrected and has excellent imaging performance.

According to each embodiment, it is possible to realize a variable magnification optical system in which various aberrations such as spherical aberration are satisfactorily corrected.

Here, each of the above examples shows a specific example of the present invention, and the present invention is not limited thereto.

The following contents can be appropriately adopted as long as the optical performance of the variable magnification optical system according to the present embodiment is not impaired.

As numerical examples of the variable magnification optical system, those having a 5-group, 6-group, and 7-group configuration are shown, but the present application is not limited to this, and variations of other group configurations (for example, 4 groups, 8 groups, etc.) are shown. A magnification optical system can also be configured. Specifically, a lens or a lens group may be added to the most object side or the most image plane side of the variable magnification optical system. The lens group refers to a portion having at least one lens separated by an air interval that changes at the time of magnification change.

The lens surface may be formed on a spherical surface or a flat surface, or may be formed on an aspherical surface. When the lens surface is spherical or flat, lens processing and assembly adjustment are facilitated, and deterioration of optical performance due to processing and assembly adjustment errors can be prevented, which is preferable. Further, even if the image plane is deviated, the depiction performance is less deteriorated, which is preferable.

When the lens surface is aspherical, the aspherical surface is an aspherical surface formed by grinding, a glass mold aspherical surface formed by forming glass into an aspherical shape, or a composite aspherical surface formed by forming resin on the glass surface into an aspherical shape. It doesn't matter which one. Further, the lens surface may be a diffraction surface, and the lens may be a refractive index distribution type lens (GRIN lens) or a plastic lens.

An antireflection film having a high transmittance in a wide wavelength range may be applied to each lens surface in order to reduce flare and ghost and achieve high contrast optical performance. As a result, flare and ghost can be reduced, and high optical performance with high contrast can be achieved.

G1 1st lens group G2 2nd lens group G3 3rd lens group G4 4th lens group G5 5th lens group G6 6th lens group G7 7th lens group I image plane S Aperture aperture

Claims (24)

A first lens group having a positive refractive power, a second lens group having a negative refractive power, a third lens group having a positive refractive power, and a third lens group having a positive refractive power arranged in order from the object side. It is a variable magnification optical system having a 4 lens group, a 5th lens group, and a 6th lens group.
At the time of scaling, a plurality of lens groups in the variable magnification optical system move, and the distance between adjacent lens groups changes.
Has an aperture that moves when scaling
A variable magnification optical system in which the lens group on the image side and the aperture of the lens group that move at the time of magnification change are integrally moved at the time of magnification change. A first lens group having a positive refractive power, a second lens group having a negative refractive power, a third lens group having a positive refractive power, and a third lens group having a positive refractive power arranged in order from the object side. It is a variable magnification optical system having a 4 lens group, a 5th lens group, and a 6th lens group.
At the time of scaling, a plurality of lens groups including the third lens group in the variable magnification optical system move, and the distance between adjacent lens groups changes.
A variable magnification optical system in which the image-side lens group and the third lens group move integrally at the time of magnification change among the lens groups that move at the time of magnification change. The variable magnification optical system according to claim 1 or 2, wherein the sixth lens group comprises two or more lenses. The variable magnification optical system according to any one of claims 1 to 3, wherein the sixth lens group and the diaphragm move integrally at the time of magnification change. The variable magnification optical system according to any one of claims 1 to 4, wherein the sixth lens group and the third lens group move integrally at the time of magnification change. The variable magnification optical system according to any one of claims 1 to 5, wherein the diaphragm and the third lens group move integrally at the time of magnification change. The variable magnification optical system according to any one of claims 1 to 6, which satisfies the following conditional expression.
3.00 <ft / fw <30.00
However, ft: the focal length of the variable magnification optical system in the telephoto end state fw: the focal length of the variable magnification optical system in the wide-angle end state. The variable magnification optical system according to any one of claims 1 to 7, which satisfies the following conditional expression.
35.0 ° <ωw <75.0 °
However, ωw: half angle of view of the variable magnification optical system in the wide-angle end state The variable magnification optical system according to any one of claims 1 to 8, which satisfies the following conditional expression.
2.5 ° <ωt <15.0 °
However, ωt: half angle of view of the variable magnification optical system in the telephoto end state The variable magnification optical system according to any one of claims 1 to 9, which satisfies the following conditional expression.
−0.30 <fw / f123w <0.60
However, fw: the focal length of the variable magnification optical system in the wide-angle end state f123w: the combined focal length of the first lens group, the second lens group, and the third lens group in the wide-angle end state. The variable magnification optical system according to any one of claims 1 to 10, which satisfies the following conditional expression.
-1.50 <ft / f123t <1.00
However, ft: the focal length of the variable magnification optical system in the telephoto end state f123t: the combined focal length of the first lens group, the second lens group, and the third lens group in the telephoto end state. The variable magnification optical system according to any one of claims 1 to 11, which satisfies the following conditional expression.
0.20 <BFw / fw <0.60
However, BFw: the distance from the lens surface to the image plane on the image side of the variable magnification optical system in the wide-angle end state fw: the focal length of the variable magnification optical system in the wide-angle end state. The variable magnification optical system according to any one of claims 1 to 12, wherein the fifth lens group moves with respect to the image plane when the lens is in focus. The variable magnification optical system according to any one of claims 1 to 13, wherein the fifth lens group includes at least one positive lens and at least one negative lens. The variable magnification optical system according to any one of claims 1 to 14, which satisfies the following conditional expression.
1.00 <(-f5) / fw <16.00
However, f5: the focal length of the fifth lens group fw: the focal length of the variable magnification optical system in the wide-angle end state. The variable magnification optical system according to any one of claims 1 to 15, which satisfies the following conditional expression.
1.00 <Mv5 / Mv6 <3.00
However, Mv5: the amount of movement of the fifth lens group when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object side is +).
Mv6: Amount of movement of the sixth lens group when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object is +). The variable magnification optical system according to any one of claims 1 to 16, wherein the first lens group moves with respect to an image plane at the time of magnification change. The variable magnification optical system according to any one of claims 1 to 17, wherein the first lens group comprises three or more lenses. The variable magnification optical system according to any one of claims 1 to 18, which satisfies the following conditional expression.
0.30 <Mv1 / (ft-fw) <0.80
However, Mv1: the amount of movement of the first lens group when scaling from the wide-angle end state to the telephoto end state (the sign of the amount of movement toward the object is +).
ft: Focal length of the variable magnification optical system in the telephoto end state fw: Focal length of the variable magnification optical system in the wide-angle end state An air lens is provided in the sixth lens group.
The variable magnification optical system according to any one of claims 1 to 19, which satisfies the following conditional expression.
0.00 <(RAR2 + RAR1) / (RAR2-RAR1) <2.00
However, RAr1: the radius of curvature of the lens surface on the object side of the air lens of the sixth lens group RAR2: the radius of curvature of the lens surface on the image side of the air lens of the sixth lens group. At the time of scaling, at least the first lens group, the third lens group, the fourth lens group, the fifth lens group, and the sixth lens group move with respect to the image plane. The variable magnification optical system according to any one of claims 1 to 20. The variable magnification optical system according to any one of claims 1 to 21, wherein the lens group that moves at the time of magnification change is the lens group that moves toward the object side when the magnification is changed from the wide-angle end state to the telephoto end state. An optical device including the variable magnification optical system according to any one of claims 1 to 22. A first lens group having a positive refractive power, a second lens group having a negative refractive power, a third lens group having a positive refractive power, and a third lens group having a positive refractive power arranged in order from the object side. A method for manufacturing a variable magnification optical system having a 4 lens group, a 5th lens group, and a 6th lens group.
At the time of scaling, a plurality of lens groups in the variable magnification optical system move, and the distance between adjacent lens groups changes.
Has an aperture that moves when scaling
Of the lens groups that move during scaling, the lens group on the image side and the aperture move integrally during scaling.
A method for manufacturing a variable magnification optical system in which each lens is arranged in a lens barrel.

Images