JP2015210383A - Variable power optical system, optical device, and method of manufacturing variable power optical system - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a compact variable power optical system having high variable power ratio and ensuring high optical performance when shifting focus from an infinite object to a nearby object, an optical device, and a variable power optical system.SOLUTION: A variable power optical system include, in order from an object side along an optic axis, a first lens group having positive refractive power, a second lens group having negative refractive power, a third lens group having positive refractive power, a fourth lens group having positive refractive power, and a fifth lens group. In variable magnification from a wide-angle end state to a telephoto end state, a distance between the first and second lens groups, a distance between the second and third groups, a distance between the third and fourth groups, and a distance between the fourth and fifth groups are changed. The fifth lens group moves with respect to an image surface. When shifting focus from an infinite object to a nearby object, the third lens group moves along the optical axis, to satisfy a predetermined conditional expression.

Description

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

  Conventionally, as a variable power optical system suitable for an interchangeable lens for a camera, a digital camera, a video camera, etc., many lenses having a positive refractive power in the most object side lens group have been proposed. Among the systems, there has been proposed an optical system capable of focusing from an infinitely distant object to a close object by moving some lens groups along the optical axis. (For example, see Patent Document 1).

JP 2009-251118 A

  However, the conventional variable power optical system as described above can obtain sufficiently high optical performance at the time of focusing from an object at infinity to a close object when trying to reduce the size while maintaining a high zoom ratio. There was a problem that it was difficult.

  The present invention has been made in view of the above problems, has a high zoom ratio, is small, and has a high optical performance at the time of focusing from an object at infinity to a short distance object. An object of the present invention is to provide an apparatus and a method for manufacturing a variable magnification optical system.

In order to solve the above-described problems, the present invention provides a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a third lens group having a positive refractive power in order from the object side along the optical axis. And an interval between the first lens group and the second lens group at the time of zooming from the wide-angle end state to the telephoto end state, The distance between the second lens group and the third lens group, the distance between the third lens group and the fourth lens group, and the distance between the fourth lens group and the fifth lens group change. The fifth lens group moves with respect to the image plane, and the third lens group moves along the optical axis when focusing from an object at infinity to an object at a short distance, and satisfies the following conditional expression: A variable magnification optical system characterized by the above.
0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

  The present invention also provides an optical apparatus comprising the variable magnification optical system.

Further, according to the present invention, in order from the object side along the optical axis, 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 positive refractive power. A method of manufacturing a variable magnification optical system having a fourth lens group and a fifth lens group, wherein the second lens group satisfies the following conditional expression and changes from the wide-angle end state to the telephoto end state: At the time of magnification, the distance between the first lens group and the second lens group, the distance between the second lens group and the third lens group, and the distance between the third lens group and the fourth lens group The distance between the fourth lens group and the fifth lens group is changed, the fifth lens group is moved with respect to the image plane, and at the time of focusing from an object at infinity to a near object. And providing a method for manufacturing a variable magnification optical system, wherein the third lens group is moved along the optical axis. That.
0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

  According to the present invention, there is provided a variable magnification optical system, an optical apparatus, and a variable magnification optical system manufacturing method having a high zoom ratio, a small size, and high optical performance when focusing from an object at infinity to a short distance object. Can be provided.

(A), (b), and (c) are sectional views in the wide-angle end state, intermediate focal length state, and telephoto end state, respectively, of the variable magnification optical system according to the first example of the present application. (A), (b), and (c) are various figures at the time of focusing on an object at infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the first example of the present application, respectively. It is an aberration diagram. (A), (b), and (c) are respectively when a short-distance object is focused in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the first example of the present application (shooting). FIG. 6 is a diagram showing various aberrations at a magnification of −0.0100. (A), (b), and (c) are sectional views of the variable magnification optical system according to the second example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. (A), (b), and (c) are various values at the time of focusing on an object at infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the second example of the present application, respectively. It is an aberration diagram. (A), (b), and (c) are respectively when a short-distance object is focused in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the second example of the present application (shooting). FIG. 6 is a diagram showing various aberrations at a magnification of −0.0100. (A), (b), and (c) are sectional views of the variable magnification optical system according to the third example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. (A), (b), and (c) are various values at the time of focusing on an object at infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the third example of the present application, respectively. It is an aberration diagram. (A), (b), and (c), respectively, when focusing on a short-distance object in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the third example of the present application (shooting) FIG. 6 is a diagram showing various aberrations at a magnification of −0.0100. (A), (b), and (c) are sectional views in the wide-angle end state, intermediate focal length state, and telephoto end state, respectively, of the variable magnification optical system according to the fourth example of the present application. (A), (b), and (c) are various values at the time of focusing on an object at infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the fourth example of the present application, respectively. It is an aberration diagram. (A), (b), and (c) are respectively when a short-distance object is focused in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the fourth example of the present application (shooting). FIG. 6 is a diagram showing various aberrations at a magnification of −0.0100. It is a figure which shows the structure of the camera provided with the variable magnification optical system of this application. It is a figure which shows the outline of the manufacturing method of the variable magnification optical system of this application.

Hereinafter, a variable magnification optical system, an optical apparatus, and a method for manufacturing the variable magnification optical system of the present application will be described.
The variable magnification optical system of the present application includes, in order from the object side along the optical axis, 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 positive refraction. A power fourth lens group and a fifth lens group, and at the time of zooming from the wide-angle end state to the telephoto end state, the distance between the first lens group and the second lens group, and the second lens The distance between the third lens group and the third lens group, the distance between the third lens group and the fourth lens group, and the distance between the fourth lens group and the fifth lens group are changed. The lens group is characterized by moving relative to the image plane. With this configuration, the variable magnification optical system of the present application realizes variable magnification from the wide-angle end state to the telephoto end state, and can suppress each variation of distortion aberration, astigmatism, and spherical aberration associated with variable magnification. .

  The variable magnification optical system of the present application is configured to move the third lens group along the optical axis for focusing from an object at infinity to an object at a short distance. With this configuration, the amount of movement during focusing on the telephoto side can be reduced, the overall length of the entire optical system can be reduced, and the size can be reduced. In addition, the telephoto side is incident on the third lens group that is the focusing lens group. It is possible to suppress variations in the height of the light beam from the optical axis, and to suppress variations in spherical aberration and astigmatism during focusing.

The variable magnification optical system of the present application is characterized by satisfying the following conditional expression (1).
(1) 0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

Conditional expression (1) defines an appropriate focal length range of the second lens group. By satisfying conditional expression (1), the zoom optical system of the present application can suppress fluctuations in spherical aberration and astigmatism during zooming from the wide-angle end state to the telephoto end state.
If the corresponding value of the conditional expression (1) of the variable magnification optical system of the present application is less than the lower limit value, it becomes difficult to suppress fluctuations in spherical aberration and astigmatism occurring in the second lens group at the time of variable magnification, and high optical performance. You will not be able to achieve performance. In order to secure the effect of the present application, it is more preferable to set the lower limit of conditional expression (1) to 0.045.
On the other hand, when the corresponding value of the conditional expression (1) of the zoom optical system of the present application exceeds the upper limit value, the distance between the first lens group and the second lens group at the time of zooming is obtained in order to obtain a predetermined zoom ratio. It is necessary to increase the amount of change. This not only makes it difficult to reduce the size, but also changes the diameter of the on-axis light beam incident from the first lens group to the second lens group as the magnification changes. For this reason, the variation of the spherical aberration becomes excessive at the time of zooming, and high optical performance cannot be realized. In order to secure the effect of the present application, it is more preferable to set the upper limit of conditional expression (1) to 0.095.

  In the zoom optical system according to the present application, it is preferable that the first lens unit moves toward the object side when zooming from the wide-angle end state to the telephoto end state. With this configuration, it is possible to suppress a change in height from the optical axis of the off-axis light beam that passes through the first lens group at the time of zooming, and not only can the outer diameter of the first lens group be reduced, but also astigmatism at the time of zooming. Variations in aberrations can be suppressed.

Moreover, it is desirable that the variable magnification optical system of the present application satisfies the following conditional expression (2).
(2) 2.970 <f3 / fw <10.000
However,
fw: focal length of the entire zoom optical system in the wide-angle end state f3: focal length of the third lens group

Conditional expression (2) defines an appropriate focal length range of the third lens group. The zooming optical system of the present application satisfies the conditional expression (2), so that spherical aberration and non-focusing at the time of zooming from a wide-angle end state to a telephoto end state and focusing from an infinitely distant object to a short-distance object Variations in point aberration can be suppressed.
If the corresponding value of conditional expression (2) of the variable magnification optical system of the present application is below the lower limit value, it becomes difficult to suppress variations in spherical aberration and astigmatism that occur in the third lens group at the time of zooming or focusing. It becomes impossible to realize high optical performance. In order to secure the effect of the present application, it is more preferable to set the lower limit of conditional expression (2) to 3.300.
On the other hand, if the corresponding value of the conditional expression (2) of the variable magnification optical system of the present application exceeds the upper limit value, the amount of movement of the third lens group at the time of focusing from an infinite object to a close object increases. As a result, the height from the optical axis of the on-axis light beam and off-axis light beam incident on the third lens group at the time of focusing largely fluctuates, so that the variation in spherical aberration and astigmatism increases, and high optical performance is achieved. It will not be possible. In order to secure the effect of the present application, it is more preferable to set the upper limit of conditional expression (2) to 7.000.

Further, it is desirable that the variable magnification optical system of the present application satisfies the following conditional expression (3).
(3) 0.010 <(d4t-d4w) / f4 <1.00
However,
d4t: Distance on the optical axis from the most image-side lens surface of the fourth lens group in the telephoto end state to the most object-side lens surface of the fifth lens group d4w: The fourth lens group in the wide-angle end state Distance on the optical axis from the lens surface closest to the image side to the lens surface closest to the object side of the fifth lens group f4: Focal length of the fourth lens group

Conditional expression (3) is obtained on the optical axis from the most image side lens surface of the fourth lens group to the most object side lens surface of the fifth lens group at the time of zooming from the wide-angle end state to the telephoto end state. It defines an appropriate range of interval change. By satisfying conditional expression (3), the zoom optical system of the present application can suppress fluctuations in astigmatism and distortion in zooming from the wide-angle end state to the telephoto end state.
When the corresponding value of conditional expression (3) of the variable magnification optical system of the present application is below the lower limit value, the fifth lens group suppresses the fluctuation of astigmatism and distortion occurring in the fourth lens group at the time of zooming. This makes it difficult to achieve high optical performance. In order to secure the effect of the present application, it is more preferable to set the lower limit of conditional expression (3) to 0.200.
On the other hand, when the corresponding value of conditional expression (3) of the variable magnification optical system of the present application exceeds the upper limit value, the height from the optical axis of the off-axis light beam incident on the fifth lens group from the fourth lens group becomes variable. It changes greatly with it. For this reason, fluctuations in astigmatism and distortion occurring in the fifth lens group during zooming become excessive, and high optical performance cannot be realized. In addition, since the height of the off-axis light beam from the optical axis in the fifth lens group increases, the outer diameter of the fifth lens group increases. In order to secure the effect of the present application, it is more preferable to set the upper limit of conditional expression (3) to 0.800.

Moreover, it is desirable that the variable magnification optical system of the present application satisfies the following conditional expression (4).
(4) 0.010 <(d5it-d5iw) / (d3it-d3iw) <1.000
However,
d3it: Distance on the optical axis from the lens surface closest to the image side of the third lens group in the telephoto end state to the image plane d3iw: From the lens surface closest to the image side of the third lens group in the wide-angle end state to the image plane D5it: Distance on the optical axis from the lens surface closest to the image side of the fifth lens group in the telephoto end state to the image plane d5iw: Distance on the most image side of the fifth lens group in the wide-angle end state Distance on the optical axis from the lens surface to the image plane

Conditional expression (4) indicates that the change in distance on the optical axis from the lens surface closest to the image side of the third lens group to the image plane at the time of zooming from the wide-angle end state to the telephoto end state, It defines an appropriate range of the ratio of the change in distance on the optical axis from the lens surface closest to the image side to the image surface. By satisfying conditional expression (4), the zoom optical system of the present application can suppress fluctuations in astigmatism and distortion in zooming from the wide-angle end state to the telephoto end state.
When the corresponding value of conditional expression (4) of the variable magnification optical system of the present application is below the lower limit value, the height from the optical axis of the off-axis light beam incident on the fifth lens group from the fourth lens group is accompanied by the variable power. It changes a lot. For this reason, fluctuations in astigmatism and distortion occurring in the fifth lens group during zooming become excessive, and high optical performance cannot be realized. Further, the height of the off-axis light beam incident on the fifth lens group from the optical axis increases, and the diameter of the fifth lens group increases. In order to secure the effect of the present application, it is more preferable to set the lower limit of conditional expression (4) to 0.020.
On the other hand, if the corresponding value of conditional expression (4) of the variable magnification optical system of the present application exceeds the upper limit value, it becomes difficult to suppress the fluctuation of astigmatism occurring in the third lens group at the time of zooming with the fifth lens group. It becomes impossible to realize high optical performance. In order to secure the effect of the present application, it is more preferable to set the upper limit of conditional expression (4) to 0.700.
In order to realize high zoom ratio, the distance on the optical axis from the lens surface closest to the image side of the third lens group to the image plane becomes large when zooming from the wide-angle end state to the telephoto end state. The denominator of conditional expression (4) is preferably a positive value. Thereby, the fluctuation of astigmatism occurring in the third lens group can be suppressed.

  In addition, it is desirable that the zoom optical system of the present application has an aperture stop, and the distance between the aperture stop and the fourth lens group is not changed when zooming from the wide-angle end state to the telephoto end state. With this configuration, it is possible to suppress a change in the height of the off-axis light beam incident on the fourth lens unit from the optical axis during zooming from the wide-angle end state to the telephoto end state, and astigmatism and distortion during zooming. Variations in aberrations can be suppressed.

  In the variable power optical system of the present application, it is desirable that the third lens group moves to the image side when focusing from an object at infinity to an object at a short distance. The variable magnification optical system of the present application can efficiently focus from an object at infinity to a close object by moving the third lens group to the image side during focusing, and can suppress spherical aberration and astigmatism. Variation can be suppressed.

  In the zoom optical system of the present application, it is desirable that the distance between the first lens group and the second lens group is increased when zooming from the wide-angle end state to the telephoto end state. With this configuration, the magnification of the second lens group can be increased, a high zoom ratio can be efficiently realized, and fluctuations in spherical aberration and astigmatism during zooming can be suppressed.

  In the zoom optical system of the present application, it is preferable that the distance between the second lens group and the third lens group is reduced when zooming from the wide-angle end state to the telephoto end state. With this configuration, the composite magnification of the third lens group to the fifth lens group can be increased, and a high zoom ratio can be efficiently realized to suppress variations in spherical aberration and astigmatism during zooming. it can.

  In the variable magnification optical system of the present application, it is desirable that the fifth lens group has a positive refractive power. With this configuration, the use magnification of the fifth lens group becomes smaller than the same magnification, and the combined focal length from the first lens group to the fourth lens group can be relatively increased. As a result, the influence of decentration coma aberration and the like caused by the decentration of the lenses generated in the first lens group to the fourth lens group at the time of manufacture can be suppressed relatively small, and high optical performance can be realized. it can.

  The optical device of the present application is characterized by having the variable magnification optical system having the above-described configuration. Thereby, an optical device having a high zoom ratio, a small size, and high optical performance can be realized.

The variable magnification optical system manufacturing method of the present application includes, in order from the object side along the optical axis, a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a third lens group having a positive refractive power. A method of manufacturing a variable magnification optical system having a fourth lens group having positive refractive power and a fifth lens group,
The second lens group satisfies the following conditional expression (1):
At the time of zooming from the wide-angle end state to the telephoto end state, the distance between the first lens group and the second lens group, the distance between the second lens group and the third lens group, and the third lens group And the distance between the fourth lens group and the distance between the fourth lens group and the fifth lens group are changed, and the fifth lens group is moved relative to the image plane,
The third lens group is moved along the optical axis when focusing from an object at infinity to a near object. As a result, it is possible to manufacture a variable power optical system that has a high zoom ratio, is small, and has high optical performance when focusing from an object at infinity to a short distance object.
(1) 0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

  Hereinafter, a variable magnification optical system according to numerical examples of the present application will be described with reference to the accompanying drawings.

(First embodiment)
1A, 1B, and 1C are cross-sectional views of the zoom optical system according to the first example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. It is.
The variable magnification optical system according to the present example includes, 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, and a third lens having a positive refractive power. The lens group G3 includes a fourth lens group G4 having a positive refractive power and a fifth lens group G5 having a positive refractive power. An aperture stop S is provided between the second lens group G2 and the third lens group G3.

The first lens group G1 includes, in order from the object side, a cemented lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side. Become.
The second lens group G2 includes, in order from the object side, a negative meniscus lens L21 having a convex surface directed toward the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a negative surface having a concave surface directed toward the object side. It consists of a cemented lens with a meniscus lens L24. The negative meniscus lens L21 is a glass mold aspheric lens having an aspheric lens surface on the object side.

The third lens group G3 is composed of a cemented lens of a negative meniscus lens L31 having a convex surface directed toward the object side and a biconvex positive lens L32 in order from the object side.
The fourth lens group G4 includes, in order from the object side, a cemented lens of a biconvex positive lens L41 and a biconcave negative lens L42, and a negative meniscus with a biconvex positive lens L43 and a concave meniscus facing the object side. A cemented lens with a lens L44, a cemented lens with a biconcave negative lens L45 and a biconvex positive lens L46, a biconvex positive lens L47, and a negative meniscus lens L48 with a concave surface facing the object side. It consists of a cemented lens. The negative meniscus lens L48 is a glass mold aspheric lens having an aspheric lens surface on the image side.

  The fifth lens group G5 includes, in order from the object side, a cemented lens including a positive meniscus lens L51 having a concave surface facing the object side and a negative meniscus lens L52 having a concave surface facing the object side. The negative meniscus lens L52 is a glass mold aspheric lens having an aspheric lens surface on the image side.

With the above-described configuration, in the zoom optical system according to the present embodiment, the air gap between the first lens group G1 and the second lens group G2 and the second lens group at the time of zooming from the wide-angle end state to the telephoto end state. The air gap between G2 and the third lens group G3, the air gap between the third lens group G3 and the fourth lens group G4, the air gap between the fourth lens group G4 and the fifth lens group G5, and the fifth lens group G5 The first lens group G1 to the fifth lens group G5 move along the optical axis so that the air spacing between the lens surface and the image plane I changes.
Specifically, the first lens group G1 to the fifth lens group G5 move to the object side. The aperture stop S moves to the object side integrally with the fourth lens group G4 during zooming.
Further, focusing from an infinitely distant object to a close object is performed by moving the third lens group G3 to the image plane I side along the optical axis.

Thereby, at the time of zooming, the air gap between the first lens group G1 and the second lens group G2 increases, the air gap between the second lens group G2 and the third lens group G3 decreases, and the third lens group G3. And the fourth lens group G4 increase, the air distance between the fourth lens group G4 and the fifth lens group G5 increases, and the air distance between the fifth lens group G5 and the image plane I increases. Note that the air space between the aperture stop S and the third lens group G3 decreases during zooming.
Accordingly, the variable magnification optical system according to the present embodiment has a high variable magnification and is configured in a small size.

Table 1 below lists values of specifications of the variable magnification optical system according to the present example.
In Table 1, f indicates the focal length, and BF indicates the back focus (the distance on the optical axis between the lens surface closest to the image side and the image plane I).
In [Surface data], the surface number is the order of the optical surfaces counted from the object side, r is the radius of curvature, d is the surface interval (the interval between the nth surface (n is an integer) and the n + 1th surface), and nd is The refractive index for d-line (wavelength 587.6 nm) and νd indicate the Abbe number for d-line (wavelength 587.6 nm), respectively. In addition, the object plane indicates the object plane, the variable indicates the variable plane spacing, the stop S indicates the aperture stop S, and the image plane indicates the image plane I. The radius of curvature r = ∞ indicates a plane. For the aspherical surface, * is added to the surface number, and the value of the paraxial radius of curvature is indicated in the column of the radius of curvature r. The description of the refractive index of air nd = 1.00000 is omitted.

[Aspherical data] shows an aspherical coefficient and a conic constant when the shape of the aspherical surface shown in [Surface data] is expressed by the following equation.
x = (h ² / r) / [1+ {1−κ (h / r) ² } ^1/2 ]
+ A4h ⁴ + A6h ⁶ + A8h ⁸ + A10h ¹⁰ + A12h ¹²
Here, h is the height in the direction perpendicular to the optical axis, x is the distance (sag amount) from the tangent plane of the apex of the aspheric surface to the aspheric surface at the height h, and κ is the conic constant. , A4, A6, A8, A10, A12 are aspherical coefficients, and r is the radius of curvature of the reference sphere (paraxial radius of curvature). “E−n” (n is an integer) indicates “× 10 ⁻ⁿ ”, for example “1.234E-05” indicates “1.234 × 10 ⁻⁵ ”. The secondary aspherical coefficient A2 is 0 and is not shown.

In [Various data], FNO is the F number, ω is the half angle of view (unit is “°”), Y is the image height, TL is the total length of the variable magnification optical system (image from the first surface when focusing on an object at infinity) (Distance on the optical axis to the surface I), dn represents the variable distance between the nth surface and the (n + 1) th surface, and φ represents the diameter of the aperture stop S. These values are those when focusing on an object at infinity. W represents the wide-angle end state, M represents the intermediate focal length state, and T represents the telephoto end state.
[Focus group movement amount at the time of focusing] indicates the movement amount of the focusing lens group (third lens group) from the infinitely focused state to the short-distance focused state (imaging magnification: -0.0100 times). Here, the moving direction of the focusing lens group is positive when moving toward the image side. The shooting distance indicates the distance from the object to the image plane.
[Lens Group Data] indicates the start surface and focal length of each lens group.
[Conditional Expression Corresponding Value] shows the corresponding value of each conditional expression of the variable magnification optical system according to the present example.

Here, the focal length f, the radius of curvature r, and other length units listed in Table 1 are generally “mm”. However, the optical system is not limited to this because an equivalent optical performance can be obtained even when proportionally enlarged or proportionally reduced.
In addition, the code | symbol of Table 1 described above shall be similarly used also in the table | surface of each Example mentioned later.

(Table 1) First Example
[Surface data]
Surface number r d nd νd
Object ∞

1 135.6506 1.6350 1.950000 29.37
2 41.9822 8.2991 1.497820 82.57
3 -344.6351 0.1000
4 45.0112 4.7994 1.834810 42.73
5 373.7571 Variable

* 6 345.5995 1.0000 1.851348 40.10
7 9.1082 4.2862
8 -21.4543 1.0000 1.903660 31.27
9 38.9573 0.7420
10 26.9213 4.0891 1.808090 22.74
11 -12.6120 1.0000 1.883000 40.66
12 -42.4301 Variable

13 (Aperture S) ∞ Variable

14 29.6793 1.0000 1.883000 40.66
15 15.0612 3.3397 1.593190 67.90
16 -42.4934 Variable

17 12.5743 8.9691 1.717000 47.97
18 -33.1381 1.0000 1.883000 40.66
19 10.7605 2.0000
20 19.2566 3.2971 1.516800 63.88
21 -11.7331 1.0000 1.850260 32.35
22 -20.8570 1.5000
23 -40.3315 1.0000 1.950000 29.37
24 11.6425 3.4850 1.672700 32.18
25 -26.8269 0.1735
26 33.9424 5.2543 1.581440 40.98
27 -8.0332 1.0000 1.820798 42.71
* 28 -31.1190 Variable

29 -40.0000 2.0872 1.497820 82.57
30 -16.7056 1.0000 1.834410 37.28
* 31 -21.8116 BF

Image plane ∞

[Aspherical data]
6th surface κ 11.00000
A4 3.74799E-05
A6 -8.44116E-08
A8 -3.25426E-09
A10 4.01677E-11
A12 -1.75260E-13

28th surface κ 1.00000
A4 -7.52150E-05
A6 -3.56328E-07
A8 1.74159E-09
A10 -3.33007E-11
A12 0.00000E + 00

31st surface κ 1.00000
A4 2.74991E-05
A6 -2.52954E-09
A8 -1.90467E-10
A10 0.00000E + 00
A12 0.00000E + 00

[Various data]
Scaling ratio 14.13

W T
f 9.27 to 130.95
FNO 4.12 to 5.77
ω 42.66-3.35 °
Y 8.00-8.00
TL 111.87 〜 169.05

W M T
f 9.27000 60.49999 130.94999
ω 42.66043 7.22371 3.35343
FNO 4.12 5.77 5.77
φ 8.49 9.57 11.01
d5 2.10000 36.64491 46.82787
d12 24.15923 5.26241 2.20000
d13 4.86826 4.21826 1.80000
d16 2.25000 2.90000 5.31826
d28 1.50000 29.01348 34.90774
BF 13.93934 14.90154 14.93894

[Focus group movement during focusing]
W M T
Shooting magnification -0.0100 -0.0100 -0.0100
Shooting distance 901.6746 5886.4066 12728.2773
Travel 0.1610 0.1701 0.3030

[Lens group data]
Group start surface f
1 1 69.37620
2 6 -9.50000
3 14 41.26133
4 17 51.13596
5 29 150.09211

[Conditional expression values]
(1) (−f2) /ft=0.073
(2) f3 / fw = 4.451
(2) (d4t−d4w) /f4=0.653
(4) (d5it-d5iw) / (d3it-d3iw) = 0.027

2 (a), 2 (b), and 2 (c) respectively show infinity in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the first example of the present application. It is an aberration diagram at the time of focusing on an object.
3 (a), 3 (b), and 3 (c) are short distances in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the first example of the present application, respectively. FIG. 6 is a diagram showing various aberrations when the object is in focus (imaging magnification: -0.0100 times).

  In each aberration diagram, FNO is the F number, NA is the numerical aperture of the light beam emitted from the lens closest to the image side, A is the light beam incident angle, that is, the half field angle (unit is “°”), and H0 is the object height (unit: mm). ) Respectively. d indicates the aberration at the d-line (wavelength 587.6 nm), g indicates the aberration at the g-line (wavelength 435.8 nm), and those without d and g indicate the aberration at the d-line. In the astigmatism diagram, the solid line indicates the sagittal image plane, and the broken line indicates the meridional image plane. Note that the same reference numerals as in this embodiment are used in the aberration diagrams of each embodiment described later.

From the respective aberration diagrams, the variable magnification optical system according to the present embodiment has various aberrations well corrected from the wide-angle end state to the telephoto end state, and from the infinite object focusing state to the short-distance object focusing state, and is high. It can be seen that it has optical performance.

(Second embodiment)
FIGS. 4A, 4B, and 4C are cross-sectional views of the zoom optical system according to the second example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. It is.
The variable magnification optical system according to the present example includes, 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, and a third lens having a positive refractive power. The lens group G3 includes a fourth lens group G4 having a positive refractive power and a fifth lens group G5 having a negative refractive power. An aperture stop S is provided between the second lens group G2 and the third lens group G3.

The first lens group G1 includes, in order from the object side, a cemented lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side. Become.
The second lens group G2 includes, in order from the object side, a negative meniscus lens L21 having a convex surface directed toward the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a biconcave negative lens L24. The cemented lens. The negative meniscus lens L21 is a glass mold aspheric lens having an aspheric lens surface on the object side.

The third lens group G3 is composed of a cemented lens of a negative meniscus lens L31 having a convex surface directed toward the object side and a biconvex positive lens L32 in order from the object side.
The fourth lens group G4 includes, in order from the object side, a cemented lens of a biconvex positive lens L41 and a biconcave negative lens L42, and a negative meniscus with a biconvex positive lens L43 and a concave meniscus facing the object side. A cemented lens with a lens L44, a cemented lens with a biconcave negative lens L45 and a biconvex positive lens L46, a biconvex positive lens L47, and a negative meniscus lens L48 with a concave surface facing the object side. It consists of a cemented lens. The negative meniscus lens L48 is a glass mold aspheric lens having an aspheric lens surface on the image side.

  The fifth lens group G5 includes, in order from the object side, a cemented lens including a positive meniscus lens L51 having a concave surface facing the object side and a negative meniscus lens L52 having a concave surface facing the object side. The negative meniscus lens L52 is a glass mold aspheric lens having an aspheric lens surface on the image side.

With the above-described configuration, in the zoom optical system according to the present embodiment, the air gap between the first lens group G1 and the second lens group G2 and the second lens group at the time of zooming from the wide-angle end state to the telephoto end state. The air gap between G2 and the third lens group G3, the air gap between the third lens group G3 and the fourth lens group G4, the air gap between the fourth lens group G4 and the fifth lens group G5, and the fifth lens group G5 The first lens group G1 to the fifth lens group G5 move along the optical axis so that the air spacing between the lens surface and the image plane I changes.
Specifically, the first lens group G1 to the fifth lens group G5 move to the object side. The aperture stop S moves to the object side integrally with the fourth lens group G4 during zooming.
Further, focusing from an infinitely distant object to a close object is performed by moving the third lens group G3 to the image plane I side along the optical axis.

Thereby, at the time of zooming, the air gap between the first lens group G1 and the second lens group G2 increases, the air gap between the second lens group G2 and the third lens group G3 decreases, and the fourth lens group G4. And the fifth lens group G5 increase, and the air distance between the fifth lens group G5 and the image plane I increases. The air space between the third lens group G3 and the fourth lens group G4 decreases from the wide-angle end state to the intermediate focal length state, and increases from the intermediate focal length state to the telephoto end state. At the time of zooming, the air gap between the aperture stop S and the third lens group G3 increases from the wide-angle end state to the intermediate focal length state and decreases from the intermediate focal length state to the telephoto end state.
Accordingly, the variable magnification optical system according to the present embodiment has a high variable magnification and is configured in a small size.
Table 2 below provides values of specifications of the variable magnification optical system according to the present example.

(Table 2) Second Example
[Surface data]
Surface number r d nd νd
Object ∞

1 141.5341 1.6350 1.950000 29.37
2 42.4212 8.4111 1.497820 82.57
3 -315.7583 0.1000
4 44.6738 4.8257 1.834810 42.73
5 329.2991 Variable

* 6 500.0000 1.0000 1.851348 40.10
7 9.1215 4.1187
8 -36.3703 1.0000 1.903660 31.27
9 36.8310 0.5585
10 20.9196 4.4577 1.808090 22.74
11 -11.3592 1.0000 1.883000 40.66
12 231.4820 Variable

13 (Aperture S) ∞ Variable

14 27.6206 1.0000 1.883000 40.66
15 13.6993 3.2013 1.593190 67.90
16 -42.3833 Variable

17 13.2112 9.5050 1.717000 47.97
18 -49.0716 1.0000 1.883000 40.66
19 11.5987 2.0000
20 23.5510 3.3277 1.516800 63.88
21 -10.5463 1.0000 1.850260 32.35
22 -17.4426 1.5000
23 -39.5142 1.0000 1.950000 29.37
24 14.3546 3.3123 1.672700 32.18
25 -31.7031 1.0351
26 20.4892 5.4304 1.581440 40.98
27 -9.0024 1.0000 1.820798 42.71
* 28 -40.3228 Variable

29 -59.5141 1.1354 1.497820 82.57
30 -26.1606 1.0000 1.834410 37.28
* 31 -50.8846 BF

Image plane ∞

[Aspherical data]
6th surface κ -9.00000
A4 3.41888E-05
A6 -2.73054E-08
A8 -3.06893E-09
A10 3.86737E-11
A12 -1.69230E-13

28th surface κ 1.00000
A4 -6.20378E-05
A6 -2.88775E-07
A8 3.11023E-09
A10 -4.32584E-11
A12 0.00000E + 00

31st surface κ 1.00000
A4 2.66064E-05
A6 1.04446E-07
A8 -5.78528E-10
A10 0.00000E + 00
A12 0.00000E + 00

[Various data]
Scaling ratio 14.13

W T
f 9.27 to 130.95
FNO 4.12 to 5.81
ω 42.67 to 3.42 °
Y 8.00-8.00
TL 111.02-169.05

W M T
f 9.27006 60.50093 130.95187
ω 42.67385 7.37624 3.41696
FNO 4.12 5.77 5.81
φ 8.83 9.26 10.38
d5 2.10000 37.01608 47.51778
d12 23.62886 5.00952 2.20000
d13 2.40610 3.40014 1.80000
d16 3.89404 2.90000 4.50014
d28 1.50000 16.70292 20.53836
BF 13.93925 26.92305 28.93970

[Focus group movement during focusing]
W M T
Shooting magnification -0.0100 -0.0100 -0.0100
Shooting distance 902.7175 5891.6497 12742.6968
Travel 0.1146 0.1322 0.2361

[Lens group data]
Group start surface f
1 1 70.20776
2 6 -8.28282
3 14 40.62229
4 17 37.83706
5 29 -216.44842

[Conditional expression values]
(1) (−f2) /ft=0.063
(2) f3 / fw = 4.382
(2) (d4t−d4w) /f4=0.503
(4) (d5it-d5iw) / (d3it-d3iw) = 0.433

FIGS. 5 (a), 5 (b), and 5 (c) respectively show infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the second example of the present application. It is an aberration diagram at the time of focusing on an object.
6 (a), 6 (b), and 6 (c) are short distances in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the second example of the present application, respectively. FIG. 6 is a diagram showing various aberrations when the object is in focus (imaging magnification: -0.0100 times).

From the respective aberration diagrams, the variable magnification optical system according to the present embodiment has various aberrations well corrected from the wide-angle end state to the telephoto end state, and from the infinite object focusing state to the short-distance object focusing state, and is high. It can be seen that it has optical performance.

(Third embodiment)
FIGS. 7A, 7B, and 7C are cross-sectional views of the zoom optical system according to the third example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. It is.
The variable magnification optical system according to the present example includes, 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, and a third lens having a positive refractive power. The lens group G3 includes a fourth lens group G4 having a positive refractive power and a fifth lens group G5 having a positive refractive power. An aperture stop S is provided between the second lens group G2 and the third lens group G3.

The first lens group G1 includes, in order from the object side, a cemented lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side. Become.
The second lens group G2 includes, in order from the object side, a negative meniscus lens L21 having a convex surface directed toward the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a biconcave negative lens L24. The cemented lens. The negative meniscus lens L21 is a glass mold aspheric lens having an aspheric lens surface on the object side.

The third lens group G3 is composed of a cemented lens of a negative meniscus lens L31 having a convex surface directed toward the object side and a biconvex positive lens L32 in order from the object side.
In order from the object side, the fourth lens group G4 includes a cemented lens of a positive meniscus lens L41 having a convex surface directed toward the object side and a negative meniscus lens L42 having a convex surface directed toward the object side, a biconvex positive lens L43, and an object. A cemented lens with a negative meniscus lens L44 having a concave surface on the side, a negative meniscus lens L45 having a convex surface on the object side, a positive lens L46 having a biconvex shape, and a negative meniscus lens L47 having a concave surface on the object side It consists of a cemented lens. The negative meniscus lens L45 is a glass mold aspheric lens having an aspheric lens surface on the object side, and the negative meniscus lens L47 is a glass mold aspheric lens having an aspheric lens surface on the image side.

  The fifth lens group G5 includes, in order from the object side, a cemented lens including a positive meniscus lens L51 having a concave surface facing the object side and a negative meniscus lens L52 having a concave surface facing the object side. The negative meniscus lens L52 is a glass mold aspheric lens having an aspheric lens surface on the image side.

With the above-described configuration, in the zoom optical system according to the present embodiment, the air gap between the first lens group G1 and the second lens group G2 and the second lens group at the time of zooming from the wide-angle end state to the telephoto end state. The air gap between G2 and the third lens group G3, the air gap between the third lens group G3 and the fourth lens group G4, the air gap between the fourth lens group G4 and the fifth lens group G5, and the fifth lens group G5 The first lens group G1 to the fifth lens group G5 move along the optical axis so that the air spacing between the lens surface and the image plane I changes.
Specifically, the first lens group G1 to the fourth lens group G4 move to the object side. The fifth lens group G5 moves toward the object side from the wide-angle end state to the intermediate focal length state, and moves toward the image side from the intermediate focal length state to the telephoto end state. The aperture stop S moves to the object side integrally with the fourth lens group G4 during zooming.
Further, focusing from an infinitely distant object to a close object is performed by moving the third lens group G3 to the image plane I side along the optical axis.

Thereby, at the time of zooming, the air gap between the first lens group G1 and the second lens group G2 increases, the air gap between the second lens group G2 and the third lens group G3 decreases, and the fourth lens group G4. And the fifth lens group G5 increase in air space. The air space between the third lens group G3 and the fourth lens group G4 decreases from the wide-angle end state to the intermediate focal length state, and increases from the intermediate focal length state to the telephoto end state. The air space between the fifth lens group G5 and the image plane I increases from the wide-angle end state to the intermediate focal length state and decreases from the intermediate focal length state to the telephoto end state. At the time of zooming, the air gap between the aperture stop S and the third lens group G3 increases from the wide-angle end state to the intermediate focal length state and decreases from the intermediate focal length state to the telephoto end state.
Accordingly, the variable magnification optical system according to the present embodiment has a high variable magnification and is configured in a small size.
Table 3 below lists values of specifications of the variable magnification optical system according to the present example.

(Table 3) Third Example
[Surface data]
Surface number r d nd νd
Object ∞

1 125.4788 1.6350 1.950000 29.37
2 42.8963 8.6176 1.497820 82.57
3 -200.0000 0.1000
4 41.6251 4.9380 1.816000 46.59
5 230.0985 Variable

* 6 500.0000 1.0000 1.851348 40.10
7 9.5652 3.8048
8 -36.8357 1.0000 1.883000 40.66
9 44.2906 0.3520
10 18.6401 4.2703 1.808090 22.74
11 -12.0124 1.0000 1.902650 35.72
12 83.8674 Variable

13 (Aperture S) ∞ Variable

14 23.0558 1.0000 1.883000 40.66
15 12.1495 3.4115 1.593190 67.90
16 -46.4710 Variable

17 13.4790 6.8280 1.816000 46.59
18 22.4551 1.0000 1.850260 32.35
19 10.9985 2.0000
20 19.0986 3.2170 1.516800 63.88
21 -11.7780 1.0000 1.850260 32.35
22 -21.0372 1.5000
* 23 689.8893 1.0000 1.806100 40.73
24 15.3049 2.8460
25 16.4239 5.9978 1.567320 42.58
26 -8.0000 1.0000 1.851348 40.10
* 27 -24.2284 Variable

28 -40.0000 1.6708 1.497820 82.57
29 -19.2635 1.0000 1.834410 37.28
* 30 -24.2511 BF

Image plane ∞

[Aspherical data]
6th surface κ 11.00000
A4 1.38428E-05
A6 2.39881E-07
A8 -9.46864E-09
A10 1.17699E-10
A12 -5.24010E-13

23rd surface κ 1.00000
A4 -1.65484E-05
A6 7.20023E-07
A8 -8.24637E-09
A10 1.55522E-10
A12 0.00000E + 00

27th surface κ 1.00000
A4 -5.27520E-05
A6 1.28445E-07
A8 -5.41725E-09
A10 1.08848E-11
A12 0.00000E + 00

30th surface κ 1.00000
A4 3.58303E-05
A6 -1.13073E-07
A8 6.69333E-10
A10 0.00000E + 00
A12 0.00000E + 00

[Various data]
Scaling ratio 14.13

W T
f 10.30 to 145.50
FNO 4.12 to 5.77
ω 39.66 to 3.01 °
Y 8.00-8.00
TL 107.35-157.35

W M T
f 10.30000 59.49997 145.49942
ω 39.65540 7.34800 3.01140
FNO 4.12 5.76 5.77
φ 8.49 8.51 10.06
d5 2.10000 32.00138 41.35684
d12 22.21167 6.19340 2.20000
d13 3.21330 4.23594 1.80000
d16 4.08103 3.05839 5.49433
d27 1.60536 23.96409 31.36057
BF 13.94931 15.18421 14.94893

[Focus group movement during focusing]
W M T
Shooting magnification -0.0100 -0.0100 -0.0100
Shooting distance 1003.1781 5789.3595 14161.5191
Travel 0.1286 0.1638 0.3103

[Lens group data]
Group start surface f
1 1 62.41033
2 6 -8.66265
3 14 37.00000
4 17 45.93796
5 28 189.05625

[Conditional expression values]
(1) (−f2) /ft=0.0595
(2) f3 / fw = 3.592
(2) (d4t−d4w) /f4=0.648
(4) (d5it-d5iw) / (d3it-d3iw) = 0.031

8 (a), 8 (b), and 8 (c) respectively show infinity in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the third example of the present application. It is an aberration diagram at the time of focusing on an object.
FIGS. 9A, 9B, and 9C are short distances in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the third example of the present application, respectively. FIG. 6 is a diagram showing various aberrations when the object is in focus (imaging magnification: -0.0100 times).

  From the respective aberration diagrams, the variable magnification optical system according to the present embodiment has various aberrations well corrected from the wide-angle end state to the telephoto end state, and from the infinite object focusing state to the short-distance object focusing state, and is high. It can be seen that it has optical performance.

(Fourth embodiment)
FIGS. 10A, 10B, and 10C are cross-sectional views of the zoom optical system according to the fourth example of the present application in the wide-angle end state, the intermediate focal length state, and the telephoto end state, respectively. It is.
The variable magnification optical system according to the present example includes, 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, and a third lens having a positive refractive power. The lens group G3 includes a fourth lens group G4 having a positive refractive power and a fifth lens group G5 having a negative refractive power. An aperture stop S is provided between the second lens group G2 and the third lens group G3.

The first lens group G1 includes, in order from the object side, a cemented lens of a negative meniscus lens L11 having a convex surface facing the object side and a biconvex positive lens L12, and a positive meniscus lens L13 having a convex surface facing the object side. Become.
The second lens group G2 includes, in order from the object side, a negative meniscus lens L21 having a convex surface directed toward the object side, a biconcave negative lens L22, a biconvex positive lens L23, and a biconcave negative lens L24. The cemented lens. The negative meniscus lens L21 is a glass mold aspheric lens having an aspheric lens surface on the object side.

The third lens group G3 is composed of a cemented lens of a negative meniscus lens L31 having a convex surface directed toward the object side and a biconvex positive lens L32 in order from the object side.
In order from the object side, the fourth lens group G4 includes a cemented lens of a positive meniscus lens L41 having a convex surface directed toward the object side and a negative meniscus lens L42 having a convex surface directed toward the object side, a biconvex positive lens L43, and an object. A cemented lens with a negative meniscus lens L44 having a concave surface on the side, a negative meniscus lens L45 having a convex surface on the object side, a positive lens L46 having a biconvex shape, and a negative meniscus lens L47 having a concave surface on the object side It consists of a cemented lens. The negative meniscus lens L45 is a glass mold aspheric lens having an aspheric lens surface on the object side, and the negative meniscus lens L47 is a glass mold aspheric lens having an aspheric lens surface on the image side.

  The fifth lens group G5 includes, in order from the object side, a cemented lens including a positive meniscus lens L51 having a concave surface facing the object side and a negative meniscus lens L52 having a concave surface facing the object side. The negative meniscus lens L52 is a glass mold aspheric lens having an aspheric lens surface on the image side.

With the above-described configuration, in the zoom optical system according to the present embodiment, the air gap between the first lens group G1 and the second lens group G2 and the second lens group at the time of zooming from the wide-angle end state to the telephoto end state. The air gap between G2 and the third lens group G3, the air gap between the third lens group G3 and the fourth lens group G4, the air gap between the fourth lens group G4 and the fifth lens group G5, and the fifth lens group G5 The first lens group G1 to the fifth lens group G5 move along the optical axis so that the air spacing between the lens surface and the image plane I changes.
Specifically, the first lens group G1 to the fifth lens group G5 move to the object side. The aperture stop S moves to the object side integrally with the fourth lens group G4 during zooming.
Further, focusing from an infinitely distant object to a close object is performed by moving the third lens group G3 to the image plane I side along the optical axis.

Thereby, at the time of zooming, the air gap between the first lens group G1 and the second lens group G2 increases, the air gap between the second lens group G2 and the third lens group G3 decreases, and the fourth lens group G4. And the fifth lens group G5 increase, and the air distance between the fifth lens group G5 and the image plane I increases. The air space between the third lens group G3 and the fourth lens group G4 decreases from the wide-angle end state to the intermediate focal length state, and increases from the intermediate focal length state to the telephoto end state. At the time of zooming, the air gap between the aperture stop S and the third lens group G3 increases from the wide-angle end state to the intermediate focal length state and decreases from the intermediate focal length state to the telephoto end state.
Accordingly, the variable magnification optical system according to the present embodiment has a high variable magnification and is configured in a small size.
Table 4 below lists values of specifications of the variable magnification optical system according to the present example.

(Table 4) Fourth Example
[Surface data]
Surface number r d nd νd
Object ∞

1 128.6583 1.6350 1.950000 29.37
2 43.3153 8.5924 1.497820 82.57
3 -200.5952 0.1000
4 41.6932 4.9416 1.816000 46.59
5 226.2028 Variable

* 6 500.0000 1.0000 1.851348 40.10
7 9.4698 3.7102
8 -51.4849 1.0000 1.883000 40.66
9 32.3052 0.4591
10 17.6836 4.3937 1.808090 22.74
11 -11.5727 1.0000 1.902650 35.72
12 68.1728 Variable

13 (Aperture S) ∞ Variable

14 23.9084 1.0000 1.883000 40.66
15 12.0540 3.5286 1.593190 67.90
16 -41.2723 Variable

17 13.3372 7.1262 1.816000 46.59
18 23.6925 1.0000 1.850260 32.35
19 10.6208 2.0000
20 22.6183 3.2312 1.516800 63.88
21 -10.6478 1.0000 1.850260 32.35
22 -17.8847 1.5000
* 23 88.9298 1.0000 1.806100 40.73
24 14.7135 3.2670
25 17.6589 5.9445 1.567320 42.58
26 -8.0000 1.0000 1.851348 40.10
* 27 -23.1716 Variable

28 -86.3077 1.3257 1.497820 82.57
29 -40.4370 1.0000 1.834410 37.28
* 30 -70.0000 BF

Image plane ∞

[Aspherical data]
6th surface κ 11.00000
A4 2.16452E-05
A6 -6.30268E-08
A8 -2.73814E-09
A10 5.05766E-11
A12 -2.61890E-13

23rd surface κ 1.00000
A4 -2.28843E-05
A6 8.75761E-07
A8 -2.20702E-08
A10 4.21746E-10
A12 0.00000E + 00

27th surface κ 1.00000
A4 -8.32547E-05
A6 -6.55824E-08
A8 1.23463E-09
A10 -5.63694E-11
A12 0.00000E + 00

30th surface κ 1.00000
A4 3.80084E-05
A6 -2.56034E-08
A8 4.99788E-11
A10 0.00000E + 00
A12 0.00000E + 00

[Various data]
Scaling ratio 14.13

W T
f 10.30 to 145.50
FNO 4.12 to 5.85
ω 39.50 to 3.03 °
Y 8.00-8.00
TL 107.35-157.35

W M T
f 10.30000 59.49985 145.49848
ω 39.49758 7.41063 3.03486
FNO 4.12 5.76 5.85
φ 8.71 8.62 10.14
d5 2.10000 32.37072 41.89456
d12 22.31334 6.07934 2.20000
d13 3.17825 4.10045 1.80000
d16 3.82220 2.90000 5.20045
d27 1.23135 12.66515 16.54997
BF 13.94909 25.45018 28.94846

[Focus group movement during focusing]
W M T
Shooting magnification -0.0100 -0.0100 -0.0100
Shooting distance 1003.5628 5791.2514 14169.5696
Travel 0.1205 0.1520 0.2832

[Lens group data]
Group start surface f
1 1 63.10081
2 6 -8.44812
3 14 37.00000
4 17 42.46436
5 28 -485.09743

[Conditional expression values]
(1) (−f2) /ft=0.058
(2) f3 / fw = 3.592
(2) (d4t−d4w) /f4=0.361
(4) (d5it-d5iw) / (d3it-d3iw) = 0.473

11 (a), 11 (b), and 11 (c) respectively show infinity in the wide-angle end state, intermediate focal length state, and telephoto end state of the variable magnification optical system according to the fourth example of the present application. It is an aberration diagram at the time of focusing on an object.
12 (a), 12 (b), and 12 (c) are short distances in the wide-angle end state, the intermediate focal length state, and the telephoto end state of the variable magnification optical system according to the fourth example of the present application, respectively. FIG. 6 is a diagram showing various aberrations when the object is in focus (imaging magnification: -0.0100 times).

  From the respective aberration diagrams, the variable magnification optical system according to the present embodiment has various aberrations well corrected from the wide-angle end state to the telephoto end state, and from the infinite object focusing state to the short-distance object focusing state, and is high. It can be seen that it has optical performance.

According to each of the above embodiments, a variable power optical system having a high zoom ratio, a small size, and high optical performance can be realized.
In addition, each said Example has shown one specific example of this invention, and this invention is not limited to these. The following contents can be adopted as appropriate as long as the optical performance of the variable magnification optical system of the present application is not impaired.

  A numerical example of the variable magnification optical system of the present application is shown as having a five-group configuration, but the present application is not limited to this, and constitutes a variable magnification optical system of other group configurations (for example, six groups, seven groups, etc.). You can also. Specifically, a configuration in which a lens or a lens group is added to the most object side or the most image side of the variable magnification optical system of the present application may be used. The lens group refers to a portion having at least one lens separated by an air interval that changes during zooming.

  In addition, the variable magnification optical system of the present application uses a part of a lens group, an entire lens group, or a plurality of lens groups as a focusing lens group for focusing from an object at infinity to a near object. It is good also as a structure moved to an axial direction. In the variable magnification optical system of the present application, an example in which the entire third lens group is the focusing lens group has been shown, but at least a part of the first lens group, at least a part of the second lens group, or at least one of the third lens group. It is also possible to form the focusing lens group by at least a part of the fourth lens group, at least a part of the fifth lens group, or a combination thereof. Such a focusing lens group can also be applied to autofocus, and is also suitable for driving by an autofocus motor, such as an ultrasonic motor.

  Further, in the variable magnification optical system of the present application, any lens group or a part thereof is moved as a vibration-proof lens group so as to include a component in a direction perpendicular to the optical axis, or a surface including the optical axis A configuration in which image blur caused by camera shake or the like is corrected by rotationally moving (swinging) inward is also possible. In particular, in the variable magnification optical system of the present application, at least a part of the second lens group, at least a part of the third lens group, at least a part of the fourth lens group, or at least a part of the fifth lens group is defined as an anti-vibration lens group. It is preferable to do.

  The lens surface of the lens constituting the variable magnification optical system of the present application may be a spherical surface, a flat surface, or an aspheric surface. When the lens surface is a spherical surface or a flat surface, it is preferable because lens processing and assembly adjustment are easy, and deterioration of optical performance due to errors in lens processing and assembly adjustment can be prevented. Further, even when the image plane is deviated, it is preferable because there is little deterioration in drawing performance. When the lens surface is aspherical, any of aspherical surface by grinding, glass mold aspherical surface in which glass is molded into an aspherical shape, or composite aspherical surface in which resin provided on the glass surface is formed in an aspherical shape Good. The lens surface may be a diffractive surface, and the lens may be a gradient index lens (GRIN lens) or a plastic lens.

In the variable magnification optical system of the present application, the aperture stop is disposed in the vicinity of the third lens group. However, a lens frame may be used as a substitute for the aperture stop without providing a member.
Further, an antireflection film having a high transmittance in a wide wavelength range may be applied to the lens surface of the lens constituting the variable magnification optical system of the present application. Thereby, flare and ghost can be reduced, and high optical performance with high contrast can be achieved.

Next, a camera equipped with the variable magnification optical system of the present application will be described with reference to FIG.
FIG. 13 is a diagram illustrating a configuration of a camera including the variable magnification optical system of the present application.
As shown in FIG. 13, the camera 1 is a so-called mirrorless camera of an interchangeable lens type that includes the variable magnification optical system according to the first example as the photographing lens 2.
In the camera 1, light from an object (subject) (not shown) is collected by the photographing lens 2 and is on the imaging surface of the imaging unit 3 via an OLPF (Optical low pass filter) (not shown). A subject image is formed on the screen. Then, the subject image is photoelectrically converted by the photoelectric conversion element provided in the imaging unit 3 to generate an image of the subject. This image is displayed on an EVF (Electronic view finder) 4 provided in the camera 1. Thus, the photographer can observe the subject via the EVF 4.
When the release button (not shown) is pressed by the photographer, the subject image generated by the imaging unit 3 is stored in a memory (not shown). In this way, the photographer can shoot the subject with the camera 1.

  Here, the zoom optical system according to the first embodiment mounted as the photographing lens 2 on the camera 1 is a zoom optical system having a high zoom ratio, a small size, and high optical performance. Therefore, the present camera 1 can achieve downsizing and high optical performance while having a high zoom ratio. Even if a camera equipped with the variable magnification optical system according to the second to fourth examples as the photographing lens 2 is configured, the same effect as the camera 1 can be obtained. Further, even when the variable magnification optical system according to each of the above embodiments is mounted on a single-lens reflex camera that has a quick return mirror and observes a subject with a finder optical system, the same effect as the camera 1 can be obtained. it can.

Finally, the outline of the manufacturing method of the variable magnification optical system of this application is demonstrated based on FIG.
The variable power optical system manufacturing method shown in FIG. 14 has, in order from the object side, a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a positive refractive power. A method for manufacturing a variable magnification optical system having a third lens group, a fourth lens group having a positive refractive power, and a fifth lens group, and includes the following steps S1, S2, and S3.

Step S1: The second lens group is made to satisfy the following conditional expression (1), and each lens group is sequentially arranged in the lens barrel from the object side.
(1) 0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

Step S2: By providing a known moving mechanism in the lens barrel, the magnification between the wide-angle end state and the telephoto end state, the distance between the first lens group and the second lens group, the second lens group, The distance between the third lens group, the distance between the third lens group and the fourth lens group, and the distance between the fourth lens group and the fifth lens group are changed, and the fifth lens group is placed on the image plane. To move against.
Step S3: A known moving mechanism is provided on the lens barrel so that the third lens group moves along the optical axis when focusing from an object at infinity to an object at a short distance.

  According to such a method for manufacturing a variable magnification optical system of the present application, a variable magnification optical system having a high zoom ratio, a small size, and high optical performance can be manufactured.

G1 1st lens group G2 2nd lens group G3 3rd lens group G4 4th lens group G5 5th lens group S Aperture stop I Image surface

Claims (12)

In order from the object side along the optical axis, 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 fourth lens group having a positive refractive power; A fifth lens group,
At the time of zooming from the wide-angle end state to the telephoto end state, the distance between the first lens group and the second lens group, the distance between the second lens group and the third lens group, and the third lens group And the distance between the fourth lens group and the distance between the fourth lens group and the fifth lens group change, the fifth lens group moves relative to the image plane,
When focusing from an object at infinity to a near object, the third lens group moves along the optical axis;
A zoom optical system characterized by satisfying the following conditional expression:
0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group   2. The zoom optical system according to claim 1, wherein the first lens unit moves toward the object side during zooming from the wide-angle end state to the telephoto end state. The variable magnification optical system according to claim 1, wherein the following conditional expression is satisfied.
2.970 <f3 / fw <10.000
However,
fw: focal length of the entire zoom optical system in the wide-angle end state f3: focal length of the third lens group The zoom lens system according to any one of claims 1 to 3, wherein the following conditional expression is satisfied.
0.010 <(d4t-d4w) / f4 <1.00
However,
d4t: Distance on the optical axis from the most image-side lens surface of the fourth lens group in the telephoto end state to the most object-side lens surface of the fifth lens group d4w: The fourth lens group in the wide-angle end state Distance on the optical axis from the lens surface closest to the image side to the lens surface closest to the object side of the fifth lens group f4: Focal length of the fourth lens group The zoom lens system according to any one of claims 1 to 4, wherein the following conditional expression is satisfied.
0.010 <(d5it-d5iw) / (d3it-d3iw) <1.00
However,
d3it: Distance on the optical axis from the lens surface closest to the image side of the third lens group in the telephoto end state to the image plane d3iw: From the lens surface closest to the image side of the third lens group in the wide-angle end state to the image plane D5it: Distance on the optical axis from the lens surface closest to the image side of the fifth lens group in the telephoto end state to the image plane d5iw: Distance on the most image side of the fifth lens group in the wide-angle end state Distance on the optical axis from the lens surface to the image plane The zoom optical system has an aperture stop,
6. The variable power optical system according to claim 1, wherein a distance between the aperture stop and the fourth lens group is unchanged when zooming from a wide-angle end state to a telephoto end state. system.   The zoom optical system according to any one of claims 1 to 6, wherein the third lens group moves toward the image side when focusing from an object at infinity to an object at a short distance.   8. The zooming according to claim 1, wherein the distance between the first lens unit and the second lens unit increases when zooming from the wide-angle end state to the telephoto end state. Optical system.   9. The zooming according to claim 1, wherein a distance between the second lens unit and the third lens unit decreases when zooming from the wide-angle end state to the telephoto end state. Optical system.   The variable power optical system according to any one of claims 1 to 9, wherein the fifth lens group has a positive refractive power.   An optical apparatus comprising the variable magnification optical system according to claim 1. In order from the object side along the optical axis, 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 fourth lens group having a positive refractive power; A variable magnification optical system manufacturing method having a fifth lens group,
The second lens group satisfies the following conditional expression:
At the time of zooming from the wide-angle end state to the telephoto end state, the distance between the first lens group and the second lens group, the distance between the second lens group and the third lens group, and the third lens group And the distance between the fourth lens group and the distance between the fourth lens group and the fifth lens group are changed, and the fifth lens group is moved relative to the image plane,
A method of manufacturing a variable magnification optical system, wherein the third lens group is moved along the optical axis when focusing from an object at infinity to an object at a short distance.
0.030 <(− f2) / ft <0.120
However,
ft: focal length of the entire zoom optical system in the telephoto end state f2: focal length of the second lens group

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