JP2008146016A - Zoom lens and electronic imaging apparatus using the same - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a zoom lens that is advantageous to both achievement of a higher varying magnification ratio and a compact zoom lens. <P>SOLUTION: The zoom lens is a four-unit zoom lens including, in order from an object side, a first lens unit G1 having a positive refractive power, a second lens unit G2 having a negative refractive power, a third lens unit G3 having a positive refractive power, and a fourth lens unit G4 having a positive refractive power, in which at a time of zooming from a wide angle end to a telephoto end, a space between the lens units changes, the first lens unit G1 includes not more than two lenses, the number of positive lenses in the first lens unit G1 is one, a total number of lenses in the second lens unit G2 is not more than three. The zoom lens system satisfies following conditional expressions: (1) 1.2<(β<SB>2t</SB>/β<SB>2w</SB>)/(β<SB>3t</SB>/β<SB>3w</SB>)<2.3 and (2) 3.0<f<SB>t</SB>/f<SB>w</SB><12.0. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

  The present invention relates to a zoom lens and an electronic imaging apparatus using the same. In particular, the present invention relates to an electronic imaging device such as a video camera or a digital camera that has been downsized.

  In recent years, digital cameras that shoot a subject using a solid-state imaging device such as a CCD or CMOS instead of a silver salt film camera have become mainstream. Furthermore, it has come to have a number of categories in a wide range from high-functional types for business use to compact popular types.

  Users of popular digital cameras have a desire to enjoy shooting in a wide range of scenes anytime and anywhere. For this reason, small cameras, in particular, digital cameras that are easy to carry in clothes and bags, and that are easy to carry, are thin in the thickness direction. On the other hand, a zoom ratio of a compact type digital camera is generally about 3 times, but a camera with a higher zoom ratio than before has been demanded in order to further widen a photographing area.

  Recently, a so-called collapsible lens barrel is generally used in which the lens barrel protrudes from the body and is housed in the body when the imaging apparatus is in use. Therefore, it is important to configure the zoom lens optical system in consideration of the thinning of the lens barrel when retracted. As a conventional technique, a four-unit zoom lens type including a first lens unit having a positive refractive power, a second lens group having a negative refractive power, a third lens group having a positive refractive power, and a fourth lens group having a positive refractive power from the object side. A compact zoom lens configured as described above is known, for example, from Patent Document 1.

  The zoom lens disclosed in Japanese Patent Application Laid-Open No. 2005-151867 is advantageous in reducing the size of the zoom lens in the radial direction because the first lens group is composed of two or less lenses and the second lens group is composed of three lenses. Yes. In addition, the number of constituent lenses is small, which is advantageous for downsizing. In the above-described prior art, a device is devised to reduce the thickness direction of the group by reducing the number of lenses in each lens group.

  In particular, in the first and second lens groups, the height of the off-axis light beam from the optical axis is high, so that when the necessary amount of the edge of the lens is to be secured, the on-axis thickness tends to be very large. Furthermore, as the number of lenses in the first and second lens groups increases, the entrance pupil position becomes farther when viewed from the object side, so that the height of off-axis rays passing through the first and second lens groups becomes higher, and the edge is secured. Therefore, the thickness on the shaft is required to be thicker. Naturally, the axial thickness increases as the number of lenses increases.

  Therefore, as the number of lenses is increased, the size in the radial direction of the lens group and the thickness on the optical axis become larger than necessary, and the lens barrel cannot be made sufficiently compact even if the lens barrel is retracted. From such a point of view, it is advantageous for making the lens barrel compact that the first lens group and the second lens group have a small number of lenses.

JP 2006-23531 A

However, the disclosed prior art has the following problems. In the zoom lens disclosed in Patent Document 1 of the prior art, the zooming load of the third lens group is relatively large relative to the zooming load of the second lens group. The amount of movement of the third lens group with respect to the image plane up to is large. Therefore, when each lens group is retracted, the thickness direction of the cam for moving the lens group becomes larger than necessary, which is disadvantageous for achieving both a high zoom ratio and compactness. It has become.

In addition, since the air gap between the second lens group and the third lens group at the wide-angle end is relatively long, and as a result, the height of light rays to the first lens group and the second lens group becomes relatively high, the first, The two lens groups have a configuration in which it is difficult to sufficiently achieve the function of reducing the outer diameter and thickness of the two lens groups.
In addition, the difference in shape between the object side surface and the image side surface of the lens with an aspherical surface is large, and the optical performance deteriorates when the lens surface is installed in the opposite direction when the lens is installed in the lens frame. It tends to occur.

  The present invention has been made in view of such problems, and a first object thereof is to provide a zoom lens that is advantageous for achieving both a high zoom ratio and a compact size. A second object is to provide a zoom lens that is advantageous in reducing the size of the first and second lens units.

Furthermore, it aims at providing the zoom lens which achieves the above-mentioned objective simultaneously. Another object is to provide a zoom lens that can achieve any one or more of downsizing, high zoom ratio, low cost, ensuring optical performance, etc., or by simultaneously devising each lens group and moving method. Is. Furthermore, it aims at providing the electronic imaging device provided with such a zoom lens.
It is a third object of the present invention to provide a zoom lens that can easily reduce deterioration in optical performance due to a wrong lens assembly when the zoom lens is assembled.

  In order to solve the above-described problem and achieve the first object, the first zoom lens includes, in order from the object side, a first lens group having a positive refractive power and a second lens having a negative refractive power. A four-group zoom lens having a group, a third lens group having a positive refractive power, and a fourth lens group having a positive refractive power, and at least the first zoom lens when zooming from the wide-angle end to the telephoto end The lens group, the second lens group, and the third lens group move to change the distance between the lens groups, and the second lens group includes three or less lenses, and satisfies the following conditional expression.

1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <6.0 (1A)
3.0 < _ft / _fw <20.0 (2A)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

The reason and effect | action which took the said structure in the 1st zoom lens are demonstrated. In the present invention, in order to achieve the zoom ratio of the conditional expression (2A) that falls within the range of zoom ratios with high user needs, in order from the object side, a positive first lens group, a negative second lens group, The third lens group and the positive fourth lens group are used, and the zooming is performed by changing the interval between the groups.
By adopting such a configuration, it is possible to reduce the aberration fluctuation at the time of zooming by efficiently sharing the burden of zooming to each group and to prevent the movement amount of each group from increasing. It leads to compactness. Further, with the four-group configuration, it is easier to suppress the movement amount of the specific lens group from becoming too large compared to the case where the number of groups is small. Further, it is advantageous to reduce the number of lens barrels as compared with the case where the number of groups is large.

In order to reduce the size of the retracted lens barrel with this configuration, it is first necessary to reduce the thickness in the depth direction when the lens is retracted. For this purpose, the zoom lens must be constructed by distributing the movement amount of each lens group in a balanced manner in consideration of the optical performance.
Therefore, by moving at least the first lens group, the second lens group, and the third lens group at the time of zooming, the size in the depth direction of the frame for moving the lens group can be easily approached, and the thickness direction when the zoom lens is retracted It is advantageous to secure a zoom ratio while suppressing the size.
Furthermore, the amount of movement of the third lens group, which has been large from the wide-angle end to the telephoto end in the prior art, is reduced, and instead a variable magnification load is secured due to a change in the distance between the first and second lens groups. This greatly contributes to high zoom ratio and compactness.

Avoiding exceeding the upper limit of conditional expression (1A), suppressing an excessive excess of the zooming burden of the second lens group, generating aberrations due to power increase, particularly axes such as field curvature and lateral chromatic aberration at the telephoto end. It is preferable to suppress the occurrence of various external aberrations.
In order not to fall below the lower limit of conditional expression (1A), the size of the lens barrel is increased by increasing the amount of movement of the third lens unit, and aberration is generated by increasing the power of the third lens unit, particularly spherical aberration at the telephoto end. It is preferable to suppress the occurrence of on-axis aberrations.

Instead of the conditional expression (1A), the following conditional expression (1) may be satisfied.
Conditional expressions (1 ′) and (1 ″), which will be described later, may be further limited by limiting the numerical range.
Instead of conditional expression (2A), conditional expression (2) described later may be satisfied.
Conditional expressions (2 ′) and (2 ″), which will be described later, may be further limited by limiting the numerical range.

  Furthermore, it is preferable that the second zoom lens is the first zoom lens, wherein the first lens group includes two or less lenses, and the number of positive lenses in the first lens group is only one. Thereby, the thickness and diameter size of the first lens group can be reduced, which is advantageous for downsizing.

  In order to solve the above-described problem and achieve the first object, the third zoom lens includes, in order from the object side, a first lens group having a positive refractive power and a first lens group having a negative refractive power. A four-group zoom lens having a two-lens group, a third lens group having a positive refractive power, and a fourth lens group having a positive refractive power, and at the time of zooming from the wide-angle end to the telephoto end, The distance between the lens groups changes, the first lens group is composed of two or less lenses, the positive lens in the first lens group is only one lens, and the second lens group is three or less lenses. And satisfies the following conditional expression.

1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <2.3 (1)
3.0 < _ft / _fw <12.0 (2)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  The reason and effect | action which took the said structure in the 3rd zoom lens are demonstrated. In the present invention, in order to achieve the zoom ratio of the conditional expression (2), in order from the object side, a positive first lens group, a negative second lens group, a positive third lens group, and a positive fourth lens group And adopting a configuration in which zooming is performed by changing the interval between each group.

  By adopting such a configuration, it is possible to reduce the aberration fluctuation at the time of zooming by efficiently sharing the burden of zooming to each group and to prevent the movement amount of each group from increasing. It leads to compactness. Further, with the four-group configuration, it is easier to suppress the movement amount of the specific lens group from becoming too large compared to the case where the number of groups is small. Further, it is advantageous to reduce the number of lens barrels as compared with the case where the number of groups is large.

  In order to reduce the size of the retracted lens barrel with this configuration, it is first necessary to reduce the thickness in the depth direction when the lens is retracted. For this purpose, the zoom lens must be constructed by distributing the movement amount of each lens group in a balanced manner in consideration of the optical performance. Therefore, the movement amount of the third lens group, which has been large in the movement amount from the wide-angle end to the telephoto end in the prior art, is reduced, and instead, a variable magnification burden due to a change in the distance between the first and second lens groups is secured. This greatly contributes to high zoom ratio and compactness.

  By avoiding exceeding the upper limit of conditional expression (1), it is possible to suppress an excessive zooming burden on the second lens unit, and to generate aberrations due to power increase, especially off-axis various factors such as field curvature and lateral chromatic aberration at the telephoto end. It is preferable to suppress the occurrence of aberration.

  The lens size is increased by increasing the amount of movement of the third lens unit, and aberrations are generated by increasing the power of the third lens unit, particularly spherical aberration at the telephoto end so as not to fall below the lower limit of conditional expression (1). It is preferable to suppress the occurrence of on-axis aberrations.

It is better to satisfy the following.
1.3 <(β _2t / β _2w ) / (β _3t / β _3w ) <2.0 (1 ′)
It is even better to satisfy the following.
1.5 <(β _2t / β _2w ) / (β _3t / β _3w ) <1.9 (1 ″)
As a result, the above-described effects can be further achieved.

  In addition, it is preferable not to fall below the lower limit of the conditional expression (2), and it is preferable to secure a zoom ratio. To prevent the upper limit of the conditional expression (2) from being exceeded, the aberration correction burden on each group is suppressed. Is preferred.

It is better to satisfy the following.
5.0 <f _t / f _w <10.0 (2 ′)
It is even better to satisfy the following.
6.0 < _ft / _fw <8.0 (2 ")
As a result, the above-described effects can be further achieved.

  In order to achieve the second object, the fourth zoom lens includes, in order from the object side, a first lens group having a positive refractive power, a second lens group having a negative refractive power, and a positive refraction. A third lens group having a power and a fourth lens group having a positive refractive power, and when changing the magnification from the wide-angle end to the telephoto end, the distance between the lens groups changes, and the first lens group changes. One lens group consists of two lenses, a negative lens and a positive lens, and satisfies the following conditional expression.

0.20 <D _2w / f _t <0.35 (3)
However,
D _2w is the air spacing on the optical axis between the second lens group and the third lens group at the wide-angle end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  Hereinafter, the reason and effect | action which took the said structure in the 4th zoom lens are demonstrated. In the present invention, in order to easily secure the zoom ratio, in order from the object side, a positive first lens group, a negative second lens group, a positive third lens group, and a positive fourth lens group are provided. A configuration in which zooming is performed by changing the interval between each group was adopted. By adopting such a configuration, it is possible to reduce the aberration fluctuation at the time of zooming by efficiently sharing the burden of zooming to each group and to prevent the movement amount of each group from increasing. It leads to compactness.

  By preventing the upper limit of conditional expression (3) from being exceeded, the increase in the total length at the wide-angle end is suppressed, and the height of light incident on the first lens group and the second lens group is suppressed, so that the first lens group and the second lens group The lens diameter of the lens group can be reduced and the thickness can be easily reduced to secure the edge, which is advantageous for reducing the size of the zoom lens and reducing the thickness when retracted.

  By making sure that the lower limit of conditional expression (3) is not exceeded, an increase in power (refractive power) of each group at the time of high zooming is suppressed, and it becomes easy to correct aberrations such as spherical aberration.

It is better to satisfy the following.
_{0.25 <D 2w / f t <} 0.34 ··· (3 ')
It is even better to satisfy the following.
_{0.28 <D 2w / f t <} 0.33 ··· (3 ")
As a result, the above-described effects can be further achieved.

  Moreover, it is preferable to secure the zoom ratio and achieve the following configuration while achieving the second object described above. For this reason, it is preferable that the fifth zoom lens satisfies the following conditional expression in the first, second, or fourth zoom lens.

3.0 < _ft / _fw <12.0 (2)
However,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

It is better to satisfy the following.
5.0 <f _t / f _w <10.0 (2 ′)
It is even better to satisfy the following.
6.0 < _ft / _fw <8.0 (2 ")
As a result, the above-described effects can be further achieved.

  In order to achieve the achievement of the first object and the second object, it is more preferable to adopt the following configuration. For this reason, it is preferable that the sixth zoom lens satisfies the following conditional expression in the first, second, or fifth zoom lens.

1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <2.3 (1)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
It is.

  Further, it is preferable that the seventh zoom lens includes an aperture stop that moves integrally with the third lens group in the first to sixth zoom lenses. Thereby, the configuration for moving the stop can be simplified, and it is effective for both adjusting the exit pupil and reducing the diameters of the first and second lens groups.

  In addition to the above-described configuration, the following configuration is more preferable in order to make it easier to reduce the size, increase the zoom ratio, and ensure optical performance.

  The power of the first lens group is preferably configured as follows. For this reason, it is preferable that the eighth zoom lens satisfies the following conditional expressions in the first to seventh zoom lenses.

_{0.40 <f 1 / f t <} 0.90 ··· (4)
However,
f ₁ is the focal length of the first lens group,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By making sure that the upper limit of conditional expression (4) is not exceeded, the power of the first lens group is secured, and the change in the overall length of the entire zoom lens system is suppressed, which is advantageous for downsizing of the lens barrel. In addition, even if the power of the second lens group is suppressed, it is easy to ensure a variable magnification burden in the second lens group, which is advantageous for reducing aberrations and reducing the size of the second lens group.

  By making sure that the lower limit of conditional expression (4) is not exceeded, the power of the first lens group can be suppressed, the occurrence of spherical aberration and coma at the telephoto end can be suppressed, and good optical performance can be easily secured.

It is better to satisfy the following.
_{0.50 <f 1 / f t <} 0.80 ··· (4 ')
It is even better to satisfy the following.
_{0.55 <f 1 / f t <} 0.70 ··· (4 ")
As a result, the above-described effects can be further achieved.

  The power of the second lens group is preferably as follows. For this reason, it is preferable that the ninth zoom lens satisfies the following conditional expression in the first to eighth zoom lenses.

0.10 <| f ₂ / f _t | <0.20 (5)
However,
f ₂ is the focal length of the second lens group,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By ensuring that the upper limit of conditional expression (5) is not exceeded, the power of the second lens group is secured, the amount of change in the distance between the lens groups for zooming is suppressed, and this is advantageous for making the lens barrel compact. Further, even if the power of the first lens group is suppressed, it becomes easy to obtain a variable magnification burden, which is advantageous in reducing the occurrence of aberrations in the first lens group.

  By making sure that the lower limit of conditional expression (5) is not exceeded, the refractive power is moderately suppressed and the occurrence of aberrations can be easily suppressed. Further, it is possible to suppress the vertical magnification from becoming too small, and it is advantageous for securing a zoom ratio with respect to the interval change amount.

It is better to satisfy the following.
0.12 <| f ₂ / f _t | <0.19 (5 ′)
It is even better to satisfy the following.
0.15 <| f ₂ / f _t | <0.18 (5 ″)
As a result, the above-described effects can be further achieved.

The power of the third lens group is preferably as follows. For this reason,
The tenth zoom lens preferably satisfies the following conditional expressions in the first to ninth zoom lenses.

0.10 <f ₃ / _ft <0.30 (6)
However,
f ₃ is the focal length of the third lens group,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By making sure that the upper limit of conditional expression (6) is not exceeded, it is easy to secure the power and suppress the amount of change in the group interval for zooming.

  By making sure that the lower limit of conditional expression (6) is not exceeded, it is easy to suppress the occurrence of aberrations in the third lens group. Further, it is possible to suppress the vertical magnification from becoming too small, and it is advantageous for securing a zoom ratio with respect to the interval change amount.

It is better to satisfy the following.
0.15 <f ₃ / _ft <0.28 (6 ′)
It is even better to satisfy the following.
0.20 <f ₃ / _ft <0.25 (6 ″)
As a result, the above-described effects can be further achieved.

  The power of the fourth lens group is preferably as follows. For this reason, it is preferable that the eleventh zoom lens satisfies the following conditional expressions in the first to tenth zoom lenses.

_{0.10 <f 4 / f t <} 0.70 ··· (7)
However,
f ₄ is the focal length of the fourth lens group,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By making sure that the upper limit of conditional expression (7) is not exceeded, the power of the fourth lens group can be secured, and insufficient correction of astigmatism and distortion in the entire zoom region can be suppressed.

  By making sure that the lower limit of conditional expression (7) is not exceeded, the power of the fourth lens group can be moderately suppressed, and astigmatism and distortion overcorrection in the entire zoom range can be suppressed.

It is better to satisfy the following.
0.30 <f ₄ / _ft <0.65 (7 ′)
It is even better to satisfy the following.
_{0.45 <f 4 / f t <} 0.60 ··· (7 ")
As a result, the above-described effects can be further achieved.

  The fourth lens group may be formed of a plastic material. In particular, a single lens configuration is preferable. When an electronic image sensor such as a CCD or CMOS is used, it is preferable that the fourth lens group be provided with a function of efficiently placing light rays on the image sensor by arranging the exit pupil position at an appropriate position. In order to fulfill such a function, a relatively large power is not required if the power is set within the range of the conditional expression (7) described above, and a glass material having a low refractive index such as a plastic lens is used. It is also possible to configure by using.

  In addition, if a plastic lens is used for the fourth lens group, the cost can be reduced and a cheaper zoom lens can be provided.

  Moreover, it is preferable that the first lens group has the following configuration. Therefore, the twelfth zoom lens is a biconvex cemented lens in which the first lens group in the first to eleventh zoom lenses is composed of two lenses of a negative lens and a positive lens in order from the object side. Preferably there is.

  The reason and action of the above configuration in the twelfth zoom lens will be described. It is easy to secure the power of the first lens group, and it is easy to suppress spherical aberration near the telephoto end by placing positive power on both the object side and the image side. In addition, by using a cemented lens including a negative lens, it is easy to correct various aberrations and to suppress the influence of decentration.

  Furthermore, it is preferable that the thirteenth zoom lens satisfies the following conditional expression in the twelfth zoom lens.

38.0 <ν _d1p −ν _d1n (8)
However,
ν _d1p is the Abbe number for the d-line of the positive lens in the first lens group,
ν _d1n is the Abbe number for the d-line of the negative lens in the first lens group,
It is.

  Conditional expression (8) is a conditional expression regarding correction of axial chromatic aberration and correction of lateral chromatic aberration. In order to satisfactorily correct chromatic aberration caused by the large positive power of the first lens group, it is preferable to use a material having a small color dispersion for the positive lens and a material having a large color dispersion for the negative lens. Specifically, it is preferable that the conditional expression (8) that defines the difference between the Abbe numbers of the two lenses is satisfied.

  By making sure that the lower limit of conditional expression (8) is not exceeded, chromatic aberration can be corrected satisfactorily, which is advantageous in securing a zoom ratio.

It is better to satisfy the following.
47.0 <ν _d1p −ν _d1n (8 ′)
It is even better to satisfy the following.
58.0 <ν _d1p −ν _d1n (8 ″)
As a result, the above-described effects can be further achieved.

  The positive lens of the first lens group is preferably configured as follows. Therefore, it is preferable that the fourteenth zoom lens satisfies the following conditional expression in the second to thirteenth zoom lenses.

62.0 <ν _d1p <95.0 (9)
However,
ν _d1p is the Abbe number of the positive lens in the first lens group with respect to the d-line,
It is.

  By avoiding exceeding the upper limit of conditional expression (9), mass production and acquisition of materials become easy, which is advantageous for cost reduction.

By making sure that the lower limit of conditional expression (9) is not exceeded, chromatic dispersion is suppressed, which is advantageous in reducing chromatic aberration.

It is better to satisfy the following.
65.0 <ν _d1p <93.0 (9 ′)
It is even better to satisfy the following.
80.0 <ν _d1p <90.0 (9 ″)
As a result, the above-described effects can be further achieved.

  The fifteenth zoom lens includes a positive lens having a convex object side surface on the most object side in the third lens group and satisfying the following conditional expression in the first to fourteenth zoom lenses. Is preferred.

62.0 <ν _d3p <95.0 (10)
However,
ν _d3p is the Abbe number for the d-line of the positive lens in the third lens group,
It is.

  The reason and action of the fifteenth zoom lens having the above configuration will be described. The axial light beam diverging from the second lens group is incident on the third lens group. For this reason, the most object side lens of the third lens group is a positive lens convex toward the object side, and it is advantageous for downsizing the third lens group by converging the divergent light beam.

  By avoiding exceeding the upper limit of conditional expression (10), mass production and availability of the material become easy, which is effective for cost reduction.

  By making sure that the lower limit of conditional expression (10) is not exceeded, chromatic dispersion is suppressed, axial chromatic aberration is reduced, and good optical performance is easily obtained over the entire zoom range.

It is better to satisfy the following.
65.0 <ν _d3p <93.0 (10 ′)
It is even better to satisfy the following.
80.0 <ν _d3p <90.0 (10 ”)
As a result, the above-described effects can be further achieved.

  Moreover, when it has a negative lens in a 1st lens group, it is preferable to set it as the following structures. Therefore, in the twelfth to fifteenth zoom lenses, the sixteenth zoom lens preferably includes a negative lens in which the first lens group satisfies the following conditional expression.

1.85 <n _d1n <2.10 (11)
However,
n _d1n is the refractive index of the negative lens in the first lens group with respect to the d-line,
It is.

  By making so as not to exceed the upper limit of conditional expression (11), mass production and acquisition of materials become easy, which is advantageous for cost reduction.

  By making sure that the lower limit of conditional expression (11) is not exceeded, the absolute value of the curvature of the lens surface can be kept small even when the desired refractive power is obtained, and distortion, field curvature, wide-angle end, and telephoto at the wide-angle end are suppressed. The occurrence of coma and the like at the edge can be reduced.

It is better to satisfy the following.
1.90 <n _d1n <2.05 (11 ′)
It is even better to satisfy the following.
1.95 <n _d1n <2.05 (11 ″)
As a result, the above-described effects can be further achieved.

  The second lens group is more preferably configured as follows. Therefore, the seventeenth zoom lens includes a negative lens having a concave object side surface on the most object side in the second lens group and satisfying the following conditional expression in the first to sixteenth zoom lenses. It is preferable.

1.76 <n _d2n <2.00 (12)
However,
n _d2n is the refractive index of the negative lens in the second lens group with respect to the d-line,
It is.

  The reason and action of the 17th zoom lens will be described. By disposing the negative lens with the concave surface facing the object side closest to the object side of the second lens group, it is advantageous for reducing the thickness on the axis of the second lens group while ensuring the angle of view.

  At this time, since this negative lens has a high incident ray height in the second lens group, it is advantageous for correction of various off-axis aberrations to suppress an increase in curvature in this negative lens. By making so as not to exceed the upper limit of conditional expression (12), mass production and availability of materials become easy, which is advantageous for cost reduction. By making sure that the lower limit of conditional expression (12) is not exceeded, the absolute value of the curvature of the lens surface can be reduced even if the refractive power is secured, and distortion at the wide-angle end, curvature of field, the wide-angle end, and the telephoto end. It is easy to suppress the occurrence of coma aberration.

It is better to satisfy the following.
1.80 <n _d2n <1.95 (12 ′)
It is even better to satisfy the following.
1.83 <n _d2n <1.90 (12 ″)
As a result, the above-described effects can be further achieved.

  In addition, the eighteenth zoom lens includes a positive lens that satisfies the following conditional expression at the most image side or second from the image side in the second lens group in the first to seventeenth zoom lenses. It is preferable.

1.80 <n _d2p <2.15 (13)
However,
n _d2p is the refractive index of the positive lens in the second lens group with respect to the d-line,
It is.

  The reason and action of the above configuration in the 18th zoom lens will be described. Disposing the positive lens closest to the image side or the second from the image side in the second lens is advantageous in reducing aberrations that are likely to occur in the negative second lens group and in downsizing by adjusting the principal point. Become.

  By making so as not to exceed the upper limit of conditional expression (13), mass production and acquisition of materials become easy, which is advantageous for cost reduction.

By making sure that the lower limit of conditional expression (13) is not exceeded, the absolute value of the curvature of the lens surface can be kept small even if the desired refractive power is obtained, and distortion, field curvature, wide-angle end, and telephoto at the wide-angle end. The occurrence of coma and the like at the edge can be reduced.

It is better to satisfy the following.
1.84 <n _d2p <2.10 (13 ′)
It is even better to satisfy the following.
1.90 <n _d2p <2.10 (13 ″)
As a result, the above-described effects can be further achieved.

  In the nineteenth zoom lens, it is preferable that, in the first to eighteenth zoom lenses, a biconcave negative lens that satisfies the following conditional expression is disposed closest to the object side in the second lens group.

−1.0 <SF _2n1 <0.8 (14)
However,
SF _2n1 = (R _2n1f + R _2n1r ) / (R _2n1f −R _2n1r )
R _2n1f is the paraxial radius of curvature of the object side surface of the negative lens disposed closest to the object side in the second lens group,
R _2n1r is a paraxial radius of curvature of the image side surface of the negative lens disposed closest to the object side in the second lens group,
It is.

  The reason and action of the nineteenth zoom lens will be described. Arranging the biconcave negative lens on the most object side in the second lens group is advantageous for securing the negative power of the second lens group and for reducing the diameter. In addition, the second lens group can be easily brought close to the first lens group, which is advantageous for the overall length at the wide-angle end and the size reduction at the time of retracting.

  By making sure that the upper limit of conditional expression (14) is not exceeded, it is possible to prevent the absolute value of the curvature of the image side surface from becoming too large even if the power of the negative lens is ensured, and particularly distortion aberration and field curvature at the wide-angle end. It becomes easy to suppress the occurrence of off-axis aberrations.

  By making sure that the lower limit of conditional expression (14) is not exceeded, it is possible to suppress the absolute value of the curvature of the object side surface from becoming too large, and to easily suppress the occurrence of coma and astigmatism at the wide-angle end.

It is better to satisfy the following.
−0.8 <SF _2n1 <0.7 (14 ′)
It is even better to satisfy the following.
−0.5 <SF _2n1 <0.5 (14 ″)
As a result, the above-described effects can be further achieved.

  Further, in the case where the second lens group includes a positive lens and a negative lens in addition to the most object side negative lens, the following configuration may be employed. For this reason, in the twentieth zoom lens, in the nineteenth zoom lens, the second lens group includes a positive lens and a negative lens on the image side of the biconcave negative lens. It is preferable to satisfy the following conditional expression.

−1.0 <SF _2n1 <0.0 (14 ′ ″)

  The reason and action of the twentieth zoom lens having the above configuration will be described. The negative lens on the object side and the two lenses that follow it are advantageous in improving optical performance, and it is preferable because both high performance and downsizing can be improved.

  By not exceeding the upper limit of the conditional expression (14 '' '), it is advantageous to suppress the thickness of the second lens group on the optical axis.

  By making sure that the lower limit of the conditional expression (14 '' ') is not exceeded, an increase in the absolute value of the curvature of the concave surface on the object side is suppressed, which is advantageous in securing optical performance.

  In the 21st zoom lens, it is preferable that the following conditional expressions are satisfied in the 2nd to 20th zoom lenses.

−0.8 <SF _1p <−0.1 (15)
However,
SF _1p = as defined in _{(R 1pf + R 1pr) /} (R 1pf -R 1pr),
R _1pf is the paraxial radius of curvature of the object side surface of the positive lens in the first lens group,
R _1pr is the paraxial radius of curvature of the image side surface of the positive lens in the first lens group,
It is.

  By making sure that the upper limit of conditional expression (15) is not exceeded, it becomes advantageous for correction of aberrations such as field curvature occurring on the side surface of the lens image on the wide-angle end side.

  On the other hand, by making sure that the lower limit of conditional expression (15) is not exceeded, it is advantageous for correction of spherical aberration on the telephoto end side, which is advantageous for increasing the zoom ratio. In addition, the principal point position of the first lens group can be prevented from being on the object side, the distance between the principal points of the first lens group and the second lens group can be made closer at the wide angle end, and a desired angle of view can be ensured. It becomes easy to lower the beam height. Therefore, even if the edge of the lens of the first lens unit is secured, the axial thickness can be reduced, which is advantageous for downsizing.

It is better to satisfy the following.
−0.75 <SF _1p <−0.11 (15 ′)
It is even better to satisfy the following.
−0.35 <SF _1p <−0.13 (15 ″)
As a result, the above-described effects can be further achieved.

  The zooming action of the second lens group may be configured as follows. For this reason, it is preferable that the 22nd zoom lens satisfies the following conditional expressions in the 1st to 21st zoom lenses.

2.6 <β _2t / β _2w <6.0 (16)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
It is.

  It is preferable not to exceed the upper limit of conditional expression (16) to suppress the occurrence of aberrations due to the increase in power of the second lens group, particularly the occurrence of various off-axis aberrations such as field curvature and lateral chromatic aberration at the telephoto end. .

It is preferable not to fall below the lower limit of conditional expression (16) to reduce the burden of zooming on other lens units. Suppressing the variable magnification load of the third lens group is advantageous in reducing the occurrence of axial aberrations such as spherical aberration at the telephoto end. In addition, by suppressing the variable magnification of the fourth lens group, it is possible to moderately suppress the power of the fourth lens group and to suppress excessive correction of astigmatism in the entire region.

It is better to satisfy the following.
2.6 <β _2t / β _2w <5.0 (16 ′)
It is even better to satisfy the following.
2.9 <β _2t / β _2w <3.5 (16 ″)
As a result, the above-described effects can be further achieved.

  In addition, regarding the zooming action of the third lens group, the following configuration is preferable. For this reason, it is preferable that the 23rd zoom lens satisfies the following conditional expressions in the 1st to 22nd zoom lenses.

1.2 <β _3t / β _3w <3.0 (17)
However,
β _2w is the lateral magnification at the wide-angle end of the third lens group,
β _2t is the lateral magnification at the telephoto end of the third lens group,
It is.

  By not exceeding the upper limit of conditional expression (17), it becomes easy to suppress the occurrence of aberrations due to the increase in power of the third lens group, especially the occurrence of axial aberrations such as spherical aberration at the telephoto end.

  It is preferable to reduce the burden of zooming on other lenses by making sure that the lower limit of conditional expression (17) is not exceeded. Suppressing the zooming load of the second lens group is advantageous in reducing the occurrence of various off-axis aberrations such as field curvature and lateral chromatic aberration at the telephoto end, and suppressing the zooming burden of the fourth lens group. As a result, the power of the fourth lens group is moderately suppressed, and it becomes easy to suppress overcorrection of astigmatism in the entire region.

It is better to satisfy the following.
1.5 <β _3t / β _3w <2.5 (17 ′)
It is even better to satisfy the following.
1.7 <β _3t / β _3w <2.0 (17 ″)
As a result, the above-described effects can be further achieved.

  In addition, it is preferable to satisfy the following configuration with respect to the zooming action of the fourth lens group. For this reason, it is preferable that the 24th zoom lens satisfies the following conditional expressions in the 1st to 23rd zoom lenses.

0.7 <β _4t / β _4w <1.7 (18)
However,
β _4w is the lateral magnification at the wide-angle end of the fourth lens group,
β _4t is the lateral magnification at the telephoto end of the fourth lens group,
It is.

  The reason and action of the above configuration in the 24th zoom lens will be described. By giving the fourth lens group an appropriate zooming load, it becomes easy to suppress the zooming load of the second and third lens groups, which is advantageous in securing a zooming ratio while suppressing aberration fluctuations.

  By making so as not to exceed the upper limit of conditional expression (18), it is possible to suppress the variable magnification burden of the fourth lens group and to suppress aberrations. When the fourth lens group is a group that moves during forcing, it is advantageous to suppress fluctuations in field curvature during focusing.

  By making sure that the lower limit of conditional expression (18) is not exceeded, it is possible to reduce the variable magnification burden of other lens groups. Suppressing the variable magnification burden of the second lens group is advantageous in reducing the occurrence of various off-axis aberrations such as field curvature and lateral chromatic aberration at the telephoto end. In addition, by suppressing the variable magnification burden of the third lens group, it is advantageous for reducing the occurrence of axial aberrations such as spherical aberration, particularly at the telephoto end.

It is better to satisfy the following.
0.8 <β _4t / β _4w <1.5 (18 ′)
It is even better to satisfy the following.
1.0 <β _4t / β _4w <1.3 (18 ”)
As a result, the above-described effects can be further achieved.

  Also, with respect to the focal length of the entire system at the telephoto end, the air spacing on the optical axes of the second lens group and the third lens group at the wide angle end, and the optical axes of the first lens group and the second lens group at the telephoto end About the sum of the air space | interval above, it is good to set it as the following structures. For this reason, it is preferable that the 25th zoom lens satisfies the following conditional expressions in the 1st to 24th zoom lenses.

_{0.4 <(D 2w + D 1t} ) / f t <0.9 ··· (19)
However,
D _2w is the air spacing on the optical axis between the second lens group and the third lens group at the wide-angle end,
D _1t is the air spacing on the optical axis between the first lens group and the second lens group at the telephoto end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By not exceeding the upper limit of the conditional expression (19), the moving amount of the moving lens group can be suppressed, and the increase in the thickness of the lens barrel can be easily suppressed.

  By making sure that the lower limit of conditional expression (19) is not exceeded, the power of each lens unit can be suppressed while achieving a high zoom ratio, and aberration variations can be easily suppressed.

It is better to satisfy the following.
_{0.5 <(D 2w + D 1t} ) / f t <0.7 ··· (19 ')
It is even better to satisfy the following.
_{0.55 <(D 2w + D 1t} ) / f t <0.65 ··· (19 ")
As a result, the above-described effects can be further achieved.

  The air spacing on the optical axis of the second lens group and the third lens group at the wide-angle end with respect to the focal length of the entire system at the telephoto end may be configured as follows. For this reason, it is preferable that the 26th zoom lens satisfy the following conditional expressions in the 1st to 25th zoom lenses.

0.2 <D _1t / _ft <0.5 (20)
However,
D _1t is the air spacing on the optical axis between the first lens group and the second lens group at the telephoto end,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By not exceeding the upper limit of conditional expression (20), the total length at the telephoto end can be easily reduced, which is advantageous for reducing the size of the lens barrel in the thickness direction.

  By making sure that the lower limit of conditional expression (20) is not exceeded, the power of each lens group can be suppressed even when the zoom ratio is increased, and the occurrence of aberrations such as spherical aberration can be easily suppressed.

It is better to satisfy the following.
0.2 <D _1t / f _t <0.4 (20 ′)
It is even better to satisfy the following.
_{0.25 <D 1t / f t <} 0.35 ··· (20 ")
As a result, the above-described effects can be further achieved.

  The total length of the lens with respect to the focal length of the entire system at the telephoto end may be configured as follows. Therefore, it is preferable that the twenty-seventh zoom lens satisfies the following conditional expressions in the first to twenty-sixth zoom lenses.

0.7 < _TL / _ft <1.5 (21)
However,
T _L is the distance on the optical axis from the top of the lens surface closest to the object side of the first lens group at the telephoto end to the image plane,
f _t is the focal length of the entire zoom lens system at the telephoto end,
It is.

  By the above-described movement of the first lens group, it becomes easy to ensure the zooming effect in the second lens group and the like.

  By not exceeding the upper limit of conditional expression (21), it is possible to suppress the overall length of the zoom lens at the telephoto end, and to easily increase the size of the lens barrel in the thickness direction.

  By making sure that the lower limit of conditional expression (21) is not exceeded, the power of each lens unit can be suppressed even when the zoom ratio is increased, and the occurrence of aberrations such as spherical aberration can be easily suppressed.

It is better to satisfy the following.
0.9 < _TL / _ft <1.3 (21 ')
It is even better to satisfy the following.
1.0 < _TL / _ft <1.2 (21 ")
As a result, the above-described effects can be further achieved.

  The twenty-eighth zoom lens preferably has the following configuration in the first to eleventh zoom lenses. The first lens group is preferably composed of a cemented doublet in which a negative lens and a positive lens are cemented.

  The reason and action of the above configuration in the 28th zoom lens will be described. When the first lens group is a cemented lens of a negative lens and a positive lens, it is possible to effectively perform axial chromatic aberration correction that becomes conspicuous when the telephoto end has a long focal length due to high zoom ratio. In addition, it is possible to suppress the deterioration of the optical performance due to the relative eccentricity of the lens due to the assembly error, which contributes to the improvement of the yield and the cost reduction.

  When the negative lens and the positive lens in the first lens group are not cemented, it is advantageous to more effectively correct distortion aberration, coma aberration at the wide-angle end, and coma aberration at the telephoto end.

  The second lens group preferably has the following configuration. For this reason, in the 29th zoom lens, in the fourth zoom lens, it is preferable that the second lens group includes three or less lenses. This is advantageous in reducing the size and cost of the second lens group.

  Furthermore, in the 30th zoom lens, in the 1st to 29th zoom lenses, it is preferable that the second lens group includes a negative lens, a negative lens, and a positive lens in order from the object side.

  As a result, the negative power of the second lens group is shared by the two negative lenses, and the positive lens is arranged on the most image side, thereby correcting the initial aberration and shortening the overall length by using the main point as an object. It will be advantageous.

  Alternatively, the following configuration is preferable. In the 29th zoom lens, in the 1st to 27th zoom lenses, it is preferable that the second lens group includes a negative lens, a positive lens, and a negative lens in order from the object side.

  Thereby, it becomes easy to suppress the fluctuation | variation at the time of zooming of various aberrations, such as spherical aberration, by making a 2nd lens group into the lens arrangement | positioning symmetrically.

  Alternatively, the following configuration is preferable. In a thirty-second zoom lens, it is preferable that in the first to nineteenth zoom lenses, the second lens group includes two lenses, a negative lens and a positive lens. This is advantageous for downsizing the second lens group while suppressing aberrations in the second lens group.

  The third lens group preferably has the following configuration. Therefore, in the 33rd zoom lens, in the 1st to 32nd zoom lenses, it is preferable that the third lens group includes three or less lenses. This is advantageous for thinning the lens barrel.

  In particular, the following configuration is preferable. For this reason, in the thirty-fourth zoom lens, in the thirty-third zoom lens, the third lens group includes, in order from the object side, a positive lens, a positive lens, and a negative lens, and the negative lens is joined to the adjacent positive lens. In addition, it is preferable to form a bonded doublet.

  By joining the positive lens and the negative lens, the axial chromatic aberration can be corrected more effectively. Also, by dispersing the power of the positive lens between the two lenses and using the positive lens and the negative lens as a cemented lens, it is possible to prevent deterioration in optical performance due to the relative decentration of the lenses in the assembly process. Lead to improvement and cost reduction.

  The fourth lens group preferably has the following configuration. Therefore, in the thirty-fifth zoom lens, in the first to thirty-fourth zoom lenses, it is preferable that the fourth lens group includes one positive lens. This is advantageous for downsizing when retracted.

  When the zoom lens is a four-group zoom lens, the fourth lens group is the final lens group, but the function of moving the exit pupil away from the image plane is provided. This is advantageous for downsizing.

  Further, when the fourth lens group is configured to move during focusing, the driving load during focusing can be reduced by using one moving lens.

  In the thirty-sixth zoom lens, in the first to thirty-fifth zoom lenses, it is preferable that the first lens group has an aspheric lens surface. This is particularly advantageous for correcting spherical aberration that is likely to occur on the telephoto end side.

In the 37th zoom lens according to the 1st to 36th zoom lenses, it is preferable that the second lens group has an aspheric lens surface.

  The reason and action of the 37th zoom lens will be described. If an attempt is made to secure the zoom ratio while suppressing the total length, the change in the incident position of the light beam of the second lens group tends to be large. Arranging an aspherical surface in this lens group is advantageous for correcting off-axis aberrations at the wide-angle end.

  In the 38th zoom lens according to the 1st to 37th zoom lenses, it is preferable that the third lens group has an aspheric lens surface. This is advantageous for correcting spherical aberration and coma as a whole.

  In the thirty-ninth zoom lens, in the thirty-eighth zoom lens, it is preferable that a lens closest to the object side in the third lens group is a positive single lens having a double-sided aspheric surface.

  The reason and operation of the 39th zoom lens will be described. By making both side surfaces of one lens aspherical, it is possible to correct spherical aberration and coma aberration more satisfactorily while suppressing optical performance deterioration due to relative decentering between the lenses in the group.

  Moreover, it is preferable to set it as the following structures. Therefore, in the 40th zoom lens, in the 1st to 39th zoom lenses, it is preferable that the fourth lens group has an aspheric lens surface. This is advantageous for maintaining optical performance, such as correcting off-axis aberrations and reducing variations in exit pupil position.

  The forty-first zoom lens is the first to forty-first zoom lens, wherein the first lens group, the second lens group, the third lens group, and the fourth lens group move during zooming, and the third lens It is preferable to provide an aperture stop that is integrated with the group and moves in the optical axis direction.

  The reason and action of the above configuration in the forty-first zoom lens will be described. Each lens group is efficiently subjected to a zooming action, and it becomes easy to correct aberrations satisfactorily in the entire zooming region, which is advantageous for high zooming.

  In addition, by moving the aperture stop together with the third lens group, it is possible to effectively correct chromatic aberration of magnification and distortion, and not only have an effect on performance, but also the entrance pupil position and exit pupil position. It becomes possible to control appropriately. That is, the light beam height of the off-axis light beam at the wide-angle end and the light beam height of the off-axis light beam at the telephoto end can be balanced, and the outer diameter of the first lens group and the outer diameter of the fourth lens group are balanced and compact. It becomes possible to do. In particular, reducing the outer diameter of the first lens group at the wide-angle end effectively leads to a compact size in the lens thickness direction.

  In addition, since it becomes possible to control the variation of the exit pupil position at the time of zooming, when using a CCD, CMOS, etc., the incident light beam angle is kept within an appropriate range, and the angle at the corner of the screen is changed. It is possible to prevent the occurrence of brightness shading, which is suitable for an electronic imaging device. In addition, it is easy to suppress aberration variation due to the compactness of the third lens group and the movement of the third lens.

  Furthermore, the forty-second zoom lens moves in the forty-first zoom lens so that the first lens unit is closer to the object side at the telephoto end than at the wide-angle end when zooming from the wide-angle end to the telephoto end. It is preferable that the second lens group moves, the third lens group moves only to the object side, and the fourth lens group moves. As a result, the overall aberration balance can be easily adjusted while ensuring the zooming effect on the second lens group and the third lens group.

  In zooming from the wide-angle end to the telephoto end, it is preferable to move the first lens group so that it is closer to the object side at the telephoto end than at the wide-angle end. At that time, it may be moved only to the object side, or may be moved along a locus convex toward the image side. The second lens group may be moved only to the image side, or may be moved along a locus convex toward the image side.

  The third lens group is preferably moved only to the object side. The fourth lens group may be moved only to the object side or only to the image side. Alternatively, it may be moved along a locus convex toward the object side or convex toward the image side.

  In the forty-third zoom lens, in the forty-first zoom lens, upon zooming from the wide-angle end to the telephoto end, the first lens group first moves to the object side and moves the object at the telephoto end rather than the wide-angle end. The second lens group first moves to the object side, and the moving direction is reversed in the middle of zooming. The third lens group first moves to the object side and telephoto from the wide angle end. It is preferable that the fourth lens unit moves so as to be closer to the object side at the end, and so that the fourth lens group is closer to the image side at the telephoto end than at the wide angle end.

  When the first lens group, the second lens group, and the third lens group first move to the object side during zooming from the wide-angle end to the telephoto end, it is advantageous for shortening the overall length of the zoom lens at the wide-angle end. Then, the movement direction of the second lens group is reversed in the middle of zooming, and the first and third lens groups are moved as described above, thereby ensuring the zooming burden of the second and third lens groups and the first and third lens groups. This is advantageous in reducing the amount of movement of the second and third lens groups.

Further, by moving the fourth lens group so that it is closer to the image side at the telephoto end than at the wide-angle end, the fourth lens group can easily have a zooming function, and the amount of movement of the lens group that moves during zooming It is advantageous for reduction of
The first lens group may be moved only toward the object side, may be moved along a locus that is convex toward the object side, or may be moved so that the moving direction is reversed a plurality of times.
Further, if the second lens group is positioned closer to the image side at the telephoto end than at the wide-angle end, it is possible to increase the magnification burden of the second lens group and to easily suppress the movement amount of the third lens group.
The third lens group may be moved only to the object side, or the moving direction may be reversed once or a plurality of times.
The fourth lens group may be moved only to the image side, or may be moved along a locus convex toward the object side or convex toward the image side, or may be moved so as to reverse the movement direction a plurality of times. good.

  Further, in the forty-fourth zoom lens, in the 41st to 43rd zoom lenses, it is preferable that the brightness diaphragm is disposed between the second lens group and the third lens group.

  The reason and action of the above configuration in the 44th zoom lens will be described. The entrance pupil can be positioned close to the object side, and the exit pupil can be moved away from the image plane. At this time, it is more preferable to arrange the shutter units that move integrally with the aperture stop. Since the height of the off-axis light beam is low, the shutter unit does not need to be enlarged, and the dead space for moving the aperture stop and the shutter unit can be reduced.

  The 45th zoom lens is a fourth zoom lens, and the zoom lens includes the first lens group, the second lens group, the third lens group, and the fourth lens group in order from the object side. A four-group zoom lens is preferable. This is advantageous for downsizing.

  According to another aspect of the present invention, there is provided an electronic image pickup apparatus comprising: the above-described zoom lens; and an electronic image pickup device that is disposed on an image side of the zoom lens and converts an image formed by the zoom lens into an electric signal. To do.

  The zoom lens of the present invention is advantageous for ensuring telecentricity. Therefore, it is preferably used for an electronic imaging apparatus using an electronic imaging element that causes image degradation due to an incident angle.

  Moreover, in the case of such an electronic imaging device using an electronic imaging element, it is more preferable to have the following configuration. For this reason, it is preferable that the electronic imaging apparatus includes a processing unit that electrically corrects distortion aberration of the zoom lens based on an electrical signal from the electronic imaging element.

  Thereby, even if the zoom lens is configured in a small size, deterioration of the reproduced image can be suppressed, which is advantageous for downsizing the electronic imaging apparatus.

  In addition, about each above-mentioned invention, when providing a focusing function in a zoom lens, it is set as the structure in the state which focused on the object point of the longest distance. It is preferable to perform the focusing operation by moving the fourth lens group in the optical axis direction because it is easy to suppress variations in the exit pupil position.

For the third purpose, the 48th zoom lens is a double-sided aspheric lens in which both the object side surface and the image side surface have aspheric shapes, and the surface shapes of both surfaces satisfy the following conditional expression: It is characterized by having.
−0.1 <(R _aspO + R _aspI ) / (R _aspO −R _aspI ) <0.1 (22)
In the range of 0 ≦ y ≦ R,
−10 ⁻⁴ <(X _{O (y)} + X _{I (y)} ) / (R _aspO −R _aspI ) <10 ⁻⁴ (23)
However,
X _{O (R)} ≠ 0,
X _{I (R)} ≠ 0,
And
R _aspO is the paraxial radius of curvature of the object side surface of the double-sided aspheric lens,
R _aspI is the paraxial radius of curvature of the image side surface of the double-sided aspheric lens,
y is the distance from the optical axis,
R is the smaller value of the effective radii of the object side surface and the image side surface of the double-sided aspheric lens,
X _{O (y)} and X _{I (y)} are the aspherical deviation amounts at the distance y on the object side surface and the image side surface of the double-sided aspheric lens
It is.

In a double-sided aspherical lens, in the case of a double-sided aspherical lens that satisfies the conditional expression (22) and has close curvatures of the object-side surface and the image-side surface, both aspherical surfaces substantially satisfy the conditional expression (23). This shape can be reduced even when the front and rear surfaces are reversed in assembly.
If any one of the upper and lower limits of conditional expressions (22) and (23) is deviated, the optical performance tends to deteriorate when the front and rear surfaces are incorporated in reverse.
More preferably, the upper and lower limit values of conditional expression (22) are 0.05 and -0.05, respectively, and 0.02 and -0.02.
More preferably, the upper and lower limit values of conditional expression (23) are 10 ⁻⁵ and −10 ⁻⁵ , respectively, and 10 ⁻⁶ and −10 ⁻⁶ .

  As shown in FIG. 30, when the spherical surface having the same apex as that of the aspherical surface and having the paraxial curvature radius of the aspherical surface as the reference radius is used as the reference spherical surface, This is the distance from the reference spherical surface to the aspherical surface when measured in the parallel direction, and the image side direction (right direction in the figure) is a positive sign. Further, if both surfaces are aspherical surfaces having the same shape, there is an advantage that only one type of mold processing is required for aspherical mold processing. Furthermore, it is more preferable to use such a lens for the fourth lens group of any of the zoom lenses described above. Even if the fourth lens group is an aspherical lens having substantially the same shape on both sides, the optical performance can be maintained satisfactorily.

  More preferably, a plurality of the above-described inventions are satisfied at the same time. Moreover, it is good also as the lower limit value and upper limit value of the conditional expression which limited only the lower limit value and upper limit value of each conditional expression. Further, the above-described configurations may be arbitrarily combined.

As is apparent from the above description, according to the present invention, it is possible to provide a zoom lens that is advantageous for achieving both a high zoom ratio and a compact size. Alternatively, it is possible to provide a zoom lens that is advantageous for reducing the size of the first and second lens groups. Furthermore, it is possible to provide a zoom lens that simultaneously achieves the above-described object.

In addition, a zoom lens that can achieve any one of a reduction in size, a high zoom ratio, a reduction in cost, ensuring of optical performance, or a plurality of them simultaneously can be provided by devising each lens group, movement method, and the like. Furthermore, an electronic imaging device including such a zoom lens can be provided.
Alternatively, it is possible to provide a zoom lens that can easily reduce deterioration in optical performance due to a mistake in assembling the lens when the zoom lens is assembled.

  Embodiments of a zoom lens and an electronic imaging device according to the present invention will be described below in detail with reference to the drawings. Note that the present invention is not limited to the embodiments.

  Examples 1 to 9 of the zoom lens according to the present invention will be described below. FIGS. 1 to 9 show lens cross-sectional views of the wide-angle end (a), the intermediate state (b), and the telephoto end (c) when focusing on an object point at infinity in Examples 1 to 9, respectively. 1 to 9, the first lens group is G1, the second lens group is G2, the aperture stop is S, the third lens group is G3, the fourth lens group is G4, and a wavelength region limiting coat that limits infrared light. The parallel flat plate constituting the low-pass filter subjected to is indicated by F, the parallel flat plate of the cover glass of the electronic image sensor is indicated by C, and the image plane is indicated by I. In addition, you may give the multilayer film for a wavelength range restriction | limiting to the surface of the cover glass C. FIG. Further, the cover glass C may have a low-pass filter action.

  As shown in FIG. 1, the zoom lens of Example 1 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top of the tenth lens surface is located on the object side of the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 2, the zoom lens according to the second embodiment includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top of the tenth lens surface is located on the object side of the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 3, the zoom lens of Example 3 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top of the tenth lens surface is located on the object side of the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 4, the zoom lens of Example 4 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top surface of the tenth lens surface is located closer to the object side than the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 5, the zoom lens of Example 5 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top of the tenth lens surface is located on the object side of the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 6, the zoom lens of Example 6 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth negative meniscus lens having a convex surface facing the object side, and a fifth positive meniscus lens having a convex surface facing the object side. The third lens group G3 includes a sixth biconvex positive lens, a seventh positive meniscus lens having a convex surface directed toward the object side, and an eighth negative meniscus lens having a convex surface directed toward the object side. The seventh positive meniscus lens and the eighth negative meniscus lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens. Note that the top of the twelfth lens surface is located closer to the object side than the aperture stop S.

  The aspherical surface includes the image side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and the object side surface of the ninth biconvex positive lens. Used on six sides. The tenth surface is a virtual surface.

As shown in FIG. 7, the zoom lens of Example 7 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth biconvex positive lens, and a fifth biconcave negative lens. The third lens group G3 includes a sixth biconvex positive lens, a seventh positive meniscus lens having a convex surface directed toward the object side, and an eighth negative meniscus lens having a convex surface directed toward the object side. The seventh positive meniscus lens and the eighth negative meniscus lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens. Note that the top of the twelfth lens surface is located closer to the object side than the aperture stop S.

  The aspherical surface includes the image side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and the object side surface of the ninth biconvex positive lens. Used on six sides. The tenth surface is a virtual surface.

  As shown in FIG. 8, the zoom lens according to the eighth embodiment includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

  In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens and a fourth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a fifth biconvex positive lens, a sixth positive meniscus lens having a convex surface directed toward the object side, and a seventh negative meniscus lens having a convex surface directed toward the object side. The sixth positive meniscus lens and the seventh negative meniscus lens are cemented. The fourth lens group G4 is composed of an eighth biconvex positive lens. Note that the top of the tenth lens surface is located on the object side of the aperture stop S.

  The aspherical surface includes the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the fifth biconvex positive lens, and the object side surface of the eighth biconvex positive lens. Used on six sides. Further, the eighth surface is a virtual surface.

  As shown in FIG. 9, the zoom lens of Example 9 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 moves to the object side, the second lens group G2 once moves to the object side, and then the moving direction reverses and moves to the image side. The lens group G3 moves to the object side together with the aperture stop S, and the fourth lens group G4 moves to the image side.

In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth biconvex positive lens, and a fifth biconcave negative lens. The third lens group G3 includes a sixth biconvex positive lens, a seventh positive meniscus lens having a convex surface directed toward the object side, and an eighth negative meniscus lens having a convex surface directed toward the object side. The seventh positive meniscus lens and the eighth negative meniscus lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens. Note that the top of the twelfth lens surface is located closer to the object side than the aperture stop S.

  The aspherical surface includes the image side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and the object side surface of the ninth biconvex positive lens. Used on six sides. The tenth surface is a virtual surface.

  Further, Examples 10, 11, and 12 of the zoom lens according to the present invention will be described below. FIGS. 24, 25, and 26 are lens cross-sectional views of the wide-angle end (a), the intermediate state (b), and the telephoto end (c) when focusing on an object point at infinity according to Examples 10, 11, and 12, respectively. 24 to 26, the first lens group is G1, the second lens group is G2, the aperture stop is S, the third lens group is G3, the fourth lens group is G4, and the parallel plate is a parallel plate which is one member. Although indicated by C, this is a united representation of a low-pass filter, an IR cut coat, and a cover glass of the image sensor. The image plane is indicated by I.

As shown in FIG. 24, the zoom lens of Example 10 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.
The aperture stop S is disposed immediately before the third lens group G3 (the same position as the top of the lens surface on the most object side of the third lens group G3), and moves together with the third lens group G3.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 first moves to the image side after moving to the object side, and is positioned on the object side at the telephoto end with respect to the wide-angle end. The second lens group G2 first moves to the image side after moving to the object side, and is positioned on the image side at the telephoto end with respect to the wide angle end. The third lens group G3 first moves to the object side after moving to the object side, and is positioned on the object side at the telephoto end with respect to the wide angle end. The fourth lens group G4 moves to the image side. Focusing is performed by moving the fourth lens group.

In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth biconcave negative lens, and a fifth positive meniscus lens having a convex surface directed toward the object side. The third lens group G3 includes a sixth biconvex positive lens, a seventh biconvex positive lens, and an eighth biconcave negative lens. The seventh biconvex positive lens and the eighth biconcave negative lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens.

  The aspherical surface includes the image side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and the object side surface of the ninth biconvex positive lens. Used on six sides.

As shown in FIG. 25, the zoom lens of Example 11 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.
The aperture stop S is disposed immediately before the third lens group G3 (the same position as the top of the lens surface on the most object side of the third lens group G3), and moves together with the third lens group G3.

  At the time of zooming from the wide-angle end to the telephoto end, the first lens group G1 first moves to the image side after moving to the object side, and is positioned on the object side at the telephoto end with respect to the wide-angle end. The second lens group G2 first moves to the image side after moving to the object side, and is positioned on the image side at the telephoto end with respect to the wide angle end. The third lens group G3 first moves to the object side after moving to the object side, and is positioned on the object side at the telephoto end with respect to the wide angle end. The fourth lens group G4 moves to the image side. Focusing is performed by moving the fourth lens group.

In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth biconcave negative lens, and a fifth biconvex positive lens. The fourth biconcave negative lens and the fifth biconvex positive lens are cemented. The third lens group G3 includes a sixth biconvex positive lens, a seventh biconvex positive lens, and an eighth biconcave negative lens. The seventh biconvex positive lens and the eighth biconcave negative lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens.

  The aspherical surface includes the image side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and the object side surface of the ninth biconvex positive lens. Used on six sides.

As shown in FIG. 26, the zoom lens of Example 12 includes, in order from the object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, A third lens group G3 having a positive refractive power and a fourth lens group G4 having a positive refractive power are disposed.
The aperture stop S is disposed immediately before the third lens group G3 (the same position as the top of the lens surface on the most object side of the third lens group G3), and moves together with the third lens group G3.

  At the time of zooming from the wide angle end to the telephoto end, the first lens group G1 moves to the object side. The second lens group G2 first moves to the image side after moving to the object side, and is positioned on the image side at the telephoto end with respect to the wide angle end. The third lens group G3 first moves to the object side after moving to the object side, and is positioned on the object side at the telephoto end with respect to the wide angle end. The fourth lens group G4 moves to the image side. Focusing is performed by moving the fourth lens group.

In order from the object side, the first lens group G1 includes a first negative meniscus lens having a convex surface directed toward the object side, and a second biconvex positive lens. The first negative meniscus lens and the second biconvex positive lens are cemented. The second lens group G2 includes a third biconcave negative lens, a fourth biconcave negative lens, and a fifth planoconvex positive lens having a convex surface directed toward the object side. The fourth biconcave negative lens and the fifth planoconvex positive lens are cemented. The third lens group G3 includes a sixth biconvex positive lens, a seventh biconvex positive lens having a convex surface directed toward the object side, and an eighth plano-concave negative lens having a concave surface directed toward the image side. The seventh plano-convex positive lens and the eighth plano-concave negative lens are cemented. The fourth lens group G4 is composed of a ninth biconvex positive lens.

  The aspherical surface has seven surfaces: the image-side surface of the second biconvex positive lens, both surfaces of the third biconcave negative lens, both surfaces of the sixth biconvex positive lens, and both surfaces of the ninth biconvex positive lens. Used.

Below, the numerical data of each said Example are shown. Symbols are the above, f is the focal length of the entire system, _FNO is the F number, ω is the half field angle, WE is the wide angle end, ST is the intermediate state, TE is the telephoto end, r ₁ , r ₂ . radius of curvature, d _1, d ₂ ... the spacing between the lens surfaces, n _d1, n _d2 ... d-line refractive index of each lens, ν _d1, ν _d2 ... is the Abbe number of each lens. The aspherical shape is represented by the following expression, where x is an optical axis with the light traveling direction being positive, and y is a direction orthogonal to the optical axis.

x = (y ² / r) / [1+ {1- (K + 1) (y / r) ² } ^1/2 ]
+ A ₄ y ⁴ + A ₆ y ⁶ + A ₈ y ⁸ + A ₁₀ y ¹⁰ + A ₁₂ y ¹²
Where r is the paraxial radius of curvature, K is the conic coefficient, and A ₄ , A ₆ , A ₈ , A ₁₀ , and A ₁₂ are the fourth, sixth, eighth, tenth, and twelfth aspheric coefficients, respectively. . In the aspheric coefficient, “e−n” (n is an integer) indicates “10 ⁻ⁿ ”.

Example 1

r ₁ = 21.698 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 17.688 d ₂ = 4.06 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -29.133 (aspherical surface) d ₃ = (variable)
r ₄ = -12.208 (aspherical surface) d ₄ = 0.90 n _d3 = 1.80610 ν _d3 = 40.88
r ₅ = 5.778 (aspheric surface) d ₅ = 0.98
r ₆ = 9.168 d ₆ = 1.90 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = 26.277 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 4.600 (aspherical surface) d ₁₀ = 3.01 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -11.717 (aspherical surface) d ₁₁ = 0.20
r ₁₂ = 4.992 d ₁₂ = 1.26 n _d6 = 1.60342 ν _d6 = 38.03
r ₁₃ = 8.287 d ₁₃ = 0.39 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.230 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 24.719 (aspherical surface) d ₁₆ = 1.93 n _d8 = 1.74330 ν _d8 = 49.33
r ₁₇ = -69.248 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric coefficient 3rd surface K = 0.000
A ₄ = 3.82038e-05
A ₆ = -8.48090e-08
A ₈ = 3.61465e-10

4th page K = 0.089
A ₄ = 4.60626e-05
A ₆ = 1.28261e-05
A ₈ = -1.58317e-07

5th page K = -0.406
A ₄ = -5.63186e-04
A ₆ = 8.35981e-06
A ₈ = 2.80302e-07

10th page K = -0.227
A ₄ = -1.01015e-03
A ₆ = -2.49056e-05

11th page K = 0.000
A ₄ = 6.04770e-04
A ₆ = -2.94658e-05
A ₈ = 1.98114e-06

16th page K = 0.000
A ₄ = 1.18442e-04
A ₆ = 3.01521e-06
A ₈ = 4.62981e-07
A ₁₀ = -2.00000e-08

Zoom data (∞)
WE ST TE
f (mm) 6.88 16.85 46.28
F _NO 3.30 4.43 5.67
2ω (°) 63.08 24.77 9.31
d ₃ 0.71 7.57 13.70
d ₇ 12.31 6.87 0.60
d ₁₅ 2.30 8.77 15.01
d ₁₇ 5.06 3.68 1.50

Example 2

r ₁ = 20.645 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 16.835 d ₂ = 4.25 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -26.751 (aspherical surface) d ₃ = (variable)
r ₄ = -14.412 (aspherical surface) d ₄ = 0.94 n _d3 = 1.88300 ν _d3 = 40.76
r ₅ = 5.846 (aspherical surface) d ₅ = 0.80
r ₆ = 8.130 d ₆ = 2.01 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = 19.830 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 4.569 (aspherical surface) d ₁₀ = 3.11 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -12.606 (aspherical surface) d ₁₁ = 0.23
r ₁₂ = 4.855 d ₁₂ = 1.20 n _d6 = 1.60342 ν _d6 = 38.03
r ₁₃ = 7.083 d ₁₃ = 0.39 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.164 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 20.534 (aspherical surface) d ₁₆ = 2.09 n _d8 = 1.74330 ν _d8 = 49.33
r ₁₇ = -174.515 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)


Aspheric coefficient 3rd surface K = 0.000
A ₄ = 4.69441e-05
A ₆ = -1.14534e-07
A ₈ = 4.94209e-10

4th page K = 0.089
A ₄ = -1.91915e-04
A ₆ = 1.92984e-05
A ₈ = -2.28818e-07

5th page K = -0.406
A ₄ = -5.68873e-04
A ₆ = 7.83764e-06
A ₈ = 6.33582e-07

10th page K = -0.227
A ₄ = -9.38774e-04
A ₆ = -2.98017e-05

11th page K = 0.000
A ₄ = 6.11227e-04
A ₆ = -3.00252e-05
A ₈ = 1.85735e-06

16th page K = 0.000
A ₄ = 2.12280e-04
A ₆ = -2.82589e-06
A ₈ = 6.55635e-07
A ₁₀ = -2.00000e-08


Zoom data (∞)
WE ST TE
f (mm) 6.88 16.84 46.28
F _NO 3.30 4.42 5.59
2ω (°) 63.68 24.93 9.36
d ₃ 0.50 6.97 12.70
d ₇ 12.16 7.05 0.99
d ₁₅ 2.22 8.72 14.86
d ₁₇ 5.09 3.81 1.61

Example 3

r ₁ = 22.538 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 18.176 d ₂ = 4.07 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -27.449 (aspherical surface) d ₃ = (variable)
r ₄ = -11.281 (aspherical surface) d ₄ = 0.90 n _d3 = 1.80610 ν _d3 = 40.88
r ₅ = 6.540 (aspherical surface) d ₅ = 0.99
r ₆ = 10.399 d ₆ = 1.88 n _d4 = 2.10227 ν _d4 = 17.10
r ₇ = 22.503 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 4.505 (aspherical surface) d ₁₀ = 3.06 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -11.895 (aspherical surface) d ₁₁ = 0.22
r ₁₂ = 5.146 d ₁₂ = 1.18 n _d6 = 1.60342 ν _d6 = 38.03
r ₁₃ = 7.646 d ₁₃ = 0.39 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.245 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 24.762 (aspherical surface) d ₁₆ = 2.06 n _d8 = 1.74330 ν _d8 = 49.33
r ₁₇ = -66.758 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)


Aspheric coefficient 3rd surface K = 0.000
A ₄ = 3.92559e-05
A ₆ = -6.29929e-08
A ₈ = 2.03948e-10

4th page K = 0.089
A ₄ = 2.03912e-04
A ₆ = 1.01180e-05
A ₈ = -1.28824e-07

5th page K = -0.406
A ₄ = -3.80310e-04
A ₆ = 1.04953e-05
A ₈ = 2.29140e-07

10th page K = -0.227
A ₄ = -1.05417e-03
A ₆ = -2.31881e-05

11th page K = 0.000
A ₄ = 6.50102e-04
A ₆ = -2.65162e-05
A ₈ = 1.92181e-06

16th page K = 0.000
A ₄ = 1.47469e-04
A ₆ = -1.30252e-06
A ₈ = 6.46852e-07
A ₁₀ = -2.00000e-08


Zoom data (∞)
WE ST TE
f (mm) 6.88 16.85 46.29
F _NO 3.30 4.43 5.64
2ω (°) 63.19 24.73 9.31
d ₃ 0.68 7.52 13.70
d ₇ 12.42 6.96 0.69
d ₁₅ 2.28 8.77 14.93
d ₁₇ 5.03 3.69 1.50

Example 4

r ₁ = 20.479 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 16.826 d ₂ = 4.06 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -32.919 (aspherical surface) d ₃ = (variable)
r ₄ = -11.994 (aspherical surface) d ₄ = 0.91 n _d3 = 1.83481 ν _d3 = 42.71
r ₅ = 6.532 (aspherical surface) d ₅ = 0.78
r ₆ = 8.849 d ₆ = 1.86 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = 21.254 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 5.038 (aspherical surface) d ₁₀ = 3.14 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -11.062 (aspherical surface) d ₁₁ = 0.29
r ₁₂ = 5.130 d ₁₂ = 1.25 n _d6 = 1.60342 ν _d6 = 38.03
r ₁₃ = 8.213 d ₁₃ = 0.39 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.497 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 22.108 (aspherical surface) d ₁₆ = 1.98 n _d8 = 1.74330 ν _d8 = 49.33
r ₁₇ = -144.779 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric coefficient 3rd surface K = 0.000
A ₄ = 3.03379e-05
A ₆ = -5.30314e-08
A ₈ = 2.38853e-10

4th page K = 0.089
A ₄ = -4.93344e-05
A ₆ = 1.67517e-05
A ₈ = -1.98391e-07

5th page K = -0.406
A ₄ = -4.16293e-04
A ₆ = 9.24712e-06
A ₈ = 4.77141e-07

10th page K = -0.227
A ₄ = -8.15716e-04
A ₆ = -2.26164e-05

11th page K = 0.000
A ₄ = 6.46494e-04
A ₆ = -3.54167e-05
A ₈ = 1.87547e-06

16th page K = 0.000
A ₄ = 2.61106e-04
A ₆ = -1.49917e-06
A ₈ = 6.34056e-07
A ₁₀ = -2.00000e-08

Zoom data (∞)
WE ST TE
f (mm) 6.88 16.85 46.28
F _NO 3.30 4.45 5.72
2ω (°) 67.46 25.81 9.52
d ₃ 0.86 7.53 13.70
d ₇ 12.34 6.75 0.63
d ₁₅ 2.15 8.73 15.24
d ₁₇ 5.07 3.69 1.43

Example 5

r ₁ = 23.668 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 19.590 d ₂ = 3.98 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -27.384 (aspherical surface) d ₃ = (variable)
r ₄ = -12.598 (aspheric surface) d ₄ = 0.91 n _d3 = 1.83481 ν _d3 = 42.71
r ₅ = 6.347 (aspherical surface) d ₅ = 0.91
r ₆ = 9.462 d ₆ = 1.88 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = 25.431 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 4.380 (aspherical surface) d ₁₀ = 2.64 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -11.978 (aspherical surface) d ₁₁ = 0.21
r ₁₂ = 5.009 d ₁₂ = 1.17 n _d6 = 1.51742 ν _d6 = 52.43
r ₁₃ = 6.232 d ₁₃ = 0.40 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.071 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 21.580 (aspherical surface) d ₁₆ = 2.06 n _d8 = 1.81474 ν _d8 = 37.03
r ₁₇ = -978.404 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric coefficient 3rd surface K = -7.111
A ₄ = -5.55917e-07
A ₆ = 1.43935e-08
A ₈ = 1.59184e-10
A ₁₀ = 2.14201e-14

4th page K = 0.164
A ₄ = -5.56372e-05
A ₆ = 2.25017e-05
A ₈ = -6.41799e-07
A ₁₀ = 7.92547e-09

5th page K = 0.426
A ₄ = -1.02133e-03
A ₆ = 2.17154e-05
A ₈ = -1.26409e-06
A ₁₀ = 6.37628e-09

10th page K = -3.075
A ₄ = 2.84705e-03
A ₆ = -1.36330e-04

11th page K = 8.240
A ₄ = 7.87536e-04
A ₆ = 4.92757e-05
A ₈ = -1.38094e-05
A ₁₀ = 8.57143e-07

16th page K = -4.140
A ₄ = 1.27942e-04
A ₆ = 2.38646e-05
A ₈ = -1.38465e-06
A ₁₀ = 2.83638e-08

Zoom data (∞)
WE ST TE
f (mm) 6.62 16.17 44.53
F _NO 3.30 4.44 5.50
2ω (°) 65.90 25.93 9.87
d ₃ 0.70 7.35 13.70
d ₇ 13.43 7.55 0.60
d ₁₅ 1.98 8.49 13.39
d ₁₇ 5.27 4.06 3.60

Example 6
 
  r₁= 22.602 d₁= 0.80 n_d1= 2.00170 ν_d1= 20.64
  r₂= 18.738 d₂= 4.13 n_d2= 1.49700 ν_d2= 81.54
  r_Three= -25.691 (aspherical surface) d_Three= (Variable)
  r_Four= -13.288 (aspherical surface) d_Four= 0.91 n_d3= 1.83481 ν_d3= 42.71
  r_Five= 16.534 (aspherical surface) d_Five= 0.55
  r₆= 28.680 d₆= 0.70 n_d4= 1.88300 ν_d4= 40.76
  r₇= 7.398 d₇= 0.47
  r₈= 8.542 d₈= 2.05 n_d5= 1.92286 ν_d5= 18.90
  r₉= 23.121 d₉= (Variable)
  r_Ten= ∞ d_Ten= 0.98
  r₁₁= ∞ (aperture) d₁₁= -0.10
  r₁₂= 4.478 (aspherical surface) d₁₂= 2.56 n_d6= 1.49700 ν_d6= 81.54
  r₁₃= -15.247 (aspherical surface) d₁₃= 0.20
  r₁₄= 4.817 d₁₄= 1.47 n_d7= 1.51742 ν_d7= 52.43
  r₁₅= 7.370 d₁₅= 0.40 n_d8= 2.00330 ν_d8= 28.27
  r₁₆= 3.171 d₁₆= 0.70
  r₁₇= ∞ d₁₇= (Variable)
  r₁₈= 17.556 (aspherical surface) d₁₈= 2.28 n_d9= 1.81474 ν_d9= 37.03
  r₁₉= -356.352 d₁₉= (Variable)
  r₂₀= ∞ d₂₀= 0.50 n_d10= 1.51633 ν_d10= 64.14
  r_{twenty one}= ∞ d_{twenty one}= 0.50
  r_{twenty two}= ∞ d_{twenty two}= 0.50 n_d11= 1.51633 ν_d11= 64.14
  r_{twenty three}= ∞ d_{twenty three}= 0.37
  r_{twenty four}= ∞ (light receiving surface, image surface of electronic image sensor)
 
  Aspheric coefficient
   Third side
     K = -2.655
     A_Four= 2.84235e-05
     A₆= -1.26821e-07
     A₈= 6.53842e-10
     A_Ten= 2.14201e-14
 
   4th page
     K = 1.985
     A_Four= -1.54238e-04
     A₆= 3.31806e-05
     A₈= -7.71567e-07
     A_Ten= 7.92547e-09
 
   5th page
     K = 7.086
     A_Four= -9.45498e-04
     A₆= 3.71912e-05
     A₈= -9.25584e-07
     A_Ten= 6.37628e-09
 
   12th page
     K = -1.244
     A_Four= 5.05817e-04
     A₆= 4.58343e-05
 
   Side 13
     K = 0.148
     A_Four= 6.24060e-04
     A₆= 7.30506e-05
     A₈= -8.70760e-06
     A_Ten= 8.57143e-07
 
   18th page
     K = -5.979
     A_Four= 1.62882e-04
     A₆= 2.08747e-05
     A₈= -1.27158e-06
     A_Ten= 2.83638e-08
 
  Zoom data (∞)
                     WE ST TE
    f (mm)         6.62 16.17 44.53
    F_NO           3.30 4.45 5.35
    2ω (°)      66.51 25.78 9.68
    d_Three           0.61 6.85 12.93
    d₉          13.00 7.50 0.60
    d₁₇           1.91 8.34 12.90
    d₁₉           4.88 4.05 3.00
 

Example 7

r ₁ = 23.899 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 19.824 d ₂ = 4.24 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -26.164 (aspherical surface) d ₃ = (variable)
r ₄ = -10.790 (aspherical surface) d ₄ = 0.91 n _d3 = 1.83481 ν _d3 = 42.71
r ₅ = 22.431 (aspherical surface) d ₅ = 0.90
r ₆ = 218.971 d ₆ = 2.10 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = -13.195 d ₇ = 0.30
r ₈ = -10.758 d ₈ = 0.50 n _d5 = 1.88300 ν _d5 = 40.76
r ₉ = 103.691 d ₉ = (variable)
r ₁₀ = ∞ d ₁₀ = 0.98
r ₁₁ = ∞ (aperture) d ₁₁ = -0.10
r ₁₂ = 4.295 (aspherical surface) d ₁₂ = 2.51 n _d6 = 1.49700 ν _d6 = 81.54
r ₁₃ = -13.710 (aspherical surface) d ₁₃ = 0.20
r ₁₄ = 4.763 d ₁₄ = 1.22 n _d7 = 1.51742 ν _d7 = 52.43
r ₁₅ = 6.332 d ₁₅ = 0.40 n _d8 = 2.00330 ν _d8 = 28.27
r ₁₆ = 3.093 d ₁₆ = 0.70
r ₁₇ = ∞ d ₁₇ = (variable)
r ₁₈ = 29.444 (aspherical surface) d ₁₈ = 1.99 n _d9 = 1.81474 ν _d9 = 37.03
r ₁₉ = -51.206 d ₁₉ = (variable)
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.50
r ₂₂ = ∞ d ₂₂ = 0.50 n _d11 = 1.51633 ν _d11 = 64.14
r ₂₃ = ∞ d ₂₃ = 0.37
r ₂₄ = ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric coefficient 3rd surface K = -3.386
A ₄ = 1.84236e-05
A ₆ = -5.49013e-08
A ₈ = 2.40556e-10
A ₁₀ = -3.81661e-13

4th page K = -3.373
A ₄ = -5.91701e-06
A ₆ = 1.42524e-05
A ₈ = -3.49467e-07
A ₁₀ = 3.04350e-09

5th page K = 3.350
A ₄ = -1.83526e-04
A ₆ = 2.07397e-05
A ₈ = -4.59555e-07
A ₁₀ = 6.67020e-09

12th page K = -1.796
A ₄ = 1.38580e-03
A ₆ = 5.53570e-06

Side 13 K = -92.455
A ₄ = -3.55086e-03
A ₆ = 7.78041e-04
A ₈ = -9.98896e-05
A ₁₀ = 5.79723e-06

18th page
K = 5.707
A ₄ = 1.30782e-04
A ₆ = 9.36732e-06
A ₈ = -4.60064e-07
A ₁₀ = 7.60826e-09


Zoom data (∞)
WE ST TE
f (mm) 6.62 16.17 44.53
F _NO 3.30 4.44 5.43
2ω (°) 68.57 26.03 9.75
d ₃ 0.58 7.10 13.39
d ₉ 12.27 6.94 0.60
d ₁₇ 2.29 8.51 13.18
d ₁₉ 4.97 3.90 3.00

Example 8

r ₁ = 23.976 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 19.903 d ₂ = 3.96 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -27.088 (aspherical surface) d ₃ = (variable)
r ₄ = -13.009 (aspherical surface) d ₄ = 0.91 n _d3 = 1.83481 ν _d3 = 42.71
r ₅ = 6.302 (aspherical surface) d ₅ = 0.92
r ₆ = 9.256 d ₆ = 1.87 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = 23.104 d ₇ = (variable)
r ₈ = ∞ d ₈ = 0.98
r ₉ = ∞ (aperture) d ₉ = -0.10
r ₁₀ = 4.405 (aspherical surface) d ₁₀ = 2.63 n _d5 = 1.49700 ν _d5 = 81.54
r ₁₁ = -10.942 (aspherical surface) d ₁₁ = 0.23
r ₁₂ = 5.290 d ₁₂ = 1.14 n _d6 = 1.51742 ν _d6 = 52.43
r ₁₃ = 6.299 d ₁₃ = 0.41 n _d7 = 2.00330 ν _d7 = 28.27
r ₁₄ = 3.124 d ₁₄ = 0.70
r ₁₅ = ∞ d ₁₅ = (variable)
r ₁₆ = 21.612 (aspherical surface) d ₁₆ = 2.06 n _d8 = 1.81474 ν _d8 = 37.03
r ₁₇ = -3334.342 d ₁₇ = (variable)
r ₁₈ = ∞ d ₁₈ = 0.50 n _d9 = 1.51633 ν _d9 = 64.14
r ₁₉ = ∞ d ₁₉ = 0.50
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.37
r ₂₂ = ∞ (light receiving surface, image surface of electronic image sensor)


Aspheric coefficient 3rd surface K = -3.358
A ₄ = 2.30297e-05
A ₆ = -1.22671e-07
A ₈ = 7.32069e-10
A ₁₀ = 2.14201e-14

4th page K = -0.491
A ₄ = -1.79874e-04
A ₆ = 2.75493e-05
A ₈ = -7.26410e-07
A ₁₀ = 7.92547e-09

5th page K = 0.311
A ₄ = -1.03567e-03
A ₆ = 2.81436e-05
A ₈ = -1.04751e-06
A ₁₀ = 6.37628e-09

10th page K = -3.062
A ₄ = 2.72342e-03
A ₆ = -1.57228e-04

11th page K = -22.869
A ₄ = -1.92400e-03
A ₆ = 1.43485e-04
A ₈ = -2.06398e-05
A ₁₀ = 8.57143e-07

16th page K = -3.300
A ₄ = 1.45283e-04
A ₆ = 2.16436e-05
A ₈ = -1.33025e-06
A ₁₀ = 2.83638e-08


Zoom data (∞)
WE ST TE
f (mm) 6.62 16.18 44.54
F _NO 3.30 4.44 5.49
2ω (°) 65.74 25.95 9.88
d ₃ 0.67 7.35 13.69
d ₇ 13.36 7.50 0.60
d ₁₅ 2.02 8.52 13.40
d ₁₇ 5.28 4.07 3.61

Example 9

r ₁ = 23.104 d ₁ = 0.80 n _d1 = 2.00170 ν _d1 = 20.64
r ₂ = 19.396 d ₂ = 4.18 n _d2 = 1.49700 ν _d2 = 81.54
r ₃ = -28.307 (aspherical surface) d ₃ = (variable)
r ₄ = -8.746 (aspherical surface) d ₄ = 0.90 n _d3 = 1.80610 ν _d3 = 40.92
r ₅ = 22.609 (aspherical surface) d ₅ = 0.96
r ₆ = 115.759 d ₆ = 1.98 n _d4 = 1.92286 ν _d4 = 18.90
r ₇ = -14.259 d ₇ = 0.21
r ₈ = -13.143 d ₈ = 0.50 n _d5 = 1.88300 ν _d5 = 40.76
r ₉ = 72.040 d ₉ = (variable)
r ₁₀ = ∞ d ₁₀ = 0.98
r ₁₁ = ∞ (aperture) d ₁₁ = -0.10
r ₁₂ = 4.226 (aspherical surface) d ₁₂ = 2.08 n _d6 = 1.49700 ν _d6 = 81.54
r ₁₃ = -16.546 (aspherical surface) d ₁₃ = 0.38
r ₁₄ = 4.496 d ₁₄ = 1.32 n _d7 = 1.51742 ν _d7 = 52.43
r ₁₅ = 6.297 d ₁₅ = 0.40 n _d8 = 2.00330 ν _d8 = 28.27
r ₁₆ = 3.029 d ₁₆ = 0.70
r ₁₇ = ∞ d ₁₇ = (variable)
r ₁₈ = 42.015 (aspherical surface) d ₁₈ = 1.93 n _d9 = 1.81474 ν _d9 = 37.03
r ₁₉ = -32.646 d ₁₉ = (variable)
r ₂₀ = ∞ d ₂₀ = 0.50 n _d10 = 1.51633 ν _d10 = 64.14
r ₂₁ = ∞ d ₂₁ = 0.50
r ₂₂ = ∞ d ₂₂ = 0.50 n _d11 = 1.51633 ν _d11 = 64.14
r ₂₃ = ∞ d ₂₃ = 0.37
r ₂₄ = ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric coefficient 3rd surface K = -5.090
A ₄ = 9.69822e-06
A ₆ = -7.03853e-09
A ₈ = 8.40603e-11
A ₁₀ = -7.99864e-13

4th page K = -7.664
A ₄ = -2.42260e-04
A ₆ = 1.92938e-05
A ₈ = -4.98886e-07
A ₁₀ = 4.81577e-09

5th page K = 14.395
A ₄ = 3.36955e-04
A ₆ = -1.56311e-06
A ₈ = -5.73815e-08
A ₁₀ = -1.93332e-09

12th page K = -4.899
A ₄ = 6.91677e-03
A ₆ = -4.70828e-04
A ₈ = 3.61315e-05
A ₁₀ = 9.97270e-22

Side 13 K = -161.860
A ₄ = -2.97697e-03
A ₆ = 9.82793e-04
A ₈ = -1.34602e-04
A ₁₀ = 1.02130e-05

18th page K = -238.183
A ₄ = 4.66205e-04
A ₆ = -2.07951e-06
A ₈ = -1.03870e-07
A ₁₀ = 1.44607e-09


Zoom data (∞)
WE ST TE
f (mm) 6.63 16.23 44.53
F _NO 3.30 4.51 5.64
2ω (°) 67.60 25.89 9.77
d ₃ 0.95 7.52 13.67
d ₉ 11.63 6.65 0.60
d ₁₇ 1.89 8.46 13.34
d ₁₉ 5.04 3.61 3.00

Example 10
Unit mm

Surface data Surface number rd nd νd
1 15.981 0.80 1.94595 17.98
2 13.053 3.75 1.59201 67.07
3 * -66.140 variable
4 * -100.665 0.90 1.83481 42.71
5 * 7.729 2.13
6 -16.155 0.70 1.88300 40.76
7 11.324 0.20
8 10.621 1.87 1.94595 17.98
9 2576.770 Variable
10 (Aperture) ∞ 0.00
11 * 5.669 2.88 1.49700 81.54
12 * -14.592 0.10
13 6.990 1.57 1.76200 40.10
14 -856.715 0.41 1.74000 28.30
15 3.868 Variable
16 * 22.699 1.80 1.74320 49.34
17 -62.571 Variable
18 ∞ 0.50 1.51633 64.14
19 ∞ 1.20
20 ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric data 3rd surface K = 0.000, A4 = 3.00437e-05, A6 = -3.01520e-08, A8 = -5.50854e-10, A10 = 3.81914e-12
4th surface K = 0.000, A4 = -1.22830e-05, A6 = 3.19778e-06, A8 = 1.49784e-08, A10 = -1.44514e-09
5th surface K = -0.836, A4 = 1.95528e-04, A6 = 1.69233e-05, A8 = 1.70976e-08, A10 = 1.78784e-08
11th surface K = -3.831, A4 = 1.95133e-03, A6 = -6.49873e-05, A8 = 2.66321e-06, A10 = -9.19166e-08
12th surface K = 0.000, A4 = 4.30798e-04, A6 = 1.52421e-07, A8 = 1.09883e-06, A10 = -9.21340e-08
16th surface K = 0.000, A4 = 5.94648e-05, A6 = 1.25383e-05, A8 = -6.35142e-07, A10 = 1.34623e-08

Various data
Wide angle Medium telephoto focal length 6.63 16.65 44.36
FNO. 3.45 4.69 4.74
Angle of view 2ω 67.91 26.70 9.79

d3 0.27 5.40 11.68
d9 12.65 7.15 1.74
d15 5.69 12.69 13.85
d17 5.17 5.10 2.96

Example 11
Unit mm

Surface data Surface number rd nd νd
1 16.869 0.80 1.94595 17.98
2 13.695 3.68 1.59201 67.07
3 * -57.815 variable
4 * -42.294 0.70 1.80610 40.92
5 * 12.696 2.08
6 -11.746 0.60 1.88300 40.76
7 9.844 2.01 1.94595 17.98
8 -13988.729 Variable
9 (Aperture) ∞ 0.00
10 * 5.454 2.39 1.49700 81.54
11 * -16.944 0.10
12 6.940 2.07 1.76200 40.10
13 -6100.501 0.41 1.74000 28.30
14 3.605 Variable
15 * 17.114 2.64 1.53110 55.91
16 -19.673 Variable
17 ∞ 0.50 1.51633 64.14
18 ∞ 1.20
19 ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric data 3rd surface K = -20.755, A4 = 1.51899e-05, A6 = -2.74484e-08, A8 = 3.19103e-11, A10 = 1.51082e-13
4th surface K = -88.808, A4 = 2.72233e-04, A6 = -1.03270e-05, A8 = 4.99104e-07, A10 = -7.03571e-09
5th surface K = 5.715, A4 = 9.76937e-07, A6 = -1.52989e-05, A8 = 5.01342e-07, A10 = -1.25456e-08
10th surface K = -3.567, A4 = 2.13009e-03, A6 = -6.35403e-05, A8 = 2.94077e-06, A10 = -2.18484e-08
11th surface K = 10.628, A4 = 8.07600e-04, A6 = 6.73556e-06, A8 = 1.75247e-06, A10 = 7.93089e-09
15th surface K = 0.124, A4 = 1.29001e-04, A6 = 1.04784e-05, A8 = -4.85185e-07, A10 = 7.93527e-09

Various data
Wide angle Medium telephoto focal length 6.62 16.87 44.97
FNO. 3.44 4.91 5.01
Angle of view 2ω 68.56 26.90 9.88

d3 0.30 5.71 11.67
d8 12.24 7.90 1.77
d14 4.00 12.49 13.10
d16 4.84 3.60 2.98

Example 12
Unit mm

Surface data Surface number rd nd νd
1 18.182 0.90 1.94595 17.98
2 14.569 3.48 1.59201 67.07
3 * -52.115 variable
4 * -34.097 0.70 1.80610 40.92
5 * 14.105 2.22
6 -13.219 0.60 1.88300 40.76
7 10.602 1.93 1.94595 17.98
8 ∞ variable
9 (Aperture) ∞ 0.00
10 * 5.288 2.43 1.49700 81.54
11 * -17.296 0.10
12 7.329 2.00 1.76200 40.10
13 ∞ 0.41 1.71736 29.52
14 3.564 Variable
15 * 22.281 2.44 1.58313 59.38
16 * -22.281 variable
17 ∞ 0.50 1.51633 64.14
18 ∞ 1.20
19 ∞ (light receiving surface, image surface of electronic image sensor)

Aspheric data 3rd surface K = -14.625, A4 = 1.26268e-05, A6 = 2.89083e-09, A8 = -5.21489e-10, A10 = 3.54481e-12
4th surface K = -123.195, A4 = -1.13231e-05, A6 = -1.61794e-06, A8 = 2.27459e-07, A10 = -3.24892e-09
5th surface K = 4.125, A4 = 8.01581e-05, A6 = -1.19119e-05, A8 = 1.80160e-07, A10 = 1.16109e-08
10th surface K = -2.714, A4 = 1.47977e-03, A6 = -2.78130e-05, A8 = 4.58287e-07, A10 = -4.11026e-09
11th surface K = 7.374, A4 = 5.60610e-04, A6 = 1.44138e-08, A8 = 5.31566e-07, A10 = 4.29532e-09
15th surface K = 0.183, A4 = 4.69985e-05, A6 = 8.18509e-06, A8 = -4.46999e-07, A10 = 8.51670e-09
16th surface K = 0.183, A4 = -4.69985e-05, A6 = -8.18509e-06, A8 = 4.46999e-07, A10 = -8.51670e-09

Various data
Wide angle Medium telephoto focal length 6.68 16.98 45.16
FNO. 3.36 4.91 5.08
Angle of view 2ω 68.06 26.50 9.76

d3 0.30 5.32 11.90
d8 12.85 7.83 1.78
d14 3.30 12.50 13.60
d16 5.39 4.14 3.02

  Aberration diagrams at the time of focusing on an object point at infinity in Examples 1 to 9 are shown in FIGS. In these aberration diagrams, (a) is a wide-angle end, (b) is an intermediate state, and (c) is spherical aberration, astigmatism, distortion, and lateral chromatic aberration at a telephoto end. In each figure, “FIY” indicates the maximum image height. “Ω” indicates a half angle of view.

Further, FIGS. 27, 28, and 29 show aberration diagrams of Examples 10, 11, and 12 when focusing on an object point at infinity, respectively. In these aberration diagrams, (a) is the wide angle end, (b) is the intermediate state, (c) is the spherical aberration (SA), astigmatism (AS), distortion (DT), and lateral chromatic aberration (CC) at the telephoto end. ). In each figure, “ω” indicates a half angle of view.

  Next, the values of conditional expressions (1) to (23) in each example will be listed.
 
                           Example 1 Example 2 Example 3 Example 4 Example 5
(1) (β_2t/ β_2w) / (β_3t/ β_3w) 1.759 1.874 1.784 1.654 1.576
(2) f_t/ f_w                 6.725 6.728 6.726 6.725 6.725
(3) D_2w/ f_t                 0.285 0.282 0.287 0.286 0.321
(4) f₁/ f_t                   0.634 0.595 0.633 0.645 0.660
(5) | f₂/ f_t0.164 0.154 0.164 0.163 0.172
(6) f_Three/ f_t                   0.220 0.217 0.220 0.219 0.234
(7) f_Four/ f_t                   0.534 0.537 0.530 0.560 0.583
(8) ν_d1p-ν_d1n            60.896 60.896 60.896 60.896 60.896
(9) ν_d1p               81.540 81.540 81.540 81.540 81.540
(10) ν_d3p              81.540 81.540 81.540 81.540 81.540
(11) n_d1n             2.002 2.002 2.002 2.002 2.002
(12) n_d2n                1.806 1.883 1.806 1.835 1.835
(13) n_d2p                  1.923 1.923 2.102 1.923 1.923
(14) SF_2n1         0.357 0.423 0.266 0.295 0.330
(15) SF_1p        -0.244 -0.228 -0.203 -0.324 -0.166
(16) β_2t/ β_2w          3.133 3.237 3.153 3.048 3.115
(17) β_3t/ β_3w          1.781 1.727 1.768 1.842 1.977
(18) β_4t/ β_4w          1.205 1.204 1.207 1.198 1.092
(19) (D_2w+ D_1t) / f_t        0.581 0.556 0.583 0.582 0.629
(20) D_1t/ f_t           0.296 0.274 0.296 0.296 0.308
(21) T_L/ f_t             1.074 1.068 1.077 1.079 1.116
 
                            Example 6 Example 7 Example 8 Example 9
(1) (β_2t/ β_2w) / (β_3t/ β_3w) 1.955 1.754 1.580 1.608
(2) f_t/ f_w                 6.724 6.722 6.727 6.721
(3) D_2w/ f_t             0.312 0.295 0.320 0.281
(4) f₁/ f_t                   0.625 0.648 0.659 0.657
(5) | f₂/ f_t0.166 0.162 0.171 0.160
(6) f_Three/ f_t                   0.235 0.224 0.234 0.216
(7) f_Four/ f_t                   0.462 0.521 0.592 0.512
(8) ν_d1p-ν_d1n       60.896 60.896 60.896 60.896
(9) ν_d1p             81.540 81.540 81.540 81.540
(10) ν_d3p            81.540 81.540 52.430 81.540
(11) n_d1n            2.002 2.002 2.002 2.002
(12) n_d2n            1.835 1.835 1.835 1.806
(13) n_d2p            1.923 1.923 1.923 1.923
(14) SF_2n1          -0.109 -0.350 0.347 -0.442
(15) SF_1p          -0.156 -0.138 -0.153 -0.187
(16) β_2t/ β_2w      3.389 3.239 3.122 3.094
(17) β_3t/ β_3w      1.733 1.847 1.975 1.924
(18) β_4t/ β_4w      1.145 1.123 1.091 1.129
(19) (D_2w+ D_1t) / f_t    0.602 0.596 0.627 0.588
(20) D_1t/ f_t        0.290 0.301 0.307 0.307
(21) T_L/ f_t          1.109 1.116 1.116 1.116
 
 
                           Example 10 Example 11 Example 12
(1) (β_2t/ β_2w) / (β_3t/ β_3w) 3.152 2.981 2.684
(2) f_t/ f_w                  6.692 6.796 6.757
(3) D_2w/ f_t                   0.285 0.272 0.284
(4) f₁/ f_t                    0.553 0.554 0.572
(5) | f₂/ f_t| 0.136 0.136 0.144
(6) f_Three/ f_t                    0.243 0.232 0.236
(7) f_Four/ f_t                    0.510 0.393 0.432
(8) ν_d1p-ν_d1n             49.085 49.085 49.085
(9) ν_d1p                   67.069 67.069 67.069
(10) ν_d3p                  81.540 81.540 81.540
(11) n_d1n                    1.946 1.946 1.946
(12) n_d2n                    1.835 1.806 1.806
(13) n_d2p                    1.883 1.883 1.883
(14) SF_2n1                   0.857 0.538 0.415
(15) SF_1p                   -0.670 -0.617 -0.563
(16) β_2t/ β_2w               4.292 4.146 3.885
(17) β_3t/ β_3w               1.362 1.391 1.447
(18) β_4t/ β_4w               1.145 1.179 1.201
(19) (D_2w+ D_1t) / f_t            0.548 0.532 0.548
(20) D_1t/ f_t                  0.263 0.260 0.263
(21) TL / f_t                  1.109 1.086 1.093
(22) (R_aspO+ R_aspI) / (R_aspO-R_aspI)
                              --0
(23) (XO (y) + XI (y)) / (R_aspO-R_aspI)
                              --0 ≦ y ≦ R and all 0
 

  The above embodiment realizes a zoom lens optical system having a high zoom ratio of about 7 times so that the camera can be easily thinned. Of course, the image quality of the photographed image is maintained well, and the zoom lens optical system is an inexpensive zoom lens system suitable for use with an electronic image sensor such as a CCD or CMOS.

  In each of the above embodiments, a flare stop may be arranged in addition to the brightness stop in order to cut unnecessary light such as ghosts and flares. The flare stop is disposed on the object side of the first lens group, between the first and second lens groups, between the second and third lens groups, between the third and fourth lens groups, and between the fourth lens group and the image plane. You may do it. The frame member may be configured to cut flare rays, or another member may be configured. Also, it may be printed directly on the optical system, painted, or adhered with a seal. Further, the shape may be any shape such as a circle, an ellipse, a rectangle, a polygon, or a range surrounded by a function curve. Further, not only harmful light flux but also light flux such as coma flare around the screen may be cut.

  Each lens may be provided with an antireflection coating to reduce ghosts and flares. A multi-coat is desirable because it can effectively reduce ghost and flare. Further, infrared cut coating may be performed on the lens surface, cover glass, or the like.

  In addition, it is desirable to perform focusing for adjusting the focus by moving the fourth lens group. When focusing is performed with the fourth lens group, the load on the motor is small because the lens weight is light. Furthermore, the total length does not change during focusing, and the drive motor can be arranged inside the lens frame, which is advantageous for making the lens frame compact. As described above, focusing with the fourth lens group is desirable, but focusing may be performed with the first, second, and third lens groups. Further, focusing may be performed by moving a plurality of lens groups. Further, focusing may be performed by extending the entire lens system, or focusing may be performed by extending or retracting some lenses.

Further, the brightness (shading) at the periphery of the image may be reduced by shifting the CCD microlens. For example, the design of the CCD microlens may be changed in accordance with the incident angle of the light beam at each image height. Further, the amount of decrease in the peripheral portion of the image may be corrected by image processing.

  Alternatively, the distortion may be intentionally generated by the optical system, and the distortion may be corrected by electrically performing image processing after shooting.

(Correction of distortion)
By the way, when the zoom lens of the present invention is used, image distortion is digitally corrected electrically. The basic concept for digitally correcting image distortion will be described below.

  For example, as shown in FIG. 19, the magnification on the circumference (image height) of the radius R inscribed in the long side of the effective imaging surface around the intersection of the optical axis and the imaging surface is fixed, and this circumference is The standard for correction. Then, correction is performed by moving each point on the circumference (image height) of any other radius r (ω) in a substantially radial direction and concentrically so as to have the radius r ′ (ω). To do.

For example, in FIG. 19, a point P ₁ on the circumference of an arbitrary radius r ₁ (ω) located inside the circle of radius R is a radius r ₁ ′ (ω) circle to be corrected toward the center of the circle. Move to point P ₂ on the circumference. A point Q ₁ on the circumference of an arbitrary radius r ₂ (ω) located outside the circle of radius R is a radius r ₂ ′ (ω) circumference to be corrected in a direction away from the center of the circle. It is moved to the point Q ₂ of the above.

Here, r ′ (ω) can be expressed as follows.
r ′ (ω) = α · f · tan ω (0 ≦ α ≦ 1)
However,
ω is the subject half angle of view, and f is the focal length of the imaging optical system (in the present invention, the zoom lens).

Here, if the ideal image height corresponding to the circle (image height) of the radius R is Y,
α = R / Y = R / (f · tan ω)
It becomes.

The optical system is ideally rotationally symmetric with respect to the optical axis, that is, distortion is also generated rotationally symmetric with respect to the optical axis. Therefore, as described above, when the optically generated distortion aberration is electrically corrected, the radius inscribed in the long side of the effective imaging surface around the intersection of the optical axis and the imaging surface on the reproduced image. The magnification on the circumference of the circle of R (image height) is fixed, and the other points on the circumference (image height) of the radius r (ω) are moved in a substantially radial direction to obtain a radius r ′ ( If correction can be performed by moving the concentric circles so that ω), it is considered advantageous in terms of data amount and calculation amount.

  However, the optical image is no longer a continuous amount (due to sampling) when captured by the electronic image sensor. Therefore, strictly speaking, the circle with the radius R drawn on the optical image is not an accurate circle unless the pixels on the electronic image sensor are arranged radially.

That is, in the shape correction of the image data represented for each discrete coordinate point, there is no circle that can fix the magnification. Therefore, for each pixel (Xi, Yj), the coordinates (Xi ', Yj') of the movement destination
) Should be used. When two or more points (Xi, Yj) have moved to the coordinates (Xi ′, Yj ′), the average value of the values possessed by each pixel is taken. If there is no moving point, interpolation may be performed using the values of the coordinates (Xi ′, Yj ′) of some surrounding pixels.

Such a method is particularly distorted with respect to the optical axis due to a manufacturing error of an optical system or an electronic imaging device in an electronic imaging device included in a zoom lens, and the circle of the radius R drawn on the optical image is It is effective for correction when it becomes asymmetric. Further, it is effective for correction when a geometric distortion or the like occurs when a signal is reproduced as an image in an image sensor or various output devices.

In the electronic imaging device of the present invention, in order to calculate the correction amount r ′ (ω) −r (ω), r (ω)
That is, the relationship between the half field angle and the image height, or the relationship between the real image height r and the ideal image height r ′ / α may be recorded on a recording medium built in the electronic imaging apparatus.

  Note that the radius R preferably satisfies the following conditional expression so that the image after distortion correction does not have an extremely short amount of light at both ends in the short side direction.

0 ≦ R ≦ 0.6Ls
However, Ls is the length of the short side of the effective imaging surface.

Preferably, the radius R satisfies the following conditional expression.
0.3Ls≤R≤0.6Ls
Furthermore, it is most advantageous to make the radius R coincide with the radius of the inscribed circle in the short side direction of the substantially effective imaging surface. In the case of correction in which the magnification is fixed in the vicinity of the radius R = 0, that is, in the vicinity of the axis, there is a slight disadvantage in terms of the actual number of images, but the effect of reducing the size is ensured even if the angle is widened. it can.

The focal length section that needs to be corrected is divided into several focal zones. Then, in the vicinity of the telephoto end in the divided focal zone, approximately r ′ (ω) = α · f · tan ω
You may correct | amend with the same correction amount as the case where the correction result which satisfies is obtained.

  However, in that case, some barrel distortion remains at the wide-angle end in the divided focal zone. Further, if the number of divided zones is increased, it becomes unnecessary to store extraneous data necessary for correction on the recording medium, which is not preferable. Therefore, one or several coefficients related to each focal length in the divided focal zone are calculated in advance. This coefficient may be determined on the basis of simulation or actual measurement.

And approximately near the telephoto end in the divided zone,
r ′ (ω) = α · f · tan ω
It is also possible to calculate a correction amount when a correction result satisfying the above is obtained, and uniformly multiply the correction amount for each focal distance to obtain a final correction amount.

By the way, if there is no distortion in the image obtained by imaging an object at infinity,
f = y / tan ω
Is established.
Where y is the height (image height) of the image point from the optical axis, f is the focal length of the imaging system (in the present invention, the zoom lens), and ω is the image point connecting from the center on the imaging surface to the y position. It is an angle (subject half field angle) with respect to the optical axis in the corresponding object direction.

If the imaging system has barrel distortion,
f> y / tan ω
It becomes. That is, if the focal length f of the imaging system and the image height y are constant, the value of ω increases.

(Digital camera)
20 to 22 are conceptual diagrams of the configuration of the digital camera according to the present invention in which the zoom lens as described above is incorporated in the photographing optical system 141. FIG. 20 is a front perspective view showing the appearance of the digital camera 140, FIG. 21 is a rear front view thereof, and FIG. 22 is a schematic cross-sectional view showing the configuration of the digital camera 140. However, in FIGS. 20 and 22, the photographing optical system 141 is not retracted. In this example, the digital camera 140 includes a photographing optical system 141 having a photographing optical path 142, a finder optical system 143 having a finder optical path 144, a shutter button 145, a flash 146, a liquid crystal display monitor 147, a focal length change button 161, When the photographic optical system 141 is retracted, including the setting change switch 162, the photographic optical system 141, the finder optical system 143, and the flash 146 are covered with the cover 160 by sliding the cover 160. When the cover 160 is opened and the camera 140 is set to the photographing state, the photographing optical system 141 is brought into the non-collapsed state of FIG. 20, and when the shutter button 145 disposed on the upper part of the camera 140 is pressed, the photographing is performed in conjunction therewith. Photographing is performed through the optical system 141, for example, the zoom lens of the first embodiment. An object image formed by the photographic optical system 141 is formed on the imaging surface of the CCD 149 through a low-pass filter F and a cover glass C that are provided with a wavelength band limiting coat. The object image received by the CCD 149 is displayed as an electronic image on a liquid crystal display monitor 147 provided on the back of the camera via the processing means 151. Further, the processing means 151 is connected to a recording means 152 so that a photographed electronic image can be recorded. The recording unit 152 may be provided separately from the processing unit 151, or may be configured to perform recording / writing electronically using a flexible disk, a memory card, an MO, or the like. Further, instead of the CCD 149, a silver salt camera in which a silver salt film is arranged may be configured.

  Further, a finder objective optical system 153 is disposed on the finder optical path 144. The finder objective optical system 153 includes a plurality of lens groups (three groups in the figure) and two prisms, and includes a zoom optical system whose focal length changes in conjunction with the zoom lens of the photographing optical system 141. The object image formed by the finder objective optical system 153 is formed on the field frame 157 of the erecting prism 155 that is an image erecting member. Behind the erecting prism 155, an eyepiece optical system 159 that guides the erect image to the observer eyeball E is disposed. A cover member 150 is disposed on the exit side of the eyepiece optical system 159.

  The digital camera 140 configured as described above has a high performance because the photographing optical system 141 is extremely thin when retracted, and has a high zoom ratio and a very stable imaging performance in the entire zoom range.・ Compact and wide angle can be realized.

(Internal circuit configuration)
FIG. 23 is a block diagram showing the internal circuitry of the main part of the digital camera 140. In the following description, the processing means includes, for example, the CDS / ADC unit 124, the temporary storage memory 117, the image processing unit 118, and the like, and the storage means includes, for example, the storage medium unit 119.

  As shown in FIG. 23, the digital camera 140 is connected to the operation unit 112, the control unit 113 connected to the operation unit 112, and the control signal output port of the control unit 113 via buses 114 and 115. An imaging drive circuit 116, a temporary storage memory 117, an image processing unit 118, a storage medium unit 119, a display unit 120, and a setting information storage memory unit 121 are provided.

  The temporary storage memory 117, the image processing unit 118, the storage medium unit 119, the display unit 120, and the setting information storage memory unit 121 are configured so that data can be input or output with each other via the bus 122. In addition, a CCD 149 and a CDS / ADC unit 124 are connected to the imaging drive circuit 116.

  The operation unit 112 includes various input buttons and switches, and is a circuit that notifies the control unit of event information input from the outside (camera user) via these input buttons and switches.

  The control unit 113 is a central processing unit composed of, for example, a CPU and the like. The control unit 113 includes a program memory (not shown) and is input from the camera user via the operation unit 112 according to a program stored in the program memory. This is a circuit that controls the entire digital camera 140 in response to an instruction command.

  The CCD 149 receives an object image formed through the photographing optical system 141 according to the present invention. The CCD 149 is an image pickup element that is driven and controlled by the image pickup drive circuit 116, converts the light amount of each pixel of the object image into an electrical signal, and outputs the electric signal to the CDS / ADC unit 124.

  The CDS / ADC unit 124 amplifies the electric signal input from the CCD 149 and performs analog / digital conversion, and temporarily stores the raw video data (Bayer data, hereinafter referred to as RAW data) that has just been subjected to the amplification and digital conversion. This is a circuit for outputting to the storage memory 117.

  The temporary storage memory 117 is a buffer made of, for example, SDRAM or the like, and is a memory device that temporarily stores the RAW data output from the CDS / ADC unit 124. The image processing unit 118 reads out the RAW data stored in the temporary storage memory 117 or the RAW data stored in the storage medium unit 119, and performs various corrections including distortion correction based on the image quality parameter designated from the control unit 113. It is a circuit that performs image processing electrically.

  The recording medium unit 119 detachably mounts a card-type or stick-type recording medium made of, for example, a flash memory, and RAW data transferred from the temporary storage memory 117 to the card-type or stick-type flash memory. This is a control circuit of an apparatus for recording and holding image data processed by the image processing unit 118.

  The display unit 120 includes a liquid crystal display monitor, and is a circuit that displays an image, an operation menu, and the like on the liquid crystal display monitor. The setting information storage memory unit 121 stores a ROM unit in which various image quality parameters are stored in advance, and an image quality parameter selected by an input operation of the operation unit 112 among the image quality parameters read from the ROM unit. RAM section is provided. The setting information storage memory unit 121 is a circuit that controls input and output to these memories.

  In the digital camera 140 configured in this way, the imaging optical system 141 has a sufficiently wide angle range and a compact configuration according to the present invention, and the imaging performance is extremely stable at a high zoom ratio and in a full zoom ratio range. Therefore, high performance, downsizing, and wide angle can be realized. In addition, fast focusing operation on the wide-angle side and the telephoto side is possible.

  As described above, the present invention is useful for a zoom lens having a high zoom ratio of about 7 times so that the camera can be easily thinned.

FIG. 2 is a lens cross-sectional view at the wide-angle end (a), the intermediate state (b), and the telephoto end (c) when focusing on an object point at infinity according to the first exemplary embodiment of the zoom lens of the present invention. It is the same figure as FIG. 1 of Example 2 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 3 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 4 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 5 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 6 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 7 of the zoom lens of this invention. It is a figure similar to FIG. 1 of Example 8 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 9 of the zoom lens of this invention. FIG. 6 is an aberration diagram for Example 1 upon focusing on an object point at infinity. FIG. 6 is an aberration diagram for Example 2 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 3 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 4 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 5 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 6 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 7 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 8 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 9 upon focusing on an object point at infinity. It is a figure explaining correction | amendment of a distortion aberration. It is a front perspective view which shows the external appearance of the digital camera incorporating the zoom lens by this invention. FIG. 21 is a rear perspective view of the digital camera of FIG. 20. It is sectional drawing of the digital camera of FIG. It is a block diagram of the internal circuit of the main part of the digital camera. FIG. 10 is an aberration diagram for Example 10 upon focusing on an object point at infinity. FIG. 10 is an aberration diagram for Example 11 upon focusing on an object point at infinity. FIG. 14 is an aberration diagram for Example 12 upon focusing on an object point at infinity. It is a figure similar to FIG. 1 of Example 10 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 11 of the zoom lens of this invention. It is the same figure as FIG. 1 of Example 12 of the zoom lens of this invention. It is a figure explaining the amount of aspherical deviation.

Explanation of symbols

G1 ... 1st lens group G2 ... 2nd lens group G3 ... 3rd lens group G4 ... 4th lens group S ... Aperture stop F ... Low pass filter C ... Cover glass I ... Image surface 112 ... Operation part 113 ... Control part 114 ... Bus 115 ... Bus 116 ... Imaging drive circuit 117 ... Temporary storage memory 118 ... Image processing unit 119 ... Storage medium unit 120 ... Display unit 121 ... Setting information storage memory unit 122 ... Bus 124 ... CDS / ADC unit 140 ... Digital camera 141 ... Shooting optical system 142 ... Shooting optical path 143 ... Viewfinder optical system 144 ... Viewfinder optical path 145 ... Shutter button 146 ... Flash 147 ... Liquid crystal display monitor 149 ... CCD
150: cover member 151 ... processing means 152 ... recording means 153 ... finder objective optical system 155 ... erecting prism 157 ... field frame 159 ... eyepiece optical system 160 ... cover 161 ... focal length change button 162 ... setting change switch

Claims (48)

From the object side,
A first lens group having a positive refractive power;
A second lens group having negative refractive power;
A third lens group having positive refractive power;
A fourth group zoom lens having a positive refractive power,
At the time of zooming from the wide-angle end to the telephoto end, at least the first lens group, the second lens group, and the third lens group move to change the distance between the lens groups,
The second lens group is composed of three or less lenses,
A zoom lens satisfying the following conditional expression:
1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <6.0 (1A)
3.0 < _ft / _fw <20.0 (2A)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is.   2. The zoom lens according to claim 1, wherein the first lens group includes two or less lenses, and the number of positive lenses in the first lens group is only one. From the object side,
A first lens group having a positive refractive power;
A second lens group having negative refractive power;
A third lens group having positive refractive power;
A fourth group zoom lens having a positive refractive power,
During zooming from the wide-angle end to the telephoto end, the distance between the lens groups changes,
The first lens group is composed of two or less lenses, and the positive lens in the first lens group is only one lens,
The second lens group is composed of three or less lenses,
A zoom lens satisfying the following conditional expression:
1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <2.3 (1)
3.0 < _ft / _fw <12.0 (2)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. From the object side,
A first lens group having a positive refractive power;
A second lens group having negative refractive power;
A third lens group having positive refractive power;
A fourth lens group having a positive refractive power,
During zooming from the wide-angle end to the telephoto end, the distance between the lens groups changes,
The first lens group includes two lenses, a negative lens and a positive lens,
A zoom lens satisfying the following conditional expression:
0.20 <D _2w / f _t <0.35 (3)
However,
D _2w is the air spacing on the optical axis between the second lens group and the third lens group at the wide-angle end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
3.0 < _ft / _fw <12.0 (2)
However,
f _w is the focal length of the entire zoom lens system at the wide-angle end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
1.2 <(β _2t / β _2w ) / (β _3t / β _3w ) <2.3 (1)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
β _3w is the lateral magnification at the wide-angle end of the third lens group,
β _3t is the lateral magnification at the telephoto end of the third lens group,
It is.   The zoom lens according to claim 1, further comprising an aperture stop that moves integrally with the third lens group. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
_{0.40 <f 1 / f t <} 0.90 ··· (4)
However,
f ₁ is the focal length of the first lens group,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
0.10 <| f ₂ / f _t | <0.20 (5)
However,
f ₂ is the focal length of the second lens group,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
0.10 <f ₃ / _ft <0.30 (6)
However,
f ₃ is the focal length of the third lens group,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
_{0.10 <f 4 / f t <} 0.70 ··· (7)
However,
f ₄ is the focal length of the fourth lens group,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is.   12. The zoom according to claim 1, wherein the first lens group is a biconvex cemented lens including two lenses of a negative lens and a positive lens in order from the object side. lens. The zoom lens according to claim 12, wherein the following conditional expression is satisfied.
38.0 <ν _d1p −ν _d1n (8)
However,
ν _d1p is the Abbe number of the positive lens of the first lens group with respect to the d-line,
ν _d1n is the Abbe number for the d-line of the negative lens of the first lens group,
It is. The zoom lens according to claim 2, wherein the following conditional expression is satisfied.
62.0 <ν _d1p <95.0 (9)
However,
ν _d1p is the Abbe number for the d-line of the positive lens in the first lens group,
It is. The zoom lens according to claim 1, further comprising a positive lens having a convex object side surface and satisfying the following conditional expression on the most object side in the third lens group. .
62.0 <ν _d3p <95.0 (10)
However,
ν _d3p is the Abbe number for the d-line of the positive lens in the third lens group,
It is. The zoom lens according to claim 12, wherein the first lens group includes a negative lens that satisfies the following conditional expression.
1.85 <n _d1n <2.10 (11)
However,
n _d1n is the refractive index of the negative lens in the first lens group with respect to the d-line,
It is. The zoom lens according to claim 1, further comprising a negative lens having a concave object side surface and satisfying the following conditional expression on the most object side in the second lens group. .
1.76 <n _d2n <2.00 (12)
However,
n _d2n is a refractive index with respect to d-line of the negative lens in the second lens group,
It is. The zoom according to any one of claims 1 to 17, further comprising a positive lens that satisfies the following conditional expression at a most image side or second from the image side in the second lens group. lens.
1.80 <n _d2p <2.15 (13)
However,
n _d2p is the refractive index of the positive lens in the second lens group with respect to the d-line,
It is. The zoom lens according to any one of claims 1 to 18, wherein a biconcave negative lens that satisfies the following conditional expression is disposed closest to the object side in the second lens group.
−1.0 <SF _2n1 <0.8 (14)
However,
SF _2n1 = (R _2n1f + R _2n1r ) / (R _2n1f −R _2n1r )
R _2n1f is a paraxial radius of curvature of the object side surface of the negative lens disposed closest to the object side in the second lens group,
R _2n1r is a paraxial radius of curvature of the image side surface of the negative lens disposed closest to the object side in the second lens group,
It is. The second lens group has a positive lens and a negative lens on the image side of the biconcave negative lens,
The zoom lens according to claim 19, wherein the biconcave negative lens satisfies the following conditional expression.
−1.0 <SF _2n1 <0.0 (14 ′ ″) The zoom lens according to any one of claims 2 to 20, wherein the following conditional expression is satisfied.
−0.8 <SF _1p <−0.1 (15)
However,
SF _1p = as defined in _{(R 1pf + R 1pr) /} (R 1pf -R 1pr),
R _1pf is the paraxial radius of curvature of the object side surface of the positive lens in the first lens group,
R _1pr is the paraxial radius of curvature of the image side surface of the positive lens in the first lens group,
It is. The zoom lens according to any one of claims 1 to 21, wherein the following conditional expression is satisfied.
2.6 <β _2t / β _2w <6.0 (16)
However,
β _2w is the lateral magnification at the wide-angle end of the second lens group,
β _2t is the lateral magnification at the telephoto end of the second lens group,
It is. The zoom lens according to any one of claims 1 to 22, wherein the following conditional expression is satisfied.
1.2 <β _3t / β _3w <3.0 (17)
However,
β _2w is the lateral magnification at the wide-angle end of the third lens group,
β _2t is the lateral magnification at the telephoto end of the third lens group,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
0.7 <β _4t / β _4w <1.7 (18)
However,
β _4w is the lateral magnification at the wide-angle end of the fourth lens group,
β _4t is the lateral magnification at the telephoto end of the fourth lens group,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
_{0.4 <(D 2w + D 1t} ) / f t <0.9 ··· (19)
However,
D _2w is the air spacing on the optical axis between the second lens group and the third lens group at the wide-angle end,
D _1t is the air spacing on the optical axis between the first lens group and the second lens group at the telephoto end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to any one of claims 1 to 25, wherein the following conditional expression is satisfied.
0.2 <D _1t / _ft <0.5 (20)
However,
D _1t is the air spacing on the optical axis between the first lens group and the second lens group at the telephoto end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is. The zoom lens according to claim 1, wherein the following conditional expression is satisfied.
0.7 < _TL / _ft <1.5 (21)
However,
T _L is the distance on the optical axis from the top of the lens surface closest to the object side of the first lens group to the image plane at the telephoto end,
_ft is the focal length of the entire zoom lens system at the telephoto end,
It is.   The zoom lens according to claim 1, wherein the first lens group includes a cemented doublet in which a negative lens and a positive lens are cemented.   The zoom lens according to claim 4, wherein the second lens group includes three or less lenses.   The zoom lens according to any one of claims 1 to 29, wherein the second lens group includes a negative lens, a negative lens, and a positive lens in order from the object side.   The zoom lens according to any one of claims 1 to 29, wherein the second lens group includes a negative lens, a positive lens, and a negative lens in order from the object side.   The zoom lens according to any one of claims 1 to 29, wherein the second lens group includes two lenses, a negative lens and a positive lens.   The zoom lens according to claim 1, wherein the third lens group includes three or less lenses. The third lens group includes a positive lens, a positive lens, and a negative lens in order from the object side.
The zoom lens according to claim 33, wherein the negative lens is cemented with the adjacent positive lens to constitute a cemented doublet.   The zoom lens according to any one of claims 1 to 34, wherein the fourth lens group includes one positive lens.   The zoom lens according to any one of claims 1 to 35, wherein the first lens group has an aspheric lens surface.   The zoom lens according to any one of claims 1 to 36, wherein the second lens group has an aspheric lens surface.   The zoom lens according to claim 1, wherein the third lens group has an aspheric lens surface. The zoom lens according to claim 38, wherein a lens closest to the object side in the third lens group is a positive single lens having a double-sided aspheric surface.   The zoom lens according to any one of claims 1 to 39, wherein the fourth lens group has an aspheric lens surface. The first lens group, the second lens group, the third lens group, and the fourth lens group move during zooming,
41. The zoom lens according to claim 1, further comprising an aperture stop that moves integrally with the third lens group in the optical axis direction. Upon zooming from the wide angle end to the telephoto end,
The first lens group moves so as to be closer to the object side at the telephoto end than at the wide-angle end,
The second lens group moves;
The third lens group moves only to the object side,
The zoom lens according to claim 41, wherein the fourth lens group moves. Upon zooming from the wide angle end to the telephoto end,
The first lens group first moves to the object side and moves to be closer to the object side at the telephoto end than at the wide-angle end,
The second lens group first moves to the object side, and the moving direction is reversed during zooming.
The third lens group first moves to the object side and moves to be closer to the object side at the telephoto end than at the wide-angle end,
42. The zoom lens according to claim 41, wherein the fourth lens group moves so as to be closer to the image side at the telephoto end than at the wide-angle end.   44. The zoom lens according to claim 41, wherein the brightness stop is disposed between the second lens group and the third lens group.   5. The zoom lens according to claim 4, wherein the zoom lens is a four-group zoom lens including the first lens group, the second lens group, the third lens group, and the fourth lens group in order from the object side. Zoom lens. A zoom lens according to any one of claims 1 to 45;
An electronic imaging device, comprising: an electronic imaging device that is disposed on an image side of the zoom lens and converts an image formed by the zoom lens into an electrical signal.   The electronic imaging apparatus according to claim 46, further comprising a processing unit that electrically corrects distortion aberration of the zoom lens based on an electrical signal from the electronic imaging element. A zoom lens comprising: a double-sided aspherical lens in which both the object side surface and the image side surface have an aspheric shape, and the surface shape of both surfaces satisfies the following conditional expression:
−0.1 <(R _aspO + R _aspI ) / (R _aspO −R _aspI ) <0.1 (22)
In the range of 0 ≦ y ≦ R,
−10 ⁻⁴ <(X _{O (y)} + X _{I (y)} ) / (R _aspO −R _aspI ) <10 ⁻⁴ (23)
However,
X _{O (R)} ≠ 0,
X _{I (R)} ≠ 0,
And
R _aspO is the paraxial radius of curvature of the object side surface of the double-sided aspheric lens,
R _aspI is the paraxial radius of curvature of the image side surface of the double-sided aspheric lens,
y is the distance from the optical axis,
R is the smaller value of the effective radii of the object side surface and the image side surface of the double-sided aspheric lens,
X _{O (y)} and X _{I (y)} are the aspherical deviation amounts at the distance y on the object side surface and the image side surface of the double-sided aspheric lens
It is.

Images