JP4819476B2 - Zoom lens and imaging apparatus using the same - Google Patents

Description

  The present invention relates to a zoom lens, and more particularly to an ultra-compact and high-performance zoom lens used in a small imaging device (for example, a digital still camera, a mobile phone, a PDA, etc.).

  2. Description of the Related Art In recent years, a large number of devices have been installed in which a mobile terminal such as a mobile phone or a PDA is mounted with an imaging module combined with a single focal length imaging lens and an imaging device such as a CCD or CMOS. These devices are becoming thinner so as not to hinder carrying, and accordingly, imaging modules are also getting thinner.

  2. Description of the Related Art Imaging modules, particularly imaging modules for mobile phones, are very frequently equipped with photographing lenses having a single focal length with a relatively small number of constituent lenses that can be easily reduced in thickness.

  On the other hand, mobile phones equipped with an image sensor of 1 to 3 megapixels have been developed with higher image quality. On the other hand, there is an increasing need for zoom lenses as photographing lenses. As a zoom lens compatible with such a small device, various negative lens group leading (negative lead type) zoom lens systems in which a lens unit having a negative refractive power is disposed on the object side have been proposed (patents). References 1, 2, and 3).

  Patent Document 1 discloses a zoom lens including three lenses as a whole system in a three-group configuration including lens groups having negative, positive, and positive refractive powers in order from the object side to the image side. During zooming, the first and second lens groups are moved so that the distance between the first and second lens groups decreases and the distance between the second and third lens groups increases.

  In this way, the number of lenses is reduced and the entire lens system is reduced in size. Furthermore, the third lens group is fixed during zooming (magnification) and is configured with positive refractive power, so that the entire exit lens system is made smaller while the exit pupil is lengthened.

  In Patent Document 2, four lenses that perform zooming by moving the first, second, and third lens groups in order from the object side to the image side in a three-group configuration including negative, positive, and positive refractive power lens groups. A zoom lens comprising a lens is disclosed.

In Patent Document 3, in order from the object side to the image side, the lens unit includes four lenses that perform zooming by moving the second and third lens units in a three-group configuration including lens units having negative, positive, and positive refractive powers. A zoom lens is disclosed.
JP 2003-177314 A JP-A-9-146001 JP 11-237549 A

  In each of the embodiments of the zoom lens disclosed in Patent Document 1, it is difficult to cope with the above-described megapixel or more sensor in terms of optical performance.

  The zoom lens disclosed in Patent Document 2 is good in that the number of constituent lenses is small. However, the F-number at the wide-angle end is as dark as about 7 to 8, and it becomes darker at the telephoto end. For this reason, there are problems such as resolution degradation due to diffraction and insufficient light quantity when applied to a small image sensor. Also, the zoom ratio is 1.6 times or less, and there is a problem that the zoom ratio is too small to be mounted on a camera using a small image sensor in recent years.

  In the zoom lens disclosed in Patent Document 3, the number of constituent lenses is reduced. In order to fix the first lens group during zooming, the power of the third lens group is weakened and the function of the compensator is provided. For this reason, although there are three groups of negative, positive and positive zoom lenses, there is a tendency for the zoom lenses of two groups of negative and positive to appear, which is disadvantageous for miniaturization.

  SUMMARY OF THE INVENTION An object of the present invention is to provide a zoom lens that has excellent optical performance and can be used for an image sensor with a megapixel or more, and an image pickup apparatus using the same, while reducing the size of the entire lens system.

The zoom lens according to the first aspect of the present invention includes, in order from the object side to the image side, a first lens group having a negative refractive power, a second lens group having a positive refractive power, and a third lens group having a positive refractive power. the entire system is composed of four lenses, in the zoom lens to perform zooming by changing the distances between the lens groups, the third lens group and a positive lens and a negative lens, the most image-side surface of the image side The focal length of the first lens group is f1, the focal length of the second lens group is f2, the focal length of the third lens group is f3 , and the focal length of the entire system at the wide angle end is fw, When the focal length of the entire system at the telephoto end is ft ,
−0.82 <f1 / f2 <−0.7
1.6 <ft / fw
0.8 <f3 / √ (fw × ft) <1.5
It is characterized by satisfying the following conditions.

According to a second aspect of the present invention, in the first aspect of the invention, the first lens group is an image so that the distance between the lens groups at the telephoto end is smaller than that at the wide-angle end during zooming from the wide-angle end to the telephoto end. moves with a locus convex to the side, the second lens group and the third lens group is characterized by moving from the image side to the object side.

The invention of claim 3 is the invention of claim 1 or 2, wherein the first lens group both lens surfaces are composed of a negative lens of a concave shape, and the second lens group is composed of a positive lens of the main Nisukasu shape It is characterized by having.

  According to a fourth aspect of the present invention, in the first aspect of the present invention, a diaphragm is disposed on the object side or the image side of the second lens group, and the diaphragm is used together with the second lens group during zooming. It is characterized by moving.

The invention of claim 5 is the invention according to any one of claims 1 to 4, and order counting the i from the object side, when the refractive index at the d-line of the material of the i-th lens and Ndi,
Nd1 <1.55
Nd2 <1.70
Nd3 <1.55
It is characterized by satisfying the following conditions.

Imaging apparatus of the invention of claim 6 is characterized in that it has a zoom lens according to any one of claims 1 to 5, and an image sensor for receiving an image formed by the zoom lens.

  According to the present invention, it is possible to achieve a zoom lens having excellent optical performance and an image pickup apparatus using the same that can be applied to an image pickup device of megapixels or more while reducing the size of the entire lens system.

  Embodiments of the zoom lens of the present invention and an image pickup apparatus using the same will be described below.

  FIG. 1 is a lens cross-sectional view at the wide-angle end of the zoom lens according to Embodiment 1 of the present invention, and FIGS. 2 and 3 are aberration diagrams at the wide-angle end and telephoto end of the zoom lens according to Embodiment 1, respectively.

  FIG. 4 is a lens cross-sectional view at the wide-angle end of the zoom lens according to Embodiment 2 of the present invention, and FIGS. 5 and 6 are aberration diagrams at the wide-angle end and telephoto end of the zoom lens according to Embodiment 2, respectively.

  FIG. 7 is a lens cross-sectional view at the wide-angle end of the zoom lens according to Embodiment 3 of the present invention, and FIGS. 8 and 9 are aberration diagrams at the wide-angle end and telephoto end of the zoom lens according to Embodiment 3, respectively.

  FIG. 10 is a lens cross-sectional view at the wide-angle end of the zoom lens according to Embodiment 4 of the present invention. FIGS. 11 and 12 are aberration diagrams at the wide-angle end and telephoto end of the zoom lens according to Embodiment 4, respectively.

  The zoom lens of each embodiment is a photographing lens system used in an imaging apparatus (optical apparatus). In the lens cross-sectional view, the left side is the object side, and the right side is the image side.

  In the lens cross-sectional view, L1 is a first lens unit having a negative refractive power (optical power = reciprocal of focal length), L2 is a second lens unit having a positive refractive power, and L3 is a third lens unit having a positive refractive power. is there.

  SP denotes an aperture stop, which is disposed on the image side of the second lens unit L2 in Examples 1, 3, and 4, and on the object side in Example 2.

  IP is an image plane, and when used as a photographing optical system of a video camera or a digital still camera, a photosensitive surface corresponding to an imaging surface of a solid-state imaging device (photoelectric conversion device) such as a CCD sensor or a CMOS sensor is placed.

  In the aberration diagrams, d and g are d-line and g-line, respectively, ΔM and ΔS are meridional image plane, sagittal image plane, and lateral chromatic aberration are represented by g-line.

  In each of the following embodiments, the wide-angle end and the telephoto end refer to zoom positions when the zoom lens unit (second lens unit L2) is positioned at both ends of the range in which it can move on the optical axis due to the mechanism.

  In each embodiment, only the first lens unit L1 having a negative refractive power, the second lens unit L2 having a positive refractive power, and the third lens unit L3 having a positive refractive power are provided as lens units in order from the object side to the image side. The entire system is composed of four lenses.

  The first lens unit L1 is composed of one negative lens having concave concave surfaces, and the second lens unit L2 is composed of one meniscus positive lens.

  The third lens unit L3 includes a positive lens and a negative lens, and the most image side surface has a convex shape on the image side.

  By configuring each lens group in this manner, excellent aberration correction that can be applied to an image sensor (sensor) of megapixels or more is performed.

  When zooming from the wide-angle end to the telephoto end, the first lens unit L1 has a convex locus on the image side so that the distance between the lens units at the telephoto end is smaller than that at the wide-angle end. The groups L2 and L3 move from the image side to the object side.

  The diaphragm SP moves together with the second lens unit L2 during zooming from the wide-angle end to the telephoto end.

  In this embodiment, the first lens unit L1 is moved to correct the image plane variation accompanying zooming (magnification). In this embodiment, since the exit pupil is short and the incident angle to the image sensor is large, the amount of light is reduced at the peripheral angle of view compared to the incident angle characteristics of the image sensor and the vicinity of the optical axis. For this reason, it is necessary to sufficiently put off-axis light flux on the pupil plane. Accordingly, the lens near the stop SP has a thick light beam, and it becomes difficult to correct aberrations with only a small number of spherical lenses. Therefore, the lens surface close to the stop SP has an aspherical shape. In order to correct off-axis halo and coma with a smaller number of lenses, an aspherical surface is also introduced in the third lens unit L3.

  Further, by making the first lens unit L1 one negative lens as described above, the curvature of the surface of the negative lens on the image plane side is relaxed, and the second lens unit L2 becomes the first lens while facilitating manufacture. It is easier to approach the group L1. Further, the second lens unit L2, which is a variable power lens unit, can ensure a sufficient amount of movement during zooming.

  Further, the second lens unit L2 is constituted by the meniscus-shaped positive lens as described above, so that the front principal point is located forward and the front lens diameter is reduced.

  Further, the third lens unit L3 is composed of the positive lens and the negative lens as described above, thereby improving the chromatic aberration. Furthermore, by making the most image side surface convex toward the image side, light rays are prevented from being bent suddenly. This suppresses the occurrence of fluctuations in off-axis aberration due to zooming.

In this embodiment, when i is shown as an order counted from the object side, the focal length of the i-th lens unit L1 is fi, the focal length of the entire system at the wide angle end is fw, and the focal length of the entire system at the telephoto end is ft.
-0.82 <f1 / f2 <-0.7 (1)
1.6 <ft / fw (2)

Satisfy the following conditions.

  Next, the technical meaning of each conditional expression will be described.

  Conditional expressions (1), (2), and (3) are for respectively defining the power (refractive power) of the entire lens system and the power arrangement of each lens group. By increasing the power of the second and third lens units that move during zooming, the amount of movement of the second and third lens units is reduced, thereby reducing the size of the entire lens system.

  If the power of the second lens group becomes weaker than the upper limit value of the conditional expression (1) while satisfying the conditional expression (2), the first lens group and the second lens group are used to obtain a predetermined zoom ratio. This is not good because the total length of the lens becomes long at the wide-angle end. Conversely, if the power of the first lens group becomes weaker than the lower limit value, the amount of movement of the first lens group increases, and the distance between the first lens group and the second lens group must be increased, and the total lens length is increased. Is not good because it becomes longer.

  Further, if the conditional expression (2) itself is not satisfied, the zoom ratio is too small, which makes the zoom lens used for imaging unattractive.

  Conditional expression (3) is for optimally maintaining the size and performance of the third lens group over the entire zoom range. If the upper limit of conditional expression (3) is exceeded and the power of the third lens group becomes weak, the variable magnification share is biased toward the second lens group, which makes it difficult to suppress zoom fluctuations of various aberrations. Conversely, when the power of the third lens group becomes stronger beyond the lower limit, it becomes difficult to improve the coma aberration while forming the third lens group with two lenses. As a result, the number of lenses needs to be increased, which is not good.

More preferably, the numerical ranges of the conditional expressions (1), (2), and (3) are set to −0.82 <f1 / f2 <−0.72 (1a)
1.8 <ft / fw (2a)

It is good to do. This facilitates further downsizing of the entire lens system and high optical performance.

  As described above, in each example, by satisfying conditional expressions (1), (2), and (3), the entire lens system is downsized, and the number of constituent lenses is reduced while maintaining high optical performance. A zoom lens with a configuration is obtained.

  In addition, when the zoom lens in this embodiment is used as a photographing lens mounted on a portable terminal such as a mobile phone or a PDA, the lens barrel that holds the zoom lens is a type that does not retract.

  For further compactness, when a numerical example described later is expressed in mm, the distance on the optical axis from the first lens surface on the object side to the image surface (sensor surface) is set to 15 mm or less.

In the zoom lens according to the present embodiment, i is shown as an order counted from the object side, and Nd1 <1.55 when the refractive index for the d-line of the material of the i-th lens is Ndi.
Nd2 <1.70 (5)
Nd3 <1.55 (6)
Is satisfied.

  The conditional expressions (4), (5), and (6) are for defining the refractive indexes of the materials of the three lenses on the object side. If the conditional expressions (4), (5), and (6) are not satisfied, the manufacturing becomes difficult (the cost of the lens becomes high), which is not good.

More preferably, the numerical range of the conditional expressions (4), (5), (6) is set to Nd1 <1.53 (4a)
Nd2 <1.68 (5a)
Nd3 <1.52 (6a)
It is good to do.

  In general, the manufacturing (cost) of a lens becomes more difficult (expensive) as the refractive index becomes higher. Therefore, it is preferable to use a lens having a low refractive index in order to achieve a simple zoom lens. Furthermore, it is preferable to use a plastic lens in order to facilitate the production of the lens.

  As described above, in the present embodiment, in the zoom lens having the lens configuration of 3 lenses in 4 groups, the interval between the lens groups is changed. A three-group zoom lens composed of negative, positive, and positive refracting power lens groups maintains characteristics suitable for miniaturization, and achieves miniaturization by appropriately sharing the magnification and image plane correction. . Further, in this embodiment, the number of lenses constituting the lens is four, so that the optical performance corresponding to the megapixel class image pickup device can be easily demonstrated while reducing the increase in the total length due to the thickness of the lens. Yes.

  Numerical examples 1 to 4 corresponding to the first to fourth examples are shown below. In each numerical example, i indicates the order of the surfaces from the object side, Ri is the radius of curvature of each surface, Di is the member thickness or air space between the i-th surface and the (i + 1) -th surface, Ni and νi represents a refractive index and an Abbe number based on the d-line, respectively.

  The aspherical shape is the X axis in the optical axis direction, the H axis in the direction perpendicular to the optical axis, the light traveling direction is positive, R is the paraxial radius of curvature, k is the conic constant, and B, C, D, and E are non- When using spherical coefficient

It is represented by Where R is a paraxial radius of curvature, and B, C, D, and E are fourth-order, sixth-order, eighth-order, and tenth-order aspherical coefficients, respectively. The display of “e−X” means “× 10 ^−X ”. f represents a focal length, Fno represents an F number, and ω represents a half angle of view. Table 1 shows the relationship between the above-described conditional expressions and numerical values in the numerical examples.

In this embodiment, focusing is performed by moving the first lens unit L1. Note that focusing may be performed by moving other lens groups or the entire lens.
[Numerical Example 1]
f = 3.75-7.50 Fno = 3.50-5.18 2ω = 65.6 °-33.2 °
R 1 = -16.670 D 1 = 0.50 N 1 = 1.524700 ν 1 = 56.2
R 2 = 3.042 D 2 = variable
R 3 = 2.026 D 3 = 1.09 N 2 = 1.677900 ν 2 = 54.8
R 4 = 2.882 D 4 = 0.15
R 5 = Aperture D 5 = Variable
R 6 = 1.594 D 6 = 1.40 N 3 = 1.516330 ν 3 = 64.1
R 7 = -4.860 D 7 = 0.28
R 8 = -1.266 D 8 = 1.00 N 4 = 1.846660 ν 4 = 23.8
R 9 = -2.666

\ Focal length 3.75 5.83 7.50
Variable interval \
D 2 2.86 1.22 0.66
D 5 1.22 0.57 0.10

Aspheric coefficient
R2 k = -7.48038e + 00 B = 2.43062e-02 C = -5.73876e-03 D = 6.37893e-04
E = -4.68864e-06
R3 k = -2.85242e-01 B = -6.77708e-03 C = 3.46583e-03 D = -4.45912e-03
E = 1.44119e-03
R6 k = -1.80659e-01 B = 1.40895e-02 C = 2.97413e-03 D = 9.50106e-03
E = 2.76403e-03
R9 k = -4.05809e + 00 B = -1.14497e-02 C = -9.55581e-04 D = 7.06327e-03
E = -1.71190e-03

[Numerical Example 2]
f = 3.75 to 7.50 Fno = 3.38 to 4.98 2ω = 65.5 ° to 33.4 °
R 1 = -17.375 D 1 = 0.70 N 1 = 1.516330 ν 1 = 64.1
R 2 = 2.611 D 2 = variable
R 3 = Aperture D 3 = 0.00
R 4 = 2.153 D 4 = 0.81 N 2 = 1.589130 ν 2 = 61.1
R 5 = 5.236 D 5 = Variable
R 6 = 2.007 D 6 = 1.50 N 3 = 1.516330 ν 3 = 64.1
R 7 = -5.286 D 7 = 0.33
R 8 = -1.582 D 8 = 1.00 N 4 = 1.846660 ν 4 = 23.8
R 9 = -3.283

\ Focal length 3.75 5.82 7.50
Variable interval \
D 2 2.59 1.14 0.63
D 5 1.42 0.68 0.15

Aspheric coefficient
R1 k = 3.96680e + 01 B = -1.42210e-02 C = 5.31004e-03 D = -3.30571e-04 E = -7.92147e-05
R2 k = -6.04719e + 00 B = 1.15069e-02 C = -4.67727e-03 D = 5.02646e-03 E = -1.48243e-03
R4 k = -2.47465e-01 B = -7.65568e-03 C = -3.36437e-03 D = 2.25711e-03 E = -4.41912e-04
R6 k = 1.62467e-01 B = 1.64740e-03 C = 8.20659e-03 D = -4.69634e-03 E = 3.63501e-03
R8 k = 6.24338e-01 B = 1.68683e-02 C = 1.77610e-02 D = -1.18706e-02 E = 1.20761e-02
R9 k = -6.47450e-01 B = 1.10768e-02 C = -1.63024e-03 D = 3.94636e-03 E = -1.16479e-03

[Numerical Example 3]
f = 3.75-7.50 Fno = 3.50-5.25 2ω = 65.6 °-33.2 °
R 1 = -11.597 D 1 = 0.70 N 1 = 1.516330 ν 1 = 64.1
R 2 = 2.722 D 2 = Variable
R 3 = 1.820 D 3 = 0.93 N 2 = 1.516330 ν 2 = 64.1
R 4 = 4.055 D 4 = 0.40
R 5 = Aperture D 5 = Variable
R 6 = 1.612 D 6 = 1.36 N 3 = 1.516330 ν 3 = 64.1
R 7 = -10.279 D 7 = 0.30
R 8 = -1.338 D 8 = 0.97 N 4 = 1.846660 ν 4 = 23.8
R 9 = -2.759

\ Focal length 3.75 5.82 7.50
Variable interval \
D 2 2.49 1.10 0.61
D 5 1.28 0.63 0.15

Aspheric coefficient
R2 k = -6.67906e + 00 B = 2.70485e-02 C = -7.97475e-03 D = 1.33278e-03 E = -9.17972e-05
R3 k = -3.93822e-01 B = -9.03954e-03 C = 4.34235e-04 D = -5.82812e-04 E = -2.13260e-04
R6 k = -3.07389e-01 B = 1.01700e-02 C = 1.51074e-02 D = -3.17839e-03 E = 6.94928e-03
R9 k = -1.97556e + 00 B = 1.07944e-03 C = 7.42895e-03 D = -2.13423e-03 E = 1.08942e-03

[Numerical Example 4]
f = 3.74-7.49 Fno = 3.49-5.23 2ω = 66.1 °-33.4 °
R 1 = -15.828 D 1 = 0.70 N 1 = 1.516330 ν 1 = 64.1
R 2 = 2.960 D 2 = Variable
R 3 = 1.669 D 3 = 0.99 N 2 = 1.516330 ν 2 = 64.1
R 4 = 2.972 D 4 = 0.40
R 5 = Aperture D 5 = Variable
R 6 = 1.458 D 6 = 1.24 N 3 = 1.516330 ν 3 = 64.1
R 7 = 29.125 D 7 = 0.25
R 8 = -1.492 D 8 = 1.00 N 4 = 1.846660 ν 4 = 23.8
R 9 = -3.152

\ Focal length 3.74 5.85 7.49
Variable interval \
D 2 2.99 1.33 0.74
D 5 0.99 0.50 0.15

Aspheric coefficient
R1 k = -1.31183e + 01 B = 7.54902e-05 C = -4.45368e-04 D = 9.69379e-06 E = 1.33059e-06
R2 k = -7.11802e + 00 B = 2.39915e-02 C = -7.03860e-03 D = 7.88973e-04 E = -3.83994e-05
R3 k = -3.07664e-01 B = -1.19775e-02 C = 3.60129e-03 D = -4.59748e-03 E = 9.85680e-04
R6 k = 1.53701e-01 B = 4.05850e-03 C = 4.92222e-03 D = 5.86288e-03 E = 1.07659e-02
R8 k = 9.11697e-01 B = -3.16887e-02 C = -3.44941e-02 D = 5.72219e-02 E = -8.44902e-02
R9 k = 8.24659e-01 B = 4.19741e-03 C = -5.02877e-03 D = 1.13503e-02 E = -4.16910e-03

  FIG. 13 is a schematic view of the main part of the imaging apparatus of the present invention.

In FIG. 13, reference numeral 1 denotes a mobile phone body, and 2 denotes an image pickup module to which the zoom lens 4 of the present invention is attached, and is composed of the zoom lens 4 and an image pickup device 5 that receives an image formed by the zoom lens . Reference numeral 6 denotes recording means for recording image data taken by the imaging module, and reference numeral 7 denotes a liquid crystal display unit for displaying a photographic image of the photographic subject at the time of shooting and reproduction.

  In this way, by applying the zoom lens of the present invention to a device such as a mobile phone, a small portable device capable of providing a high-quality image is realized.

Lens sectional view of Numerical Example 1 of the present invention Various aberrations at the zoom position at the wide-angle end according to Numerical Embodiment 1 of the present invention Various aberrations at the zoom position at the telephoto end according to Numerical Example 1 of the present invention Lens sectional view of Numerical Example 2 of the present invention Various aberrations at the zoom position at the wide angle end according to Numerical Embodiment 2 of the present invention Various aberrations at the zoom position at the telephoto end according to Numerical Example 2 of the present invention Lens sectional view of Numerical Example 3 of the present invention Various aberrations at the zoom position at the wide angle end according to Numerical Embodiment 3 of the present invention Various aberrations at the zoom position at the telephoto end according to Numerical Example 3 of the present invention Lens sectional view of Numerical Example 4 of the present invention Various aberrations at the zoom position at the wide angle end according to Numerical Embodiment 4 of the present invention Various aberrations at the zoom position at the telephoto end according to Numerical Example 4 of the present invention Schematic diagram of the main part of an embodiment of the optical apparatus of the present invention

Explanation of symbols

L1 1st lens group L2 2nd lens group L3 3rd lens group SP Aperture IP image surface d d line g g line ΔS sagittal image surface ΔM meridional image surface

Claims (6)

In order from the object side to the image side, a first lens unit having a negative refractive power, a second lens unit having positive refractive power, a third lens unit having positive refractive power, the entire system is constituted by four lenses In the zoom lens that performs zooming by changing the interval between the lens groups, the third lens group includes a positive lens and a negative lens, and the most image-side surface has a convex shape on the image side, and the first lens The focal length of the group is f1, the focal length of the second lens group is f2, the focal length of the third lens group is f3 , the focal length of the entire system at the wide angle end is fw, and the focal length of the entire system at the telephoto end is ft. when you and,
−0.82 <f1 / f2 <−0.7
1.6 <ft / fw
0.8 <f3 / √ (fw × ft) <1.5
A zoom lens characterized by satisfying the following conditions: When zooming from the wide-angle end to the telephoto end, the first lens unit moves along a convex locus toward the image side so that the distance between the lens units at the telephoto end is smaller than that at the wide-angle end, and the second lens The zoom lens according to claim 1, wherein the group and the third lens group move from the image side to the object side. The first lens group both lens surfaces are composed of a negative lens concave, zoom according to claim 1 or 2, wherein the second lens group is characterized by being composed of a positive lens of the main Nisukasu shape lens. The second lens diaphragm on the object side or the image side of the group is arranged, the restrictor when zooming, zooming according to any one of claims 1 to 3, characterized in that moves together with the second lens group lens. The i and order counting from the object side, when the refractive index at the d-line of the material of the i-th lens and Ndi,
Nd1 <1.55
Nd2 <1.70
Nd3 <1.55
The zoom lens according to any one of claims 1 to 4, characterized by satisfying the following condition. A zoom lens according to any one of claims 1 to 5, an imaging apparatus characterized by comprising an imaging element for receiving an image formed by the zoom lens.