CN109960023A - Zoom lens and photographic device - Google Patents
Zoom lens and photographic device Download PDFInfo
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- CN109960023A CN109960023A CN201811123285.2A CN201811123285A CN109960023A CN 109960023 A CN109960023 A CN 109960023A CN 201811123285 A CN201811123285 A CN 201811123285A CN 109960023 A CN109960023 A CN 109960023A
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B15/00—Optical objectives with means for varying the magnification
- G02B15/14—Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective
- G02B15/16—Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group
- G02B15/177—Optical objectives with means for varying the magnification by axial movement of one or more lenses or groups of lenses relative to the image plane for continuously varying the equivalent focal length of the objective with interdependent non-linearly related movements between one lens or lens group, and another lens or lens group having a negative front lens or group of lenses
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Abstract
The present invention discloses a kind of zoom ratio with higher, and is able to maintain that in entire zoom area good optical property, small-sized and high performance zoom lens.The zoom lens are configured to, and are configured in order from object side: the 1st lens group (G with negative refractive power1), the 2nd lens group (G with positive refractive power2), the 3rd lens group (G with negative refractive power3) and subsequent lens group (GR).The zoom lens are being always maintained at the 1st lens group (G when carrying out the zoom from wide-angle side to telescope end1) relative to image planes IMG it is fixed in the state of, at least make the 2nd lens group (G2) and the 3rd lens group (G3) moved along optical axis, to change interval of each lens group on optical axis.Also, by meeting predetermined condition, zoom ratio with higher is realized, and is able to maintain that in entire zoom area good optical property, small-sized and high performance zoom lens.
Description
Technical field
The present invention relates to zoom lens and photographic device, more particularly, to suitable for equipped with solid-state image pickups such as CCD and CMOS
The zoom lens of the photographic device of element and photographic device with the zoom lens.
Background technique
It is solid equipped with CCD such as single-lens reflex camera, digital still camera, video camera, monitor camera and COMS etc.
The photographic device of body photographing element is just in rapid proliferation.It is accompanied by this, proposing one kind can be applied to equipped with CCD and CMOS
Deng solid-state imager photographic device in zoom lens (referring for example to patent document 1).
Zoom lens disclosed in patent document 1 are following optical systems: from object side, successively by the 1st of negative refractive power the
Lens group, the 2nd lens group of positive refractive power, the 3rd lens group, the 4th lens group of positive or negative refractive power, Yi Jizheng of negative refractive power
5th lens group of refractive power is constituted, and by fixing the 1st lens group and the 5th lens group relative to imaging surface, and is made the 2nd thoroughly
Microscope group, the 3rd lens group and the 4th lens group are mobile, to carry out the zoom from wide-angle side to telescope end.
Existing technical literature
Patent document
Patent document 1: No. 3226297 bulletins of Japanese Patent Publication No.
As the zoom lens of monitor camera, preferably high magnification heavy caliber zoom lens always, but in recent years,
Due to the development of the high pixelation of solid-state image pickup element, to the high-resolution with the subtleer feature that can confirm subject
The expectation of the lens of (high-performance) is higher and higher.It is accompanied by this, tight demand is on the basis for the high performance for realizing optical system
On, realize the zoom lens of miniaturization, further high zoom and low cost.
However, although zoom lens disclosed in patent document 1 are wide-angles, but zoom ratio is down to 4 times or so, therefore can not fill
Divide the needs of meeting in recent years.
Summary of the invention
In order to eliminate above-mentioned problem of the prior art point, it is an advantage of the invention to provide zooms with higher
Than, and it is able to maintain that in entire zoom area good optical property, small-sized and high performance zoom lens.The present invention
Another purpose be, zoom ratio with higher, small-sized and high performance zoom lens photographic device are provided.
In order to solve the above problems, to achieve the goal, zoom lens of the invention are characterized in that, which is
By configured in order from object side the 1st lens group with negative refractive power, the 2nd lens group with positive refractive power, have it is negative
What the 3rd lens group and subsequent lens group of refractive power were constituted, wherein by be always maintained at the 1st lens group relative to
In the state that image planes are fixed, move the 2nd lens group and the 3rd lens group along optical axis, to change described each
Thus interval of the lens group on optical axis carries out the zoom from wide-angle side to telescope end, also, zoom lens satisfaction is as follows
Shown in conditional:
(1)3.5≦|F1/Fw|≦20.0
(2)0.7≦|F1/Ft|≦2.0
(3)1.9≦|F2/F3|≦5.0
Wherein, F1 indicates the focal length of the 1st lens group, Fw indicate the zoom lens wide-angle side focus away from
From Ft indicates the zoom lens in the focal length of telescope end, and F2 indicates that the focal length of the 2nd lens group, F3 indicate institute
State the focal length of the 3rd lens group.
According to the present invention it is possible to provide a kind of zoom ratio with higher, and it is able to maintain that in entire zoom area
Good optical property, small-sized and high performance zoom lens.
Beneficial effects of the present invention are as follows:
According to the present invention it is possible to play following effect: being capable of providing zoom ratio with higher, and in entire zoom area
Good optical property, small-sized and high performance zoom lens are able to maintain that in domain.Furthermore it is also possible to play following effect:
It is capable of providing zoom ratio with higher, small-sized and high performance zoom lens photographic device.
Detailed description of the invention
Fig. 1 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 1.
Fig. 2 shows the various aberration diagrams of the zoom lens of embodiment 1.
Fig. 3 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 2.
Fig. 4 shows the various aberration diagrams of the zoom lens of embodiment 2.
Fig. 5 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 3.
Fig. 6 shows the various aberration diagrams of the zoom lens of embodiment 3.
Fig. 7 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 4.
Fig. 8 shows the various aberration diagrams of the zoom lens of embodiment 4.
Fig. 9 illustrates that the figure of an example of the photographic device with zoom lens of the invention.
Specific embodiment
Hereinafter, the ideal embodiment of zoom lens and photographic device of the invention is described in detail.
Zoom lens of the invention be by configured in order from object side the 1st lens group with negative refractive power, have
What the 2nd lens group, the 3rd lens group with negative refractive power and the subsequent lens group of positive refractive power were constituted.Also, from wide-angle
It holds the zoom of telescope end to carry out in the following way: being always maintained at the 1st lens group state fixed relative to image planes
Under, move the 2nd lens group and the 3rd lens group along optical axis, to change interval of each lens group on optical axis.
In zoom lens of the invention, the 2nd lens group and the 3rd lens group take on zoom effect.When zooming, by making
2nd lens group and the 3rd lens group move together, and it is good can to change progress to the focus movement generated when zooming and aberration
Correction, so as to realize with high-resolution varifocal optical system.In addition to this, when zooming, by the 1st lens group
It is fixed, optical system overall length can be maintained shorter, so as to realize small-sized optical system.In addition, due to the 1st
The outer diameter of lens group is larger to have the tendency that as ponderable lens group, therefore when zooming, by the way that it is fixed,
It can be realized the simplification of the driving mechanism of optical system.By doing so, the aberration correction in entire zoom area becomes
It is easy, and the small-sized zoom lens with good optical property may be implemented.
Also, in zoom lens of the invention, in view of the high pixelation of solid-state image pickup element, in order to realize that have can be true
The high-resolution lens for recognizing the more fine feature of subject set various conditions as follows.
Firstly, zoom lens of the invention the focal length of the 1st lens group is set as F1, by the zoom lens in wide-angle
When the focal length at end is set as Fw, preferably satisfy the following conditional expression.
(1)3.5≦|F1/Fw|≦20.0
Conditional (1) be define the 1st lens group focal length and the zoom lens wide-angle side focal length it
Between ratio formula.By meeting conditional (1), high zoom ratios can be realized in wide-angle side, and remain good optical
Energy.
In conditional (1), when being less than its lower limit, the refractive power of the 1st lens group is become too strong, to be difficult to carry out picture
The correction of field bend, astigmatism, therefore it is unable to maintain that good optical property.On the other hand, in conditional (1), when greater than it
When the upper limit, the refractive power of the 1st lens group is become too weak, to realize high zoom ratios it is necessary to make the 2nd lens group when zooming and
The amount of movement of 3rd lens group increases, so that optical system overall length extends, therefore, it is difficult to realize the miniaturization of optical system.In addition,
When being responsible for the increase of the amount of movement of lens group of zoom, the focus generated when zooming is mobile and aberration becomes larger, therefore light
Learn penalty.
In addition, the lower limit value of the above conditions (1) can mode as following set: preferably 5.0 with
On, more preferably 6.0 or more, more preferably 7.0 or more, more preferably 8.0 or more, more preferably 8.5 or more, more preferably
More than 8.9.In addition, the upper limit value of the above conditions (1) can mode as following set: preferably 19.0 with
Under, more preferably 18.0 hereinafter, more preferably 17.0 hereinafter, more preferably 16.0 hereinafter, more preferably 15.5 hereinafter, more preferably
It is 15.0 or less.
Then, when the focal length by the zoom lens in telescope end is set as Ft, the focal length of the 2nd lens group is set as
When F2, preferably satisfy the following conditional expression.
(2)0.7≦|F1/Ft|≦2.0
Conditional (2) be define the 1st lens group focal length and the zoom lens telescope end focal length it
Between ratio formula.By meeting conditional (2), high zoom ratios can be realized in telescope end, and remain good optical
Energy.
In conditional (2), when being less than its lower limit, the refractive power of the 1st lens group is become too strong, to be difficult to carry out picture
The correction of field bend, astigmatism, therefore it is unable to maintain that good optical property.On the other hand, in conditional (2), when greater than it
When the upper limit, the refractive power of the 1st lens group is become too weak, to realize high zoom ratios it is necessary to make the 2nd lens group when zooming and
The amount of movement of 3rd lens group increases, so that optical system overall length extends, therefore, it is difficult to realize the miniaturization of optical system.In addition,
When being responsible for the increase of the amount of movement of lens group of zoom, the focus generated when zooming is mobile and aberration becomes larger, therefore light
Learn penalty.
In addition, the lower limit value of the above conditions (2) can mode as following set: preferably 0.74 with
On, more preferably 0.78 or more.In addition, the upper limit value of the above conditions (2) can mode as following set:
Preferably 1.8 hereinafter, more preferably 1.4 or less.
In addition, the focal length of the 3rd lens group is set as when the focal length by the zoom lens in telescope end is set as Ft
When F3, preferably satisfy the following conditional expression.
(3)1.9≦|F2/F3|≦5.0
Conditional (3) is the public affairs for defining the ratio between the focal length of the 2nd lens group and the focal length of the 3rd lens group
Formula.It, can be real reducing the amount of movement of the 2nd lens group when zooming and the 3rd lens group by meeting conditional (3)
Existing high zoom ratios.As a result, it is suppressed that the focus generated when zooming is mobile and aberration changes so as to remain good
Optical property, also, optical system overall length is maintained into obtain the shorter miniaturization so as to realize optical system.
In conditional (3), when being less than its lower limit, compared to the 3rd lens group, the refractive power variable of the 2nd lens group obtains mistake
By force, thus be difficult to carry out in entire zoom area spherical aberration, on axis color difference correction, therefore be unable to maintain that good optics
Performance.On the other hand, in conditional (3), when prescribing a time limit thereon greatly, compared with the 2nd lens group, the refractive power of the 3rd lens group
It become too strong, to be difficult to carry out the correction of filed curvature, astigmatism in entire zoom area, therefore is unable to maintain that good light
Learn performance.
In addition, the lower limit value of the above conditions (3) can mode as following set: preferably 2.0 with
On, more preferably 2.5 or more.In addition, the upper limit value of the above conditions (3) can mode as following set:
Preferably 4.5 hereinafter, more preferably 4.0 hereinafter, more preferably 3.6 or less.
By meeting each conditional, above-mentioned effect can be played.It, can be with also, by meeting conditional (1)~(3)
It realizes zoom ratio with higher, also, is able to maintain that in entire zoom area good optical property, small-sized and high property
The zoom lens of energy.
It, will when the 3rd lens group is set as β 3t in the lateral magnification of telescope end also, in zoom lens of the invention
3rd lens group is preferably satisfied the following conditional expression when the lateral magnification of wide-angle side is set as β 3w.
(4)3.0≦|β3t/β3w|≦9.0
Conditional (4) be define the 3rd lens group in the formula of the ratio of the lateral magnification of wide-angle side and telescope end, and
Show the ratio of the zoom of the 3rd lens group.By meeting conditional (4), though reduce the 2nd lens group when zooming and
The amount of movement of 3rd lens group also can be realized high zoom ratios.As a result, it is suppressed that the focus movement generated when zooming and picture
Difference changes to maintain good optical property, also, maintains shorter so as to realizing light by optical system overall length
The miniaturization of system.
In conditional (4), when being less than its lower limit, since the ratio of the zoom of the 3rd lens group reduces, it is therefore necessary to increase
The ratio of the zoom of the other lenses group of big responsible zoom, so that the amount of movement for being responsible for the other lenses group of zoom increases.It is tied
Fruit is, it is difficult to realize the miniaturization of optical system.On the other hand, in conditional (4), when prescribing a time limit thereon greatly, the 3rd lens group
The ratio of zoom increase, be difficult to carry out the correction of filed curvature, astigmatism in entire zoom area, therefore be unable to maintain that good
Optical property.
In addition, the lower limit value of the above conditions (4) can mode as following set: preferably 3.2 with
On, more preferably 3.4 or more.In addition, the upper limit value of the above conditions (4) can mode as following set:
Preferably 8.0 hereinafter, more preferably 7.0 hereinafter, more preferably 6.5 hereinafter, more preferably 6.0 hereinafter, more preferably 5.5 with
Under, more preferably 5.0 or less.
Also, in zoom lens of the invention, preferably the subsequent lens group is configured to include from object side
Act configure in order, the 4th lens group with positive refractive power and the 5th lens group with positive refractive power.
And, it is preferred that when carrying out zoom, make any one in the 4th lens group or the 5th lens group along light
Axis is mobile.At this point, when the movable group in subsequent lens group is set as β pt in the lateral magnification of telescope end, by subsequent lens group
In movable group when the lateral magnification of wide-angle side is set as β pw, preferably satisfy the following conditional expression.
(5)3.0≦|βpt/βpw|≦10.0
Conditional (5) is to define the movable group in subsequent lens group in the ratio of the lateral magnification of wide-angle side and telescope end
Formula, and show the ratio of the zoom of the movable group.By meeting conditional (5), both inhibited when zooming can
The amount of movement of dynamic group, and can be realized high zoom ratios.As a result, it is suppressed that the focus generated when zooming is mobile and aberration becomes
It is dynamic so as to maintain good optical property, also, optical system overall length is maintained shorter so as to realizing optical system
The miniaturization of system.
In conditional (5), when being less than its lower limit, since the ratio of the zoom of the movable group in subsequent lens group subtracts
It is small, it is therefore necessary to increase the ratio for being responsible for the zoom of other lenses group of zoom, to be responsible for the shifting of the other lenses group of zoom
Momentum increases.As a result, especially when wanting to realize high zoom ratios, it is difficult to realize the miniaturization of optical system.Another party
Face, in conditional (5), when prescribing a time limit thereon greatly, the ratio of the zoom of the movable group in subsequent lens group increases, thus whole
It is difficult to carry out the correction of filed curvature, astigmatism in a zoom area, therefore is unable to maintain that good optical property.
In addition, the lower limit value of the above conditions (5) can mode as following set: preferably 3.4 with
On, more preferably 3.9 or more.In addition, the upper limit value of the above conditions (5) can mode as following set:
Preferably 9.0 hereinafter, more preferably 8.0 hereinafter, more preferably 7.0 hereinafter, more preferably 6.7 hereinafter, more preferably 6.2 with
Under.
It is further preferred, that when carrying out zoom, in the lens group that includes in subsequent lens group, the 4th lens group or
Any one lens group in 5th lens group is movable group.By the way that any one lens group is set as movable group, zoom can be made
Mechanism simplifying, so as to realize the miniaturization of optical system.In addition, being the feelings being made of 2 lens groups in subsequent lens group
Under condition, the 4th lens group can be, any one in the 5th lens group is movable group.It is by 3 or more in subsequent lens group
Lens group is constituted, and the lens group (the 6th lens group) configured in the image side of the 5th lens is fixed on optical axis when zooming
In the case of, it is preferred that the 5th lens group is set as movable group, the 4th lens group is fixed on when zooming on optical axis, is being configured
In the case where the lens group (the 6th lens group) of the image side of the 5th lens is movable when zooming, can be the 4th lens group or
Any one in 5th lens group is movable group.
Also, in zoom lens of the invention, it is preferred that the 1st lens group is made of 1 lens.Due to the 1st lens
The outer diameter of group has bigger tendency, therefore by constituting the 1st lens group by 1 lens, can be realized the light weight of the 1st lens group
Change, also, by the 1st lens group is thinning and maintain shorter by optical system overall length, can be realized the small of optical system
Type.In addition, the mechanism for keeping the 1st lens group can be simplified since the 1st lens group is made of 1 lens.
The lens for constituting the 1st lens group have negative refractive power, and shape can be meniscus shape, be also possible to bi-concave shape.However,
To generate stronger negative refractive power, preferably bi-concave shape.
Also, in zoom lens of the invention, it is preferred that in subsequent lens group, the 5th lens group image planes side
Configured with the 6th lens group with positive refractive power.By doing so, can to by before the 5th lens group without complete school
Correction is effectively performed in the various aberrations of filed curvature just etc., and can be realized in entire zoom area with higher
The zoom lens of resolution ratio.
Also, in zoom lens of the invention, it is preferred that when carrying out the zoom from wide-angle side to telescope end, the 1st
Lens group and being spaced at the intermediate region of zoom for the 2nd lens group reach maximum.Here, the intermediate region of zoom refers to from wide
Angle end is also possible to the arbitrary focal length other than wide-angle side and telescope end to the region of the zoom midway of telescope end.
By the configuration of lens group when taking such zoom, it can be realized high zoom ratios.
Also, in zoom lens of the invention, it is preferred that aperture is configured in the 4th lens group.Also, work as light
It is excellent in the case that circle moves together with the 4th lens group when zooming or the 4th lens group is fixed on optical axis when zooming
Choosing, aperture slot are fixed.Here, aperture is configured in the 4th lens group and refers to, aperture is configured in the 4th lens group
In any one in object side, image side or the lens that are configured in the 4th lens group, if it is along optical axis direction with
4th lens group moves together or fixed structure, then the position being configured is not particularly limited.By the way that aperture configuration is existed
In 4th lens group, aberration when being able to suppress zoom changes, so as to realize high performance.
Also, in zoom lens of the invention, it is preferred that the 3rd lens group is in the zoom from wide-angle side to telescope end
When it is mobile to image side.By the configuration of lens group when taking such zoom, it can be realized high zoom ratios.
As described above, according to the present invention, by can be realized zoom with higher with above structure
Than, and it is able to maintain that in entire zoom area good optical property, small-sized and high performance zoom lens.The zoom
Lens be it is a kind of particularly suitable for the photographic device equipped with the solid-state imager for having carried out high pixelation, optical property it is higher
Lens.
In addition, the object of the present invention is to provide zoom ratio with higher, small-sized and high performance zoom lens
Photographic device.To realize the purpose, if photographic device is configured to include the zoom lens for having above structure, and
The optical image formed by the zoom lens is converted to the solid-state imager of electric signal.By doing so, can be realized
High-resolution photographic device.
Hereinafter, with reference to the accompanying drawings, the embodiment of zoom lens of the invention is described in detail.In addition, the present invention is not
It is limited to embodiment below.
[embodiment 1]
Fig. 1 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 1.The zoom lens are configured
To be configured in order from object side (not shown): the 1st lens group G with negative refractive power1, the with positive refractive power 2nd thoroughly
Microscope group G2, the 3rd lens group G with positive refractive power3And subsequent lens group GR.In the 3rd lens group G3With subsequent lens group GRIt
Between configured with defining the opening aperture STP of predetermined bore.In subsequent lens group GRCover glass is configured between image planes IMG
CG.Cover glass CG is configured as needed.
In addition, subsequent lens group GRIt is configured to, is configured in order from object side: the 4th lens with positive refractive power
Group G4, the 5th lens group G with positive refractive power5And the 6th lens group G with positive refractive power6。
1st lens group G1It is only by double-concave negative lens L11It constitutes.
2nd lens group G2It is configured to, is configured in order from object side: diverging meniscus lens of the convex surface towards object side
L21, biconvex positive lens L22And biconvex positive lens L23.Diverging meniscus lens L21With biconvex positive lens L22It engages.Biconvex just
Lens L23Two surfaces on formed it is aspherical.
3rd lens group G3It is configured to, is configured in order from object side: double-concave negative lens L31, double-concave negative lens L32, it is double
Convex positive lens L33And convex surface is towards the diverging meniscus lens L of image side34.In double-concave negative lens L31Two surfaces on form aspheric
Face.Biconvex positive lens L33With diverging meniscus lens L34It engages.
4th lens group G4It is configured to, is configured in order from object side: biconvex positive lens L41With convex surface towards image side
Diverging meniscus lens L42.Biconvex positive lens L41With diverging meniscus lens L42It engages.
5th lens group G5It is configured to, is configured in order from object side: biconvex positive lens L51, biconvex positive lens L52, it is double
Recessed negative lens L53, biconvex positive lens L54, convex surface towards object side diverging meniscus lens L55, biconvex positive lens L56And convex surface court
To the diverging meniscus lens L of image side57.In biconvex positive lens L51Two surfaces on formed it is aspherical.Biconvex positive lens L52, concave-concave
Negative lens L53And biconvex positive lens L54It engages.Diverging meniscus lens L55, biconvex positive lens L56And diverging meniscus lens L57
It engages.
6th lens group G6It is configured to, is configured in order from object side: diverging meniscus lens L of the convex surface towards object side61
With convex surface towards the positive meniscus lens L of object side62。
The zoom lens are being always maintained at the 1st lens group G when carrying out the zoom from wide-angle side to telescope end1, the 4th thoroughly
Microscope group G4And the 6th lens group G6In the state of being fixed relative to image planes IMG, the 2nd lens group G2Along optical axis in image planes IMG
The mode that side forms convex track is mobile, the 3rd lens group G3It is moved along optical axis from object side to the side image planes IMG dullness, the 5th thoroughly
Microscope group G5It is moved along optical axis from the side image planes IMG to object side dullness.
Hereinafter, showing various numeric datas relevant to the zoom lens of embodiment 1.
(surface data)
r1=-258.600
d1=1.300 nd1=1.8042 ν d1=46.50
r2=39.170
d2=D (2) (variable)
r3=56.700
d3=0.900 nd2=1.8548 ν d2=24.80
r4=31.260
d4=5.700 nd3=1.4970 ν d3=81.61
r5=-79.000
d5=0.150
r6=30.850 (aspherical)
d6=5.000 nd4=1.6935 ν d4=53.20
r7=-96.512 (aspherical)
d7=D (7) (variable)
r8=-103.233 (aspherical)
d8=0.600 nd5=1.8514 ν d5=40.10
r9=10.784 (aspherical)
d9=3.441
r10=-10.850
d10=0.600 nd6=1.6385 ν d6=55.45
r11=186.000
d11=0.176
r12=76.800
d12=2.310 nd7=1.9229 ν d7=20.88
r13=-16.960
d13=0.600 nd8=1.7292 ν d8=54.67
r14=-88.880
d14=D (14) (variable)
r15=∞ (opening aperture)
d15=0.600
r16=39.720
d16=4.210 nd9=1.4970 ν d9=81.61
r17=-19.300
d17=0.600 nd10=1.8042 ν d10=46.50
r18=-40.040
d18=D (18) (variable)
r19=48.511 (aspherical)
d19=3.200 nd11=1.6935 ν d11=53.20
r20=-68.078 (aspherical)
d20=0.150
r21=15.300
d21=7.440 nd12=1.4970 ν d12=81.61
r22=-15.300
d22=1.000 nd13=1.8061 ν d13=40.73
r23=118.600
d23=3.480 nd14=1.8081 ν d14=22.76
r24=-30.260
d24=0.150
r25=26.300
d25=1.000 nd15=2.0010 ν d15=29.13
r26=8.672
d26=5.290 nd16=1.4970 ν d16=81.61
r27=-12.864
d27=0.600 nd17=1.6204 ν d17=60.34
r28=-49.000
d28=D (28) (variable)
r29=46.000
d29=0.600 nd18=1.9037 ν d18=31.31
r30=18.300
d30=2.711
r31=20.440
d31=2.250 nd19=1.6968 ν d19=55.46
r32=126.500
d32=4.400
r33=∞
d33=1.000 nd20=1.5163 ν d20=64.14
r34=∞
d34=1.000
r35=∞ (image planes)
Circular cone coefficient (k) and asphericity coefficient (A4, A6, A8, A10, A12, A14)
(the 6th face)
K=0,
A4=-2.8400 × 10-6, A6=3.9875 × 10-8,
A8=-4.8993 × 10-10, A10=8.6640 × 10-12,
A12=-6.7380 × 10-14, A14=2.2082 × 10-16
(the 7th face)
K=0,
A4=3.3475 × 10-7, A6=1.0920 × 10-8,
A8=3.7294 × 10-10, A10=-1.5000 × 10-12,
A12=-1.2478 × 10-14, A14=1.1593 × 10-16
(the 8th face)
K=0,
A4=1.3969 × 10-5, A6=-1.3224 × 10-7,
A8=6.1860 × 10-9, A10=-1.0476 × 10-10,
A12=0, A14=0
(the 9th face)
K=0,
A4=4.9520 × 10-6, A6=-7.5303 × 10-7,
A8=5.6418 × 10-8, A10=-7.6164 × 10-10,
A12=0, A14=0
(the 19th face)
K=0,
A4=7.6863 × 10-6, A6=-1.0741 × 10-8,
A8=2.1915 × 10-9, A10=-1.7507 × 10-11,
A12=-1.2945 × 10-14, A14=0
(the 20th face)
K=0,
A4=2.0382 × 10-5, A6=-8.9746 × 10-8,
A8=3.1841 × 10-9, A10=-3.1291 × 10-11,
A12=2.2543 × 10-14, A14=0
(various data)
(variable focus lens package data)
(the relevant numerical value of conditional (1))
| F1/Fw |=9.86
(the relevant numerical value of conditional (2))
| F1/Ft |=0.87
(the relevant numerical value of conditional (3))
| F2/F3 |=3.16
(the relevant numerical value of conditional (4))
β 3t (the 3rd lens group G3In the lateral magnification of telescope end)=- 0.85
β 3w (the 3rd lens group G3In the lateral magnification of wide-angle side)=- 0.24
| β 3t/ β 3w |=3.49
(the relevant numerical value of conditional (5))
β pt (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of telescope end)=- 0.86
β pw (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of wide-angle side)=- 0.14
| β pt/ β pw |=6.09
Fig. 2 shows the various aberration diagrams of the zoom lens of embodiment 1.In spherical aberration diagram, the longitudinal axis indicates F number (figure
In indicated with FNO), solid line shows the characteristic for being equivalent to the wavelength of d line (587.56nm), and single dotted broken line, which is shown, is equivalent to C line
The characteristic of the wavelength of (656.28nm), dotted line show the characteristic for being equivalent to the wavelength of F line (486.13nm).In astigmatism figure, indulge
Axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.In addition, in astigmatism figure, it is real
Line shows the characteristic of sagittal plane (indicating in figure with S), and dotted line shows the characteristic of meridional plane (indicating in figure with M).It is distorting
In aberration diagram, the longitudinal axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.
[embodiment 2]
Fig. 3 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 2.The zoom of the present embodiment is saturating
The movement of the optical texture of mirror and each lens group when zooming is identical as zoom lens shown in embodiment 1.Therefore, in this reality
It applies in example, identical label is added to component same as Example 1, and omit the detailed description about them.
Hereinafter, the relevant various numeric datas of the zoom lens for showing embodiment 2.
(surface data)
r1=-128.642
d1=1.300 nd1=1.8042 ν d1=46.50
r2=86.633
d2=D (2) (variable)
r3=97.555
d3=0.900 nd2=1.8548 ν d2=24.80
r4=40.754
d4=5.700 nd3=1.4970 ν d3=81.61
r5=-81.000
d5=0.150
r6=33.462 (aspherical)
d6=5.000 nd4=1.6935 ν d4=53.20
r7=-105.004 (aspherical)
d7=D (7) (variable)
r8=-184.258 (aspherical)
d8=0.600 nd5=1.8514 ν d5=40.10
r9=9.660 (aspherical)
d9=3.441
r10=-12.151
d10=0.600 nd6=1.6385 ν d6=55.45
r11=67.822
d11=0.176
r12=40.190
d12=2.310 nd7=1.9229 ν d7=20.88
r13=-21.037
d13=0.600 nd8=1.7292 ν d8=54.67
r14=-106.143
d14=D (14) (variable)
r15=∞ (opening aperture)
d15=0.600
r16=35.038
d16=4.210 nd9=1.4970 ν d9=81.61
r17=-22.407
d17=0.600 nd10=1.8042 ν d10=46.50
r18=-67.185
d18=D (18) (variable)
r19=39.835 (aspherical)
d19=3.200 nd11=1.6935 ν d11=53.20
r20=-80.656 (aspherical)
d20=0.150
r21=15.683
d21=7.440 nd12=1.4970 ν d12=81.61
r22=-15.929
d22=1.000 nd13=1.8061 ν d13=40.73
r23=115.784
d23=3.480 nd14=1.8081 ν d14=22.76
r24=-31.156
d24=0.150
r25=24.351
d25=1.000 nd15=2.0010 ν d15=29.13
r26=8.639
d26=5.290 nd16=1.4970 ν d16=81.61
r27=-13.086
d27=0.600 nd17=1.6204 ν d17=60.34
r28=-43.515
d28=D (28) (variable)
r29=15.050
d29=0.600 nd18=1.9037 ν d18=31.31
r30=9.741
d30=2.711
r31=15.775
d31=2.250 nd19=1.6968 ν d19=55.46
r32=50.681
d32=4.400
r33=∞
d33=1.000 nd20=1.5163 ν d20=64.14
r34=∞
d34=1.000
r35=∞ (image planes)
Circular cone coefficient (k) and asphericity coefficient (A4, A6, A8, A10, A12, A14)
(the 6th face)
K=0,
A4=-2.7204 × 10-6, A6=4.0454 × 10-8,
A8=-4.6815 × 10-10, A10=8.5225 × 10-12,
A12=-6.9515 × 10-14, A14=2.2082 × 10-16
(the 7th face)
K=0,
A4=1.0655 × 10-6, A6=1.5711 × 10-8,
A8=3.6582 × 10-10, A10=-1.8761 × 10-12,
A12=-1.3073 × 10-14, A14=1.1593 × 10-16
(the 8th face)
K=0,
A4=-2.3816 × 10-7, A6=-2.2000 × 10-7,
A8=8.6543 × 10-9, A10=-1.1481 × 10-10,
A12=0, A14=0
(the 9th face)
K=0,
A4=-2.4723 × 10-5, A6=-1.7377 × 10-6,
A8=7.4493 × 10-8, A10=-1.1663 × 10-9,
A12=0, A14=0
(the 19th face)
K=0,
A4=4.9385 × 10-6, A6=-1.2067 × 10-8,
A8=2.2353 × 10-9, A10=-1.8036 × 10-11,
A12=-1.2945 × 10-14, A14=0
(the 20th face)
K=0,
A4=2.2832 × 10-5, A6=-8.0148 × 10-8,
A8=3.1887 × 10-9, A10=-3.1279 × 10-11,
A12=2.2543 × 10-14, A14=0
(various data)
(variable focus lens package data)
(the relevant numerical value of conditional (1))
| F1/Fw |=15.00
(the relevant numerical value of conditional (2))
| F1/Ft |=1.33
(the relevant numerical value of conditional (3))
| F2/F3 |=3.57
(the relevant numerical value of conditional (4))
β 3t (the 3rd lens group G3In the lateral magnification of telescope end)=- 0.88
β 3w (the 3rd lens group G3In the lateral magnification of wide-angle side)=- 0.24
| β 3t/ β 3w |=3.66
(the relevant numerical value of conditional (5))
β pt (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of telescope end)=- 0.91
β pw (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of wide-angle side)=- 0.21
| β pt/ β pw |=4.33
Fig. 4 shows the various aberration diagrams of the zoom lens of embodiment 2.In spherical aberration diagram, the longitudinal axis indicates F number (figure
In indicated with FNO), solid line shows the characteristic for being equivalent to the wavelength of d line (587.56nm), and single dotted broken line, which is shown, is equivalent to C line
The characteristic of the wavelength of (656.28nm), dotted line show the characteristic for being equivalent to the wavelength of F line (486.13nm).In astigmatism figure, indulge
Axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.In addition, in astigmatism figure, it is real
Line shows the characteristic of sagittal plane (indicating in figure with S), and dotted line shows the characteristic of meridional plane (indicating in figure with M).It is distorting
In aberration diagram, the longitudinal axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.
[embodiment 3]
Fig. 5 illustrates that the sectional view along optical axis of the structure of the zoom lens of embodiment 3.The zoom of the present embodiment is saturating
The movement of the optical texture of mirror and each lens group when zooming is identical as zoom lens shown in embodiment 1.Therefore, in this reality
It applies in example, identical label is added to component same as Example 1, and omit the detailed description about them.
Hereinafter, the relevant various numeric datas of the zoom lens for showing embodiment 3.
(surface data)
r1=-106.965
d1=1.300 nd1=1.8042 ν d1=46.50
r2=43.788
d2=D (2) (variable)
r3=69.161
d3=0.900 nd2=1.8548 ν d2=24.80
r4=35.650
d4=5.700 nd3=1.4970 ν d3=81.61
r5=-64.651
d5=0.150
r6=34.803 (aspherical)
d6=5.000 nd4=1.6935 ν d4=53.20
r7=-69.145 (aspherical)
d7=D (7) (variable)
r8=-75.672 (aspherical)
d8=0.600 nd5=1.8514 ν d5=40.10
r9=11.109 (aspherical)
d9=3.441
r10=-11.051
d10=0.600 nd6=1.6385 ν d6=55.45r11=72.120
d11=0.176
r12=54.292
d12=2.310 nd7=1.9229 ν d7=20.88
r13=-21.981
d13=0.600 nd8=1.7292 ν d8=54.67
r14=-31.329
d14=D (14) (variable)
r15=∞ (opening aperture)
d15=0.600
r16=38.054
d16=4.210 nd9=1.4970 ν d9=81.61
r17=-30.804
d17=0.600 nd10=1.8042 ν d10=46.50
r18=-134.701
d18=D (18) (variable)
r19=36.618 (aspherical)
d19=3.200 nd11=1.6935 ν d11=53.20
r20=-102.581 (aspherical)
d20=0.150
r21=14.586
d21=7.440 nd12=1.4970 ν d12=81.61
r22=-16.933
d22=1.000 nd13=1.8061 ν d13=40.73
r23=70.311
d23=3.480 nd14=1.8081 ν d14=22.76
r24=-34.965
d24=0.150
r25=23.865
d25=1.000 nd15=2.0010 ν d15=29.13
r26=7.955
d26=5.290 nd16=1.4970 ν d16=81.61
r27=-15.619
d27=0.600 nd17=1.6204 ν d17=60.34
r28=-66.177
d28=D (28) (variable)
r29=13.302
d29=0.600 nd18=1.9037 ν d18=31.31
r30=10.303
d30=2.711
r31=23.890
d31=2.250 nd19=1.6968 ν d19=55.46
r32=78.008
d32=4.400
r33=∞
d33=1.000 nd20=1.5163 ν d20=64.14
r34=∞
d34=1.000
r35=∞ (image planes)
Circular cone coefficient (k) and asphericity coefficient (A4, A6, A8, A10, A12, A14)
(the 6th face)
K=0,
A4=-2.7204 × 10-6, A6=4.0454 × 10-8,
A8=-4.6815 × 10-10, A10=8.5225 × 10-12,
A12=-6.9515 × 10-14, A14=2.2082 × 10-16
(the 7th face)
K=0,
A4=1.0655 × 10-6, A6=1.5711 × 10-8,
A8=3.6582 × 10-10, A10=-1.8761 × 10-12,
A12=-1.3073 × 10-14, A14=1.1593 × 10-16
(the 8th face)
K=0,
A4=-2.3816 × 10-7, A6=-2.2000 × 10-7,
A8=8.6543 × 10-9, A10=-1.1481 × 10-10,
A12=0, A14=0
(the 9th face)
K=0,
A4=-2.4723 × 10-5, A6=-1.7377 × 10-6,
A8=7.4493 × 10-8, A10=-1.1663 × 10-9,
A12=0, A14=0
(the 19th face)
K=0,
A4=4.9385 × 10-6, A6=-1.2067 × 10-8,
A8=2.2353 × 10-9, A10=-1.8036 × 10-11,
A12=-1.2945 × 10-14, A14=0
(the 20th face)
K=0,
A4=2.2832 × 10-5, A6=-8.0148 × 10-8,
A8=3.1887 × 10-9, A10=-3.1279 × 10-11,
A12=2.2543 × 10-14, A14=0
(various data)
(variable focus lens package data)
(the relevant numerical value of conditional (1))
| F1/Fw |=8.99
(the relevant numerical value of conditional (2))
| F1/Ft |=0.80
(the relevant numerical value of conditional (3))
| F2/F3 |=2.60
(the relevant numerical value of conditional (4))
β 3t (the 3rd lens group G3In the lateral magnification of telescope end)=- 0.94
β 3w (the 3rd lens group G3In the lateral magnification of wide-angle side)=- 0.26
| β 3t/ β 3w |=3.59
(the relevant numerical value of conditional (5))
β pt (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of telescope end)=- 0.96
β pw (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of wide-angle side)=- 0.24
| β pt/ β pw |=4.05
Fig. 6 shows the various aberration diagrams of the zoom lens of embodiment 3.In spherical aberration diagram, the longitudinal axis indicates F number (figure
In indicated with FNO), solid line shows the characteristic for being equivalent to the wavelength of d line (587.56nm), and single dotted broken line, which is shown, is equivalent to C line
The characteristic of the wavelength of (656.28nm), dotted line show the characteristic for being equivalent to the wavelength of F line (486.13nm).In astigmatism figure, indulge
Axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.In addition, in astigmatism figure, it is real
Line shows the characteristic of sagittal plane (indicating in figure with S), and dotted line shows the characteristic of meridional plane (indicating in figure with M).It is distorting
In aberration diagram, the longitudinal axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.
[embodiment 4]
Fig. 7 is the sectional view along optical axis for indicating the structure of the zoom lens of embodiment 4.The zoom lens of the present embodiment
Optical texture and each lens group when zooming movement, in addition in the 6th lens group G6Middle configuration biconvex positive lens L462Carry out generation
For positive meniscus lens L62It is identical as zoom lens shown in embodiment 1 except this point.Therefore, in the present embodiment, to
The identical component of embodiment 1 adds identical label, and omits the detailed description about them.
Hereinafter, the relevant various numeric datas of the zoom lens for showing embodiment 4.
(surface data)
r1=-87.698
d1=1.300 nd1=1.8042 ν d1=46.50
r2=52.797
d2=D (2) (variable)
r3=93.413
d3=0.900 nd2=1.8548 ν d2=24.80
r4=37.838
d4=5.700 nd3=1.4970 ν d3=81.61
r5=-53.869
d5=0.150
r6=33.677 (aspherical)
d6=5.000 nd4=1.6935 ν d4=53.20
r7=-67.360 (aspherical)
d7=D (7) (variable)
r8=-70.691 (aspherical)
d8=0.600 nd5=1.8514 ν d5=40.10
r9=10.250 (aspherical)
d9=3.441
r10=-11.717
d10=0.600 nd6=1.6385 ν d6=55.45
r11=80.294
d11=0.176
r12=43.624
d12=2.310 nd7=1.9229 ν d7=20.88
r13=-24.524
d13=0.600 nd8=1.7292 ν d8=54.67
r14=-46.616
d14=D (14) (variable)
r15=∞ (opening aperture)
d15=0.600
r16=36.940
d16=4.210 nd9=1.4970 ν d9=81.61
r17=-37.184
d17=0.600 nd10=1.8042 ν d10=46.50
r18=-82.098
d18=D (18) (variable)
r19=43.988 (aspherical)
d19=3.200 nd11=1.6935 ν d11=53.20
r20=-92.518 (aspherical)
d20=0.150
r21=14.558
d21=7.440 nd12=1.4970 ν d12=81.61
r22=-17.048
d22=1.000 nd13=1.8061 ν d13=40.73
r23=63.629
d23=3.480 nd14=1.8081 ν d14=22.76
r24=-33.337
d24=0.150
r25=26.905
d25=1.000 nd15=2.0010 ν d15=29.13
r26=8.052
d26=5.290 nd16=1.4970 ν d16=81.61
r27=-14.799
d27=0.600 nd17=1.6204 ν d17=60.34
r28=-49.354
d28=D (28) (variable)
r29=18.620
d29=0.600 nd18=1.9037 ν d18=31.31
r30=9.463
d30=2.711
r31=15.084
d31=2.250 nd19=1.6968 ν d19=55.46
r32=-181.440
d32=4.400
r33=∞
d33=1.000 nd20=1.5163 ν d20=64.14
r34=∞
d34=1.000
r35=∞ (image planes)
Circular cone coefficient (k) and asphericity coefficient (A4, A6, A8, A10, A12, A14)
(the 6th face)
K=0,
A4=-4.2932 × 10-6, A6=4.0241 × 10-8,
A8=-4.7280 × 10-10, A10=8.4476 × 10-12,
A12=-6.7890 × 10-14, A14=2.1651 × 10-16
(the 7th face)
K=0,
A4=4.1939 × 10-7, A6=8.9980 × 10-9,
A8=4.0304 × 10-10, A10=-1.6528 × 10-12,
A12=-1.5116 × 10-14, A14=1.1739 × 10-16
(the 8th face)
K=0,
A4=-3.9949 × 10-6, A6=1.8192 × 10-7,
A8=2.0321 × 10-9, A10=-6.3171 × 10-11,
A12=0, A14=0
(the 9th face)
K=0,
A4=-3.8713 × 10-5, A6=-1.0134 × 10-6,
A8=5.2657 × 10-8, A10=-7.4101 × 10-10,
A12=0, A14=0
(the 19th face)
K=0,
A4=4.7575 × 10-6, A6=-4.5557 × 10-8,
A8=2.1444 × 10-9, A10=-1.7342 × 10-11,
A12=-1.2945 × 10-14, A14=0
(the 20th face)
K=0,
A4=2.2402 × 10-5, A6=-9.4619 × 10-8,
A8=3.0257 × 10-9, A10=-2.9738 × 10-11,
A12=2.2543 × 10-14, A14=0
(various data)
(variable focus lens package data)
(the relevant numerical value of conditional (1))
| F1/Fw |=9.54
(the relevant numerical value of conditional (2))
| F1/Ft |=0.85
(the relevant numerical value of conditional (3))
| F2/F3 |=2.85
(the relevant numerical value of conditional (4))
β 3t (the 3rd lens group G3In the lateral magnification of telescope end)=- 1.21
β 3w (the 3rd lens group G3In the lateral magnification of wide-angle side)=- 0.25
| β 3t/ β 3w |=4.90
(the relevant numerical value of conditional (5))
β pt (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of telescope end)=- 0.63
β pw (movable group (the 5th lens group G in subsequent lens group5) in the lateral magnification of wide-angle side)=- 0.11
| β pt/ β pw |=5.60
Fig. 8 shows the various aberration diagrams of the zoom lens of embodiment 4.In spherical aberration diagram, the longitudinal axis indicates F number (figure
In indicated with FNO), solid line shows the characteristic for being equivalent to the wavelength of d line (587.56nm), and single dotted broken line, which is shown, is equivalent to C line
The characteristic of the wavelength of (656.28nm), dotted line show the characteristic for being equivalent to the wavelength of F line (486.13nm).In astigmatism figure, indulge
Axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.In addition, in astigmatism figure, it is real
Line shows the characteristic of sagittal plane (indicating in figure with S), and dotted line shows the characteristic of meridional plane (indicating in figure with M).It is distorting
In aberration diagram, the longitudinal axis indicates angle of half field-of view (indicating in figure with ω), and shows the characteristic for being equivalent to the wavelength of d line.
The correspondence table of conditional in the various embodiments described above described below.
[table 1]
Embodiment | 1 | 2 | 3 | 4 |
Conditional 1 | 9.86 | 15.00 | 8.99 | 9.54 |
Conditional 2 | 0.87 | 1.33 | 0.80 | 0.85 |
Conditional 3 | 3.16 | 3.57 | 2.60 | 2.85 |
Conditional 4 | 3.49 | 3.66 | 3.59 | 4.90 |
Conditional 5 | 6.09 | 4.33 | 4.05 | 5.60 |
In addition, in numeric data of the various embodiments described above, r1, r2... ... indicate the radius of curvature of lens surface etc.,
d1, d2... ... indicate the surface interval between the wall thickness or lens of lens etc., nd1, nd2... ... indicate lens etc. relative to d
The refractive index of line (λ=587.56nm), ν d1, ν d2... ... indicate the Abbe number relative to d line (λ=587.56nm) such as lens.
Also, the unit of length is all " mm ", and the unit of angle is all " ° ".
In addition, h is being set as by the height on the direction vertical with optical axis for above-mentioned each aspherical shape, it will be with lens
Displacement at height h when surface vertices are origin in the direction of the optical axis is set as X, paraxial curvature radius is set as R, by circular cone
Coefficient is set as k, and by 4 times, 6 times, 8 times, 10 times, 12 times, 14 asphericity coefficients are set to A4, A6, A8, A10, A12, A14,
When image planes direction is set as positive direction, above-mentioned each aspherical shape can be indicated by formula as follows.
[formula 1]
As shown in the above embodiments, by meeting above-mentioned each conditional, it can be realized with higher
Zoom ratio, and it is able to maintain that in entire zoom area good optical property, small-sized and high performance zoom lens.
< application examples >
Then, it shows zoom lens applications of the invention in the example of photographic device.Fig. 9, which is illustrated that, has the present invention
Zoom lens photographic device an example figure.As shown in figure 9, photographic device 100 is by being accommodated with the saturating of zoom lens 10
What mirror lens barrel portion 11 and camera body 21 with solid-state imager 20 were constituted.Zoom lens 10 pass through machinery (not shown)
The driving of mechanism executes zoom etc..In addition, as zoom lens 10, showing the change of embodiment 1 (referring to Fig.1) in Fig. 9
Focus lens, but zoom lens shown in embodiment 2~4 can be similarly carried on photographic device 100.
In the photographic device 100 with zoom lens 10 and solid-state imager 20, image planes IMG shown in FIG. 1 is suitable
In the imaging surface of solid-state imager 20.As solid-state imager 20, CCD (Charge Coupled can be used for example
Device: charge coupled device) or CMOS (Complementary Metal Oxide Semiconductor: Complementary metal
Oxide semiconductor) etc. photo-electric conversion element.
In photographic device 100, from final the taking the photograph in solid-state imager 20 of the light of the object side incidence of zoom lens 10
It is imaged in image planes.Also, solid-state imager 20 carries out photoelectric conversion to the light received and exports as electric signal.The output
Signal carries out calculation processing by signal processing circuit (not shown), and generates digital picture corresponding with subject image.Number
Word image for example can recorde the record of HDD (Hard Disk Drive: hard disk drive), storage card, CD, tape etc.
In medium.
By with structure as shown in Figure 9, may be implemented zoom ratio with higher, it is small-sized and high performance
The photographic device of zoom lens.
In fig. 9 it is shown that by zoom lens applications of the invention in the example of monitor camera.But it is of the invention
Zoom lens can be applied not only to monitor camera, can also be applied to video camera, digital still camera, single lens reflex type
In camera, reflector-free single-lens reflex camera etc..
[industrial utilizability]
As described above, zoom lens of the invention take the photograph the small-sized of the solid-state imager equipped with CCD or CMOS etc.
As device be it is useful, be particularly suitable for requiring the monitor camera of higher optical property.
Detailed description of the invention:
G1: the 1st lens group;G2: the 2nd lens group;G3: the 3rd lens group;G4: the 4th lens group;G5: the 5th lens group;G6: the 6th
Lens group;GR: subsequent lens group;L11, L31, L32, L53: double-concave negative lens;L21, L34, L42, L55, L57, L61: diverging meniscus lens;
L22, L23, L33, L41, L51, L52, L54, L56, L462: biconvex positive lens;L62: positive meniscus lens;STP: opening aperture;CG: outer cover
Glass;IMG: image planes;10: zoom lens;11: lens barrel portion;20: solid-state imager;21: camera body;100: taking the photograph
As device.
Claims (7)
1. a kind of zoom lens, which is characterized in that
The zoom lens are the 1st lens groups with negative refractive power, with positive refractive power by configuring in order from object side
What the 2nd lens group, the 3rd lens group with negative refractive power and subsequent lens group were constituted,
Wherein, by least making the 2nd lens in the state of being always maintained at the 1st lens group relative to image planes fixation
Group and the 3rd lens group are moved along optical axis, to change interval of each lens group on optical axis, are thus carried out from wide-angle
The zoom of telescope end is held,
Also, the zoom lens meet conditional as follows:
(1)3.5≦|F1/Fw|≦20.0
(2)0.7≦|F1/Ft|≦2.0
(3)1.9≦|F2/F3|≦5.0
Wherein, F1 indicates that the focal length of the 1st lens group, Fw indicate the zoom lens in the focal length of wide-angle side, Ft
The zoom lens are indicated in the focal length of telescope end, F2 indicates that the focal length of the 2nd lens group, F3 indicate the described 3rd
The focal length of lens group.
2. zoom lens according to claim 1, which is characterized in that
The zoom lens meet conditional as follows:
(4)3.0≦|β3t/β3w|≦9.0
Wherein, β 3t indicates the 3rd lens group in the lateral magnification of telescope end, and β 3w indicates the 3rd lens group in wide-angle
The lateral magnification at end.
3. zoom lens according to claim 1, which is characterized in that
The subsequent lens group is with the 4th lens group configuring in order from object side, with positive refractive power and has just in the wrong
5th lens group of luminous power.
4. zoom lens according to claim 3, which is characterized in that
When carrying out zoom, any one in the 4th lens group or the 5th lens group is moved along optical axis, and
Meet conditional as follows:
(5)3.0≦|βpt/βpw|≦10.0
Wherein, β pt indicates the movable group in the subsequent lens group in the lateral magnification of telescope end, and β pw indicates described subsequent
The lateral magnification of movable group in lens group in wide-angle side.
5. zoom lens according to claim 1, which is characterized in that
1st lens group is made of 1 lens.
6. zoom lens according to claim 3, which is characterized in that
The image planes side of 5th lens group in the subsequent lens group, described is configured with the 6th lens group with positive refractive power.
7. a kind of photographic device, which is characterized in that the photographic device includes
Zoom lens described in any one in claim 1~6, and
The optical image formed by the zoom lens is converted to electric signal by solid-state imager.
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JP2017247046A JP6840661B2 (en) | 2017-12-22 | 2017-12-22 | Zoom lens and imaging device |
JP2017-247046 | 2017-12-22 |
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CN109960023A true CN109960023A (en) | 2019-07-02 |
CN109960023B CN109960023B (en) | 2021-10-29 |
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Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH05107476A (en) * | 1991-10-14 | 1993-04-30 | Canon Inc | Wide angle system zoom lens |
JPH05323196A (en) * | 1992-05-21 | 1993-12-07 | Canon Inc | Rear focus type zoom lens |
CN102262290A (en) * | 2010-05-24 | 2011-11-30 | 佳能株式会社 | Zoom lens and image pickup apparatus having the zoom lens |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS613113A (en) * | 1984-06-15 | 1986-01-09 | Canon Inc | Zoom lens |
JPH0656453B2 (en) * | 1985-12-27 | 1994-07-27 | 株式会社ニコン | Zoom lenses |
JP2005106948A (en) * | 2003-09-29 | 2005-04-21 | Canon Inc | Projection optical system and picture projection device |
JP2007187879A (en) * | 2006-01-13 | 2007-07-26 | Konica Minolta Photo Imaging Inc | Imaging optical system and imaging apparatus |
US8503102B2 (en) * | 2011-04-19 | 2013-08-06 | Panavision International, L.P. | Wide angle zoom lens |
JP6632320B2 (en) * | 2015-10-20 | 2020-01-22 | キヤノン株式会社 | Zoom lens and imaging device having the same |
CN106990515B (en) * | 2016-12-16 | 2019-06-18 | 嘉兴中润光学科技有限公司 | A kind of zoom lens |
-
2017
- 2017-12-22 JP JP2017247046A patent/JP6840661B2/en active Active
-
2018
- 2018-09-26 CN CN201811123285.2A patent/CN109960023B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH05107476A (en) * | 1991-10-14 | 1993-04-30 | Canon Inc | Wide angle system zoom lens |
JPH05323196A (en) * | 1992-05-21 | 1993-12-07 | Canon Inc | Rear focus type zoom lens |
CN102262290A (en) * | 2010-05-24 | 2011-11-30 | 佳能株式会社 | Zoom lens and image pickup apparatus having the zoom lens |
Also Published As
Publication number | Publication date |
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JP2019113700A (en) | 2019-07-11 |
CN109960023B (en) | 2021-10-29 |
JP6840661B2 (en) | 2021-03-10 |
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