JP4917922B2 - Zoom lens system, imaging device and camera - Google Patents

Description

  The present invention relates to a zoom lens system, an imaging device, and a camera. In particular, the present invention not only has a high resolution, but also has a sufficiently high peripheral illuminance in the entire zoom range, a high ability to correct curvature of field, and a short optical total length when not in use. The present invention relates to an imaging apparatus using a zoom lens system and a camera including the imaging apparatus.

  2. Description of the Related Art Conventionally, many optical devices that form an image of a subject on an image sensor via a lens and capture the image as an image have been developed. Recently, products such as digital still cameras and digital video cameras have become widespread, and as the number of users increases, the demand for these products has also increased. Among various product forms, an optical device having a zoom ratio of about 3 times is relatively small and has an optical zoom function, and is particularly popular as a digital camera classified into a compact type and a stylish type.

  The compact digital camera is required to be further miniaturized in order to facilitate carrying. In order to achieve further miniaturization of digital cameras, the overall optical length when not in use (distance from the apex of the lens surface closest to the object side to the image plane in the entire lens system) is shortened, and the main body is used with a multistage barrel when in use. It is necessary to have a lens arrangement that can store the lens element that protrudes before the main body.

  By the way, as a zoom lens system suitable for a compact digital still camera, for example, in order from the object side to the image side, a negative power first lens group, a positive power second lens group, and a positive power third lens are used. Many zoom lens systems having a three-group configuration in which a lens group is arranged have been proposed.

  In the zoom lens system having the three-group structure as described above, the air space between the first lens group and the second lens group monotonously decreases during zooming from the wide-angle end to the telephoto end. And the third lens group is configured to be fixed or moved.

  Focus adjustment in a zoom lens system having a three-group configuration is performed by moving the first lens group or the third lens group in the optical axis direction. In particular, in order to reduce the size of the entire optical apparatus, focus adjustment is often performed with a lightweight third lens group, and the focus is adjusted on a subject at an infinite distance to a short distance. On the other hand, when focus adjustment is performed using the first lens group, the first lens group is larger than the third lens group, so a large motor is required, and the entire optical apparatus tends to be large.

  The third lens group with positive power normally corrects the curvature of field and makes the incident light on the light receiving surface of the image sensor telecentric. The third lens group is often composed of one or two lens elements having a small outer diameter, and can be driven at high speed using a small motor. Therefore, when the third lens group is a lens group for focus adjustment, it is possible to provide an optical device that is small and capable of focusing in a short time.

  Both the first lens group and the second lens group move in parallel along the optical axis along a cam groove cut in the cylindrical cam. The cam groove is connected to the zooming groove and the non-use groove, and the non-use groove has a configuration in which the distance between the lens groups is reduced and all three lens groups are moved toward the image sensor. By taking it, it becomes possible to shorten the optical total length when not in use. In this case, if the thickness of each lens group is small, the optical total length when not in use can be further shortened.

  As described above, conventionally, the zoom lens system is configured as described above, and a device for engaging in the focus adjustment and the entire lens system when not in use are designed to be small, and the total optical length of the digital still camera is shortened.

  For example, Patent Document 1 discloses, in order from the object side to the image side, a negative power first lens group composed of a negative power lens and a positive power lens having an aspherical surface, a positive power second lens group, and a positive power lens. A three-group zoom lens comprising a power third lens group is disclosed. In such a three-group zoom lens, by increasing the refractive index of the negative power lens closest to the object side in the first lens group, while correcting the curvature of field at the wide-angle end, the lens thickness at the peripheral portion is suppressed to be small. The entire lens group is thinned to reduce the size of the optical system.

  Further, for example, Patent Document 2 includes, in order from the object side to the image side, a negative power first lens group, a positive power second lens group having a stop, and a positive power third lens group. When zooming, the first lens group moves so as to be relatively close to the second lens group, the second lens group monotonously moves to the object side, and the third lens group moves to the object side and then reverses. When the object distance is infinity, a three-unit zoom lens is disclosed in which the position at the wide angle end is closer to the object side than the position at the telephoto end. In such a three-group zoom lens, the focal length condition of the first lens group is defined so that correction of curvature of field and downsizing of the optical system are compatible.

  Furthermore, recently, new optical materials having a refractive index and an Abbe number that could not exist in the past have become relatively easily available. Thus, there has been a proposal for reducing the size of the optical system by applying such an optical material to a lens included in a zoom lens.

For example, Patent Document 3 discloses, in order from the object side to the image side, a negative power first lens group including a negative power lens and a positive power lens having an aspherical surface, a positive power second lens group, and a positive power lens. A zoom lens is disclosed that includes a power third lens group and uses a lens element having a refractive index exceeding 1.9 in the first lens group.
JP 2005-134746 A Japanese Patent Laying-Open No. 2005-084597 JP 2006-011096 A

  However, in the configuration of the three-group zoom lens disclosed in Patent Document 1, since the positive power lens on the image side of the first lens group has a low refractive index and is a spherical lens, correction of field curvature is insufficient. There is a problem that.

  In the configuration of the three-group zoom lens disclosed in Patent Document 2, the focal length of the first lens group is set to be short in order to reduce the size. However, in this case, although the radial direction of the lens can be made relatively small, if the first lens group is composed of two lenses, the power of the object side lens is increased, and the thickness of the image side lens is also increased in order to correct chromatic aberration. It gets bigger. As a result, there is a problem that the total optical length when not in use is increased.

  In addition, the zoom lens configuration disclosed in Patent Document 3 has a problem that the incident angle of light incident on the image sensor is particularly large at the wide-angle end. When the incident angle increases in this way, a light amount loss occurs due to the shading characteristics of the image sensor, and the peripheral light amount of the captured image decreases. Further, the zoom lens configuration disclosed in Patent Document 3 has a problem in that the appearance of the image in the peripheral portion varies greatly because the variation in the incident angle during zooming is large.

  The present invention has been made in order to solve the above-described problems in the background art. In addition to high resolution, the present invention has a sufficient peripheral illumination intensity in the entire zoom range and the ability to correct curvature of field. An object of the present invention is to provide a zoom lens system that is high and has a short optical total length when not in use, an imaging device using the zoom lens system, and a camera equipped with the imaging device.

The object is achieved by the following zoom lens system. That is, the zoom lens system of the present invention is a zoom lens system for forming an optical image of an object so as to be variable in magnification, and in order from the object side to the image side, the first lens group having a negative power and the positive lens group. a second lens group of power, and a third lens group of positive power, upon zooming from the wide-angle end to the telephoto end, the interval between the first lens group and the second lens group decreases, and the second lens Each lens group is moved along the optical axis so as to change the distance between the group and the third lens group, and zooming is performed. The first lens group is a single object with a convex surface facing the object side. A first negative lens element, and a first positive lens element having a convex surface directed toward the object side and spaced apart from the image side of the negative object lens element. Each of the two lens elements constituting the lens element has an aspheric surface, and the following condition (1) (2), (3) and (9):
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
(here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is the half angle of view at the wide-angle end)
It is characterized by satisfying.

The object is achieved by the following imaging device. That is, the imaging apparatus of the present invention is an imaging apparatus capable of converting an optical image of a subject into an electrical image signal and outputting the same, and a zoom lens system that forms the optical image of the subject so that the magnification can be changed. And an image sensor that converts an optical image of a subject formed by the zoom lens system into an electrical image signal, and the zoom lens system is sequentially from the object side that is the subject side to the image side, a first lens unit having a negative power, a second lens group having positive power, and a third lens group of positive power, upon zooming from the wide-angle end to the telephoto end, the first lens group and the second lens group The first lens group is moved by moving the respective lens groups along the optical axis so that the distance between the second lens group and the third lens group is changed. One object-side negative lens element with a convex surface facing the side, The two lens elements constituting the first lens group are composed of one image-side positive lens element having a convex surface facing the object side and arranged on the image side of the body-side negative lens element with an air gap. , Each of which has an aspherical surface, and the following conditions (1), (2) , (3) and (9) :
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
(here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is the half angle of view at the wide-angle end)
It is characterized by satisfying.

Furthermore, the object is achieved by the following camera. That is, the camera of the present invention is a camera capable of photographing a subject and outputting it as an electrical image signal, and a zoom lens system that forms an optical image of the subject so as to be variable, and the zoom lens system. An image pickup device that converts an optical image of the subject formed by the image sensor into an electrical image signal, and the zoom lens system has negative power in order from the object side to the image side that is the subject side. a first lens group, a second lens group having positive power, and a third lens group of positive power, upon zooming from the wide-angle end to the telephoto end, the interval between the first lens group and the second lens group And the zooming is performed by moving each lens group along the optical axis so that the distance between the second lens group and the third lens group is changed, and the first lens group is moved toward the object side. One object-side negative lens element with the convex surface facing; Two lens elements constituting the first lens group, including one image-side positive lens element having a convex surface directed toward the object side and spaced from the image side of the object-side negative lens element. Are all aspheric, and the following conditions (1), (2) , (3) and (9) :
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
(here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is the half angle of view at the wide-angle end)
It is characterized by satisfying.

  According to the present invention, not only the resolution is high, but also the peripheral illuminance is sufficiently ensured in the entire zooming range, and the thickness of the first lens unit is small while correcting the field curvature well, when not in use. A zoom lens system having a short optical total length and an imaging device using the zoom lens system can be provided. Furthermore, according to the present invention, it is possible to provide a small and high-performance camera equipped with such an imaging device.

(Embodiments 1 to 3 and Reference Embodiments 1 to 2 )
FIG. 1 is a configuration diagram of a zoom lens system according to the first embodiment. FIG. 3 is a configuration diagram of a zoom lens system according to the second embodiment. Figure 5 is a construction diagram of a zoom lens system according to Embodiment 1 of the reference. FIG. 7 is a configuration diagram of a zoom lens system according to Embodiment 3 . FIG. 9 is a configuration diagram of a zoom lens system according to Reference Embodiment 2 . Each figure shows a zoom lens system in an infinite focus state. In each figure, (a) is a lens configuration at the wide-angle end (shortest focal length state: focal length f _W ), and (b) is a substantially intermediate position (intermediate focal length state: focal length f _M = √ (f _W * f). _T )) and (c) represent the telephoto end (longest focal length state: focal length f _T ), respectively.

In each of the zoom lens systems according to Embodiments 1 to 3 and Reference Embodiments 1 to 2 , in order from the object side to the image side, the negative lens first lens group G1, the aperture A, and the positive power A second lens group G2 and a positive power third lens group G3 are provided. In the zoom lens systems according to Embodiments 1 to 3 and Reference Embodiments 1 to 2, when zooming from the wide-angle end to the telephoto end, the first lens group G1 moves along a locus that is convex toward the image side, The second lens group G2 and the aperture stop A move monotonously toward the object side, and the third lens group G3 moves while changing the distance from the second lens group G2. That is, in the zoom lens systems according to Embodiments 1 to 3 and Reference Embodiments 1 to 2, the distance between the first lens group G1 and the second lens group G2 decreases during zooming from the wide-angle end to the telephoto end. In addition, each lens group is moved along the optical axis so that the distance between the second lens group G2 and the third lens group G3 changes. In each figure, the straight line described on the rightmost side in the figure represents the position of the image plane S, and on the object side, a parallel flat plate P equivalent to an IR (infrared) cut filter, a face plate of an image sensor, or the like. Is provided.

  As shown in FIG. 1, in the zoom lens system according to Embodiment 1, the first lens group G1 includes a negative meniscus object-side negative lens element having a convex surface directed toward the object side in order from the object side to the image side. L1 and a positive meniscus image-side positive lens element L2 having a convex surface facing the object side and spaced apart from the image side of the object-side negative lens element L1. Each of the object-side negative lens element L1 and the image-side positive lens element L2 has an aspheric image side surface.

  In the zoom lens system according to Embodiment 1, the second lens group G2 includes, in order from the object side to the image side, a positive meniscus third lens element L3 with a convex surface facing the object side, and a convex surface facing the object side. Negative meniscus fourth lens element L4, negative meniscus fifth lens element L5 having a convex surface facing the object side, and biconvex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are positively cemented lens elements joined together, and the fifth lens element L5 and the sixth lens element L6 are positively joined lens elements joined together. is there. The third lens element L3 that is the most object side lens element of the second lens group G2 has an aspheric object side surface.

  In the zoom lens system according to Embodiment 1, the third lens unit G3 comprises solely a positive meniscus seventh lens element L7 with the convex surface facing the image side. The seventh lens element L7 has an aspheric image side surface.

  In the zoom lens system according to Embodiment 1, as shown in Table 16 later, the refractive index of the image-side positive lens element L2 constituting the first lens group G1 is particularly high, and the ray height at the object-side negative lens element L1 is high. The thickness of the high portion can be easily secured and the lens thickness can be reduced. Therefore, the zoom lens system according to Embodiment 1 has a short optical total length when not in use.

  As shown in FIG. 3, in the zoom lens system according to Embodiment 2, the first lens group G1 includes a negative meniscus object-side negative lens element having a convex surface directed toward the object side in order from the object side to the image side. L1 and a positive meniscus image-side positive lens element L2 having a convex surface facing the object side and spaced apart from the image side of the object-side negative lens element L1. Each of the object-side negative lens element L1 and the image-side positive lens element L2 has an aspheric image side surface.

  In the zoom lens system according to Embodiment 2, the second lens group G2 includes, in order from the object side to the image side, a positive meniscus third lens element L3 with a convex surface facing the object side, and a convex surface facing the object side. Is formed of a positive meniscus fourth lens element L4 with a convex surface, a negative meniscus fifth lens element L5 with a convex surface facing the object side, and a biconvex sixth lens element L6. Among these, the fourth lens element L4 and the fifth lens element L5 are cemented lens elements that are cemented with each other. The third lens element L3 that is the most object side lens element of the second lens group G2 has an aspheric object side surface.

  In the zoom lens system according to Embodiment 2, the third lens unit G3 comprises solely a bi-convex seventh lens element L7. The seventh lens element L7 has an aspheric image side surface.

  In the zoom lens system according to Embodiment 2, as shown in Table 16 later, the refractive index of the image-side positive lens element L2 constituting the first lens group G1 is relatively high, and even if the lens center thickness is reduced, the zoom lens system is not covered. It is relatively easy to ensure the thickness, and the lens thickness can be reduced. Therefore, the zoom lens system according to Embodiment 2 has a short optical total length when not in use.

As shown in FIG. 5, in the zoom lens system according to Reference Embodiment 1 , the first lens group G1 includes, in order from the object side to the image side, a biconcave object-side negative lens element L1, and the object The positive negative meniscus image side positive lens element L2 having a convex surface facing the object side is arranged on the image side of the negative side lens element L1 with an air gap. Each of the object-side negative lens element L1 and the image-side positive lens element L2 has an aspheric image side surface.

In the zoom lens system according to Reference Embodiment 1 , the second lens group G2 includes, in order from the object side to the image side, a positive meniscus third lens element L3 having a convex surface directed toward the object side, and an object side A negative meniscus fourth lens element L4 with a convex surface facing the surface, a negative meniscus fifth lens element L5 with a convex surface facing the object side, and a biconvex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are positively cemented lens elements joined together, and the fifth lens element L5 and the sixth lens element L6 are positively joined lens elements joined together. is there. The third lens element L3 that is the most object side lens element of the second lens group G2 has an aspheric object side surface.

In the zoom lens system according to Reference Embodiment 1 , the third lens unit G3 includes solely a positive meniscus seventh lens element L7 with the convex surface facing the image side. The seventh lens element L7 has an aspheric image side surface.

In the zoom lens system according to Reference Embodiment 1 , as shown later in Table 16, the refractive index of the object-side negative lens element L1 constituting the first lens group G1 is low, and the thickness of the portion where the light beam height is high is small. It has become. However, since the refractive index of the image side positive lens element L2 of the first lens group G1 is relatively high and the image side has an aspherical surface, the light ray height of the object side negative lens element L1 is high. thickness is small, even if the correction of distortion and field curvature at the wide angle end is insufficient, the effect of correcting the image side positive lens element L2, the entire zoom lens system according to embodiment 1 of the reference image side positive lens distortion and curvature of field at the wide-angle end side element L2 can be compensation.

As shown in FIG. 7, in the zoom lens system according to Embodiment 3 , the first lens group G1 includes a negative meniscus object-side negative lens element having a convex surface directed toward the object side in order from the object side to the image side. L1 and a positive meniscus image-side positive lens element L2 having a convex surface facing the object side and spaced apart from the image side of the object-side negative lens element L1. Each of the object-side negative lens element L1 and the image-side positive lens element L2 has an aspheric image side surface.

In the zoom lens system according to Embodiment 3 , the second lens group G2 includes, in order from the object side to the image side, a biconvex third lens element L3, a biconcave fourth lens element L4, A negative meniscus fifth lens element L5 having a convex surface facing the object side and a biconvex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are positively cemented lens elements joined together, and the fifth lens element L5 and the sixth lens element L6 are positively joined lens elements joined together. is there. The third lens element L3 that is the most object side lens element of the second lens group G2 has an aspheric object side surface.

In the zoom lens system according to Embodiment 3 , the third lens unit G3 comprises solely a bi-convex seventh lens element L7. The seventh lens element L7 has an aspheric image side surface.

In the zoom lens system according to Embodiment 3 , since the two lens elements L1 and L2 constituting the first lens group G1 are brought into contact with each other in the vicinity where the light beam from the object passes, the thickness of the entire first lens group G1 is reached. Can be reduced. Further, even if the object-side negative lens element L1 and the image-side positive lens element L2 of the first lens group G1 approach each other and the ability to correct distortion is reduced, the image-side positive lens element L2 is later shown in Table 16. In addition, since the lens element has a relatively high refractive index and an aspheric surface on the image side, the entire zoom lens system according to Embodiment 3 can satisfactorily correct distortion at the wide-angle end.

As shown in FIG. 9, in the zoom lens system according to Reference Embodiment 2 , the first lens unit G1 has a negative meniscus object-side negative with a convex surface facing the object side in order from the object side to the image side. The lens element L1 is composed of two elements: a positive meniscus image side positive lens element L2 having a convex surface facing the object side, which is disposed with an air gap on the image side of the object side negative lens element L1. Each of the object-side negative lens element L1 and the image-side positive lens element L2 has an aspheric image side surface.

In the zoom lens system according to Reference Embodiment 2 , the second lens group G2 includes, in order from the object side to the image side, a biconvex third lens element L3 and a biconcave fourth lens element L4. And a biconvex fifth lens element L5. Among these, the third lens element L3 and the fourth lens element L4 are positively cemented lens elements joined together. The third lens element L3 that is the most object side lens element of the second lens group G2 has an aspheric object side surface.

In the zoom lens system according to Embodiment 2 of the reference, the third lens unit G3 includes only the sixth lens element L6 of a positive meniscus shape with a convex surface facing the image side. The sixth lens element L6 has two aspheric surfaces.

In the zoom lens system according to Reference Embodiment 2 , as shown in Table 16 later, in particular, the refractive index of the image-side positive lens element L2 constituting the first lens group G1 is relatively high, and the object-side negative lens element L1. can ray height Hoshi sure the thickness of the high part, to reduce the lens thickness at. Therefore, the zoom lens system according to Reference Embodiment 2 has a short optical total length when not in use.

As described above, the zoom lens systems according to Embodiments 1 to 3 can reduce the size of the entire lens system while maintaining excellent optical performance by arranging the lens groups G1 to G3 in a desired power arrangement. ing.

In particular, in the zoom lens systems according to Embodiments 1 to 3 , the first lens unit G1 has one object-side negative lens element with the convex surface facing the object side and one image-side positive lens with the convex surface facing the object side. The second lens group G2 is composed of two pairs of positively cemented lens elements each composed of two lens elements, or one pair of cemented lens elements from the object side and the image side. The third lens group G3 is composed of a single lens element. Thus, the zoom lens systems according to Embodiments 1 to 3 are lens systems in which the number of lens elements constituting each lens group is small, and the optical total length when not in use is short.

In the zoom lens systems according to Embodiments 1 to 3 , as described above, the second lens group G2 is composed of two pairs of positively-joined lens elements, or one pair of cemented lens elements is arranged on the object side and the image side. However, in addition to this, for example, it may be composed of a pair of positive cemented lens elements and one positive lens element in order from the object side to the image side. After all, a lens system having a short optical total length when not in use can be obtained.

Furthermore, in the zoom lens systems according to Embodiments 1 to 3 , the two object-side negative lens elements and the image-side positive lens element that form the first lens group G1 both have aspheric surfaces, and The positive lens element has a specific refractive index and Abbe number. Therefore, the zoom lens systems according to Embodiments 1 to 3 are particularly excellent in optical performance such as a field curvature correction capability.

Hereinafter, as in the zoom lens systems according to Embodiments 1 to 3 , for example, in order from the object side to the image side, a first lens unit having a negative power, a second lens unit having a positive power, and a third lens having a positive power. consists of a lens group, the first lens unit is composed of a single object-side negative lens element having a convex surface directed toward the object side, and one image-side positive lens element with the convex surface facing the object side, A condition that the zoom lens system in which each of the two lens elements constituting the first lens group has an aspheric surface will be described. In the zoom lens system according to each embodiment, a plurality of conditions to be satisfied are defined, but the configuration of the zoom lens system that satisfies all the conditions is most desirable. However, by satisfying individual conditions, it is possible to obtain a zoom lens system that exhibits corresponding effects.

For example, a zoom lens system such as the zoom lens systems according to Embodiments 1 to 3 satisfies the following conditions (1), (2), and (3).
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
(However, ω _W > 30)
here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
ω _W is a half angle of view at the wide angle end.

The conditions (1) and (2) are conditions that define the refractive index and Abbe number of the image-side positive lens element constituting the first lens group. Satisfying these conditions (1) and (2) reduces the center thickness of the image-side positive lens element, and further suppresses curvature of field at the wide-angle end without increasing the curvature, particularly the curvature of the image side surface. In addition, since it is easy to secure the edge thickness, the thickness of the first lens group can be reduced. Therefore, the thickness of the entire zoom lens system is also reduced, and the total optical length when not in use can be shortened. In particular, when the condition (1) is satisfied, the Z value (difference between the curvature of the object side surface and the curvature of the image side surface) of the image side positive lens element of the first lens group can be increased, and the centering of the lens can be achieved. It becomes easier. In particular, when the condition (2) is satisfied, the chromatic aberration generated in the first lens group can be corrected more satisfactorily.

  The condition (3) is an expression that defines the incident angle of the chief ray at the maximum image height at the wide-angle end. By satisfying the condition (3), the incidence angle of the most off-axis chief ray incident on the image sensor is reduced, so that the influence of shading is reduced. If the upper limit of the condition (3) is exceeded, the image sensor There is a risk that the amount of peripheral light may be reduced due to the influence of shading. If the lower limit of the condition (3) is not reached, the angle of the negative most off-axis principal ray at the telephoto end becomes large at the time of zooming, and there is a concern that the peripheral light amount at the telephoto end may be reduced.

Further, by satisfying the following condition (3) ′, the change in the incident angle of the chief ray at the maximum image height during zooming is suppressed, so that fluctuations in the amount of peripheral light are also suppressed, which is particularly effective. is there.
αi _W <15.0 (3) '

For example, a zoom lens system like the zoom lens systems according to Embodiments 1 to 3 preferably satisfies the following conditions (4), (5), (6), and (7).
n11> 1.50 (4)
ν11> 35 (5)
n12-n11> 0.10 (6)
ν11−ν12> 15.0 (7)
here,
n11: Refractive index of the object side negative lens element of the first lens group,
ν11: Abbe number of the object side negative lens element of the first lens unit,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens unit.

  The conditions (4) and (5) are conditions that define the refractive index and Abbe number of the object-side negative lens element constituting the first lens group. Conditions (6) and (7) are zoom lens systems in which the first lens group is a negative lead having negative power, and the first lens group is composed of an object-side negative lens element and an image-side positive lens element. This is a condition for satisfactorily correcting the chromatic aberration. By satisfying these conditions (4), (5), (6), and (7), the thickness in the optical axis direction of the lens element increases as the light beam height increases, and the center thickness is increased in order to increase the productivity. Increasing the value eliminates the risk of further increasing the thickness of the entire first lens group and corrects chromatic aberration satisfactorily.

In addition, the above effect can be further achieved by further satisfying at least one of the following conditions (4) ′, (5) ′, (6) ′, and (7) ′. Further, by satisfying at least one of the following conditions (5) ″ and (7) ″, chromatic aberration generated in the first lens group can be corrected more satisfactorily.
n11> 1.75 (4) ′
ν11> 38 (5) ′
65> ν11 (5) ''
n12-n11> 0.12 (6) ′
ν11−ν12> 17.5 (7) ′
45.0> ν11−ν12 (7) ″

For example, a zoom lens system like the zoom lens system according to Embodiments 1 to 3 preferably satisfies the following condition (8).
T1 / Y <1.5 (8)
here,
T1: Center thickness of the first lens group,
Y: Maximum image height.

  The condition (8) is a condition that defines the center thickness of the first lens group in a zoom lens system that tends to be large because the first lens group is a negative lead having negative power. By satisfying the condition (8), it is possible to eliminate the possibility that the thickness of the first lens group becomes too large and the optical total length when not in use is increased.

Further, by satisfying the following condition (8) ′, it is possible to give power to the air lens in the first lens group, so that it becomes easier to correct curvature of field especially on the wide angle side.
0.8 <T1 / Y (8) '

Further, for example, the zoom lens system like the zoom lens system according to Embodiment 1-3 of the embodiment is characterized by satisfying the following condition (9).
2.5 < (T1 + T2 + T3) / Y < 3.2 (9)
here,
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height.

The condition (9) is a condition that defines the sum of the center thicknesses of the lens groups. By satisfying the upper limit value of the condition (9) , it is possible to eliminate the possibility that the total thickness of the lens groups becomes too large and the optical total length when not in use becomes long. Further, by satisfying the lower limit value of the condition (9), it is possible to secure the thickness of each lens group, particularly the thickness of the first lens group and the thickness of the second lens group, and more favorable field curvature. Correction is possible.

For example, a zoom lens system like the zoom lens systems according to Embodiments 1 to 3 preferably satisfies the following condition (10).
3.0 <f ₃ / f _W <5.5 (10)
(However, ω _W > 30)
here,
f ₃ : focal length of the third lens group,
f _W : focal length at the wide-angle end of the entire system,
ω _W is a half angle of view at the wide angle end.

  The condition (10) is an expression that defines an appropriate focal length of the third lens group. If the lower limit of the condition (10) is not reached, the power of the third lens group becomes large, and it becomes difficult to correct spherical aberration and coma aberration in the variable power range where the third lens group is relatively close to the object side. If the upper limit of the condition (10) is exceeded, the power of the third lens group becomes small, the amount of movement of the third lens group becomes large, and it becomes difficult to reduce the size of the optical system.

Furthermore, the above effect can be further achieved by further satisfying at least one of the following conditions (10) ′ and (10) ″.
3.8 <f ₃ / f _W (10) ′
f ₃ / f _W <4.4 (10) ''

For example, a zoom lens system like the zoom lens systems according to Embodiments 1 to 3 preferably satisfies the following condition (11).
| Αi _W −αi _T | <15.0 (11)
(However, ω _W > 30)
here,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
αi _T : imaging element incident angle of the principal ray at the maximum image height at the telephoto end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis),
ω _W is a half angle of view at the wide angle end.

  The condition (11) is an expression that defines the incident angle of the chief ray at the maximum image height during zooming. By satisfying the condition (11), the change in the incident angle of the most off-axis chief ray incident on the image sensor is reduced, so that the variation in the appearance of the peripheral image is maintained within an allowable range.

  Note that it is particularly preferable that the illuminance around the image can be appropriately maintained by satisfying the condition (3) and the condition (11) at the same time.

Each lens group constituting the zoom lens system according to Embodiments 1 to 3 and Reference Embodiments 1 to 2 includes a refractive lens element that deflects incident light by refraction (that is, a medium having a different refractive index). However, the present invention is not limited to this. For example, a diffractive lens element that deflects incident light by diffraction, a refractive / diffractive hybrid lens element that deflects incident light by a combination of diffractive action and refractive action, and a refractive index that deflects incident light according to the refractive index distribution in the medium Each lens group may be composed of a distributed lens element or the like.

In the zoom lens systems according to Embodiments 1 to 3 and Reference Embodiments 1 to 2 , the optical path may be bent before, after, or in the middle of the zoom lens system by disposing the reflecting surface in the optical path. . The folding position may be set as necessary, and the apparent thinning of the camera can be achieved by appropriately bending the optical path.

  As described above, according to the present invention, it is possible to obtain a zoom lens system in which the curvature of the field is satisfactorily corrected, the first lens group is thin, and the optical total length when not in use is short.

(Embodiment 4 )
FIG. 11 is a schematic configuration diagram of a digital still camera according to the fourth embodiment. In FIG. 11, the digital still camera includes an image pickup apparatus including a zoom lens system 1 and an image pickup device 2 that is a CCD, a liquid crystal monitor 3, and a housing 4. As the zoom lens system 1, the zoom lens system according to Embodiment 1 is used. In FIG. 11, the zoom lens system 1 includes a first lens group G1, a diaphragm A, a second lens group G2, and a third lens group G3. In the housing 4, the zoom lens system 1 is disposed on the front side, and the imaging element 2 is disposed on the rear side of the zoom lens system 1. A liquid crystal monitor 3 is disposed on the rear side of the housing 4, and an optical image of the subject by the zoom lens system 1 is formed on the image plane S.

  The lens barrel includes a main lens barrel 5, a movable lens barrel 6, and a cylindrical cam 7. When the cylindrical cam 7 is rotated, the first lens group G1, the second lens group G2, and the third lens group G3 are moved to predetermined positions with reference to the image sensor 2, and the magnification is changed from the wide-angle end to the telephoto end. It can be performed. The third lens group G3 is movable in the optical axis direction by a focus adjustment motor.

Thus, by using the zoom lens system according to Embodiment 1 for a digital still camera, it is possible to provide a small digital still camera that has a high ability to correct resolution and curvature of field and has a short optical total length when not in use. it can. Note that the digital still camera shown in FIG. 11 may use any of the zoom lens systems according to Embodiments 2 to 3 instead of the zoom lens system according to Embodiment 1. Further, the optical system of the digital still camera shown in FIG. 11 can be used for a digital video camera for moving images. In this case, not only a still image but also a moving image with high resolution can be taken.

In addition, an imaging apparatus including the zoom lens system according to Embodiments 1 to 3 described above and an imaging element such as a CCD or a CMOS is used as a monitoring camera in a mobile phone device, a PDA (Personal Digital Assistance), or a monitoring system. It can also be applied to Web cameras, in-vehicle cameras, and the like.

ここで、ｈは光軸からの高さ、ｃは曲率、ｋはコーニック定数、Ａ、Ｂ、Ｃ、Ｄ及びＥはそれぞれ４次、６次、８次、１０次及び１２次の非球面係数である。 Hereinafter, numerical examples and numerical reference examples in which the zoom lens systems according to Embodiments 1 to 3 and Reference Embodiments 1 to 2 are specifically implemented will be described. In each numerical example and numerical reference example , the units of length in the tables are all mm, the units of angles are all degrees, r is the radius of curvature, d is the surface spacing, and nd is the refractive index at the d-line. , Νd represents the Abbe number in the d-line. In each numerical example and numerical reference example , the surface marked with * is an aspheric surface, and the sag z of the aspheric surface is defined by the following equation.

Here, h is the height from the optical axis, c is the curvature, k is the conic constant, A, B, C, D and E are the 4th, 6th, 8th, 10th and 12th aspherical coefficients, respectively. It is.

Example 1
The zoom lens system of Example 1 corresponds to Embodiment 1 shown in FIG. The lens data of the zoom lens system of Example 1 is shown in Table 1, the aspherical data is shown in Table 2, and the focal length f, F number, angle of view 2ω, optical total length L, and variable surface distance data when the shooting distance is ∞. Table 4 shows d4, d11, and d13.

(Example 2)
The zoom lens system of Example 2 corresponds to Embodiment 2 shown in FIG. The lens data of the zoom lens system of Example 2 is shown in Table 4, the aspherical data is shown in Table 5, and the focal length f, F number, angle of view 2ω, optical total length L, and variable surface distance data when the shooting distance is ∞. Table 6 shows d4, d12, and d14.

( Reference Example 1 )
The zoom lens system of Reference Example 1 corresponds to Reference Embodiment 1 shown in FIG. The lens data of the zoom lens system of Reference Example 1 is shown in Table 7, the aspherical data is shown in Table 8, and the focal length f, F number, angle of view 2ω, optical total length L, and variable surface distance data when the shooting distance is ∞. Table 9 shows d4, d11, and d13.

(Example 3 )
The zoom lens system of Example 3 corresponds to the third embodiment shown in FIG. The lens data of the zoom lens system of Example 3 is shown in Table 10, the aspherical data is shown in Table 11, and the focal length f, F number, angle of view 2ω, optical total length L, and variable surface interval data when the shooting distance is ∞. Table 12 shows d4, d11, and d13.

( Reference Example 2 )
The zoom lens system of Reference Example 2 corresponds to Reference Embodiment 2 shown in FIG. The lens data of the zoom lens system of Reference Example 2 is shown in Table 13, the aspherical data is shown in Table 14, and the focal length f, F number, angle of view 2ω, optical total length L, and variable surface distance data when the shooting distance is ∞. Table 4 shows d4, d10, and d12.

Table 16 below shows corresponding values of the conditions in Examples 1 to 3 and Reference Examples 1 and 2 .

2 is a longitudinal aberration diagram of the zoom lens system of Example 1. FIG. FIG. 4 is a longitudinal aberration diagram of the zoom lens system of Example 2. 6 is a longitudinal aberration diagram of the zoom lens system of Reference Example 1. FIG. FIG. 8 is a longitudinal aberration diagram of the zoom lens system of Example 3 . 10 is a longitudinal aberration diagram of the zoom lens system of Reference Example 2. FIG.

  In each longitudinal aberration diagram, (a) shows the respective aberrations at the wide-angle end, (b) at the substantially intermediate position, and (c) at the telephoto end. Each longitudinal aberration diagram shows spherical aberration, astigmatism, and distortion aberration in order from the left side. In the spherical aberration diagram, the vertical axis represents the F number, the solid line is the d line, the short broken line is the F line, and the long broken line is the C line characteristic. In the astigmatism diagram, the vertical axis represents the half angle of view ω, the solid line is the sagittal plane (indicated by s), and the broken line is the meridional plane (indicated by m in the figure). In the distortion diagram, the vertical axis represents the half angle of view ω.

  The zoom lens system according to the present invention is applicable to cameras such as a digital still camera, a digital video camera, a mobile phone device, a PDA (Personal Digital Assistance), a surveillance camera in a surveillance system, a web camera, and an in-vehicle camera. It is suitable for cameras that require high image quality, such as still cameras and digital video cameras.

Configuration diagram of a zoom lens system according to Embodiment 1 (Example 1) Longitudinal aberration diagram of the zoom lens system of Example 1 Configuration diagram of a zoom lens system according to Embodiment 2 (Example 2) Longitudinal aberration diagram of the zoom lens system of Example 2 Construction diagram of a zoom lens system according to Embodiment 1 of Reference (Example 1) Longitudinal aberration diagram of zoom lens system of Reference Example 1 Configuration diagram of a zoom lens system according to Embodiment 3 (Example 3 ) Longitudinal aberration diagram of the zoom lens system of Example 3 Construction diagram of a zoom lens system according to Embodiment 2 of Reference (Example 2) Longitudinal aberration diagram of zoom lens system of Reference Example 2 Schematic configuration diagram of a digital still camera according to Embodiment 4

G1 1st lens group G2 2nd lens group G3 3rd lens group L1 1st lens element L2 2nd lens element L3 3rd lens element L4 4th lens element L5 5th lens element L6 6th lens element L7 7th lens element A Aperture P Parallel plate S Image plane 1 Zoom lens system 2 Image sensor 3 Liquid crystal monitor 4 Case 5 Main barrel 6 Moving barrel 7 Cylindrical cam

Claims (13)

A zoom lens system for forming an optical image of an object so as to be variable,
In order from the object side to the image side consists of a first lens unit having a negative power, a second lens group having positive power, a third lens group of positive power,
During zooming from the wide-angle end to the telephoto end, each lens group is irradiated with light so that the distance between the first lens group and the second lens group decreases and the distance between the second lens group and the third lens group changes. Move along each axis to change magnification,
The first lens group has a single object-side negative lens element with a convex surface facing the object side, and a convex surface facing the object side that is disposed with an air gap on the image side of the object-side negative lens element. Consisting of a single image-side positive lens element,
Each of the two lens elements constituting the first lens group has an aspheric surface,
A zoom lens system characterized by satisfying the following conditions (1), (2) , (3) and (9) :
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is a half angle of view at the wide angle end. The zoom lens system according to claim 1, wherein the zoom lens system satisfies the following conditions (4), (5), (6), and (7):
n11> 1.50 (4)
ν11> 35 (5)
n12-n11> 0.10 (6)
ν11−ν12> 15.0 (7)
here,
n11: Refractive index of the object side negative lens element of the first lens group,
ν11: Abbe number of the object side negative lens element of the first lens unit,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens unit. The zoom lens system according to claim 1, satisfying the following condition (8):
T1 / Y <1.5 (8)
here,
T1: Center thickness of the first lens group,
Y: Maximum image height.   The zoom lens system according to claim 1, wherein the third lens group includes one lens element.   The object side surface of the most object side lens element constituting the second lens group is an aspherical surface, and the second lens group is arranged in order from the object side to the image side, with one set of positive cemented lens elements and one positive lens element. The lens element according to claim 1, comprising one positive lens element and one set of cemented lens elements and one positive lens element, or comprising two sets of positive cemented lens elements. Zoom lens system. An imaging device capable of converting an optical image of a subject into an electrical image signal and outputting the electrical image signal,
A zoom lens system for forming an optical image of the subject so as to be variable, and
An image sensor that converts an optical image of a subject formed by the zoom lens system into an electrical image signal;
Wherein the zoom lens system consists of from the object side is the object side to the image side in this order, a first lens group having negative power, a second lens group having positive power, a third lens group of positive power,
During zooming from the wide-angle end to the telephoto end, each lens group is irradiated with light so that the distance between the first lens group and the second lens group decreases and the distance between the second lens group and the third lens group changes. Move along each axis to change magnification,
The first lens group has a single object-side negative lens element with a convex surface facing the object side, and a convex surface facing the object side that is disposed with an air gap on the image side of the object-side negative lens element. Consisting of a single image-side positive lens element,
Each of the two lens elements constituting the first lens group has an aspheric surface,
An imaging apparatus characterized by satisfying the following conditions (1), (2) , (3) and (9) :
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is a half angle of view at the wide angle end. The imaging device according to claim 6 , wherein the zoom lens system satisfies the following conditions (4), (5), (6), and (7):
n11> 1.50 (4)
ν11> 35 (5)
n12-n11> 0.10 (6)
ν11−ν12> 15.0 (7)
here,
n11: Refractive index of the object side negative lens element of the first lens group,
ν11: Abbe number of the object side negative lens element of the first lens unit,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens unit. The imaging device according to claim 6 , wherein the zoom lens system satisfies the following condition (8):
T1 / Y <1.5 (8)
here,
T1: Center thickness of the first lens group,
Y: Maximum image height. The imaging device according to claim 6 , wherein the third lens group of the zoom lens system includes one lens element. The object side surface of the most object side lens element constituting the second lens group of the zoom lens system is an aspheric surface, and the second lens group includes a pair of positive junction lens elements in order from the object side to the image side. A single positive lens element, or a single positive lens element and a pair of cemented lens elements and a single positive lens element, or two pairs of positive lens elements. 6. The imaging device according to 6 . A camera that can shoot a subject and output it as an electrical image signal,
An imaging apparatus comprising: a zoom lens system that forms an optical image of the subject so as to be variable in magnification; and an imaging device that converts an optical image of the subject formed by the zoom lens system into an electrical image signal. Prepared,
Wherein the zoom lens system consists of from the object side is the object side to the image side in this order, a first lens group having negative power, a second lens group having positive power, a third lens group of positive power,
During zooming from the wide-angle end to the telephoto end, each lens group is irradiated with light so that the distance between the first lens group and the second lens group decreases and the distance between the second lens group and the third lens group changes. Move along each axis to change magnification,
The first lens group has a single object-side negative lens element with a convex surface facing the object side, and a convex surface facing the object side that is disposed with an air gap on the image side of the object-side negative lens element. Consisting of a single image-side positive lens element,
Each of the two lens elements constituting the first lens group has an aspheric surface,
A camera that satisfies the following conditions (1), (2) , (3), and (9) :
n12> 1.95 (1)
ν12 < 24 (2)
5.0 <αi _W <20.0 (3)
2.5 <(T1 + T2 + T3) / Y <3.2 (9)
(However, ω _W > 30)
here,
n12: refractive index of the image-side positive lens element of the first lens group,
ν12: Abbe number of the image-side positive lens element of the first lens group,
αi _W : imaging element incident angle of the principal ray at the maximum image height at the wide-angle end (when the principal ray is incident on the light receiving surface of the imaging element while being separated from the optical axis)
T1: Center thickness of the first lens group,
T2: center thickness of the second lens group,
T3: Center thickness of the third lens group,
Y: Maximum image height
ω _W is a half angle of view at the wide angle end. The camera according to claim 11 , wherein the camera is a digital still camera capable of acquiring a still image of a subject. The camera according to claim 11 , which is a digital video camera capable of acquiring a moving image of a subject.

Images