VARIABLE MAGNIFICATION OPTICAL SYSTEM, OPTICAL APPARATUS, IMAGING APPARATUS AND METHOD FOR MANUFACTURING VARIABLE MAGNIFICATION OPTICAL SYSTEM

Information

  • Patent Application
  • 20200310087
  • Publication Number
    20200310087
  • Date Filed
    June 12, 2020
    3 years ago
  • Date Published
    October 01, 2020
    3 years ago
Abstract
A variable magnification optical system includes a positive first lens group disposed at a most object side, a negative intermediate group disposed at an image side of the first lens group, a positive focusing group disposed at an image side of the intermediate group, and a positive image side group disposed at an image side of the focusing group. Upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group are varied; and the image side group includes, in order from an object side, a positive A group, a negative B group satisfying a predetermined conditional expression with respect to the A group, and a C group, whereby excellent optical performance, high speed focusing, and other advantages are achieved.
Description
TECHNICAL FIELD

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


BACKGROUND ART

There has been proposed a variable magnification optical system that is suitable to be used for a photographic camera, an electronic still camera, a video camera and the like. For example, please refer to a Japanese Patent application Laid-Open Gazette No. H4-293007. However, a variable magnification optical system as disclosed in the Japanese Patent application Laid-Open Gazette No. H4-293007 is not intended to reduce a focusing group in weight sufficiently and is not suitable for attain high speed focusing operation.


PRIOR ART REFERENCE
Patent Document

Patent Document 1: Japanese Patent application Laid-Open Gazette No. H4-293007.


SUMMARY OF THE INVENTION

According to a first aspect of the present invention, there is provided a variable magnification optical system comprising a first lens group disposed at a most object side and having positive refractive power,


an intermediate group disposed at an image side of the first lens group and having negative refractive power,


a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and


an image side group disposed at an image side of the focusing group and having positive refractive power;


upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group being varied; and


the image side group comprising, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group:





1.67<fA/(−fB)<2.80


where fA denotes a focal length of the A group,


and fB denotes a focal length of the B group.


Further, according to a second aspect of the present invention, there is provided a method for manufacturing a variable magnification optical system comprising steps of


arranging a first lens group disposed at a most object side and having positive refractive power, an intermediate group disposed at an image side of the first lens group and having negative refractive power, a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and an image side group disposed at an image side of the focusing group and having positive refractive power such that, upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group are varied; and


arranging such that the image side group is composed of, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group:





1.67<fA/(−fB)<2.80


where fA denotes a focal length of the A group,


and fB denotes a focal length of the B group.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is a sectional view of a variable magnification optical system according to a First Example.



FIGS. 2A, 2B and 2C are graphs showing various aberrations of the variable magnification optical system according to the First Example.



FIGS. 3A and 3B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the First Example.



FIGS. 4A, 4B and 4C are graphs showing various aberrations of the variable magnification optical system according to the First Example.



FIG. 5 is a sectional view of a variable magnification optical system according to a Second Example.



FIGS. 6A, 6B and 6C are graphs showing various aberrations of the variable magnification optical system according to the Second Example.



FIGS. 7A and 7B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Second Example.



FIGS. 8A, 8B and 8C are graphs showing various aberrations of the variable magnification optical system according to the Second Example.



FIG. 9 is a sectional view of a variable magnification optical system according to a Third Example.



FIGS. 10A, 10B and 10C are graphs showing various aberrations of the variable magnification optical system according to the Third Example.



FIGS. 11A and 11B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Third Example.



FIGS. 12A, 12B and 12C are graphs showing various aberrations of the variable magnification optical system according to the Third Example.



FIG. 13 is a sectional view of a variable magnification optical system according to a Fourth Example.



FIGS. 14A, 14B and 14C are graphs showing various aberrations of the variable magnification optical system according to the Fourth Example.



FIGS. 15A and 15B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Fourth Example.



FIGS. 16A, 16B and 16C are graphs showing various aberrations of the variable magnification optical system according to the Fourth Example.



FIG. 17 is a sectional view of a variable magnification optical system according to a Fifth Example.



FIGS. 18A, 18B and 18C are graphs showing various aberrations of the variable magnification optical system according to the Fifth Example.



FIGS. 19A and 19B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Fifth Example.



FIGS. 20A, 20B and 20C are graphs showing various aberrations of the variable magnification optical system according to the Fifth Example.



FIG. 21 is a sectional view of a variable magnification optical system according to a Sixth Example.



FIGS. 22A, 22B and 22C are graphs showing various aberrations of the variable magnification optical system according to the Sixth Example.



FIGS. 23A and 23B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Sixth Example.



FIGS. 24A, 24B and 24C are graphs showing various aberrations of the variable magnification optical system according to the Sixth Example.



FIG. 25 is a sectional view of a variable magnification optical system according to a Seventh Example.



FIGS. 26A, 26B and 26C are graphs showing various aberrations of the variable magnification optical system according to the Seventh Example.



FIGS. 27A and 27B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Seventh Example.



FIGS. 28A, 28B and 28C are graphs showing various aberrations of the variable magnification optical system according to the Seventh Example.



FIG. 29 is a sectional view of a variable magnification optical system according to an Eighth Example.



FIGS. 30A, 30B and 30C are graphs showing various aberrations of the variable magnification optical system according to the Eighth Example.



FIGS. 31A and 31B are graphs showing meridional transverse aberrations of the variable magnification optical system according to the Eighth Example.



FIGS. 32A, 32B and 32C are graphs showing various aberrations of the variable magnification optical system according to the Eighth Example.



FIG. 33 shows a configuration of a camera equipped with the variable magnification optical system.



FIG. 34 is a flowchart schematically explaining a method for manufacturing the variable magnification optical system.





EMBODIMENT FOR CARRYING OUT THE INVENTION

Next, a variable magnification optical system according to the embodiment of the present invention, an optical apparatus, an imaging apparatus and a method for manufacturing the variable magnification optical system, will be explained.


The variable magnification optical system according to the present embodiment comprises a first lens group disposed at a most object side and having positive refractive power, an intermediate group disposed at an image side of the first lens group and having negative refractive power, a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and an image side group disposed at an image side of the focusing group and having positive refractive power; upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group being varied; and the image side group being composed of, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression (1) with respect to the A group and having negative refractive power, and a C group:





1.67<fA/(−fB)<2.80   (1)


where fA denotes a focal length of the A group, and


fB denotes a focal length of the B group.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the focusing group is composed of one or two lens components.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the B group is disposed to be movable to have a displacement component in a direction perpendicular to the optical axis.


The focusing group of the present embodiment comprises at least one lens group. Further, the image side group of the present embodiment comprises at least one lens group. Furthermore, each of the A group, the B group and the C group of the present embodiment comprises at least one lens. Meanwhile, the term “lens group” in the present embodiment is a portion comprising at least one lens separated by an air space which varies upon varying magnification. Further, distance(s) between lenses included in lens groups in the present embodiment, is(are) not varied upon varying magnification, but is(are) changeable properly.


As described above, the variable magnification optical system according to the present embodiment comprises at least four lens groups and varies distances between lens groups upon varying magnification. With this configuration, it is possible to correct superbly various aberrations upon varying magnification.


Further, in the variable magnification optical system according to the present embodiment, as described above, the focusing group is composed of one or two lens components. With such configuration, the focusing group can be downsized and reduced in weight. Meanwhile, the term “lens component” in the present embodiment means a single lens or a cemented lens. Further, in the variable magnification optical system according to the present embodiment, the focusing group means a portion comprising at least one lens separated by an air space that changes upon focusing.


Furthermore, in the variable magnification optical system according to the present embodiment, as described above, the image side group is composed of, in order from the object side, the A group having positive refractive power, the B group having negative refractive power, and the C group, the B group being moved, as a vibration reduction group, to have a displacement component in a direction perpendicular to the optical axis. With such configuration, it is possible to correct displacement of imaging position caused by a camera shake or the like, in other words, vibration reduction can be carried out. Moreover, the vibration reduction group can be downsized, and in addition thereto deterioration in optical performance upon carrying out vibration reduction can be effectively suppressed. Meanwhile, the vibration reduction group in the present embodiment means a portion that is moved to have a component in a direction perpendicular to the optical axis upon carrying out vibration reduction.


The above conditional expression (1) defines a ratio of the focal length of the A group to the focal length of the B group that is the vibration reduction group. With satisfying the conditional expression (1), the variable magnification optical system according to the present embodiment can suppress effectively deterioration in optical performance upon carrying out vibration reduction.


When the value of fA/(−fB) is equal to or exceeds the upper limit value of the conditional expression (1) of the variable magnification optical system according to the present embodiment, refractive power of the vibration reduction group becomes large, and deterioration in eccentric coma aberration upon carrying out vibration reduction becomes large. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (1) to 2.70. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (1) to 2.60.


On the other hand, when the value of fA/(−fB) is equal to or falls below the lower limit value of the conditional expression (1) of the variable magnification optical system according to the present embodiment, refractive power of the A group becomes large, and it becomes difficult to correct spherical aberration and other various aberrations. Further, refractive power of the vibration reduction group becomes small, and an amount of movement of the vibration reduction group upon carrying out vibration reduction becomes large. For this reason, a lens barrel that receives the variable magnification optical system according to the present embodiment becomes large in size, so this is not preferable. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (1) to 1.68. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (1) to 1.69.


With configurations as described above, it is possible to realize a variable magnification optical system having excellent optical performance and a focusing lens group reduced in weight in order to attain high speed focusing operation.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that a distance between the A group and the B group is larger than a distance between the B group and the C group.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the following conditional expression (1A) is satisfied:





2.50<f1/(−fc)<6.20   (1A)


where f1 denotes a focal length of the first lens group, and fc denotes a focal length of the intermediate group.


The conditional expression (1A) defines a ratio of the focal length of the first lens group to the focal length of the intermediate group. With satisfying the conditional expression (1A), the variable magnification optical system according to the present embodiment can suppress variations in spherical aberration and other various aberrations upon varying magnification from a wide angle end state to a telephoto end state.


When the value of f1/(−fc) is equal to or exceeds the upper limit value of the conditional expression (1A) of the variable magnification optical system according to the present embodiment, refractive power of the intermediate group becomes large, and it becomes difficult to correct spherical aberration and other various aberrations. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (1A) to 5.90. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (1A) to 5.60.


On the other hand, when the value of f1/(−fc) is equal to or falls below the lower limit value of the conditional expression (1A) of the variable magnification optical system according to the present embodiment, refractive power of the first lens group becomes large, and it becomes difficult to correct spherical aberration and other various aberrations. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (1A) to 2.80. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (1A) to 3.70.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the following conditional expression (1B) is satisfied:





3.00<f1fw/ff<9.00   (1B)


where f1fw denotes a composite focal length from the first lens group to the focusing group in the wide angle end state, and ff denotes a focal length of the focusing group.


The conditional expression (1B) defines a ratio of the composite focal length from the first lens group to the focusing group in the wide angle end state to the focal length of the focusing group. With satisfying the conditional expression (1B), the variable magnification optical system according to the present embodiment can suppress variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object in the wide angle end state.


When the value of f1fw/ff is equal to or exceeds the upper limit value of the conditional expression (1B) of the variable magnification optical system according to the present embodiment, refractive power of the focusing group becomes large, and it becomes difficult to suppress variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object in the wide angle end state. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (1B) to 8.50. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (1B) to 8.00.


On the other hand, when the value of f1fw/ff is equal to or falls below the lower limit value of the conditional expression (1B) of the variable magnification optical system according to the present embodiment, refractive power from the first lens group to the focusing group in the wide angle end state becomes large, and it becomes difficult to suppress variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object in the wide angle end state. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (1B) to 3.30. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (1B) to 3.60.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the following conditional expression (2) is satisfied:





1.50<f1/ff<2.35   (2)


where f1 denotes a focal length of the first lens group, and ff denotes a focal length of the focusing group.


The conditional expression (2) defines a ratio of the focal length of the first lens group to the focal length of the focusing group. With satisfying the conditional expression (2), the variable magnification optical system according to the present embodiment can suppress variations in spherical aberration and other various aberrations upon carrying out focusing from an infinitely distant object to a close distance object.


When the value of f1/ff is equal to or exceeds the upper limit value of the conditional expression (2) of the variable magnification optical system according to the present embodiment, refractive power of the focusing group becomes large, and it becomes difficult to suppress variations in spherical aberration and other various aberrations upon carrying out focusing from an infinitely distant object to a close distance object. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (2) to 2.30. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (2) to 2.25.


On the other hand, when the value of f1/ff is equal to or falls below the lower limit value of the conditional expression (2) of the variable magnification optical system according to the present embodiment, refractive power of the first lens group becomes large, and it becomes difficult to correct spherical aberration and other various aberrations. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (2) to 1.60. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (2) to 1.70.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the first lens group is moved toward the object side upon varying magnification from the wide angle end state to the telephoto end state. With such a configuration, the whole length of the variable magnification optical system according to the present embodiment can be reduced in the wide angle end state, thereby it becoming possible to downsize the variable magnification optical system according to the present embodiment.


Further, in the variable magnification optical system according to the present embodiment it is desirable that a distance between the focusing group and the image side group is increased upon varying magnification from the wide angle end state to the telephoto end state. With this configuration, various aberrations upon varying magnification can be corrected superbly. In particular, it is possible to secure sufficiently a space for moving the focusing group for focusing in the telephoto end state, so it is possible to correct excellently spherical aberration upon focusing on a close distance object in the telephoto end state.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the following conditional expression (3) is satisfied:





0.25<ff/fi<1.10   (3)


where ff denotes a focal length of the focusing group, and fi denotes a focal length of the image side group.


The conditional expression (3) defines a ratio of the focal length of the focusing group to the focal length of the image side group. With satisfying the conditional expression(3), the variable magnification optical system according to the present embodiment can suppress variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object.


When the value of ff/fi is equal to or exceeds the upper limit value of the conditional expression (3) of the variable magnification optical system according to the present embodiment, refractive power of the image side group becomes large, and it becomes difficult to suppress coma aberration and other various aberrations. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (3) to 1.05. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (3) to 1.00.


On the other hand, when the value of ff/fi is equal to or falls below the lower limit value of the conditional expression (3) of the variable magnification optical system according to the present embodiment, refractive power of the focusing group becomes large, and it becomes difficult to correct variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (3) to 0.28. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (3) to 0.31.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the following conditional expression (4) is satisfied:





1.80<fi/(−fB)<5.20   (4)


where fi denotes a focal length of the image side group, and fB denotes a focal length of the B group.


The conditional expression (4) defines a ratio of the focal length of the image side group to the focal length of the B group that is the vibration reduction group. With satisfying the conditional expression (4), the variable magnification optical system according to the present embodiment can suppress effectively deterioration of optical performance upon carrying out vibration reduction.


When the value of fi/(−fB) is equal to or exceeds the upper limit value of the conditional expression (4) of the variable magnification optical system according to the present embodiment, refractive power of the vibration reduction group becomes large, and deterioration of eccentric coma aberration upon carrying out vibration reduction becomes large. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (4) to 5.00. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (4) to 4.90.


On the other hand, when the value of fi/(−fB) is equal to or falls below the lower limit value of the conditional expression (4) of the variable magnification optical system according to the present embodiment, refractive power of the image side group becomes large, and it becomes difficult to correct coma aberration and other various aberrations. Further, refractive power of the vibration reduction group becomes small, and an amount of movement of the vibration reduction group upon carrying out vibration reduction becomes large. For this reason, a lens barrel that receives the variable magnification optical system according to the present embodiment becomes large in size, so this is not preferable. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (4) to 1.90. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (4) to 2.00.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the first lens group comprises at least two positive lenses. With this configuration, spherical aberration and chromatic aberration can be corrected effectively.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the focusing group is composed of one lens component. With this configuration, the focusing group can be made smaller in size and made lighter in weight.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the focusing group is composed of one single lens. With this configuration, the focusing group can be made lighter in weight.


Further, in the variable magnification optical system according to the present embodiment, it is desirable that the focusing group comprises at least one positive lens and the following conditional expression (5) is satisfied:





58.00<νFP   (5)


where νFP denotes an Abbe number for d-line (wavelength 587.6 nm) of the positive lens comprised in the focusing group.


The conditional expression (5) defines an Abbe number of the positive lens comprised in the focusing group. With satisfying the conditional expression (5), the variable magnification optical system according to the present embodiment can suppress variation in chromatic aberration upon focusing from an infinitely distant object to a close distance object.


When the value of νFP is equal to or falls below the lower limit value of the conditional expression (5) of the variable magnification optical system according to the present embodiment, large chromatic aberration in the focusing group occurs, so that variation in chromatic aberration upon focusing from an infinitely distant object to a close distance object becomes large. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (5) to 59.00. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (5) to 60.00.


Further, in the variable magnification optical system according to the present embodiment it is desirable that the following conditional expression (6) is satisfied:





0.15<ff/ft<0.30   (6)


where ff denotes a focal length of the focusing group, and ft denotes a focal length of the variable magnification optical system in the telephoto end state.


The conditional expression (6) defines a ratio of the focal length of the focusing group to the focal length of the variable magnification optical system according to the present embodiment in the telephoto end state. With satisfying the conditional expression (6), the variable magnification optical system according to the present embodiment can suppress variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object.


When the value of ff/ft is equal to or exceeds the upper limit value of the conditional expression (6) of the variable magnification optical system according to the present embodiment, an amount of movement of the focusing group upon focusing from an infinitely distant object to a close distance object becomes large, and it becomes difficult to suppress variations in spherical aberration and other various aberrations. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the upper limit value of the conditional expression (6) to 0.28. Further, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the upper limit value of the conditional expression (6) to 0.26.


On the other hand, when the value of ff/ft is equal to or falls below the lower limit value of the conditional expression (6) of the variable magnification optical system according to the present embodiment, refractive power of the focusing group becomes large, and it becomes difficult to correct variations in spherical aberration and other various aberrations upon focusing from an infinitely distant object to a close distance object. Meanwhile, in order to ensure the advantageous effect of the present embodiment, it is preferable to set the lower limit value of the conditional expression (6) to 0.17. Furthermore, in order to ensure the advantageous effect of the present embodiment more surely, it is preferable to set the lower limit value of the conditional expression (6) to 0.19.


An optical apparatus according to an embodiment of the present invention comprises a variable magnification optical system configured as above-mentioned.


An imaging apparatus according to an embodiment of the present invention is equipped with a variable magnification optical system configured as above-mentioned and an imaging unit for capturing an image formed by the variable magnification optical system.


With such configurations, it is possible to realize an optical apparatus and an imaging apparatus which have excellent optical performance and a focusing lens group reduced in weight in order to attain high speed focusing operation.


According to an embodiment of the present invention, there is provided a method for manufacturing a variable magnification optical system comprising steps of arranging a first lens group disposed at a most object side and having positive refractive power, an intermediate group disposed at an image side of the first lens group and having negative refractive power, a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and an image side group disposed at an image side of the focusing group and having positive refractive power such that, upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group are varied; and arranging such that the image side group is composed of, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression (1) with respect to the A group and having negative refractive power, and a C group:





1.67<fA/(−fB)<2.80   (1)


where fA denotes a focal length of the A group, and


fB denotes a focal length of the B group.


With such configurations, it is possible to manufacture a variable magnification optical system which has excellent optical performance and a focusing lens group reduced in weight in order to attain high speed focusing operation.


Hereinafter, examples relating to a variable magnification optical system according to an embodiment of the present invention will be explained with reference to the accompanying drawings.


FIRST EXAMPLE


FIG. 1 is a sectional view of a variable magnification optical system according to a First Example. Note that each arrow in FIG. 1 and FIGS. 5, 9, 13, 17, 21, 25 and 29 as described later indicates moving trajectory of each lens group upon varying magnification from the wide angle end state (W) to the telephoto end state (T).


The variable magnification optical system according to the First Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a double concave negative lens L42, and a double convex positive lens L43.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a double convex positive lens L44 cemented with a double concave negative lens L45.


The C group G4C consists of, in order from the object side, a double convex positive lens L46, and a negative meniscus lens L47 having a concave surface facing the object side.


In the variable magnification optical system according to the First Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the First Example, the third lens group


G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the First Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby carrying out vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in a lens having a focal length f of the whole lens system and a vibration reduction coefficient K (a ratio of a moving amount of an image on the image plane I to a moving amount of the vibration reduction group), it is possible to correct a rotational camera shake of an angle θ, by moving the vibration reduction group by the amount of (f·tan θ)/K perpendicularly to the optical axis. Accordingly, in the variable magnification optical system according to the First Example, in the wide angle end state, the vibration reduction coefficient is 1.06, and the focal length is 71.40 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.35 (mm). In the telephoto end state, the vibration reduction coefficient is 1.86, and the focal length is 294.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.55 (mm).


Table 1 below shows various values of the variable magnification optical system according to the First Example.


In table 1, “f” denotes a focal length, and “BF” denotes a back focal length (a distance on the optical axis between a most image side lens surface and the image plane I).


In [Surface Data], a surface number denotes an order of an optical surface counted from the object side, “r” denotes a radius of curvature, “d” denotes a surface-to-surface distance (a distance from an n-th surface to an (n+1)-th surface, where n is an integer), “nd” denotes refractive index for d-line (wavelength 587.6 nm) and “νd” denotes an Abbe number for d-line (wavelength 587.6 nm). Further, “Object Plane” denotes an object surface, “variable” denotes a variable surface-to-surface distance, “Stop S” denotes an aperture stop, and “I” denotes an image plane. Meanwhile, radius of curvature r=∞ denotes a plane surface. Refractive index of air nd=1.00000 is omitted.


In [Various Data], “FNO” denotes an F-number, “2ω” denotes an angle of view (unit “°”), “Ymax” denotes a maximum image height, “TL” denotes a total length of the variable magnification optical system according to the First Example (a distance along the optical axis from the first surface to the image plane I), and “dn” denotes a variable distance between an n-th surface and an (n+1)-th surface. Meanwhile, “W” denotes a wide angle end state, “M” denotes an intermediate focal length state, “T” denotes a telephoto end state, “Infinitely distant” denotes a time when focusing on an infinitely distant object is conducted, and “Close distance” denotes a time when focusing on a close distance object is conducted.


In [Lens Group Data], a starting surface and a focal length for each lens group are shown.


In [Values for Conditional Expressions], values corresponding to respective conditional expressions of the variable magnification optical system according to the First Example are shown.


Here, that “mm” is generally used for the unit of length such as the focal length f, the radius of curvature r and the unit for other lengths shown in Table 1. However, since similar optical performance can be obtained by an optical system proportionally enlarged or reduced in its dimension, the unit is not necessarily to be limited to “mm”.


The reference symbols in Table 1 described above, are used in the same way in Tables for the other Examples.









TABLE 1





First Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
72.3688
6.972
1.51680
63.88



 2
−604.5951
0.499



 3
88.4675
1.500
1.62004
36.40



 4
32.5526
8.844
1.51680
63.88



 5
149.4554
variable



 6
−453.8182
1.000
1.69680
55.52



 7
18.7304
3.761
1.80518
25.45



 8
40.0562
3.501



 9
−33.7169
1.000
1.69680
55.52



10
3769.5898
variable



11
91.7620
4.268
1.51680
63.88



12
−46.5887
variable



13
54.6217
5.361
1.48749
70.31



14
−31.8367
1.000
1.85026
32.35



15
829.9126
0.200



16
34.8197
4.124
1.48749
70.31



17
−190.4880
1.633



18 (Stop S)

27.478 



19
316.7035
2.575
1.80518
25.45



20
−37.0122
1.000
1.74400
44.81



21
28.1012
3.267



22
27.6380
3.921
1.54814
45.79



23
−54.2282
2.418



24
−22.4640
1.000
1.77250
49.62



25
−55.2971
BF



Image Plane












[Various Data]


Variable magnification ratio 4.12













W
M
T







f
71.4
105.0
294.0



FNO
4.17
4.18
6.38




22.84
15.30
5.48



Ymax
14.25
14.25
14.25



TL
166.32
183.64
219.32



BF
38.52
38.53
73.71







Infinitely distant












d5
3.555
24.790
43.361



d10
26.610
21.614
2.000



d12
12.316
13.381
14.933







Close distance












d5
3.555
24.790
43.361



d10
27.368
22.723
3.114



d12
11.558
12.271
13.819











[Lens Group Data]









Group
Starting Surface
f





1
1
115.478


2
6
−26.653


3
11
60.427


4
13
138.481










[Values for Conditional Expression]













(1)
fA/(−fB) = 1.717



(1A)
f1/(−fc) = 4.333



(1B)
f1fw/ff = 6.400



(2)
f1/ff = 1.911



(3)
ff/fi = 0.436



(4)
fi/(−fB) = 3.064



(5)
νFP = 63.88



(6)
ff/ft = 0.206











FIGS. 2A, 2B and 2C are graphs showing various aberrations of the variable magnification optical system according to the First Example upon focusing on an infinitely distant object, in which FIG. 2A is in a wide angle end state, FIG. 2B is in an intermediate focal length state, and FIG. 2C is in the telephoto end state.



FIG. 3A is a graph showing meridional transverse aberration of the variable magnification optical system according to the First Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 3B is a graph showing meridional transverse aberration of the variable magnification optical system according to the First Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 4A, 4B and 4C are graphs showing various aberrations of the variable magnification optical system according to the First Example upon focusing on a close distance object, in which FIG. 4A is in the wide angle end state, FIG. 4B is in the intermediate focal length state, and FIG. 4C is in the telephoto end state.


In respective aberration graphs, FNO denotes an F-number, Y denotes an image height, and NA denotes a numerical aperture. For more information, there are shown a value of F-number FNO or numerical aperture NA corresponding to the maximum diameter in a spherical aberration graph, the maximum value of the image height Y in each of an astigmatism graph and a distortion graph, and a value of each image height in a coma aberration graph. Additionally, in respective aberration graphs, d denotes an aberration at d-line (wavelength 587.6 nm), and g denotes an aberration at g-line (wavelength 435.8 nm). In the astigmatism graph, a solid line indicates a sagittal image plane, and a broken line indicates a meridional image plane. The coma aberration graph shows a coma aberration for each image height Y. Incidentally, the same symbols as used in the First Example are employed in the other Examples as described later.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the First Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


SECOND EXAMPLE


FIG. 5 is a sectional view of a variable magnification optical system according to a Second Example.


The variable magnification optical system according to the Second Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a negative meniscus lens L42 having a concave surface facing the object side.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L43 having a concave surface facing the object side cemented with a double concave negative lens L44.


The C group G4C consists of, in order from the object side, a double convex positive lens L45 and a negative meniscus lens L46 having a concave surface facing the object side.


In the variable magnification optical system according to the Second Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Second Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Second Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Second Example, in the wide angle end state, the vibration reduction coefficient is 1.17, and the focal length is 71.35 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.32 (mm). In the telephoto end state, the vibration reduction coefficient is 1.80, and the focal length is 294.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.57 (mm).


Table 2 below shows various values of the variable magnification optical system according to the Second Example.









TABLE 2





Second Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
84.0136
6.369
1.51680
63.88



 2
−569.5201
0.287



 3
111.7962
1.500
1.62004
36.40



 4
36.8295
8.708
1.51680
63.88



 5
239.6437
variable



 6
−196.3998
1.000
1.69680
55.52



 7
17.8250
4.472
1.80518
25.45



 8
63.8758
2.220



 9
−50.1550
1.000
1.80100
34.92



10
107.3132
variable



11
98.4276
3.799
1.51680
63.88



12
−44.7987
variable



13
33.5689
5.221
1.48749
70.31



14
−34.6171
1.000
1.75520
27.57



15
−464.1612
1.880



16 (Stop S)

31.253 



17
−215.7008
3.558
1.80610
40.97



18
−18.9067
1.000
1.69680
55.52



19
29.6933
2.000



20
25.4517
4.902
1.51742
52.20



21
−34.1288
6.212



22
−19.1689
1.000
1.77250
49.62



23
−46.3649
BF



Image Plane












[Various Data]


Variable magnification ratio 4.12













W
M
T







f
71.4
105.0
294.0



FNO
4.70
4.74
6.44




22.84
15.30
5.46



Ymax
14.25
14.25
14.25



TL
167.32
188.67
222.32



BF
38.52
39.12
64.52







Infinitely distant












d5
3.000
27.419
53.254



d10
29.124
23.882
2.000



d12
9.294
10.871
15.165







Close distance












d5
3.000
27.419
53.254



d10
29.965
25.078
3.487



d12
8.453
9.675
13.679











[Lens Group Data]









Group
Starting Surface
f





1
1
128.484


2
6
−29.436


3
11
60.115


4
13
180.542










[Values for Conditional Expression]













(1)
fA/(−fB) = 2.468



(1A)
f1/(−fc) = 4.365



(1B)
f1fw/ff = 3.954



(2)
f1/ff = 2.137



(3)
ff/fi = 0.333



(4)
fi/(−fB) = 3.886



(5)
νFP = 63.88



(6)
ff/ft = 0.204











FIGS. 6A, 6B and 6C are graphs showing various aberrations of the variable magnification optical system according to the Second Example upon focusing on an infinitely distant object, in which FIG. 6A is in a wide angle end state, FIG. 6B is in an intermediate focal length state, and FIG. 6C is in a telephoto end state.



FIG. 7A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Second Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 7B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Second Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 8A, 8B and 8C are graphs showing various aberrations of the variable magnification optical system according to the Second Example upon focusing on a close distance object, in which FIG. 8A is in the wide angle end state, FIG. 8B is in the intermediate focal length state, and FIG. 8C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Second Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


THIRD EXAMPLE


FIG. 9 is a sectional view of a variable magnification optical system according to a Third Example.


The variable magnification optical system according to the Third Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a negative meniscus lens L42 having a concave surface facing the object side.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L43 having a concave surface facing the object side cemented with a double concave negative lens L44.


The C group G4C consists of, in order from the object side, a double convex positive lens L45, and a cemented negative lens constructed by a double concave negative lens L46 cemented with a double convex positive lens L47.


In the variable magnification optical system according to the Third Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Third Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Third Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Third Example, in the wide angle end state, the vibration reduction coefficient is 1.22, and the focal length is 71.40 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.31 (mm). In the telephoto end state, the vibration reduction coefficient is 1.79, and the focal length is 294.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.57 (mm).


Table 3 below shows various values of the variable magnification optical system according to the Third Example.









TABLE 3





Third Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
85.0462
5.776
1.51680
63.88



 2
−660.6172
0.468



 3
127.3802
1.500
1.62004
36.40



 4
39.1726
7.903
1.51680
63.88



 5
338.5447
variable



 6
−132.1891
1.000
1.69680
55.52



 7
19.2602
4.667
1.80518
25.45



 8
76.0183
2.071



 9
−54.4201
1.000
1.80100
34.92



10
119.2030
variable



11
101.6158
3.707
1.51680
63.88



12
−48.1136
variable



13
32.8274
5.339
1.48749
70.31



14
−36.1413
1.000
1.80518
25.45



15
−208.8127
1.719



16 (Stop S)

20.897 



17
−111.8106
3.901
1.66755
41.87



18
−18.5066
1.000
1.58913
61.22



19
35.2076
2.000



20
26.2172
5.000
1.48749
70.31



21
−44.8232
10.387 



22
−18.5590
1.000
1.77250
49.62



23
39.9065
4.006
1.60342
38.03



24
−29.6411
BF



Image Plane












[Various Data]


Variable magnification ratio 4.12













W
M
T







f
71.4
105.0
294.0



FNO
4.68
4.76
6.45




22.80
15.28
5.44



Ymax
14.25
14.25
14.25



TL
166.39
188.89
221.32



BF
38.52
39.12
64.52







Infinitely distant












d5
3.000
27.909
54.414



d10
30.861
25.246
2.000



d12
9.676
12.274
16.047







Close distance












d5
3.000
27.909
54.414



d10
31.772
26.533
3.581



d12
8.765
10.987
14.466











[Lens Group Data]









Group
Starting Surface
f





1
1
130.814


2
6
−30.984


3
11
63.720


4
13
184.004










[Values for Conditional Expression]













(1)
fA/(−fB) = 1.836



(1A)
f1/(−fc) = 4.222



(1B)
f1fw/ff = 3.924



(2)
f1/ff = 2.063



(3)
ff/fi = 0.345



(4)
fi/(−fB) = 3.433



(5)
νFP = 63.88



(6)
ff/ft = 0.216











FIGS. 10A, 10B and 10C are graphs showing various aberrations of the variable magnification optical system according to the Third Example upon focusing on an infinitely distant object, in which FIG. 10A is in a wide angle end state, FIG. 10B is in an intermediate focal length state, and FIG. 10C is in a telephoto end state.



FIG. 11A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Third Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 11B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Third Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 12A, 12B and 12C are graphs showing various aberrations of the variable magnification optical system according to the Third Example upon focusing on a close distance object, in which FIG. 12A is in the wide angle end state, FIG. 12B is in the intermediate focal length state, and FIG. 12C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Third Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


FOURTH EXAMPLE


FIG. 13 is a sectional view of a variable magnification optical system according to a Fourth Example.


The variable magnification optical system according to the Fourth Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a negative meniscus lens L42 having a concave surface facing the object side.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L43 having a concave surface facing the object side cemented with a double concave negative lens L44.


The C group G4C consists of, in order from the object side, a double convex positive lens L45, and a cemented negative lens constructed by a double concave negative lens L46 cemented with a double convex positive lens L47.


In the variable magnification optical system according to the Fourth Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Fourth Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Fourth Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Fourth Example, in the wide angle end state, the vibration reduction coefficient is 1.21, and the focal length is 71.40 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.31 (mm). In the telephoto end state, the vibration reduction coefficient is 1.79, and the focal length is 292.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.57 (mm).


Table 4 below shows various values of the variable magnification optical system according to the Fourth Example.









TABLE 4





Fourth Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
86.4475
5.443
1.51680
63.88



 2
−981.1690
0.200



 3
146.3378
1.500
1.62004
36.40



 4
41.2453
8.000
1.51680
63.88



 5
1154.1773
variable



 6
−105.1301
1.000
1.69680
55.52



 7
20.4832
4.124
1.80518
25.45



 8
77.3629
1.964



 9
−62.6354
1.000
1.83400
37.18



10
142.2611
variable



11
123.7504
3.431
1.58913
61.22



12
−57.1062
variable



13
33.8130
5.634
1.49700
81.73



14
−38.7693
1.000
1.80518
25.45



15
−194.5892
1.688



16 (Stop S)

21.000 



17
−99.8095
3.775
1.66755
41.87



18
−18.8632
1.000
1.58913
61.22



19
36.8056
2.500



20
34.3226
3.724
1.51680
63.88



21
−51.2601
11.445 



22
−20.6818
1.000
1.77250
49.62



23
51.2093
3.854
1.60342
38.03



24
−30.0976
BF



Image Plane












[Various Data]


Variable magnification ratio 4.09













W
M
T







f
71.4
100.0
292.0



FNO
4.70
4.69
6.48




22.78
16.04
5.48



Ymax
14.25
14.25
14.25



TL
169.32
189.52
221.32



BF
39.12
38.52
66.12







Infinitely distant












d5
3.000
26.086
53.441



d10
32.425
27.561
2.000



d12
11.493
14.070
16.477







Close distance












d5
3.000
26.086
53.441



d10
33.360
28.885
3.621



d12
10.558
12.746
14.856











[Lens Group Data]









Group
Starting Surface
f





1
1
128.221


2
6
−31.614


3
11
66.796


4
13
176.525










[Values for Conditional Expression]













(1)
fA/(−fB) = 1.691



(1A)
f1/(−fc) = 4.056



(1B)
f1fw/ff = 4.017



(2)
f1/ff = 1.920



(3)
ff/fi = 0.378



(4)
fi/(−fB) = 3.308



(5)
νFP = 61.22



(6)
ff/ft = 0.229











FIGS. 14A, 14B and 14C are graphs showing various aberrations of the variable magnification optical system according to the Fourth Example upon focusing on an infinitely distant object, in which FIG. 14A is in a wide angle end state, FIG. 14B is in an intermediate focal length state, and FIG. 14C is in a telephoto end state.



FIG. 15A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Fourth Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 15B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Fourth Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 16A, 16B and 16C are graphs showing various aberrations of the variable magnification optical system according to the Fourth Example upon focusing on a close distance object, in which FIG. 16A is in the wide angle end state, FIG. 16B is in the intermediate focal length state, and FIG. 16C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Fourth Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


FIFTH EXAMPLE


FIG. 17 is a sectional view of a variable magnification optical system according to a Fifth Example.


The variable magnification optical system according to the Fifth Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a negative meniscus lens L42 having a concave surface facing the object side.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L43 having a concave surface facing the object side cemented with a double concave negative lens L44.


The C group G4C consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L45 cemented with a negative meniscus lens L46 having a concave surface facing the object side, and a negative meniscus lens L47 having a concave surface facing the object side.


In the variable magnification optical system according to the Fifth Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Fifth Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Fifth Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Fifth Example, in the wide angle end state, the vibration reduction coefficient is 1.61, and the focal length is 72.10 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.23 (mm). In the telephoto end state, the vibration reduction coefficient is 2.44, and the focal length is 292.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.42 (mm).


Table 5 below shows various values of the variable magnification optical system according to the Fifth Example.









TABLE 5





Fifth Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
90.0000
5.600
1.51680
63.88



 2
−517.3850
0.200



 3
123.0815
1.700
1.62004
36.40



 4
39.0000
7.800
1.51680
63.88



 5
324.1762
variable



 6
−110.0000
1.300
1.69680
55.52



 7
21.2201
3.957
1.84666
23.80



 8
73.0429
1.848



 9
−75.3714
1.200
1.85026
32.35



10
106.1768
variable



11
148.9696
3.374
1.58913
61.22



12
−56.4978
variable



13
28.2564
5.746
1.49700
81.73



14
−48.4258
1.200
1.84666
23.80



15
−580.3411
2.897



16 (Stop S)

23.051 



17
−77.0000
3.951
1.72825
28.38



18
−14.4874
1.000
1.67003
47.14



19
29.3362
2.500



20
29.8903
5.510
1.62004
36.40



21
−17.4201
1.000
1.84666
23.80



22
−35.2773
7.314



23
−22.7541
1.000
1.77250
49.62



24
−46.2730
BF



Image Plane












[Various Data]


variable magnification ratio 4.05













W
M
T







f
72.1
100.0
292.0



FNO
4.70
4.63
6.53




22.62
16.08
5.50



Ymax
14.25
14.25
14.25



TL
169.32
187.97
221.32



BF
39.61
38.52
66.61







Infinitely distant












d5
3.001
26.619
53.461



d10
33.373
28.524
2.000



d12
11.187
12.162
17.100







Close distance












d5
3.001
26.619
53.461



d10
34.372
29.969
3.698



d12
10.188
10.718
15.402











[Lens Group Data]









Group
Starting Surface
f





1
1
131.155


2
6
−32.550


3
11
69.956


4
13
165.331










[Values for Conditional Expression]













(1)
fA/(−fB) = 2.356



(1A)
f1/(−fc) = 4.029



(1B)
f1fw/ff = 4.519



(2)
f1/ff = 1.902



(3)
ff/fi = 0.417



(4)
fi/(−fB) = 4.755



(5)
νFP = 61.22



(6)
ff/ft = 0.236











FIGS. 18A, 18B and 18C are graphs showing various aberrations of the variable magnification optical system according to the Fifth Example upon focusing on an infinitely distant object, in which FIG. 18A is in a wide angle end state, FIG. 18B is in an intermediate focal length state, and FIG. 18C is in a telephoto end state.



FIG. 19A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Fifth Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 19B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Fifth Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 20A, 20B and 20C are graphs showing various aberrations of the variable magnification optical system according to the Fifth Example upon focusing on a close distance object, in which FIG. 20A is in the wide angle end state, FIG. 20B is in the intermediate focal length state, and FIG. 20C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Fifth Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


SIXTH EXAMPLE


FIG. 21 is a sectional view of a variable magnification optical system according to a Sixth Example.


The variable magnification optical system according to the Sixth Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a double concave negative lens L42, and a double convex positive lens L43.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a negative meniscus lens L44 having a concave surface facing the object side cemented with a double concave negative lens L45.


The C group G4C consists of, in order from the object side, a double convex positive lens L46, and a negative meniscus lens L47 having a concave surface facing the object side.


In the variable magnification optical system according to the Sixth Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Sixth Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Sixth Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Sixth Example, in the wide angle end state, the vibration reduction coefficient is 1.54, and the focal length is 72.10 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.25 (mm). In the telephoto end state, the vibration reduction coefficient is 2.42, and the focal length is 292.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.42 (mm).


Table 6 below shows various values of the variable magnification optical system according to the Sixth Example.









TABLE 6





Sixth Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
94.0000
5.600
1.51680
63.88



 2
−475.5757
0.200



 3
128.0000
1.700
1.62004
36.40



 4
39.6000
8.000
1.51680
63.88



 5
425.5305
variable



 6
−190.0000
1.300
1.69680
55.52



 7
20.4656
4.300
1.84666
23.80



 8
66.5049
2.063



 9
−61.8359
1.200
1.85026
32.35



10
109.1965
variable



11
128.7113
3.300
1.58913
61.22



12
−63.7222
variable



13
37.0000
5.400
1.49700
81.73



14
−45.9212
1.300
1.85026
32.35



15
148.3744
0.200



16
45.1050
3.600
1.48749
70.31



17
−172.8812
4.000



18 (Stop S)

26.764 



19
−95.3704
3.900
1.74950
35.25



20
−14.2257
1.000
1.69680
55.52



21
24.1570
2.279



22
26.2427
4.000
1.62004
36.40



23
−55.0000
2.250



24
−20.2886
1.000
1.84666
23.80



25
−34.0000
BF



Image Plane












[Various Data]


Variable magnification ratio 4.05













W
M
T







f
72.1
100.0
292.0



FNO
4.69
4.66
6.54




22.56
16.04
5.50



Ymax
14.25
14.25
14.25



TL
169.32
189.24
221.32



BF
38.93
38.52
65.93







Infinitely distant












d5
2.500
25.118
52.806



d10
33.481
28.557
2.155



d12
11.047
13.692
17.068







Close distance












d5
2.500
25.118
52.806



d10
34.454
29.917
3.849



d12
10.075
12.332
15.373











[Lens Group Data]









Group
Starting Surface
f





1
1
130.472


2
6
−32.352


3
11
72.809


4
13
142.608










[Values for Conditional Expression]













(1)
fA/(−fB) = 2.479



(1A)
f1/(−fc) = 4.033



(1B)
f1fw/ff = 6.295



(2)
f1/ff = 1.792



(3)
ff/fi = 0.511



(4)
fi/(−fB) = 4.779



(5)
νFP = 61.22



(6)
ff/ft = 0.249











FIGS. 22A, 22B and 22C are graphs showing various aberrations of the variable magnification optical system according to the Sixth Example upon focusing on an infinitely distant object, in which FIG. 22A is in a wide angle end state, FIG. 22B is in an intermediate focal length state, and FIG. 22C is in a telephoto end state.



FIG. 23A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Sixth Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 23B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Sixth Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 24A, 24B and 24C are graphs showing various aberrations of the variable magnification optical system according to the Sixth Example upon focusing on a close distance object, in which FIG. 24A is in the wide angle end state, FIG. 24B is in the intermediate focal length state, and FIG. 24C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Sixth Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


SEVENTH EXAMPLE


FIG. 25 is a sectional view of a variable magnification optical system according to a Seventh Example.


The variable magnification optical system according to the Seventh Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, and a fourth lens group G4 having positive refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a double concave negative lens L42, and a double convex positive lens L43.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L44 having a concave surface facing the object side cemented with a double concave negative lens L45.


The C group G4C consists of, in order from the object side, a double convex positive lens L46, and a negative meniscus lens L47 having a concave surface facing the object side.


In the variable magnification optical system according to the Seventh Example, the first to fourth lens groups G1 to G4 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3 and a distance between the third lens group G3 and the fourth lens group G4 are varied.


In the variable magnification optical system according to the Seventh Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Seventh Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Seventh Example, in the wide angle end state, the vibration reduction coefficient is 1.61, and the focal length is 72.10 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.23 (mm). In the telephoto end state, the vibration reduction coefficient is 2.42, and the focal length is 292.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.42 (mm).


Table 7 below shows various values of the variable magnification optical system according to the Seventh Example.









TABLE 7





Seventh Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
94.0000
5.600
1.51680
63.88



 2
−477.1369
0.200



 3
127.9954
1.700
1.62004
36.40



 4
39.7182
8.000
1.51680
63.88



 5
477.0326
variable



 6
−133.8008
1.300
1.69680
55.52



 7
20.5210
4.000
1.84666
23.80



 8
68.1000
2.028



 9
−63.5000
1.200
1.85026
32.35



10
113.2367
variable



11
102.3130
3.400
1.58913
61.22



12
−69.1650



13
39.2000
5.500
1.49700
81.73



14
−39.2000
1.300
1.85026
32.35



15
209.5771
0.200



16
50.7811
3.700
1.48749
70.31



17
−101.5494
1.393



18 (Stop S)

22.905 



19
−80.0000
3.300
1.80100
34.92



20
−18.0344
1.000
1.70000
48.11



21
29.8801
2.000



22
34.2607
3.800
1.60342
38.03



23
−54.3498
7.014



24
−20.2978
1.000
1.77250
49.62



25
−34.3298
BF



Image plane












[Various Data]


Variable magnification ratio 4.05













W
M
T







f
72.1
100.0
292.0



FNO
4.71
4.68
6.51




22.58
16.04
5.50



Ymax
14.25
14.25
14.25



TL
169.32
188.35
221.32



BF
42.82
42.30
69.82







Infinitely distant












d5
2.500
25.131
52.658



d10
32.209
27.505
2.151



d12
11.251
12.875
16.152







Close distance












d5
2.500
25.131
52.658



d10
33.116
28.781
3.756



d12
10.345
11.599
14.546











[Lens Group Data]









Group
Starting Surface
f





1
1
128.381


2
6
−31.506


3
11
70.567


4
13
143.423










[Values for Conditional Expression]













(1)
fA/(−fB) = 2.044



(1A)
f1/(−fc) = 4.075



(1B)
f1fw/ff = 6.330



(2)
f1/ff = 1.819



(3)
ff/fi = 0.492



(4)
fi/(−fB) = 4.048



(5)
νFP = 61.22



(6)
ff/ft = 0.242











FIGS. 26A, 26B and 26C are graphs showing various aberrations of the variable magnification optical system according to the Seventh Example upon focusing on an infinitely distant object, in which FIG. 26A is in a wide angle end state, FIG. 26B is in an intermediate focal length state, and FIG. 26C is in a telephoto end state.



FIG. 27A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Seventh Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 27B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Seventh Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 28A, 28B and 28C are graphs showing various aberrations of the variable magnification optical system according to the Seventh Example upon focusing on a close distance object, in which FIG. 28A is in the wide angle end state, FIG. 28B is in the intermediate focal length state, and FIG. 28C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Seventh Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


EIGHTH EXAMPLE


FIG. 29 is a sectional view of a variable magnification optical system according to an Eighth Example.


The variable magnification optical system according to the Eighth Example is composed of, in order from an object side, a first lens group G1 having positive refractive power, a second lens group G2 having negative refractive power, and a rear group GR having positive refractive power. The rear group GR is composed of, in order from the object side, a third lens group G3 having positive refractive power, a fourth lens group G4 having positive refractive power, and a fifth lens group G5 having negative refractive power.


The first lens group G1 consists of, in order from the object side, a double convex positive lens L11, and a cemented positive lens constructed by a negative meniscus lens L12 having a convex surface facing the object side cemented with a positive meniscus lens L13 having a convex surface facing the object side.


The second lens group G2 consists of, in order from the object side, a cemented negative lens constructed by a double concave negative lens L21 cemented with a positive meniscus lens L22 having a convex surface facing the object side, and a double concave negative lens L23.


The third lens group G3 consists of a double convex positive lens L31.


The fourth lens group G4 is composed of, in order from the object side, an A group G4A having positive refractive power, a B group G4B having negative refractive power, and a C group G4C having positive refractive power. Meanwhile, an aperture stop S is disposed between the A group G4A and the B group G4B.


The A group G4A consists of, in order from the object side, a cemented positive lens constructed by a double convex positive lens L41 cemented with a double concave negative lens L42, and a double convex positive lens L43.


The B group G4B consists of, in order from the object side, a cemented negative lens constructed by a positive meniscus lens L44 having a concave surface facing the object side cemented with a double concave negative lens L45.


The C group G4C consists of a double convex positive lens L46.


The fifth lens group G5 consists of a negative meniscus lens L51 having a concave surface facing the object side.


In the variable magnification optical system according to the Eighth Example, the first to the fifth lens groups G1 to G5 are moved along the optical axis so that, upon varying magnification between the wide angle end state and the telephoto end state, a distance between the first lens group G1 and the second lens group G2, a distance between the second lens group G2 and the third lens group G3, a distance between the third lens group G3 and the fourth lens group G4 and a distance between the fourth lens group G4 and the fifth lens group G5 are varied.


In the variable magnification optical system according to the Eighth Example, the third lens group G3 is moved toward an image side along the optical axis, as the focusing lens group, thereby focusing from an infinitely distant object to a close distance object.


In the variable magnification optical system according to the Eighth Example, the B group G4B is moved, as a vibration reduction group, to have a component in a direction perpendicular to the optical axis, thereby conducting vibration reduction. Meanwhile, upon carrying out vibration reduction, positions of the A group G4A and the C group G4C in a direction perpendicular to the optical axis are fixed.


It is noted that in the variable magnification optical system according to the Eighth Example, in the wide angle end state, the vibration reduction coefficient is 1.62, and the focal length is 72.10 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.30 degrees is 0.23 (mm). In the telephoto end state, the vibration reduction coefficient is 2.42, and the focal length is 292.00 (mm), so that the moving amount of the B group G4B for correcting a rotational camera shake of 0.20 degrees is 0.42 (mm).


Table 8 below shows various values of the variable magnification optical system according to the Eighth Example.









TABLE 8





Eighth Example







[Surface Data]













Surface number
r
d
nd
νd







Object Plane




 1
94.0000
5.600
1.51680
63.88



 2
−475.1178
0.200



 3
128.0000
1.700
1.62004
36.40



 4
39.6000
8.000
1.51680
63.88



 5
485.7465
variable



 6
−132.5210
1.300
1.69680
55.52



 7
20.5172
4.000
1.84666
23.80



 8
68.1000
2.042



 9
−63.5000
1.200
1.85026
32.35



10
115.6235
variable



11
101.8918
3.400
1.58913
61.22



12
−69.9544
variable



13
39.2000
5.500
1.49700
81.73



14
−39.2000
1.300
1.85026
32.35



15
212.6596
0.200



16
51.4164
3.700
1.48749
70.31



17
−99.0728
1.373



18 (Stop S)

23.152 



19
−80.0000
3.300
1.80100
34.92



20
−17.8244
1.000
1.70000
48.11



21
29.4302
2.000



22
34.1234
3.800
1.60342
38.03



23
−54.6969
variable



24
−20.3466
1.000
1.77250
49.62



25
−34.1069
BF



Image Plane












[Various Data]


Variable magnification ratio 4.05













W
M
T







f
72.1
100.0
292.0



FNO
4.71
4.69
6.49




22.58
16.06
5.50



Ymax
14.25
14.25
14.25



TL
169.32
188.16
221.32



BF
43.07
42.89
70.02







Infinitely distant












d5
2.500
24.944
52.518



d10
32.517
27.845
2.150



d12
10.875
12.288
16.347



d23
6.586
6.430
6.515







Close distance












d5
2.500
24.944
52.518



d10
33.434
29.131
3.779



d12
9.958
11.001
14.718



d23
6.586
6.430
6.515











[Lens Group Data]









Group
Starting Surface
f





1
1
128.138


2
6
−31.607


3
11
70.925


4
13
71.734


5
24
−67.420










[Values for Conditional Expression]













(1)
fA/(−fB) = 2.058



(1A)
f1/(−fc) = 4.054



(1B)
f1fw/ff = 6.215



(2)
f1/ff = 1.807



(3)
ff/fi = 0.989



(4)
fi/(−fB) = 2.046



(5)
νFP = 61.22



(6)
ff/ft = 0.243











FIGS. 30A, 30B and 30C are graphs showing various aberrations of the variable magnification optical system according to the Eighth Example upon focusing on an infinitely distant object, in which FIG. 30A is in a wide angle end state, FIG. 30B is in an intermediate focal length state, and FIG. 30C is in a telephoto end state.



FIG. 31A is a graph showing meridional transverse aberration of the variable magnification optical system according to the Eighth Example upon focusing on an infinitely distant object in the wide angle end state with carrying out vibration reduction against a rotational camera shake of 0.30 degrees, and FIG. 31B is a graph showing meridional transverse aberration of the variable magnification optical system according to the Eighth Example upon focusing on an infinitely distant object in the telephoto end state with carrying out vibration reduction against a rotational camera shake of 0.20 degrees.



FIGS. 32A, 32B and 32C are graphs showing various aberrations of the variable magnification optical system according to the Eighth Example upon focusing on a close distance object, in which FIG. 32A is in the wide angle end state, FIG. 32B is in the intermediate focal length state, and FIG. 32C is in the telephoto end state.


As is apparent from the respective aberration graphs, the variable magnification optical system according to the Eighth Example shows superb imaging performance as a result of good corrections to various aberrations in the wide angle end state to the telephoto end state, and also shows superb imaging performance upon carrying out vibration reduction and upon focusing on a close distance object.


According to the above-mentioned examples, it is possible to realize a variable magnification optical system which can superbly suppress variations in various aberrations upon varying magnification from the wide angle end state to the telephoto end state and variations in various aberrations upon focusing from an infinitely distant object to a close distance object and can downsize a focusing group and make it light in weight. That is, in this variable magnification optical system, by downsizing the focusing group and making it light in weight, the focusing group can be driven by a small-sized motor or mechanical mechanism, thereby realizing a high speed and silent focusing operation with avoiding enlargement of a lens barrel.


Note that each of the above described Examples is a concrete example of the invention of the present application, and the invention of the present application is not limited to them. The contents described below can be properly adopted without deteriorating optical performance of the variable magnification optical systems according to the embodiment of the present application.


Although the variable magnification optical systems each having a four or five group configuration are illustrated above as examples of the variable magnification optical systems according to the embodiment of the present application, the present application is not limited to them and the variable magnification optical systems having other configurations, such as a six group configuration and the like, can be configured. Concretely, a configuration that a lens or a lens group is added to a most object side or a most image side of the variable magnification optical system according to each of the above-mentioned examples is also possible.


Further, in each of the above-mentioned examples, the second lens group is illustrated as an intermediate group disposed at an image side of the first lens group and having negative refractive power, but the present invention is not limited to such configuration. Further, in each of the above-mentioned examples, the third lens group is illustrated as a focusing group disposed at an image side of the second lens group as an intermediate group and having positive refractive power, but the present invention is not limited to such configuration. Further, in each of the above-mentioned examples, the fourth lens group is illustrated as an image side group disposed at an image side of the focusing group and having positive refractive power, but the present invention is not limited to such configuration. Concretely, it is also possible that a lens group having a positive or negative refractive power is disposed between the first lens group and the intermediate group (the second lens group) and distances between these lens groups are varied upon varying magnification. Further, it is also possible that a lens group having a positive or negative refractive power is disposed between the intermediate group (the second lens group) and the focusing group (the third lens group) and distances between these lens groups are varied upon varying magnification. Further, it is also possible that a lens group having a positive or negative refractive power is disposed between the focusing group (the third lens group) and the image side group (the fourth lens group) and distances between these lens groups are varied upon varying magnification.


In the variable magnification optical system according to each of the above-mentioned examples, it is preferable that the vibration reduction group is disposed at an image side of the focusing group, and it is more preferable that other lens(es) is(are) disposed between the focusing group and the vibration reduction group. Further, regarding the rear group, in a case where other lens(es) is(are) disposed between the focusing group and the vibration reduction group, it is preferable that an air distance between a lens facing an object side of the vibration reduction group and the vibration reduction group is the largest one of the air distances in the rear group.


Further, regarding the rear group, it is preferable that an aperture stop is disposed between the focusing group and the vibration reduction group, and it is more preferable that an aperture stop is disposed at a position facing an object side of the vibration reduction group. Meanwhile, the function of an aperture stop may be substituted by a lens frame without disposing a member as the aperture stop.


Further, the refractive power of the C group is positive in each of the Examples, but it may be negative.


Further, a sub-combination of feature groups of respective examples also is deemed as an invention of the present application.


Further, in the variable magnification optical system according to each of the above-mentioned examples, the whole third lens group is used as a focusing group, but a part of lens group or two or more lens groups may be used as a focusing group. Further, it is preferable that the focusing group has a positive refractive power. Further, one or two lens components are enough for configuration of the focusing group, but more preferably the focusing group is composed of one lens component. The focusing group can be used for auto focus, and also can be suitably driven by a motor for auto focus, for example, an ultrasonic motor, a stepping motor, a VCM motor or the like.


Further, in the variable magnification optical system according to each of the above-mentioned examples, any lens group in the entirety thereof or a portion thereof can be shifted in a direction including a component perpendicular to the optical axis as a vibration reduction group, or rotationally moved (swayed) in an in-plane direction including the optical axis for conducting vibration reduction. Particularly, in the variable magnification optical system according to each of the above-mentioned examples, it is preferable that the B group is used as a vibration reduction group. Further, although vibration reduction group may be composed of one cemented lens as in each of the above-mentioned examples, it may be also composed of a single lens or two or more lens components without particularly limiting the number of lenses. Further, it is preferable that the vibration reduction group has negative refraction power. Further, it is preferable that the vibration reduction group is composed of a part of one lens group, and it is more preferable that one lens group is divided into three parts and the vibration reduction group is composed of a center part of the three parts. Furthermore, it is preferable that one lens group is divided into three positive-negative-positive parts or positive-negative-negative parts, and the vibration reduction group is composed of a center negative part of the three parts.


Further, in the variable magnification optical system according to each of the above-mentioned examples, a lens surface of a lens may be a spherical surface, a plane surface, or an aspherical surface. Further, each lens may be formed by a glass material, a resin material or a composite of a glass material and a resin material. When a lens surface is a spherical surface or a plane surface, lens processing and assembly adjustment become easy, so that deterioration in optical performance caused by a lens processing error and an assembly adjustment error can be prevented and thus it is preferable. Moreover, even if the image plane is shifted, deterioration in optical performance is little conveniently. When a lens surface is an aspherical surface, the aspherical surface may be fabricated by a grinding process, a glass molding process that a glass material is formed into an aspherical shape by a mold, or a compound type process that a resin material on a glass surface is formed into an aspherical shape. Further, a lens surface may be a diffractive optical surface, and a lens may be a graded-index type lens (GRIN lens) or a plastic lens.


Moreover, lens surfaces of lenses configuring the variable magnification optical system according to each example may be coated with anti-reflection coating. With this contrivance, it is feasible to reduce a flare as well as ghost and attain high contrast and high optical performance. Particularly, in the variable magnification optical system according to each of the above-mentioned examples, it is preferable to coat an object side lens surface of the second lens counted from a most object side with anti-reflection coating.


Next, a camera equipped with a variable magnification optical system according to an embodiment of the present application, will be explained with referring to FIG. 33.



FIG. 33 is a sectional view showing a configuration of the camera equipped with the variable magnification optical system according to the embodiment of the present application.


As shown in FIG. 33, a camera 1 is a so-called mirrorless camera of lens-replaceable type equipped with the variable magnification optical system according to the above-mentioned First Example as an imaging lens 2.


In the present camera 1, light emitted from an unillustrated object is converged by the imaging lens 2, and an object image is formed on an imaging surface of an imaging unit 3 through an unillustrated OLPF (Optical low pass filter). Then, the object image is photo-electrically converted by a photoelectric conversion element in the imaging unit 3 to generate an image of the object. This image is displayed on an EVF (Electronic view finder) 4 mounted in the camera 1. Accordingly, a photographer can observe the object image through the EVF 4.


Further, when the photographer presses an unillustrated release button down, the image of the object generated in the imaging unit 3 is stored in an unillustrated memory. In this manner, the photographer can take a picture of an object by the present camera 1.


Hence, the variable magnification optical system according to the above First Example, mounted as the imaging lens 2 in the present camera 1, has excellent optical performance and a focusing lens group reduced in weight. That is, the present camera 1 can realize excellent optical performance and high speed focusing operation. Moreover, even when a camera is configured to mount thereon the variable magnification optical system according to each of the above Second to Eighth Examples, as the imaging lens 2, the camera can provide the same advantageous effects as the above camera 1 can do. Further, even when the variable magnification optical system according to each of the above examples is mounted on a camera of single-lens reflex type having a quick return mirror and observing an object by a finder optical system, the camera can provide the same advantageous effects as the above camera 1 can do.


Finally, an outline of a method for manufacturing a variable magnification optical system according to the present embodiment, is described with referring to FIG. 34.



FIG. 34 is a flowchart showing an outline of a method for manufacturing the variable magnification optical system according to the present embodiment.


A method for manufacturing a variable magnification optical system according to the present embodiment as shown in FIG. 34 comprises a step S1 of preparing a first lens group disposed at a most object side and having positive refractive power, an intermediate group disposed at an image side of the first lens group and having negative refractive power, a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and an image side group disposed at an image side of the focusing group and having positive refractive power, and a step S2 of arranging the first lens group, the intermediate group, the focusing group, and the image side group such that, upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group are varied, the image side group being composed of, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression (1) with respect to the A group and having negative refractive power, and a C group:





1.67<fA/(−fB)<2.80   (1)


where fA denotes a focal length of the A group, and fB denotes a focal length of the B group.


According to the method for manufacturing a variable magnification optical system of the present embodiment, it is possible to manufacture a variable magnification optical system having excellent optical performance and a focusing lens group reduced in weight in order to attain high speed focusing operation.

Claims
  • 1. A variable magnification optical system, comprising: a first lens group disposed at a most object side and having positive refractive power;an intermediate group disposed at an image side of the first lens group and having negative refractive power;a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing; andan image side group disposed at an image side of the focusing group and having positive refractive power;upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group being varied;the image side group comprising, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)<2.80where fA denotes a focal length of the A group, and fB denotes a focal length of the B group; andthe following conditional expression being satisfied: 2.50<f1/(−fc)≤4.365where f1 denotes a focal length of the first lens group, and fc denotes a focal length of the intermediate group.
  • 2. A variable magnification optical system according to claim 1, wherein the following conditional expression is satisfied: 0.25<ff/fi<1.10where ff denotes a focal length of the focusing group, and fi denotes a focal length of the image side group.
  • 3. A variable magnification optical system according to claim 1, wherein the following conditional expression is satisfied: 1.80<fi/(−fB)<5.20where fi denotes a focal length of the image side group.
  • 4. A variable magnification optical system according to claim 1, wherein the focusing group comprises at least one positive lens and the following conditional expression is satisfied: 58.00<νFPwhere νFP denotes an Abbe number for d-line (wavelength 587.6 nm) of the positive lens.
  • 5. A variable magnification optical system, comprising: a first lens group disposed at a most object side and having positive refractive power;an intermediate group disposed at an image side of the first lens group and having negative refractive power;a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing; andan image side group disposed at an image side of the focusing group and having positive refractive power;upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group being varied;the image side group comprising, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)<2.80where fA denotes a focal length of the A group, and fB denotes a focal length of the B group; andthe following conditional expression being satisfied: 0.492≤ff/fi<1.10where ff denotes a focal length of the focusing group, and fi denotes a focal length of the image side group.
  • 6. A variable magnification optical system according to claim 5, wherein the following conditional expression is satisfied: 2.50<f1/(−fc)<6.20where f1 denotes a focal length of the first lens group, and fc denotes a focal length of the intermediate group.
  • 7. A variable magnification optical system according to claim 5, wherein the following conditional expression is satisfied: 1.80<fi/(−fB)<5.20.
  • 8. A variable magnification optical system according to claim 5, wherein the focusing group comprises at least one positive lens and the following conditional expression is satisfied: 58.00<νFPwhere νFP denotes an Abbe number for d-line (wavelength 587.6 nm) of the positive lens.
  • 9. A variable magnification optical system, comprising: a first lens group disposed at a most object side and having positive refractive power;an intermediate group disposed at an image side of the first lens group and having negative refractive power;a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing; andan image side group disposed at an image side of the focusing group and having positive refractive power;upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group being varied; andthe image side group comprising, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)≤1.836where fA denotes a focal length of the A group, and fB denotes a focal length of the B group.
  • 10. A variable magnification optical system according to claim 9, wherein the following conditional expression is satisfied: 2.50<f1/(−fc)<6.20where f1 denotes a focal length of the first lens group, and fc denotes a focal length of the intermediate group.
  • 11. A variable magnification optical system according to claim 9, wherein the following conditional expression is satisfied: 0.25<ff/fi<1.10where ff denotes a focal length of the focusing group, and fi denotes a focal length of the image side group.
  • 12. A variable magnification optical system according to claim 9, wherein the following conditional expression is satisfied: 1.80<fi/(−fB)<5.20where fi denotes a focal length of the image side group.
  • 13. A variable magnification optical system according to claim 9, wherein the focusing group comprises at least one positive lens and the following conditional expression is satisfied: 58.00<νFPwhere νFP denotes an Abbe number for d-line (wavelength 587.6 nm) of the positive lens.
  • 14. A method for manufacturing a variable magnification optical system, comprising steps of: arranging a first lens group disposed at a most object side and having positive refractive power, an intermediate group disposed at an image side of the first lens group and having negative refractive power, a focusing group disposed at an image side of the intermediate group and having positive refractive power, the focusing group being moved upon focusing, and an image side group disposed at an image side of the focusing group and having positive refractive power;the arrangement being such that, upon varying magnification, a distance between the first lens group and the intermediate group, a distance between the intermediate group and the focusing group and a distance between the focusing group and the image side group are varied; andthe method further comprising at least one or more of the following features (A), (B) and (C):(A) configuring the image side group to comprise, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)<2.80where fA denotes a focal length of the A group, and fB denotes a focal length of the B group, andsatisfying the following conditional expression: 2.50<f1/(−fc)≤4.365where f1 denotes a focal length of the first lens group, and fc denotes a focal length of the intermediate group;(B) configuring the image side group to comprise, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)<2.80where fA denotes a focal length of the A group, and fB denotes a focal length of the B group, and satisfying the following conditional expression: 0.492≤ff/fi<1.10where ff denotes a focal length of the focusing group, and fi denotes a focal length of the image side group;(C) configuring the image side group to comprise, in order from an object side, an A group having positive refractive power, a B group satisfying the following conditional expression with respect to the A group and having negative refractive power, and a C group: 1.67<fA/(−fB)≤1.836where fA denotes a focal length of the A group, and fB denotes a focal length of the B group.
Priority Claims (1)
Number Date Country Kind
2015-185502 Sep 2015 JP national
Divisions (1)
Number Date Country
Parent 15759829 Apr 2018 US
Child 16900321 US