The present application claims priority under 35 U.S.C. §119 to Japanese Patent Application No. 2014-034896, filed on Feb. 26, 2014. The above application is hereby expressly incorporated by reference, in its entirety, into the present application.
1. Field of the Invention
The present invention relates to a zoom lens used in an electronic camera, such as a digital camera, a video camera, a camera for broadcasting, and a camera for surveillance, and also to an imaging apparatus including the zoom lens.
2. Description of the Related Art
Japanese Unexamined Patent Publication No. 2011-081063 (Patent Document 1), Japanese Unexamined Patent Publication No. 2012-242766 (Patent Document 2) and International Patent Publication No. WO2013/031205 (Patent Document 3) are known about zoom lenses used in electronic cameras, such as a digital camera, a video camera, a camera for broadcasting, and a camera for surveillance. Especially, a zoom lens in Example 5 of Patent Document 1, a zoom lens in Example 4 of Patent Document 2, and a zoom lens in Patent Document 3 consist of five groups, and have high performance.
In the zoom lenses of Patent Documents 1 and 2, a zoom lens having an ordinary angle of view and a high magnification ratio and a zoom lens having a wide angle of view and a low magnification ratio are included in examples. However, the zoom lenses are not regarded as small-sized light-weight zoom lenses, because the outer diameter of a first lens group is large or the total length is long. Further, the zoom lens of Patent Document 3 has a high magnification ratio, and the size of the zoom lens is sufficiently reduced. However, the zoom lens of Patent Document 3 does not have a wide angle of view.
In view of the foregoing circumstances, it is an object of the present invention to provide a high-performance zoom lens having a wide angle of view and a high magnification ratio while the size of the zoom lens is small and the weight of the zoom lens is light, and an imaging lens including the zoom lens.
A zoom lens of the present invention essentially consists of a first lens group having positive refractive power, a second lens group having negative refractive power, a third lens group having negative refractive power, a fourth lens group having negative refractive power, and a fifth lens group having positive refractive power in this order from an object side. The first lens group and the fifth lens group are fixed with respect to an image plane, and the second lens group, the third lens group and the fourth lens group move in such a manner that a distance from each other changes when magnification is changed from a wide angle end to a telephoto end. The first lens group essentially consists of an 11th lens group having negative refractive power, a 12th lens group having positive refractive power, and a 13th lens group having positive refractive power in this order from the object side. The 11th lens group and the 13th lens group are fixed with respect to the image plane and the 12th lens group moves during focusing. Further, the following conditional expression (1) is satisfied:
2.10<f12/f13<4.10 (1), where
f12: a focal length of the 12th lens group, and
f13: a focal length of the 13th lens group.
In the zoom lens of the present invention, it is desirable that the following conditional expression (2) is satisfied:
1.00<f13/f1<1.50 (2), where
f13: a focal length of the 13th lens group, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (3) is satisfied:
0.90<Z2/f1<1.40 (3), where
Z2: a movement amount of the second lens group from a wide angle end to a telephoto end, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (4) is satisfied:
−1.30<f11/f13<−0.68 (4), where
f11: a focal length of the 11th lens group, and
f13: a focal length of the 13th lens group.
Further, it is desirable that the following conditional expression (5) is satisfied:
−1.23<f11/f1<−0.80 (5), where
f11: a focal length of the 11th lens group, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (6) is satisfied:
5.10<f1/Yimg<10.00 (6), where
f1: a focal length of the first lens group, and
Yimg: a maximum image height.
Further, it is desirable that the following conditional expression (1-1) is satisfied:
2.20<f12/f13<3.80 (1-1).
Further, it is desirable that the following conditional expression (2-1) is satisfied. It is more desirable that the following conditional expression (2-2) is satisfied:
1.20<f13/f1<1.50 (2-1); and
1.20<f13/f1<1.30 (2-2).
Further, it is desirable that the following conditional expression (3-1) is satisfied:
1.10<Z2/f1<1.20 (3-1).
Further, it is desirable that the following conditional expression (4-1) is satisfied:
−1.00<f11/f13<−0.70 (4-1).
Further, it is desirable that the following conditional expression (5-1) is satisfied:
−1.22<f11/f1<−0.90 (5-1).
Further, it is desirable that the following conditional expression (6-1) is satisfied. It is more desirable that the following conditional expression (6-2) is satisfied:
6.10<f1/Yimg<10.00 (6-1); and
6.40<f1/Yimg<7.50 (6-2).
An imaging apparatus of the present invention includes the aforementioned zoom lens of the present invention.
The expression “essentially consists of” means that a lens or lenses essentially without refractive power, an optical element, such as a stop, a mask, a cover glass and a filter, other than lenses, a mechanism part, such as a lens flange, a lens barrel, an imaging device and a hand shake blur correction mechanism, and the like may be included besides the mentioned composition elements.
Further, the surface shape and the sign of the refractive power of the aforementioned lenses are considered in a paraxial region when an aspherical surface is included.
The zoom lens of the present invention essentially consists of a first lens group having positive refractive power, a second lens group having negative refractive power, a third lens group having negative refractive power, a fourth lens group having negative refractive power, and a fifth lens group having positive refractive power in this order from an object side. Further, the first lens group and the fifth lens group are fixed with respect to an image plane, and the second lens group, the third lens group and the fourth lens group move in such a manner that a distance from each other changes when magnification is changed from a wide angle end to a telephoto end. Further, the first lens group essentially consists of an 11th lens group having negative refractive power, a 12th lens group having positive refractive power, and a 13th lens group having positive refractive power in this order from the object side. Further, the 11th lens group and the 13th lens group are fixed with respect to the image plane and the 12th lens group moves during focusing, and the following conditional expression (1) is satisfied. Therefore, it is possible to provide a high-performance zoom lens having a wide angle of view and a high magnification ratio while the size of the zoom lens is small and the weight of the zoom lens is light:
2.10<f12/f13<4.10 (1).
Further, the imaging apparatus of the present invention includes the zoom lens of the present invention. Therefore, the imaging apparatus can obtain high image-quality images with wide angles of view and high magnification ratios.
Next, embodiments of the present invention will be described in detail with reference to drawings.
As illustrated in
When this zoom lens is applied to an imaging apparatus, it is desirable to arrange a cover glass, a prism, and various filters, such as an infrared-ray-cut filter and a low-pass filter, between an optical system and image plane Sim based on the configuration of the apparatus part, on which the lens is mounted. Therefore,
This zoom lens is configured in such a manner that first lens group G1 and fifth lens group G5 are fixed with respect to an image plane, and second lens group G2, third lens group G3 and fourth lens group G4 move in such a manner that a distance from each other changes when magnification is changed from a wide angle end to a telephoto end.
Further, first lens group G1 consists of 11th lens group G11 having negative refractive power, 12th lens group G12 having positive refractive power, and 13th lens group G13 having positive refractive power in this order from the object side. Further, first lens group G1 is configured in such a manner that 11th lens group G11 and 13th lens group G13 are fixed with respect to an image plane and 12th lens group G12 moves during focusing.
When the whole zoom lens is configured as described above, it is possible to achieve high optical performance while the size of the zoom lens is small and the weight of the zoom lens is light. Further, when first lens group G1 is configured as described above, it is possible to reduce a fluctuation of an angle of view and fluctuations of aberrations during focusing.
Further, this zoom lens is configured to satisfy the following conditional expression (1). When the value does not exceed the upper limit of this conditional expression (1), it is possible to suppress the height of an axial marginal ray entering 13th lens group G13 at a telephoto end. Therefore, it is possible to reduce the size and the weight of 13th lens group G13 by suppressing the outer diameter of 13th lens group G13. Further, it is possible to secure excellent F-number Fno at the telephoto end. Further, when the value is not lower than the lower limit of conditional expression (1), it is possible to excellently correct a spherical aberration and curvature of field at the telephoto end while the configuration is advantageous to increasing an angle of view. Further, when the following conditional expression (1-1) is satisfied, more excellent characteristics are obtainable.
2.10<f12/f13<4.10 (1); and
2.20<f12/f13<3.80 (1-1), where
f12: a focal length of the 12th lens group, and
f13: a focal length of the 13th lens group.
In the zoom lens according to the embodiment of the present invention, it is desirable that the following conditional expression (2) is satisfied. When the value does not exceed the upper limit of this conditional expression (2), it is possible to suppress an increase in a distance between first lens group G1 and second lens group G2 at the telephoto end. Therefore, the configuration is advantageous to reducing the size and the weight of the zoom lens. Further, when the value is not lower than the lower limit of conditional expression (2), it is possible to prevent the refractive power of 13th lens group G13 from becoming too strong. Therefore, it is possible to excellently correct a spherical aberration and curvature of field at the telephoto end. When the following conditional expression (2-1) is satisfied, and more desirably, when conditional expression (2-2) is satisfied, more excellent characteristics are obtainable.
1.00<f13/f1<1.50 (2);
1.20<f13/f1<1.50 (2-1); and
1.20<f13/f1<1.30 (2-2), where
f13: a focal length of the 13th lens group, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (3) is satisfied. When the value does not exceed the upper limit of this conditional expression (3), it is possible to suppress a movement amount of second lens group G2. Therefore, the configuration is advantageous to reducing the size and the weight. Further, when the value is not lower than the lower limit of conditional expression (3), it is possible to prevent the refractive power of second lens group G2 from becoming too strong. Therefore, it is possible to reduce a fluctuation of aberrations during magnification change. Here, when the following conditional expression (3-1) is satisfied, more excellent characteristics are obtainable.
0.90<Z2/f1<1.40 (3); and
1.10<Z2/f1<1.20 (3-1), where
Z2: a movement amount of the second lens group from a wide angle end to a telephoto end, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (4) is satisfied. When the value does not exceed the upper limit of this conditional expression (4), it is possible to suppress the height of rays output from 11th lens group G11. As a result, it is possible to reduce the outer diameters of 12th lens group G12 and 13th lens group G13. Therefore, the configuration is advantageous to reducing the size and the weight. Further, when the value is not lower than the lower limit of conditional expression (4), it is possible to prevent the refractive power of 13th lens group G13 from becoming too strong. Therefore, it is possible to excellently correct a spherical aberration and curvature of field at the telephoto end. When the following conditional expression (4-1) is satisfied, more excellent characteristics are obtainable.
−1.30<f11/f13<−0.68 (4); and
−1.00<f11/f13<−0.70 (4-1), where
f11: a focal length of the 11th lens group, and
f13: a focal length of the 13th lens group.
Further, it is desirable that the following conditional expression (5) is satisfied. When the value does not exceed the upper limit of this conditional expression (5), it is possible to suppress the height of rays output from 11th lens group G11. As a result, it is possible to reduce the outer diameters of 12th lens group G12 and 13th lens group G13. Therefore, the configuration is advantageous to reducing the size and the weight. Further, when the value is not lower than the lower limit of conditional expression (5), it is possible to prevent the refractive power of 11th lens group G11 from becoming too weak. Therefore, it is possible to excellently correct a spherical aberration and curvature of field at the telephoto end. When the following conditional expression (5-1) is satisfied, more excellent characteristics are obtainable.
−1.23<f11/f1<−0.80 (5); and
−1.22<f11/f1<−0.90 (5-1), where
f11: a focal length of the 11th lens group, and
f1: a focal length of the first lens group.
Further, it is desirable that the following conditional expression (6) is satisfied. When the value does not exceed the upper limit of this conditional expression (6), it is possible to suppress the height of rays output from first lens group G1. As a result, it is possible to suppress an increase in a distance between first lens group G1 and second lens group G2 at the telephoto end. Therefore, the configuration is advantageous to reducing the size and the weight of the zoom lens. Further, when the value is not lower than the lower limit of conditional expression (6), it is possible to excellently correct a spherical aberration, astigmatism and curvature of field at the telephoto end. Here, when the following conditional expression (6-1) is satisfied, and more desirably, when the following conditional expression (6-2) is satisfied, more excellent characteristics are obtainable.
5.10<f1/Yimg<10.00 (6);
6.10<f1/Yimg<10.00 (6-1); and
6.40<f1/Yimg<7.50 (6-2), where
f1: a focal length of the first lens group, and
Yimg: a maximum image height.
Specifically, in the zoom lens according to the embodiment of the present invention, it is desirable to use glass, as a material arranged closest to the object side. Alternatively, transparent ceramic may be used.
When the zoom lens according to the embodiment of the present invention is used in tough conditions, it is desirable that a multi-layer coating for protection is applied to the zoom lens. Further, an anti-reflection coating for reducing ghost light during use or the like may be applied to the zoom lens in addition to the coating for protection.
Next, numerical value examples of the zoom lens of the present invention will be described.
First, the zoom lens in Example 1 will be described.
Table 1 shows basic lens data of the zoom lens in Example 1. Table 2 shows data about the specification of the zoom lens in Example 1. Table 3 shows data about moving surface distances. Table 4 shows data about aspheric coefficients. In the following descriptions, the meanings of signs in the tables will be described by using the tables of Example 1, as an example. The meanings of signs in the tables of Examples 2 through 6 are basically similar to those of Example 1.
In the lens data of Table 1, a column of surface numbers shows surface numbers when a surface of composition elements closest to the object side is the first surface and the surface numbers sequentially increase toward the image side. A column of curvature radii shows the curvature radius of each surface. A column of surface distances shows a distance, on optical axis Z, between each surface and its next surface. Further, a column of nd shows the refractive index of each optical element for d-line (wavelength is 587.6 nm). A column of vd shows the Abbe number of each optical element for d-line (wavelength is 587.6 nm). Further, a column of θgf shows a partial dispersion ratio of each optical element.
Here, partial dispersion ratio θgf is represented by the following equation:
θgf=(Ng−NF)/(NF−NC), where
Ng: a refractive index for g-line,
NF: a refractive index for F-line, and
NC: a refractive index for C-line.
Here, the sign of a curvature radius is positive when a surface shape is convex toward the object side, and negative when a surface shape is convex toward the image side. The basic lens data show data including aperture stop St and optical members PP1 through PP3. In the column of surface numbers, the term “(STOP)” is written together with the surface number of a surface corresponding to aperture stop St. Further, in the lens data of Table 1, “DD[i]” is written in a row of a surface distance that changes during magnification change. Numerical values corresponding to this DD[i] are shown in Table 3.
Data about specification in Table 2 show values of zoom ratios, focal length f, back focus Bf, F-number Fno, maximum image heights and full angle of view 2ω.
In the basic lens data, data about specification and data about moving surface distances, degree is used as the unit of an angle, and mm is used as the unit of a length. Since an optical system is usable by proportionally enlarging the optical system or by proportionally reducing the optical system, other appropriate units may be used.
In the lens data of Table 1, mark “*” is attached to the surface numbers of aspherical surfaces. Further, a numerical value of a paraxial curvature radius is used as the curvature radius of an aspherical surface. The data about aspheric coefficients in Table 4 show the surface numbers of aspherical surfaces and aspheric coefficients about the aspherical surfaces. The aspheric coefficients are values of coefficients KA, Am (m=3 . . . 20) in an aspheric equation represented by the following equation:
Zd=C·h
2/{1+(1−KA·C2·h2)1/2}+ΣAm·hu m, where
Zd: the depth of an aspherical surface (the length of a perpendicular from a point on the aspherical surface at height h to a flat plane that contacts with the vertex of the aspherical surface and is perpendicular to the optical axis),
h: height (a length from the optical axis),
C: a reciprocal of a paraxial curvature radius, and
KA, Am: aspheric coefficients (m=3 . . . 20).
Next, a zoom lens in Example 2 will be described.
Next, a zoom lens in Example 3 will be described.
Next, a zoom lens in Example 4 will be described.
Next, a zoom lens in Example 5 will be described.
Next, a zoom lens in Example 6 will be described.
Table 25 shows values corresponding to conditional expressions (1) through (6) in Examples 1 through 6. In all of the examples, d-line is a reference wavelength, and the following Table 25 shows values at the reference wavelength.
As these data show, all of the zoom lenses in Example 1 through 6 satisfy conditional expressions (1) through (6). The zoom lenses are high-performance zoom lenses having wide angles of view and high magnification ratios while the size of the zoom lenses is small and the weight of the zoom lenses is light.
Next, an imaging apparatus according to an embodiment of the present invention will be described.
An imaging apparatus 10 illustrated in
An image imaged by the zoom lens 1 is formed on the imaging surface of the imaging device 7, and signals about the image are output from the imaging device 7. Operation processing is performed on the output signals at a signal processing circuit 8, and an image is displayed on a display device 9.
So far, the present invention has been described by using embodiments and examples. However, the present invention is not limited to the aforementioned embodiments nor examples, and various modifications are possible. For example, the values of the curvature radius, a distance between surfaces, a refractive index, an Abbe number and the like of lens elements are not limited to the values in the aforementioned numerical value examples, and may be other values.
Number | Date | Country | Kind |
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2014-034896 | Feb 2014 | JP | national |