JPS60260912A - Zoom lens - Google Patents
Zoom lensInfo
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- JPS60260912A JPS60260912A JP11787384A JP11787384A JPS60260912A JP S60260912 A JPS60260912 A JP S60260912A JP 11787384 A JP11787384 A JP 11787384A JP 11787384 A JP11787384 A JP 11787384A JP S60260912 A JPS60260912 A JP S60260912A
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- lens
- refractive power
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- object side
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Abstract
Description
【発明の詳細な説明】
本発明はズームレンズに関し、特にカラービデオカメラ
に適したズームレンズに関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a zoom lens, and particularly to a zoom lens suitable for a color video camera.
従来よりビデオカメラ用の撮影レンズは、撮像素子が比
較的低感度の為になるべく明るいレンズであることが要
求されている。又、ビデオカメラの小型軽量化を図る為
にレンズ全長の短い撮影レンズが要求されている。更に
、単管式カラー撮像管やOO、Dの撮像板等のストライ
プフィルターを使用しているカラービデオカメラに用い
られる撮影レンズでは、混色の発生を防止する為にスト
ライプフィルターに入射する光線を略垂直に入射させる
ようにした所謂テレセンYリンクな光学系とし、しかも
高解像力の光学系であることが要求されている。このよ
うに、ビデオカメラに使用される撮影レンズは各種の事
項が要求されている。一般にズームレンズを用いて前述
の要求事項を満足させようとすると、良好に収差補正を
行うことが困難になってくる。特に、ズームレンズの小
型化を図ろうとすると歪曲収差2球面収差そしてコマ収
差等を良好に補正するのが困難となり、この結果、画像
のコントラストを低下させる原因となる。2. Description of the Related Art Photographic lenses for video cameras have traditionally been required to be as bright as possible because the sensitivity of an image sensor is relatively low. Furthermore, in order to make video cameras smaller and lighter, there is a need for a photographic lens with a short overall lens length. Furthermore, in color video cameras that use stripe filters such as single-tube color image pickup tubes and OO and D image pickup plates, the light rays incident on the stripe filter are shortened to prevent color mixture. It is required that the optical system be a so-called telecentric Y-link optical system in which the light is incident perpendicularly, and that the optical system has a high resolution. As described above, various requirements are required of photographic lenses used in video cameras. Generally, when trying to satisfy the above-mentioned requirements using a zoom lens, it becomes difficult to properly correct aberrations. In particular, when trying to downsize a zoom lens, it becomes difficult to satisfactorily correct distortion, bispherical aberration, coma, and the like, which results in a reduction in image contrast.
本発明はレンズ全系が略テレセントリックとなるように
し、しかも明るさがFl、4と大口径の良好に収差補正
を達成した小型のズームレンズの提供を目的とする。An object of the present invention is to provide a compact zoom lens in which the entire lens system is substantially telecentric, has a brightness of Fl.4, has a large aperture, and achieves good aberration correction.
本発明の目的を達成する為のズームレンズの主たる特徴
は、物体側より順に7オーカシング用の正の屈折力の第
ルンズ群、変倍用の負の屈折力の第2レンズ群、変倍に
より変動する像面を補正する為の負の屈折力の第6レン
ズ群そして結像作 ”用をする正の屈折力の第4レンズ
群の4つのレン1□ □ズ群を有し、前記第2レンズ群
は像面側に凹面を向けたメニスカス状の負の屈折力の第
2ルンズと物体側に凸面を向けた貼合せ面を持つ負と正
の屈折力のレンズの貼合せレンズを有し、前記第4レン
ズ群は正の屈折力の第4ルンズ群と同じく正の屈折力の
第42レンズ群の2つのレンズ群を有し、前記第4ルン
ズ群は物体側のレンズ面に比べ像面側のレンズ面の方が
強い屈折力(以下「像面側に強い屈折力」という。)を
有する両レンズ面が凸面の第41ルンズ、像面側のレン
ズ面に比べ物体側のレンズ面の方が強い屈折力(以下「
物体側に強い屈折力」という。)を有する両レンズ面が
凸面の第412レンズ、物体側に強い屈折力を有する負
の屈折力の第413レンズそして物体側に強い屈折力を
有する両レンズ面が凸面の第414レンズの4つのレン
ズを有し、前記第42レンズ群は像面側に強い屈折力を
有する両レンズ面が凹面の第42ルンズ、像面側に強い
屈折力を有する両レンズ面が凸面の第422レンズそし
て物体側に強い屈折力を有する両レンズ面が凸面の第4
25レンズの6つのレンズを有し、前記第2レンズ群の
物体側より数えて第を番目のレンズ面の曲率半径をR1
(、前記第4レンズ群の物体側より数えて第を番目のレ
ンズの物体側と像面側のレンズ面の曲率半径を各々R■
i1.R■i2、第1番目のレンズと第(+1番目のレ
ンズとの間隔をDi −1−4−1そして全系の広角端
のズーム位置での焦点距離をfwとするとき、0.79
< IRII2/ Ru5t<0.85(但しJn2>
o、Ru3<a)・Φ・(1)t 5 < l RIV
21/ RNslK 1.7 (但し、Ru21〉0.
Ru31〈0)・・・(2)1.6 < Rya1/
fw < 1.8・・・(3)11 < RV52/
fw< 1.5 @@@(4>t 1 < l R■6
2/ Ru711< 1.4 (但し、Ru62<O,
Ru71>O)・・・(5)t 1 < RNy1/
fw < 1.4 *”(6)0.15〈Dy2〜5<
0.2 @・・(7)0.95< Dy4〜5<1.2
・・・(8)なる諸条件を満足することである。The main features of the zoom lens for achieving the purpose of the present invention are, in order from the object side, a lens group with a positive refractive power for focusing, a second lens group with a negative refractive power for zooming, and a lens group with a negative refractive power for zooming. It has four lens groups: a sixth lens group with negative refractive power for correcting a changing image plane, and a fourth lens group with positive refractive power for image formation. The second lens group has a meniscus-shaped second lens with a negative refractive power with a concave surface facing the image side, and a laminated lens of negative and positive refractive power lenses with a laminated surface with a convex surface facing the object side. However, the fourth lens group has two lens groups: a fourth lens group with positive refractive power and a 42nd lens group with positive refractive power, and the fourth lens group is A 41st lens in which both lens surfaces are convex, with the lens surface on the image side having stronger refractive power (hereinafter referred to as "stronger refractive power on the image side"), and the lens surface on the object side compared to the lens surface on the image side. has a stronger refractive power (hereinafter referred to as “
"strong refractive power on the object side." ), the 412th lens has a negative refractive power and has a strong refractive power on the object side, and the 414th lens has a strong refractive power on the object side and has both convex lens surfaces. The 42nd lens group includes a 42nd lens with both concave lens surfaces having a strong refractive power on the image side, a 422nd lens with both lens surfaces having a convex surface and a strong refractive power on the image side, and an object. The fourth lens has both convex lens surfaces with strong refractive power on the side.
The radius of curvature of the second lens surface counting from the object side of the second lens group is R1.
(, the radius of curvature of the object-side and image-side lens surfaces of the th lens counting from the object side of the fourth lens group is R
i1. R■i2, when the distance between the 1st lens and the +1st lens is Di -1-4-1, and the focal length at the wide-angle end zoom position of the entire system is fw, 0.79
<IRII2/ Ru5t<0.85 (However, Jn2>
o, Ru3<a)・Φ・(1)t5<l RIV
21/RNslK 1.7 (However, Ru21>0.
Ru31〈0)...(2)1.6 <Rya1/
fw < 1.8...(3) 11 < RV52/
fw< 1.5 @@@(4>t 1 < l R■6
2/ Ru711<1.4 (However, Ru62<O,
Ru71>O)...(5)t1<RNy1/
fw < 1.4 *” (6) 0.15〈Dy2~5<
0.2 @...(7) 0.95<Dy4~5<1.2
...(8) must be satisfied.
このように、本発明では特に、変倍用の第2レンズ群と
結像用の第4レンズ群のレンズ構成を前述の如く設定す
ることにより、良好に収差補正を行った小型のズームレ
ンズを達成している。このうち、第2レンズ群の第2ル
ンズの像面側のレンズ面と第22レンズの物体側のレン
ズ面の屈折力を所定の範囲内に設定することにより、変
倍による収差変動を少なくし、又、第4レンズ群の各レ
ンズの形状及び屈折力を前述の如く設定することにより
、明るくしかもテレセントリックな光学系を良好に達成
すると共に、全ズーム範囲にわたり良好に収差補正を行
っている。In this way, the present invention particularly provides a compact zoom lens with excellent aberration correction by setting the lens configurations of the second lens group for variable power and the fourth lens group for imaging as described above. Achieved. Among these, by setting the refractive power of the image side lens surface of the second lens of the second lens group and the object side lens surface of the 22nd lens within a predetermined range, aberration fluctuations due to zooming can be reduced. Furthermore, by setting the shape and refractive power of each lens in the fourth lens group as described above, a bright and telecentric optical system is successfully achieved, and aberrations are well corrected over the entire zoom range.
次に、前述の各条件式の技術的な意味について述べる。Next, the technical meaning of each of the above conditional expressions will be described.
条件式(1)は、第2レンズ群の移動量をなるべく少な
くしつつ所定の変倍比を得ると共に、全ズーム範囲にわ
たって収差変動特に球面収差とコマ収差の変動を少なく
する為である。上限値を越えて第2ルンズの像面側のレ
ンズ面の屈折力が第22レンズの物体側のレンズ面の屈
折力より小さくなると内向性のコマ収差が発生し、又、
下限値を越えると望遠側のズーム位置での球面収差が補
正過剰となってくる。Conditional expression (1) is intended to obtain a predetermined zoom ratio while minimizing the amount of movement of the second lens group, and to reduce fluctuations in aberrations, particularly fluctuations in spherical aberration and coma aberration, over the entire zoom range. If the upper limit is exceeded and the refractive power of the lens surface on the image side of the second lens becomes smaller than the refractive power of the lens surface on the object side of the second lens, introverted coma aberration occurs;
If the lower limit is exceeded, the spherical aberration at the telephoto zoom position becomes overcorrected.
条件式(2)は、第412レンズと第413レンズの物
体側のレンズ面の屈折力比に関し、特に、全ズーム範囲
にわたり球面収差を適切に補正する為である。上限値を
越えると球面収差が補正過剰となり、又、下限値を越え
ると補正不足となる。Conditional expression (2) relates to the refractive power ratio of the object-side lens surfaces of the 412th lens and the 413th lens, and is particularly intended to appropriately correct spherical aberration over the entire zoom range. If the upper limit is exceeded, the spherical aberration will be over-corrected, and if the lower limit is exceeded, the spherical aberration will be under-corrected.
条件式(3)は、第414レンズの物体側のレンズ面の
屈折力を適切に設定し、球面収差の発生量を極力少なく
すると共に光束を効率良く収斂させる為である。上限値
を越えると光束を十分に収斂させることが難しく後方の
第42レンズ群全体のレンズ径を小さくすることが困難
となり、又、下限値を越えるとレンズ全長を短くしズー
ムレンズの小型化を図ることはできるが、球面収差が多
く発生してくるので好ましくない。Conditional expression (3) is intended to appropriately set the refractive power of the object-side lens surface of the 414th lens, to minimize the amount of spherical aberration, and to efficiently converge the light beam. If the upper limit is exceeded, it will be difficult to sufficiently converge the light beam, and it will be difficult to reduce the overall lens diameter of the rear 42nd lens group.If the lower limit is exceeded, the overall length of the lens will be shortened, making it difficult to downsize the zoom lens. Although this can be achieved, it is not preferable because a large amount of spherical aberration occurs.
条件式(4)は、第42ルンズの像面側のレンズ面の屈
折力に関し、コマ収差を極力発生させずにレンズ系全体
を良好なるテレセントリックな光学系とする為である。Conditional expression (4) relates to the refractive power of the lens surface on the image side of the 42nd lens in order to minimize the occurrence of coma aberration and make the entire lens system a good telecentric optical system.
上限値を越えると良好なるテレセンドリンク光学系を得
るのが難しく、又、下限値を越えると画面中間での外向
性コマ収差の発生が多くなり、このときの外向性コマ収
差を他のレンズ面で補正するのが困難となる。If the upper limit is exceeded, it will be difficult to obtain a good telescopic link optical system, and if the lower limit is exceeded, extroverted coma aberration will occur frequently in the middle of the screen, and the extroverted coma at this time will be transferred to other lens surfaces. This makes it difficult to correct.
条件式(5)、(6)は、第422レンズの像面側のレ
ンズ面と第423レンズの物体側のレンズ面の屈折力に
関し、特に、球面収差とコマ収差を良好に補正すると共
に画面全体の像面湾曲を少なくする為である。条件式(
5)の上限値と条件式(6)の下限値を越えると第42
ルンズで発生する一外向性コマ収差を良好に補正するの
が困爵となり、又、像面湾曲も大きくなる。条件式(5
)の下限値と条件式(6)の上限値を越えると全ズーム
範囲にわたり球面収差が補正過剰となり、更に、コマ収
差が多く発生してくる。Conditional expressions (5) and (6) relate to the refractive power of the image-side lens surface of the 422nd lens and the object-side lens surface of the 423rd lens. This is to reduce the overall curvature of field. Conditional expression (
If the upper limit of conditional expression (5) and the lower limit of conditional expression (6) are exceeded, the 42nd
It becomes difficult to satisfactorily correct the one-extroverted coma aberration that occurs in the lens, and the curvature of field also increases. Conditional expression (5
) and the upper limit of conditional expression (6) are exceeded, spherical aberration becomes overcorrected over the entire zoom range, and more coma aberration occurs.
条件式(力は、第412レンズと第413レンズとの空
気間隔を適切に保ち球面収差と画面全体のコマ収差を良
好に補正する為である。上限値を越えると球面収差が補
正過剰となり、更に、コマ収差の発生が多くなる。又、
下限値を越えると球面収差が補正不足となる。Conditional Expression (The force is used to properly maintain the air distance between the 412th lens and the 413th lens and properly correct spherical aberration and comatic aberration of the entire screen. If the upper limit is exceeded, spherical aberration will be overcorrected, Furthermore, the occurrence of coma aberration increases.Also,
If the lower limit is exceeded, spherical aberration will be insufficiently corrected.
条件式(8)は、第414レンズと第42ルンズとの間
隔すなわち第4ルンズ群と第42レンズ群との間隔を適
切に設定し、画面全体のコマ収差と軸外色収差をバラン
ス良く補正し、かつ、良好なるテレセントリックな光学
系を達成する為である。上限値を越えると外向性コマ収
差の発生が多くなり、又、軸外色収差が補正過剰傾向と
なり、又、下限値を越えると軸外色収差が補正不足とな
り、かつ、良好なるテレセントリックな光学系を達成す
るのが困難となる。Conditional expression (8) sets the distance between the 414th lens and the 42nd lens appropriately, that is, the distance between the 4th lens group and the 42nd lens group, and corrects comatic aberration and off-axis chromatic aberration of the entire screen in a well-balanced manner. , and to achieve a good telecentric optical system. If the upper limit value is exceeded, outward comatic aberration will occur more often, and off-axis chromatic aberration will tend to be over-corrected.If the lower limit value is exceeded, off-axis chromatic aberration will be under-corrected, and a good telecentric optical system will not be possible. difficult to achieve.
以上説明した如く、本発明においては、前述の諸条件を
満足させることにより大口径の良好に収差補正を行った
、しかも良好なるテレセントリックな光学系を有した小
型のズームレンズを達成することができる。As explained above, in the present invention, by satisfying the above-mentioned conditions, it is possible to achieve a compact zoom lens with a large aperture, well-corrected aberrations, and a good telecentric optical system. .
尚、本発明においては、第6レンズ群を像面側に凸面を
向けたメニスカス状の1枚のレンズで構成することによ
り、レンズ全長の短縮化を図りつつ変倍による収差変動
を少なくしている。In addition, in the present invention, by configuring the sixth lens group with a single meniscus lens with a convex surface facing the image plane side, the overall length of the lens can be shortened and aberration fluctuations due to zooming can be reduced. There is.
次に本発明の数値実施例を示す。数値実施例において、
Riは物体側より順に第を番目のレンズ面の曲率半径、
Diは物体側より順に第を番目のレンズ厚及び空気間隔
、Niとνtは各々物体側より順に第を番目のレンズの
ガラスの屈折率とアツベ数である。Next, numerical examples of the present invention will be shown. In numerical examples,
Ri is the radius of curvature of the th lens surface in order from the object side,
Di is the thickness and air gap of the first lens from the object side, and Ni and νt are the refractive index and Abbe number of the glass of the second lens from the object side, respectively.
数値実施例1,2におけるR30.R31、数値実施例
6,4における12B、 R29はフェースプレート、
ローパスフィルター、近赤外カットフィルター等のガラ
スブロック、数値実施例1,2におけるR15.R16
はファインダー光束や自動焦点検出用の光束の取数値実
縛例1
F−1〜5.7 FNO−1:1.42ω−492’−
8,7゜R17−絞り Dl7−0.1667
b、f−0,595レンズ全長−10,35,0数値実
施例2
F−1〜5.7 FNO−1F1.42ω−492°〜
8.7゜R17−絞り Dl 7−0.1667b、f
−0,549レンズ全長−10,285数値実施例6
F−1〜5.7 FNO−1:i、42ω−492°〜
8.7゜R1−9,2544D I−0,1627N
1−1.80518ν1−25.4R2−5A925D
2−0.6507 N 2−1.60511シ2−6
0.7R5−−10,4139D 3−0.0121R
4−2,8656D 4−0.4349 N 3−1.
69680ν3−55.5R5−12ニア675 D
5−可変
R6−22,8612D 6−0.0815 N 4−
1.77250ν4−49.6R7−1,1808D
7−0.5091R8−−14607D B=0.08
13 N 5−1.69680ν5−55.5R9−1
4920D 9−0.2603 N 6−1.8466
6シ6−23.9R10−−31,5074Dlo−可
変R11−−18871Dll−0,0815N 7−
169680シアー55.5R12=18.3046
D12−可変R13−7,8584D13−0.414
8 N 8−1.77250ν8−49.6R14−−
2159D14−0.305(lR15−絞り D15
−0.1667
R16−5,0984D16−0.3498 N 9−
1.69/)80ν9−55.5R17−−9,189
1D17−0.1864R18−−19654D18−
α0976 N10−1.84666シ10−23.9
R19−−10,5125D1?−0,0122R20
−1,7462D20−0.4880 N11−151
633シ11−64.lR21−−8,1420D21
−1.0564R22−−4,5097D22−0.0
813 N12−1.83400ν12−37.2R2
5−1,3115D25−0130R24−4,129
4D24−0.5254 N13−1.51633シ1
3−64.1R25−−1,6847D25−0.01
22R26−1,2905D26−0.4067 N1
4−1.57135シ14−53.0R27−−12.
5351 D27−0.1627R28−※ D28−
0.7906 N15−1.51633シ15−64.
1R29−代
す、f−0,5772レンズ全長−9831数値実施例
4
F=1〜5.7 FNO−1,:1.42ω−492°
〜8.7゜R1−9,4373D I−0,1627N
1−1.80518ν1−25.4R2−3,218
2D 2−06507 N 2−1.60511シ2−
60.7R5−−10,1451D 5−0.0115
R4−2,8535D 4−0.4298 N 3−1
.69680ν5−55.5R5−12,3999D
5−可変
R6−20,6618D 6−0.081!l N 4
−1.77250ν4−49.6R7−1,1880D
7−0.3109R8−−14575D 8−0.0
813 N 5−1.69680ν5−55.5R9−
1,50!+7 D 9−0.2603N 6−1.8
4666シ6−23.9R10−−37,1497I)
10−可変R11−−1,8819Dll−0,081
3N 7−1.69680シアー55.5R12−−1
7,8?162 D12−可変R13−7,8552D
15−0.4148 N 8−1.77250ν8−4
9.6R14−−2,1140D14−0.3009R
15−絞り D15−0.1667
R16−5,1345DI6−0.3497 N 9−
1.69680ν9−55.5R17−−9,0919
D17−0.1877R1B−−1,9516D18−
0.0976 N10−1.84666シ10−23.
9R19−−−9,9099D19−0.0122R2
0−1,7583D20−0.4880 N11−1.
51653シ1l−S4.lR21−−7,73<S9
D21−1.0564R22−−4,3587D22
−0.0813 N12−1.83400ν12−37
.2R25−1,3268D23−0.1119R24
−4,3082D24−0.3253 N13−1.5
1633シ13−64.lR25−−1,6552D2
5−0.0122R26−1,2909D26−0.4
067 N14−1.57135シ14−53.0R2
7−−13.7234 D27−0.17527R28
−o= D28−0.7906N15=1.51633
シ15−64.I29−00
b、f−0,577レンズ全長−9831次に、表1に
前述の諸条件と本発明の数値実施例との対応関係を示す
。R30 in Numerical Examples 1 and 2. R31, 12B in Numerical Examples 6 and 4, R29 is a face plate,
Glass blocks such as low-pass filters and near-infrared cut filters, R15 in Numerical Examples 1 and 2. R16
is the actual value of the finder light flux and the light flux for automatic focus detection Example 1 F-1 ~ 5.7 FNO-1: 1.42ω-492'-
8,7°R17-Aperture Dl7-0.1667 b, f-0,595 Lens total length-10,35,0 Numerical example 2 F-1~5.7 FNO-1F1.42ω-492°~
8.7゜R17-Aperture Dl 7-0.1667b, f
-0,549 Lens total length -10,285 Numerical example 6 F-1~5.7 FNO-1:i, 42ω-492°~
8.7゜R1-9,2544D I-0,1627N
1-1.80518ν1-25.4R2-5A925D
2-0.6507 N 2-1.60511 C 2-6
0.7R5--10,4139D 3-0.0121R
4-2,8656D 4-0.4349N 3-1.
69680ν3-55.5R5-12 Near 675 D
5-Variable R6-22,8612D 6-0.0815 N 4-
1.77250ν4-49.6R7-1, 1808D
7-0.5091R8--14607D B=0.08
13 N 5-1.69680ν5-55.5R9-1
4920D 9-0.2603 N 6-1.8466
6shi6-23.9R10--31,5074Dlo-Variable R11--18871Dll-0,0815N 7-
169680 sear 55.5R12=18.3046
D12-variable R13-7, 8584D13-0.414
8 N 8-1.77250ν8-49.6R14--
2159D14-0.305 (lR15-Aperture D15
-0.1667 R16-5,0984D16-0.3498 N 9-
1.69/)80ν9-55.5R17--9,189
1D17-0.1864R18--19654D18-
α0976 N10-1.84666 10-23.9
R19--10,5125D1? -0,0122R20
-1,7462D20-0.4880 N11-151
633shi11-64. lR21--8, 1420D21
-1.0564R22--4,5097D22-0.0
813 N12-1.83400ν12-37.2R2
5-1,3115D25-0130R24-4,129
4D24-0.5254 N13-1.51633si1
3-64.1R25--1,6847D25-0.01
22R26-1, 2905D26-0.4067 N1
4-1.57135shi14-53.0R27--12.
5351 D27-0.1627R28-* D28-
0.7906 N15-1.51633 15-64.
1R29-substitute, f-0,5772 Lens total length-9831 Numerical example 4 F=1~5.7 FNO-1,: 1.42ω-492°
~8.7゜R1-9,4373D I-0,1627N
1-1.80518ν1-25.4R2-3,218
2D 2-06507 N 2-1.60511 C 2-
60.7R5--10,1451D 5-0.0115
R4-2,8535D 4-0.4298 N 3-1
.. 69680ν5-55.5R5-12, 3999D
5-Variable R6-20,6618D 6-0.081! l N 4
-1.77250ν4-49.6R7-1,1880D
7-0.3109R8--14575D 8-0.0
813 N 5-1.69680ν5-55.5R9-
1,50! +7 D 9-0.2603N 6-1.8
4666shi6-23.9R10--37,1497I)
10-Variable R11--1,8819Dll-0,081
3N 7-1.69680 sear 55.5R12--1
7,8?162 D12-variable R13-7,8552D
15-0.4148 N 8-1.77250ν8-4
9.6R14--2,1140D14-0.3009R
15-Aperture D15-0.1667 R16-5, 1345DI6-0.3497 N 9-
1.69680ν9-55.5R17--9,0919
D17-0.1877R1B--1,9516D18-
0.0976 N10-1.84666 10-23.
9R19---9,9099D19-0.0122R2
0-1,7583D20-0.4880 N11-1.
51653S1l-S4. lR21--7,73<S9
D21-1.0564R22--4,3587D22
-0.0813 N12-1.83400ν12-37
.. 2R25-1, 3268D23-0.1119R24
-4,3082D24-0.3253 N13-1.5
1633shi 13-64. lR25--1,6552D2
5-0.0122R26-1, 2909D26-0.4
067 N14-1.57135shi14-53.0R2
7--13.7234 D27-0.17527R28
-o=D28-0.7906N15=1.51633
C15-64. I29-00 b, f-0,577 Lens total length -9831 Next, Table 1 shows the correspondence between the above-mentioned conditions and numerical examples of the present invention.
表11n条件と本発明の数値実施例との関係Relationship between Table 11n conditions and numerical examples of the present invention
第1.第2.第3.第4図は各々本発明の数値実施例1
,2,3.4のレンズ断面図、第5図(〜。
(b)+(’) +第6図(a)、(b)、(C) 、
第7図(a)、(b)、(C) 、第8図(a)、(b
)。
(0)は各々本発明の数値実施例1,2,5.4の諸収
差図であり、図中、(a) 、 (b) 、 (Cりは
各々広角端。
中間、望遠端のズーム位置での諸収差図、696面、Δ
Mはメリデイオナル像面、■、…+”+■1+■2は各
々第1.第2.第3.第41.第42レンズ群である。
特許出願人 キャノン株式会社
箋 1 図
第2図
第 3 図
第 4 図
第 5 同 頃)
毛 5 邸cb>
第 S 囲。。、
第 6 図、。、
第 6 2 (b)
箋 6 図、。、
第 7 凹(2)
第 7 図(1))
第71c。
塊 δ 図偵)
第 δ 開 市〕
第δ 図(C)1st. Second. Third. Figure 4 shows numerical example 1 of the present invention.
, 2, 3.4 lens sectional view, Fig. 5 (~. (b) + (') + Fig. 6 (a), (b), (C),
Figure 7 (a), (b), (C), Figure 8 (a), (b)
). (0) are various aberration diagrams of numerical examples 1, 2, and 5.4 of the present invention, and in the figures, (a), (b), and (C) are respectively at the wide-angle end.Zoom at the intermediate and telephoto end. Various aberration diagrams at various positions, 696 planes, Δ
M is the meridional image plane, and ■, ...+"+■1+■2 are the 1st, 2nd, 3rd, 41st, and 42nd lens groups, respectively. Patent applicant Canon Co., Ltd. 1 Figure 2 3 Fig. 4 Fig. 5 Same time) Mao 5 Residence cb> No. S Encircle..., Fig. 6, ., Fig. 6 2 (b) Notebook 6 Fig.,..., 7th concave (2) Fig. 7 (1) )) Section 71c.
Claims (1)
ズ群、変倍用の負の屈折力の第2レンズ群、変倍により
変動する像面を補正する為の負の屈折力の第3レンズ群
そして結像作用をする正の屈折力の第4レンズ群の4つ
のレンズ群を有し、前記第2レンズ群は像面側に凹面を
向けたメニスカス状の負の屈折力の第2ルンズと、物体
側に凸面を向けた貼合せ面を持つ負と正の屈折力のレン
ズの貼合せレンズを有し、前記第4レンズ群は正の屈折
力の第4ルンズ群と第42レンズ群の2つのレンズ群を
有し、前記第4ルンズ群は像面側に強い屈折力を有する
両レンズ面が凸面の第41ルンズ、物体側に強い屈折力
を有する両レンズ面が凸面の第412レンズ、物体側に
強い屈折力を有する負の屈折力の第413レンズそして
物体側に強い屈折力を有する両レンズ面が凸面の第41
4レンズの4つのレンズを有し、前記第42レンズ群は
像面側に強い屈折力を有する両レンズ面が凹面の第42
ルンズ、像面側に強い屈折力を有する両レンズ面が凸面
の第422レンズ − ゛ そし て物体側に強い屈折力を有する両レンズ面が凸面の第4
23レンズの6つのレンズを有し、前記第2レンズ群の
物体側より数えて第を番目のレンズ面の曲率半径をRI
[i1前記第4レンズ群の物体側より数えて第を番目の
レンズの物体側と像面側のレンズ面の曲率半径を各々R
1vi1゜RIvi2、第1番目のレンズと第1+1番
目のレンズとの間隔をDi−1+1 そして全系の広角
端のズーム位置での焦点距離をfWとするとき、0.7
9< lRI[2/ RI[31〈0.85(但し、R
1[2>O,RII3<0)1、’5 (lR■21/
R■511(1,7(但し−R■21>O,RIvSl
<0)1.6< RIV41 / fw <1.81.
1 < RIV52 / fw < 1.51.1 と
IR■62/ R■71 l< 1.4 (但し、R■
62〈0.R■71〉0)1.1 < RNy+ /
fw < 1.40.15<DN2〜S〈02 0.95 < Dy4〜5<1.2 なる罷条件を満足することを特徴とするズームレンズ。[Claims] In order from the object side, a first lens group with positive refractive power for focusing, a second lens group with negative refractive power for zooming, and a negative lens group for correcting the image plane that changes due to zooming. It has four lens groups: a third lens group with refractive power and a fourth lens group with positive refractive power that performs an imaging function, and the second lens group has a meniscus-shaped negative lens group with a concave surface facing the image plane The fourth lens group includes a second lens with a refractive power, and a laminated lens of a lens with a negative and positive refractive power having a laminated surface with a convex surface facing the object side, and the fourth lens group includes a fourth lun with a positive refractive power. The fourth lens group includes a 41st lens whose both lens surfaces are convex and has a strong refractive power on the image side, and both lenses have a strong refractive power on the object side. A 412th lens with a convex surface, a 413rd lens with a negative refractive power having a strong refractive power on the object side, and a 41st lens with both lens surfaces convex and having a strong refractive power on the object side.
The 42nd lens group has four lenses, and the 42nd lens group has a strong refractive power on the image side and both lens surfaces are concave.
The 422nd lens has both convex lens surfaces and has strong refractive power on the image side - ゛ And the 4th lens has both convex lens surfaces and has strong refractive power on the object side
The radius of curvature of the second lens surface counting from the object side of the second lens group is RI.
[i1 The radius of curvature of the object-side and image-side lens surfaces of the th lens counting from the object side of the fourth lens group is R, respectively.
1vi1°RIvi2, when the distance between the 1st lens and the 1st+1st lens is Di-1+1, and the focal length at the wide-angle end zoom position of the entire system is fW, 0.7
9< lRI[2/ RI[31<0.85 (however, R
1[2>O, RII3<0) 1,'5 (lR■21/
R ■ 511 (1, 7 (however - R ■ 21 > O, RIvSl
<0)1.6<RIV41/fw<1.81.
1 < RIV52 / fw < 1.51.1 and IR■62/R■71 l < 1.4 (However, R■
62〈0. R ■71〉0)1.1 <RNy+ /
A zoom lens that satisfies the following condition: fw<1.40.15<DN2~S<02 0.95<Dy4~5<1.2.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11787384A JPS60260912A (en) | 1984-06-08 | 1984-06-08 | Zoom lens |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11787384A JPS60260912A (en) | 1984-06-08 | 1984-06-08 | Zoom lens |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS60260912A true JPS60260912A (en) | 1985-12-24 |
JPH0558165B2 JPH0558165B2 (en) | 1993-08-25 |
Family
ID=14722378
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11787384A Granted JPS60260912A (en) | 1984-06-08 | 1984-06-08 | Zoom lens |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60260912A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6440808A (en) * | 1987-08-05 | 1989-02-13 | Canon Kk | Zoom lens |
US5095387A (en) * | 1989-07-26 | 1992-03-10 | Canon Kabushiki Kaisha | Zoom lens |
JP2019138941A (en) * | 2018-02-06 | 2019-08-22 | キヤノン株式会社 | Zoom lens and image capturing device having the same |
-
1984
- 1984-06-08 JP JP11787384A patent/JPS60260912A/en active Granted
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6440808A (en) * | 1987-08-05 | 1989-02-13 | Canon Kk | Zoom lens |
US5095387A (en) * | 1989-07-26 | 1992-03-10 | Canon Kabushiki Kaisha | Zoom lens |
JP2019138941A (en) * | 2018-02-06 | 2019-08-22 | キヤノン株式会社 | Zoom lens and image capturing device having the same |
US11067779B2 (en) | 2018-02-06 | 2021-07-20 | Canon Kabushiki Kaisha | Zoom lens and image pickup apparatus including the same |
Also Published As
Publication number | Publication date |
---|---|
JPH0558165B2 (en) | 1993-08-25 |
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