JP2001228395A - Rear focus type zoom lens and optical equipment using the same - Google Patents

Rear focus type zoom lens and optical equipment using the same

Info

Publication number
JP2001228395A
JP2001228395A JP2000041671A JP2000041671A JP2001228395A JP 2001228395 A JP2001228395 A JP 2001228395A JP 2000041671 A JP2000041671 A JP 2000041671A JP 2000041671 A JP2000041671 A JP 2000041671A JP 2001228395 A JP2001228395 A JP 2001228395A
Authority
JP
Japan
Prior art keywords
lens
group
object side
refractive power
rear focus
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP2000041671A
Other languages
Japanese (ja)
Other versions
JP2001228395A5 (en
JP4593716B2 (en
Inventor
Yasunori Murata
安規 村田
Nobuyuki Tochigi
伸之 栃木
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP2000041671A priority Critical patent/JP4593716B2/en
Publication of JP2001228395A publication Critical patent/JP2001228395A/en
Publication of JP2001228395A5 publication Critical patent/JP2001228395A5/ja
Application granted granted Critical
Publication of JP4593716B2 publication Critical patent/JP4593716B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B15/00Optical objectives with means for varying the magnification
    • G02B15/14Optical 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
    • G02B15/144Optical 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 having four groups only
    • G02B15/1441Optical 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 having four groups only the first group being positive
    • G02B15/144113Optical 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 having four groups only the first group being positive arranged +-++

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lenses (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a rear focus type zoom lens provided with excellent performance all over the zoom area and all over the object distance and having a high variable power ratio, and optical equipment using the same. SOLUTION: This zoom lens is provided wit four lens groups, that is, a 1st group having positive refractive power, a 2nd group having negative refractive power, a 3rd group provided with a diaphragm and having positive refractive power and a 4th group having positive refractive power in order from an object side. In the case of variable power from a wide-angle end to a telephoto end, the 2nd group is moved to an image surface side and also the 4th group is moved so as to hold a locus projected to the object side, and focusing is performed by moving the 4th group. The 2nd group is constituted of a 21st negative meniscus lens whose convex surface faces to the object side, a 22nd negative lens whose both lens surfaces are concave and a combined lens obtained by bonding a 23rd positive lens whose both lens surfaces are convex and a 24th negative lens in order from the object side, and the 3rd group is constituted of one positive lens having an aspherical surface.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、リヤーフォーカス
式のズームレンズ及びそれを用いた光学機器に関し、特
にビデオカメラやフィルムカメラ、そして放送用カメラ
等に好適に用いられる高変倍比でありながら、大口径比
であり、構成するレンズ枚数が比較的少ないリヤーフォ
ーカス式のズームレンズ及びそれを用いた光学機器に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rear focus type zoom lens and an optical apparatus using the same, and more particularly to a rear focus type zoom lens having a high zoom ratio suitably used for a video camera, a film camera, a broadcast camera, and the like. The present invention relates to a rear focus type zoom lens having a large aperture ratio and a relatively small number of constituent lenses, and an optical apparatus using the same.

【0002】[0002]

【従来の技術】従来よりビデオカメラや写真カメラ等の
光学機器に用いられるズームレンズにおいて、物体側の
第1レンズ群以外のレンズ群を移動させてフォーカスを
行なう所謂リヤーフォーカス式を採用したものが種々提
案されている。一般にリヤーフォーカス式ズームレンズ
は比較的小型軽量のレンズ群を移動させて焦点合せを行
なう為にフォーカスレンズ群の駆動力が小さくなり、迅
速な焦点合せが出来る等の特長がある。
2. Description of the Related Art Conventionally, a zoom lens used for an optical apparatus such as a video camera or a photographic camera employs a so-called rear focus type in which a lens group other than a first lens group on the object side is moved to perform focusing. Various proposals have been made. In general, a rear focus type zoom lens has a feature that a relatively small and lightweight lens group is moved to perform focusing, so that the driving force of the focus lens group is small, and quick focusing is possible.

【0003】例えば、特開昭62−24213号公報、
特開平2−48621号公報、そして特開平4−433
11号公報などでは、物体側より順に正の屈折力の第1
レンズ群、変倍作用の負の屈折力の第2レンズ群、正の
屈折力の第3レンズ群、そして正の第4レンズ群の4つ
のレンズ群を有し、前記第1、第3レンズ群の各レンズ
群を固定とし、前記第2レンズ群を光軸に沿って移動さ
せて変倍を行い、前記第4レンズ群を変倍に伴う像面位
置変動を補正するように光軸に沿って移動させるととも
に、該第4レンズ群を移動させて合焦を行うリヤーフォ
ーカス式ズームレンズが提案されている。
[0003] For example, JP-A-62-24233,
JP-A-2-48621 and JP-A-4-433
In Japanese Patent Publication No. 11 and the like, the first positive refractive power in
The first and third lenses include four lens groups, a lens group, a second lens group having a negative refractive power for zooming, a third lens group having a positive refractive power, and a positive fourth lens group. Each lens group of the group is fixed, the second lens group is moved along the optical axis to perform zooming, and the fourth lens group is moved along the optical axis so as to correct the image plane position variation accompanying zooming. A rear focus zoom lens has been proposed which moves the fourth lens group along and moves the fourth lens group for focusing.

【0004】又、特開昭63−29718号公報では、
物体側より順に正の屈折力の第1群と、負レンズ、負レ
ンズ、正レンズの3枚のレンズにて構成され、全体とし
て負の屈折力で変倍時に可動であって主として変倍をつ
かさどる第2群と、正の屈折力を有し非球面を含む第3
群と、少し大きな空気間隔をあけて正の屈折力を有し変
倍に伴う像面変動を補正し、合焦のために移動する第4
群より構成したズームレンズを開示している。
In Japanese Patent Application Laid-Open No. 63-29718,
The first lens unit has a positive refractive power and a negative lens, a negative lens, and a positive lens in order from the object side. A second group that controls the first group and a third group that has a positive refractive power and includes an aspheric surface.
A fourth lens unit having a positive refracting power with a slightly large air gap between the lens unit and the image surface to correct for image plane fluctuation due to zooming, and moving for focusing.
A zoom lens composed of a group is disclosed.

【0005】又、特開平5−72472号公報では、物
体側より順に正の屈折力で固定の第1群、負の屈折力で
変倍のための第2群、固定で集光作用を有し正の屈折力
の第3群、像面位置を維持するために光軸上を移動する
正の屈折力の第4群を有する非球面を用いたズームレン
ズを開示している。これは、第2群はメニスカス状の負
レンズと両凹レンズと正レンズを配し、第3群は1面以
上の非球面である単レンズから構成され、第4群は1面
以上の非球面を有するレンズで構成されている。
In Japanese Patent Application Laid-Open No. 5-72472, a first lens unit having a positive refractive power and a second lens unit for zooming with a negative refractive power are arranged in order from the object side. A zoom lens using an aspheric surface having a third lens unit having a positive refractive power and a fourth lens unit having a positive refractive power that moves on the optical axis to maintain the image plane position is disclosed. The second group includes a meniscus negative lens, a biconcave lens, and a positive lens, the third group includes a single lens having one or more aspheric surfaces, and the fourth group includes one or more aspheric surfaces. .

【0006】[0006]

【発明が解決しようとする課題】一般にズームレンズに
おいてリヤーフォーカス方式を採用するとレンズ系全体
が小型化され、又、迅速なるフォーカスが可能となり、
更に近接撮影が容易になる等の特長が得られる。
In general, when a rear focus system is employed in a zoom lens, the entire lens system is reduced in size, and quick focusing becomes possible.
Further, features such as easy close-up photography can be obtained.

【0007】しかしながら反面、フォーカスの際の収差
変動が大きくなり、無限遠物体から近距離物体に至る物
体距離全般に渡り高い光学性能を得るのが大変難しくな
ってくる。
[0007] On the other hand, however, aberration fluctuation at the time of focusing becomes large, and it becomes very difficult to obtain high optical performance over the entire object distance from an object at infinity to an object at a short distance.

【0008】特に大口径比で高変倍比のズームレンズで
は機構の簡素化を図りつつ、全変倍範囲にわたり、又、
物体距離全般にわたり高い光学性能を得るのが大変難し
くなってくる。
In particular, in a zoom lens having a large aperture ratio and a high zoom ratio, the mechanism is simplified, over the entire zoom range, and
It becomes very difficult to obtain high optical performance over the entire object distance.

【0009】例えば、先の特開昭62−24213号公
報で提案されているリヤーフォーカス式のズームレンズ
の実施例をみると、変倍の機能を有する第2レンズ群
は、物体側より順に物体側に凸面を向けたメニスカス状
の負の単レンズ、両レンズ面が凹面の負レンズと正レン
ズとを接合した貼合せレンズより構成されている。該貼
合せレンズは主に軸上の色収差、球面収差および軸外の
コマ収差の補正を行なっている。
For example, in the embodiment of the rear focus type zoom lens proposed in Japanese Patent Application Laid-Open No. Sho 62-24213, the second lens group having the function of zooming is arranged in the order from the object side to the object side. It is composed of a meniscus negative single lens with the convex surface facing the side, and a cemented lens in which a negative lens and a positive lens whose both lens surfaces are concave are joined. The laminated lens mainly corrects axial chromatic aberration, spherical aberration, and off-axis coma.

【0010】前記ズームタイプにおいて更に小型化、高
変倍化を図ろうとして第2レンズ群の屈折力を強める
と、該第2レンズ群の貼合せレンズ面での収差補正の負
担が大きくなり過ぎ、全ズーム域で高性能を実現するの
が困難となる。
If the refractive power of the second lens group is increased in order to further reduce the size and increase the zoom ratio of the zoom type, the burden of aberration correction on the cemented lens surface of the second lens group becomes too large. It is difficult to achieve high performance in the entire zoom range.

【0011】また、該第2レンズ群の屈折力を強める
と、該第2レンズ群を構成する各レンズの曲率が小さく
なると伴に高次の収差発生量が増加し、ズーム全域で良
好に収差補正を行うことが困難になってくる。
Further, when the refractive power of the second lens group is increased, the curvature of each lens constituting the second lens group is reduced, and the amount of higher-order aberrations is increased. It becomes difficult to make corrections.

【0012】本発明は、レンズ系全体を小型化し、高変
倍比であるにもかかわらず高い光学性能を有し、かつレ
ンズの構成枚数を減らした簡易な構成のレンズ全長の短
いズームレンズ及びそれを用いた光学機器の提供を目的
とする。
SUMMARY OF THE INVENTION The present invention provides a zoom lens having a short overall lens length and a simple configuration in which the entire lens system is reduced in size, has high optical performance despite a high zoom ratio, and has a reduced number of lenses. It is intended to provide an optical device using the same.

【0013】[0013]

【課題を解決するための手段】請求項1の発明のズーム
レンズは、物体側より順に正の屈折力の第1群、負の屈
折力の第2群、絞り正の屈折力の第3群、そして正の屈
折力の第4群の4つのレンズ群を有し、広角端から望遠
端への変倍の際には、該第2群を像面側へ移動させると
共に第4群を物体側に凸状の軌跡を有するように移動さ
せ、合焦の際には該第4群を移動させて行い、該第2群
を物体側から順に、物体側に凸面を向けたメニスカス状
の負の第21レンズ、両レンズ面が凹面の負の第22レ
ンズ、両レンズ面が凸面の正の第23レンズと負の第2
4レンズとを接合した貼合わせレンズより構成し、該第
3群は非球面を有する正の1枚のレンズにより構成した
ことを特徴としている。
According to a first aspect of the present invention, there is provided a zoom lens having a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, and a third lens unit having a positive refractive power. And a fourth lens unit having a positive refractive power. In zooming from the wide-angle end to the telephoto end, the second unit is moved to the image plane side and the fourth unit is moved to the object side. The lens is moved so as to have a convex locus on the side, and the focusing is performed by moving the fourth lens group. The second lens group is sequentially moved from the object side to a negative meniscus shape having a convex surface facing the object side. The 21st lens, the negative 22nd lens with both lens surfaces concave, the positive 23rd lens with both lens surfaces convex, and the negative 2nd lens
The third lens unit is composed of a cemented lens in which four lenses are joined, and the third group is composed of one positive lens having an aspheric surface.

【0014】請求項2の発明は請求項1の発明におい
て、前記第22レンズの像側のレンズ面の曲率半径をR
222、前記第23レンズの物体側のレンズ面の曲率半
径をR231とするとき
According to a second aspect of the present invention, in the first aspect, the radius of curvature of the image-side lens surface of the 22nd lens is R.
222, when the radius of curvature of the object-side lens surface of the 23rd lens is R231

【0015】[0015]

【数3】 (Equation 3)

【0016】なる条件を満足することを特徴としてい
る。
It is characterized by satisfying the following conditions.

【0017】請求項3の発明は請求項1又は2の発明に
おいて、前記第23レンズの材質のアッベ数をν23、
前記第24レンズの材質のアッベ数をν24とするとき 15<(ν24−ν23)<30…(2) なる条件を満足することを特徴としている。
According to a third aspect of the present invention, in the first or second aspect, the Abbe number of the material of the 23rd lens is ν23,
When the Abbe number of the material of the twenty-fourth lens is ν24, the following condition is satisfied: 15 <(ν24−ν23) <30 (2)

【0018】請求項4の発明は請求項1,2又は3の発
明において、前記第2レンズ群の焦点距離をf2、前記
第23レンズと前記第24レンズとの接合レンズ面の曲
率半径をR234とするとき
According to a fourth aspect of the present invention, in the first, second, or third aspect, the focal length of the second lens group is f2, and the radius of curvature of the cemented lens surface between the 23rd lens and the 24th lens is R234. And when

【0019】[0019]

【数4】 (Equation 4)

【0020】なる条件を満足することを特徴としてい
る。
It is characterized by satisfying the following conditions.

【0021】請求項5の発明の光学機器は請求項1から
4のいずれか1項のリヤーフォーカス式のズームレンズ
を有することを特徴としている。
According to a fifth aspect of the present invention, there is provided an optical apparatus including the rear focus type zoom lens according to any one of the first to fourth aspects.

【0022】[0022]

【発明の実施の形態】図1は本発明のリヤーフォーカス
式のズームレンズの実施形態1の要部断面図、図2,図
3,図4は実施形態1の広角端,中間,望遠端のズーム
位置における収差図である。
FIG. 1 is a sectional view of an essential part of a rear focus type zoom lens according to a first embodiment of the present invention, and FIGS. 2, 3 and 4 show a wide angle end, a middle position and a telephoto end of the first embodiment. FIG. 7 is an aberration diagram at a zoom position.

【0023】図5は本発明のリヤーフォーカス式のズー
ムレンズの実施形態2の要部断面図、図6,図7,図8
は実施形態2の広角端,中間,望遠端のズーム位置にお
ける収差図である。
FIG. 5 is a sectional view of a main part of a rear focus type zoom lens according to a second embodiment of the present invention, and FIGS.
9A is an aberration diagram at a zoom position at a wide-angle end, a middle position, and a telephoto end according to the second embodiment.

【0024】図9は本発明のリヤーフォーカス式のズー
ムレンズの実施形態3の要部断面図、図10,図11,
図12は実施形態3の広角端,中間,望遠端のズーム位
置における収差図である。
FIG. 9 is a sectional view of a principal part of a rear focus type zoom lens according to a third embodiment of the present invention, and FIGS.
FIG. 12 is an aberration diagram at a zoom position at a wide angle end, a middle position, and a telephoto end according to the third embodiment.

【0025】図13は本発明のリヤーフォーカス式のズ
ームレンズの実施形態4の要部断面図、図14,図1
5,図16は実施形態4の広角端,中間,望遠端のズー
ム位置における収差図である。
FIG. 13 is a sectional view of a principal part of a rear focus type zoom lens according to a fourth embodiment of the present invention, and FIGS.
5 and FIG. 16 are aberration diagrams of the fourth embodiment at zoom positions at the wide-angle end, the middle position, and the telephoto end.

【0026】図17は本発明のリヤーフォーカス式のズ
ームレンズの実施形態5の要部断面図、図18,図1
9,図20は実施形態5の広角端,中間,望遠端のズー
ム位置における収差図である。
FIG. 17 is a sectional view of a main portion of a rear focus type zoom lens according to a fifth embodiment of the present invention, and FIGS.
9 and 20 are aberration diagrams of the fifth embodiment at zoom positions at the wide-angle end, the middle position, and the telephoto end.

【0027】図21は本発明のリヤーフォーカス式のズ
ームレンズの実施形態6の要部断面図、図22,図2
3,図24は実施形態6の広角端,中間,望遠端のズー
ム位置における収差図である。
FIG. 21 is a sectional view of a main part of a rear focus type zoom lens according to a sixth embodiment of the present invention, and FIGS.
3 and FIG. 24 are aberration diagrams at the wide-angle end, a middle position, and a telephoto end according to the sixth embodiment.

【0028】図25は本発明のリヤーフォーカス式のズ
ームレンズの実施形態7の要部断面図、図26,図2
7,図28は実施形態7の広角端,中間,望遠端のズー
ム位置における収差図である。
FIG. 25 is a sectional view of a main part of a rear focus type zoom lens according to a seventh embodiment of the present invention, and FIGS.
7 and 28 are aberration diagrams of the seventh embodiment at zoom positions at the wide-angle end, the middle position, and the telephoto end.

【0029】図中L1は正の屈折力の第1群、L2は負
の屈折力の第2群、L3は正の屈折力の第3群、L4は
正の屈折力の第4群である。SPは開口絞りであり、第
3群L3の前方に配置している。Gは色分解プリズムや
フェースプレートやフィルター等のガラスブロックであ
る。IPは像面であり、CCD等の撮像素子が配置され
ている。
In the figure, L1 is a first group having a positive refractive power, L2 is a second group having a negative refractive power, L3 is a third group having a positive refractive power, and L4 is a fourth group having a positive refractive power. . SP denotes an aperture stop, which is arranged in front of the third lens unit L3. G is a glass block such as a color separation prism, a face plate, and a filter. IP is an image plane on which an image sensor such as a CCD is arranged.

【0030】本実施形態では広角端から望遠端への変倍
に際して矢印のように第2群を像面側へ移動させると共
に、変倍に伴う像面変動を第4群の一部又は全部(本実
施形態では全部)を物体側に凸状の軌跡を有しつつ移動
させて補正している。
In this embodiment, when zooming from the wide-angle end to the telephoto end, the second lens unit is moved to the image plane side as indicated by an arrow, and the image plane fluctuation due to zooming is partly or entirely included in the fourth lens unit. In the present embodiment, all of them are corrected while moving along a convex locus toward the object side.

【0031】又、第4群の一部又は全部(本実施形態で
は全部)を光軸上移動させてフォーカスを行うリヤーフ
ォーカス式を採用している。同図に示す第4群の実線の
曲線4aと点線の曲線4bは各々無限遠物体と近距離物
体にフォーカスしているときの広角端から望遠端への変
倍に伴う際の像面変動を補正するための移動軌跡を示し
ている。尚、第1群と第3群は変倍及びフォーカスの際
固定である。
Also, a rear focus system is employed in which a part or the whole (all in the present embodiment) of the fourth group is moved on the optical axis to perform focusing. A solid line curve 4a and a dotted line curve 4b of the fourth lens group shown in the same figure show the image plane fluctuation caused by zooming from the wide-angle end to the telephoto end when focusing on an object at infinity and an object at a short distance, respectively. The movement locus for correction is shown. The first and third units are fixed during zooming and focusing.

【0032】本実施例においては第4群を移動させて変
倍に伴う像面変動の補正を行うと共に第4群を移動させ
てフォーカスを行うようにしている。特に同図の曲線4
a,4bに示すように広角端から望遠端への変倍に際し
て物体側へ凸状の軌跡を有するように移動させている。
これにより第3群と第4群との空間の有効利用を図りレ
ンズ全長の短縮化を効果的に達成している。
In the present embodiment, the fourth lens unit is moved to correct the image plane fluctuation caused by zooming, and the fourth lens unit is moved to perform focusing. In particular, curve 4 in FIG.
When zooming from the wide-angle end to the telephoto end, the lens is moved so as to have a convex trajectory toward the object side as shown in FIGS.
Thereby, the space between the third and fourth units is effectively used, and the overall length of the lens is effectively reduced.

【0033】本実施例において、例えば望遠端において
無限遠物体から近距離物体へフォーカスを行う場合は同
図の直線4cに示すように第4群を前方へ繰り出すこと
により行っている。
In this embodiment, for example, when focusing from an object at infinity to an object at a short distance at the telephoto end, the fourth unit is moved forward as shown by a straight line 4c in FIG.

【0034】本発明において最も特徴的な点は、第2群
L2を前述したレンズ形状の3枚の負レンズと1枚の正
レンズの3群4枚のレンズより構成し、更に第3群L3
を構成する1つの正レンズに非球面を用いている点にあ
る。
The most characteristic point of the present invention is that the second lens unit L2 is composed of three negative lenses and one positive lens having the above-mentioned lens shape, and four lenses of the third lens unit L3.
Is that an aspherical surface is used for one positive lens.

【0035】高変倍比のズームレンズにおいて、小型で
ズーム全域に渡り良好に収差補正するためには、主に変
倍作用を担うバリエータと呼ばれる該第2レンズ群(以
下バリエータとも呼ぶ)での収差変動を小さく押さえる
事が重要である。しかし、小型で高変倍のレンズ仕様を
満たすためには変倍作用を担うバリエータに強い負の屈
折力を設定する必要があり、収差補正には不利な条件と
なる。
In a zoom lens having a high zoom ratio, in order to correct aberrations compactly and satisfactorily over the entire zoom range, the second lens group (hereinafter also referred to as a variator) mainly called a variator that performs a zooming action. It is important to minimize aberration fluctuations. However, in order to satisfy the specifications of a small-sized and high-magnification lens, it is necessary to set a strong negative refractive power to a variator that performs a magnification function, which is disadvantageous for aberration correction.

【0036】従来のバリエータは例えば特開平4−88
309号公報実施例に見られるような負レンズ、負レン
ズと正レンズの接合レンズの2群3枚構成のレンズタイ
プが主流であった、このタイプのバリエータで高変倍比
のズームレンズを実現しようとすると、バリエーターの
負の屈折力が強くなるに伴い、バリエータ内の負レンズ
と正レンズの接合レンズの接合レンズ面の曲率がきつく
なり、この接合レンズ面での高次収差の発生がズーム全
域での収差変動を大きくする原因となっていた。
A conventional variator is disclosed, for example, in Japanese Patent Laid-Open No. 4-88.
The mainstream is a lens type having two groups and three lenses of a negative lens and a cemented lens of a negative lens and a positive lens as seen in the embodiment of Japanese Patent Publication No. 309. A variator of this type realizes a zoom lens with a high zoom ratio. If this is attempted, as the negative refractive power of the variator becomes stronger, the curvature of the cemented lens surface of the cemented lens of the negative lens and the positive lens in the variator becomes tight, and the occurrence of higher-order aberrations on this cemented lens surface will zoom. This causes the aberration fluctuation in the entire region to be large.

【0037】そこで本発明のズームレンズにおいては、
変倍に大きく寄与する第2レンズ群L2を上記のような
レンズ構成にすることにより、各レンズのパワーの分担
を減らしペッツバール和の低減を図っている。これによ
って、高変倍比にしてもズーミングによる像面の変動を
少なくしている。更に該第2レンズ群から発散で入って
くる光束を受け止める第3レンズ群の正レンズに非球面
を配することにより光学性能の向上も図っている。各実
施形態においては、第3レンズ群L3の物体側のレンズ
面に非球面を用いている。
Therefore, in the zoom lens of the present invention,
By configuring the second lens unit L2, which greatly contributes to zooming, to the above-described lens configuration, the sharing of power of each lens is reduced, and the Petzval sum is reduced. As a result, even at a high zoom ratio, fluctuations in the image plane due to zooming are reduced. Further, the optical performance is improved by arranging an aspherical surface on the positive lens of the third lens group that receives the divergent light beam from the second lens group. In each embodiment, an aspheric surface is used for the lens surface on the object side of the third lens unit L3.

【0038】又、各数値実施例では、第1群を物体側に
凸面を向けたメニスカス状の負の第11レンズ、両レン
ズ面が凸面の正レンズ、そしてメニスカス状の正レンズ
より構成している。又、第4群を両レンズ面が凹面の負
レンズ、両レンズ面が凸面の正レンズ、そして両レンズ
面が凸面の正レンズより構成している。
In each numerical example, the first lens unit includes a negative meniscus eleventh lens having a convex surface facing the object side, a positive lens having both lens surfaces convex, and a positive meniscus lens. I have. The fourth lens unit is composed of a negative lens having both lens surfaces concave, a positive lens having both lens surfaces convex, and a positive lens having both lens surfaces convex.

【0039】本実施形態では以上のようにレンズ構成を
設定することにより、全変倍範囲にわたり、又、物体距
離全体にわたり高い光学性能を得ている。
In this embodiment, by setting the lens configuration as described above, high optical performance is obtained over the entire zoom range and over the entire object distance.

【0040】本発明のリヤーフォーカス式のズームレン
ズは、以上のような構成を満足することにより実現され
るが、更に高変倍比を維持しつつ光学性能を良好に維持
する為には、以下の条件のうち少なくとも1つを満足す
ることが望ましい。
The rear focus type zoom lens according to the present invention can be realized by satisfying the above-described configuration. To maintain the optical performance satisfactorily while maintaining a high zoom ratio, the following is required. It is desirable that at least one of the conditions is satisfied.

【0041】(ア-1)前記第22レンズの像側のレンズ面
の曲率半径をR222、前記第23レンズの物体側のレ
ンズ面の曲率半径をR231とするとき
(A-1) When the radius of curvature of the lens surface on the image side of the 22nd lens is R222, and the radius of curvature of the lens surface on the object side of the 23rd lens is R231

【0042】[0042]

【数5】 (Equation 5)

【0043】なる条件を満足することである。The following condition must be satisfied.

【0044】バリエータ(第2レンズ群)を物体側から
順に、負レンズ、負レンズ、正レンズと負レンズの接合
レンズとし、従来タイプのバリエータでは接合レンズで
あった第2負レンズと第3正レンズの間に空気層を設け
空隙レンズ作用をもたせた。この空隙レンズを積極的に
活用し条件式(1)を満足することで従来、接合レンズ面
であったバリエータの第2負レンズと第3正レンズの向
き合ったレンズ面の曲率を緩くすることを可能としてい
る。このレンズ面の曲率を緩くすることにより、高次の
球面収差や高次のコマ収差発生を少なくしている。
The variator (second lens group) is, in order from the object side, a negative lens, a negative lens, a cemented lens of a positive lens and a negative lens, and the second negative lens and the third positive lens, which were cemented lenses in the conventional type variator. An air layer was provided between the lenses to provide a gap lens function. By actively utilizing the gap lens and satisfying the conditional expression (1), the curvature of the facing lens surface of the second negative lens and the third positive lens of the variator, which was conventionally a cemented lens surface, is reduced. It is possible. By reducing the curvature of the lens surface, occurrence of higher-order spherical aberration and higher-order coma aberration is reduced.

【0045】条件式(1)の下限を超えると、空隙レンズ
自体で発生する高次球面収差が増大し収差補正困難とな
る、上限の0.5を超え1に近づくと空隙レンズ作用の
効果が薄れる。
If the lower limit of conditional expression (1) is exceeded, higher-order spherical aberration occurring in the gap lens itself will increase, making it difficult to correct aberrations. If it exceeds the upper limit of 0.5 and approaches 1, the effect of the gap lens effect will be lost. Fades.

【0046】(ア-2)前記第23レンズの材質のアッベ数
をν23、前記第24レンズの材質のアッベ数をν24
とするとき 15<(ν24−ν23)<30…(2) なる条件を満足することである。
(A-2) The Abbe number of the material of the 23rd lens is ν23, and the Abbe number of the material of the 24th lens is ν24.
The condition 15 <(ν24−ν23) <30 (2) is to be satisfied.

【0047】(ア-3) 前記第2レンズ群の焦点距離をf
2、前記第23レンズと前記第24レンズとの接合レン
ズ面の曲率半径をR234とするとき
(A-3) The focal length of the second lens group is f
2. When the radius of curvature of the cemented lens surface of the 23rd lens and the 24th lens is R234

【0048】[0048]

【数6】 (Equation 6)

【0049】なる条件を満足することである。前述の条
件式(1)で第22レンズの像面側のレンズ面と第23レ
ンズの物体側のレンズ面の曲率を緩くしたため色収差が
補正不足となる場合がある。そこでバリエータの色収差
をバランスよく補正するために、バリエータの第3レン
ズの後ろに第4レンズを接合し、条件式(2)及び(3)を満
足することで、ズーム全域に渡り色収差変動を少なく押
さえ、良好な収差補正を可能にしている。
The following condition must be satisfied. Since the curvature of the lens surface on the image surface side of the 22nd lens and the lens surface on the object side of the 23rd lens in the above-mentioned conditional expression (1) are reduced, chromatic aberration may be insufficiently corrected. Therefore, in order to correct the chromatic aberration of the variator in a well-balanced manner, a fourth lens is cemented behind the third lens of the variator, and by satisfying conditional expressions (2) and (3), chromatic aberration fluctuation is reduced over the entire zoom range. Hold down and good aberration correction are possible.

【0050】条件式(2)の下限を超えると色収差補正が
不足になり、上限を超えると現存する硝材では屈折率の
低いものとなり高次球面収差や高次コマ収差の発生が問
題になる。
If the lower limit of conditional expression (2) is exceeded, chromatic aberration correction will be insufficient. If the upper limit is exceeded, the refractive index of existing glass materials will be low, and high-order spherical aberration and high-order coma aberration will occur.

【0051】条件式(3)の下限を超えると色収差補正に
は有利となるが、この接合レンズ面での高次球面収差、
コマ収差の発生が問題となる、下限を超えると色収差補
正が不足となり、ズーム広角端から望遠端での色収差変
動が困難となる。
If the lower limit of conditional expression (3) is surpassed, it is advantageous for chromatic aberration correction.
If the coma aberration is a problem, and if the lower limit is exceeded, chromatic aberration correction becomes insufficient, and chromatic aberration variation from the zoom wide-angle end to the telephoto end becomes difficult.

【0052】上記条件を満たし第2レンズ群であるバリ
エータでの高次収差発生量と収差変動を少なく押さえる
ことにより、第3レンズ群を1枚の非球面レンズ構成で
収差補正を可能にしている。
By satisfying the above conditions and suppressing the amount of high-order aberrations and aberration fluctuations in the variator as the second lens unit to a small extent, the third lens unit can be corrected with a single aspherical lens. .

【0053】次に本発明のリヤーフォーカス式のズーム
レンズを撮影光学系として用いたビデオカメラ(光学機
器)の実施形態を図29を用いて説明する。
Next, an embodiment of a video camera (optical apparatus) using the rear focus type zoom lens of the present invention as a photographic optical system will be described with reference to FIG.

【0054】図29において、10はビデオカメラ本
体、11は本発明のズームレンズによって構成された撮
影光学系、12は撮影光学系11によって被写体像を受
光するCCD等の撮像素子、13は撮像素子12が受光
した被写体像を記録する記録手段、14は不図示の表示
素子に表示された被写体像を観察するためのファインダ
ーである。上記表示素子は液晶パネル等によって構成さ
れ、撮像素子12上に形成された被写体像が表示され
る。
In FIG. 29, 10 is a video camera body, 11 is a photographing optical system constituted by the zoom lens of the present invention, 12 is an image pickup device such as a CCD for receiving a subject image by the photographing optical system 11, and 13 is an image pickup device Reference numeral 12 denotes a recording unit for recording the received subject image, and reference numeral 14 denotes a finder for observing the subject image displayed on a display element (not shown). The display element includes a liquid crystal panel or the like, and displays a subject image formed on the image sensor 12.

【0055】このように本発明のズームレンズをビデオ
カメラ等の光学機器に適用することにより、小型で高い
光学性能を有する光学機器を実現している。
As described above, by applying the zoom lens of the present invention to an optical device such as a video camera, an optical device having a small size and high optical performance is realized.

【0056】以下に本発明の数値実施例を記載する。Hereinafter, numerical examples of the present invention will be described.

【0057】各数値実施例においてRiは物体側より順
に第i番目の面の曲率半径、Diは物体側より順に第i
番目の面と第(i+1)番目の面の間隔、Niとνiは
各々物体側より順に第i番目の光学部材のガラスの屈折
率とアッベ数である。
In each numerical example, Ri is the radius of curvature of the i-th surface in order from the object side, and Di is i-th surface in order from the object side.
The distance between the i-th surface and the (i + 1) -th surface, Ni and νi, are the refractive index and Abbe number of the glass of the i-th optical member in order from the object side.

【0058】非球面形状は光軸方向にX軸、光軸と垂直
方向にH軸、光の進行方向を正とし、Rを近軸曲率半
径、各非球面係数をK,B,C,D,E,Fとしたと
き、
The aspherical surface has an X axis in the optical axis direction, an H axis in a direction perpendicular to the optical axis, a positive traveling direction of light, R represents a paraxial radius of curvature, and each aspherical coefficient represents K, B, C, D. , E, F,

【0059】[0059]

【数7】 (Equation 7)

【0060】なる式で表している。This is represented by the following equation.

【0061】また、例えば「e−Z」の表示は「1
-Z」を意味する。
For example, the display of “eZ” is “1”.
0- Z ".

【0062】数値実施例において最終の2つのレンズ面
はフェースプレートやフィルター等のガラスブロックで
ある。又、前述の各条件式と数値実施例における諸数値
との関係を表1に示す。
In the numerical examples, the last two lens surfaces are glass blocks such as a face plate and a filter. Table 1 shows the relationship between the above-described conditional expressions and various numerical values in the numerical examples.

【0063】 数値実施例1 f=5.90〜57.80 fno=1:2.89〜2.95 2ω=60.6°〜6.4° r1=73.290 d1=1.30 n1=1.84666 ν1=23.9 r2=27.358 d2=5.00 n2=1.48749 ν2=70.2 r3=-185.356 d3=0.20 r4=26.768 d4=3.10 n3=1.88300 ν3=40.8 r5=98.007 d5=可変 r6=51.122 d6=0.80 n4=1.88300 ν4=40.8 r7=6.964 d7=2.83 r8=-31.195 d8=0.70 n5=1.88300 ν5=40.8 r9=36.000 d9=0.60 r10=14.590 d10=2.40 n6=1.84666 ν6=23.9 r11=-37.403 d11=0.60 n7=1.77250 ν7=49.6 r12=64.852 d12=可変 r13=(絞り) d13=2.20 *r14=50.190 d14=1.80 n8=1.58313 ν8=59.4 r15=-29.216 d15=可変 r16=-40.597 d16=0.70 n9=1.84666 ν9=23.8 r17=20.155 d17=2.80 n10=1.67790 ν10=54.9 *r18=-19.748 d18=0.50 r19=22.173 d19=1.60 n11=1.77250 ν11=49.6 r20=-154.454 d20=可変 r21=∞ d21=3.17 n12=1.51680 ν12=64.9 r22=∞ 非球面係数 r14面 r=5.01902D+01 k=-4.28770D+01 B=-2.56450D-07 C=1.20645D-07 D=1.59659D-08 E=1.63563D-09 F=-2.00233D-10 r18面 r=-1.97484D+01 k=1.79416D-01 B=2.42450D-06 C=1.88915D-07 D=-3.15899D-10 E=-1.16563D-10 F=7.84552D-13Numerical Example 1 f = 5.90 to 57.80 fno = 1: 2.89 to 2.95 2ω = 60.6 ° to 6.4 ° r1 = 73.290 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 27.358 d2 = 5.00 n2 = 1.48749 ν2 = 70.2 r3 = -185.356 d3 = 0.20 r4 = 26.768 d4 = 3.10 n3 = 1.88300 ν3 = 40.8 r5 = 98.007 d5 = variable r6 = 51.122 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.964 d7 = 2.83 r8 = -31.195 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 36.000 d9 = 0.60 r10 = 14.590 d10 = 2.40 n6 = 1.84666 ν6 = 23.9 r11 = -37.403 d11 = 0.60 n7 = 1.77250 ν7 = 49.6 r12 = 64.852 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 50.190 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -29.216 d15 = variable r16 = -40.597 d16 = 0.70 n9 = 1.84666 ν9 = 23.8 r17 = 20.155 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 * r18 =- 19.748 d18 = 0.50 r19 = 22.173 d19 = 1.60 n11 = 1.77250 ν11 = 49.6 r20 = -154.454 d20 = variable r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.9 r22 = ∞ Aspheric coefficient r14 surface r = 5.01902D + 01 k = -4.28770D + 01 B = -2.56450D-07 C = 1.20645D-07 D = 1.59659D-08 E = 1.63563D-09 F = -2.00233D-10 r18 surface r = -1.97484D + 01 k = 1.79416 D-01 B = 2.42450D-06 C = 1.88915D-07 D = -3.15899D-10 E = -1.16563D-10 F = 7.84552D- 13

【0064】[0064]

【表1】 [Table 1]

【0065】 数値実施例2 f=5.91〜57.84 fno=1:2.90〜2.93 2ω=60.4°〜6.4° r1=69.352 d1=1.30 n1=1.84666 ν1=23.9 r2=27.986 d2=5.10 n2=1.49700 ν2=81.5 r3=-177.475 d3=0.20 r4=26.474 d4=3.15 n3=1.88300 ν3=40.8 r5=86.929 d5=可変 r6=46.955 d6=0.80 n4=1.88300 ν4=40.8 r7=6.790 d7=2.89 r8=-34.381 d8=0.70 n5=1.88300 ν5=40.8 r9=51.533 d9=0.60 r10=12.882 d10=2.70 n6=1.84666 ν6=23.9 r11=-36.547 d11=0.60 n7=1.83481 ν7=42.7 r12=29.002 d12=可変 r13=(絞り) d13=2.20 *r14=39.181 d14=1.80 n8=1.58313 ν8=59.4 r15=-32.638 d15=可変 r16=-40.263 d16=0.70 n9=1.84666 ν9=23.9 r17=19.663 d17=2.80 n10=1.67790 ν10=54.9 *r18=-19.463 d18=0.50 r19=21.386 d19=1.85 n11=1.77250 ν11=49.6 r20=-195.606 d20=可変 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=3.91813D+01 k=-3.29956D+01 B=3.11655D-05 C=-2.69492D-07 D=-2.37202D-08 E=3.10037D-09 F=-1.59613D-10 r18面 r=-1.94634D+01 k=2.36307D-01 B=7.95708D-06 C=1.41805D-07 D=-7.93131D-09 E=1.43526D-10 F=3.95032D-13Numerical Example 2 f = 5.91 to 57.84 fno = 1: 2.90 to 2.93 2ω = 60.4 ° to 6.4 ° r1 = 69.352 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 27.986 d2 = 5.10 n2 = 1.49700 ν2 = 81.5 r3 = -177.475 d3 = 0.20 r4 = 26.474 d4 = 3.15 n3 = 1.88300 ν3 = 40.8 r5 = 86.929 d5 = variable r6 = 46.955 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.790 d7 = 2.89 r8 = -34.381 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 51.533 d9 = 0.60 r10 = 12.882 d10 = 2.70 n6 = 1.84666 ν6 = 23.9 r11 = -36.547 d11 = 0.60 n7 = 1.83481 ν7 = 42.7 r12 = 29.002 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 39.181 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -32.638 d15 = variable r16 = -40.263 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 19.663 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 * r18 =- 19.463 d18 = 0.50 r19 = 21.386 d19 = 1.85 n11 = 1.77250 ν11 = 49.6 r20 = -195.606 d20 = variable r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 3.91813D + 01 k = -3.29956D + 01 B = 3.11655D-05 C = -2.69492D-07 D = -2.37202D-08 E = 3.10037D-09 F = -1.59613D-10 r18 surface r = -1.94634D + 01 k = 2.36307D-01 B = 7.95708D-06 C = 1.41805D-07 D = -7.93131D-09 E = 1.43526D-10 F = 3.95032D- 13

【0066】[0066]

【表2】 [Table 2]

【0067】 数値実施例3 f=5.91〜57.79 fno=1:2.90〜3.01 2ω=59.2°〜6.02° r1=68.270 d1=1.35 n1=1.84666 ν1=23.9 r2=27.077 d2=5.60 n2=1.48749 ν2=70.2 r3=-127.735 d3=0.20 r4=25.006 d4=3.35 n3=1.83481 ν3=42.7 r5=84.576 d5=可変 r6=39.094 d6=0.80 n4=1.88300 ν4=40.8 r7=6.603 d7=2.92 r8=-34.526 d8=0.70 n5=1.88300 ν5=40.8 r9=38.104 d9=0.60 r10=12.977 d10=2.70 n6=1.84666 ν6=23.9 r11=-36.129 d11=0.60 n7=1.83481 ν7=42.7 r12=35.704 d12=可変 r13=(絞り) d13=2.20 *r14=44.157 d14=1.80 n8=1.58313 ν8=59.4 r15=-28.817 d15=可変 r16=-37.417 d16=0.70 n9=1.84666 ν9=23.9 r17=18.709 d17=2.80 n10=1.67790 ν10=54.9 *r18=-20.373 d18=0.50 r19=20.715 d19=1.80 n11=1.77250 ν11=49.6 r20=-92.038 d20=可変 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=4.41567D+01 k=-3.79319D+01 B=1.28884D-05 C=-2.45252D-08 D=3.55930D-08 E=7.85890D-10 F=-2.43503D-10 r18面 r=-2.03734D+01 k=-1.30631D-01 B=3.41480D-06 C=1.83231D-07 D=-2.36926D-09 E=-2.35948D-11 F=3.24000D-13Numerical Example 3 f = 5.91 to 57.79 fno = 1: 2.90 to 3.01 2ω = 59.2 ° to 6.02 ° r1 = 68.270 d1 = 1.35 n1 = 1.84666 ν1 = 23.9 r2 = 27.077 d2 = 5.60 n2 = 1.48749 ν2 = 70.2 r3 = -127.735 d3 = 0.20 r4 = 25.006 d4 = 3.35 n3 = 1.83481 ν3 = 42.7 r5 = 84.576 d5 = variable r6 = 39.094 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.603 d7 = 2.92 r8 = -34.526 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 38.104 d9 = 0.60 r10 = 12.977 d10 = 2.70 n6 = 1.84666 ν6 = 23.9 r11 = -36.129 d11 = 0.60 n7 = 1.83481 ν7 = 42.7 r12 = 35.704 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 44.157 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -28.817 d15 = variable r16 = -37.417 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 18.709 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 * r18 =- 20.373 d18 = 0.50 r19 = 20.715 d19 = 1.80 n11 = 1.77250 ν11 = 49.6 r20 = -92.038 d20 = variable r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 4.41567D + 01 k = -3.79319D + 01 B = 1.28884D-05 C = -2.45252D-08 D = 3.55930D-08 E = 7.85890D-10 F = -2.43503D-10 r18 surface r = -2.03734D + 01 k =- 1.30631D-01 B = 3.41480D-06 C = 1.83231D-07 D = -2.36926D-09 E = -2.35948D-11 F = 3.24000D -13

【0068】[0068]

【表3】 [Table 3]

【0069】 数値実施例4 f=6.00〜58.83 fno=1:2.89〜3.00 2ω=58.2°〜6.4° r1=70.307 d1=1.30 n1=1.84666 ν1=23.9 r2=26.658 d2=5.10 n2=1.48749 ν2=70.2 r3=-175.593 d3=0.20 r4=26.160 d4=3.15 n3=1.88300 ν3=40.8 r5=93.149 d5=可変 r6=30.946 d6=0.80 n4=1.88300 ν4=40.8 r7=6.518 d7=2.99 r8=-36.767 d8=0.70 n5=1.88300 ν5=40.8 r9=38.324 d9=0.60 r10=12.527 d10=2.70 n6=1.84666 ν6=23.9 r11=-65.030 d11=0.60 n7=1.83481 ν7=42.7 r12=29.726 d12=可変 r13=(絞り) d13=2.20 *r14=42.592 d14=1.80 n8=1.58313 ν8=59.4 r15=-24.975 d15=可変 r16=-40.384 d16=0.70 n9=1.84666 ν9=23.9 r17=18.252 d17=2.80 n10=1.67790 ν10=54.9 *r18=-19.890 d18=0.50 r19=20.267 d19=1.80 n11=1.77250 ν11=49.6 r20=-199.591 d20=5.00 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=4.25924D+01 k=-3.51255D+01 B=1.27254D-05 C=-2.17513D-07 D=2.57324D-08 E=1.69969D-09 F=-2.13852D-10 r18面 r=-1.98900D+01 k=-1.17923D-01 B=1.39270D-07 C=9.06409D-08 D=2.70260D-09 E=-1.94211D-10 F=1.65295D-12Numerical Example 4 f = 6.00 to 58.83 fno = 1: 2.89 to 3.00 2ω = 58.2 ° to 6.4 ° r1 = 70.307 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 26.658 d2 = 5.10 n2 = 1.48749 ν2 = 70.2 r3 = -175.593 d3 = 0.20 r4 = 26.160 d4 = 3.15 n3 = 1.88300 ν3 = 40.8 r5 = 93.149 d5 = variable r6 = 30.946 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.518 d7 = 2.99 r8 = -36.767 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 38.324 d9 = 0.60 r10 = 12.527 d10 = 2.70 n6 = 1.84666 ν6 = 23.9 r11 = -65.030 d11 = 0.60 n7 = 1.83481 ν7 = 42.7 r12 = 29.726 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 42.592 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -24.975 d15 = variable r16 = -40.384 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 18.252 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 * r18 =- 19.890 d18 = 0.50 r19 = 20.267 d19 = 1.80 n11 = 1.77250 ν11 = 49.6 r20 = -199.591 d20 = 5.00 r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 4.25924D + 01 k = -3.51255D + 01 B = 1.27254D-05 C = -2.17513D-07 D = 2.57324D-08 E = 1.69969D-09 F = -2.13852D-10 r18 surface r = -1.98900D + 01 k =- 1.17923D-01 B = 1.39270D-07 C = 9.06409D-08 D = 2.70260D-09 E = -1.94211D-10 F = 1.65295D-12

【0070】[0070]

【表4】 [Table 4]

【0071】 数値実施例5 f=6.01〜59.01 fno=1:2.89〜2.89 2ω=59.8°〜6.4° r1=64.967 d1=1.30 n1=1.84666 ν1=23.9 r2=29.027 d2=5.15 n2=1.48749 ν2=70.2 r3=-177.652 d3=0.20 r4=25.154 d4=3.05 n3=1.88481 ν3=42.7 r5=61.808 d5=可変 r6=34.762 d6=0.80 n4=1.88300 ν4=40.8 r7=6.432 d7=2.85 r8=-27.224 d8=0.70 n5=1.88300 ν5=40.8 r9=41.608 d9=0.60 r10=13.918 d10=2.70 n6=1.84666 ν6=23.9 r11=-28.983 d11=0.60 n7=1.83481 ν7=42.7 r12=53.374 d12=可変 r13=(絞り) d13=2.20 *r14=36.600 d14=1.80 n8=1.58313 ν8=59.4 r15=-28.083 d15=可変 r16=-44.150 d16=0.70 n9=1.84666 ν9=23.9 r17=20.380 d17=2.80 n10=1.67790 ν10=54.9 r18=-22.314 d18=0.50 r19=29.859 d19=1.95 n11=1.77250 ν11=49.6 r20=-94.191 d20=5.00 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=3.66003D+01 k=-2.21824D+01 B=1.91217D-05 C=-9.28714D-07 D=3.22454D-08 E=1.31625D-09 F=-8.90730D-1Numerical Example 5 f = 6.01 to 59.01 fno = 1: 2.89 to 2.89 2ω = 59.8 ° to 6.4 ° r1 = 64.967 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 29.027 d2 = 5.15 n2 = 1.48749 ν2 = 70.2 r3 = -177.652 d3 = 0.20 r4 = 25.154 d4 = 3.05 n3 = 1.88481 ν3 = 42.7 r5 = 61.808 d5 = variable r6 = 34.762 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.432 d7 = 2.85 r8 = -27.224 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 41.608 d9 = 0.60 r10 = 13.918 d10 = 2.70 n6 = 1.84666 ν6 = 23.9 r11 = -28.983 d11 = 0.60 n7 = 1.83481 ν7 = 42.7 r12 = 53.374 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 36.600 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -28.083 d15 = variable r16 = -44.150 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 20.380 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 r18 = -22.314 d18 = 0.50 r19 = 29.859 d19 = 1.95 n11 = 1.77250 ν11 = 49.6 r20 = -94.191 d20 = 5.00 r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 3.66003D + 01 k = -2.21824D + 01 B = 1.91217D-05 C = -9.28714D-07 D = 3.22454D-08 E = 1.31625D-09 F = -8.90730D-1

【0072】[0072]

【表5】 [Table 5]

【0073】 数値実施例6 f=6.01〜59.00 fno=1:2.89〜2.93 2ω=59.2°〜6.4° r1=70.577 d1=1.30 n1=1.84666 ν1=23.9 r2=28.102 d2=5.25 n2=1.48749 ν2=70.2 r3=-135.912 d3=0.20 r4=25.710 d4=3.20 n3=1.83481 ν3=42.7 r5=85.671 d5=可変 r6=48.172 d6=0.80 n4=1.88300 ν4=40.8 r7=6.784 d7=2.81 r8=-34.302 d8=0.70 n5=1.88300 ν5=40.8 r9=41.261 d9=0.60 r10=13.312 d10=2.70 n6=1.84666 ν6=23.9 r11=-35.939 d11=0.60 n7=1.83481 ν7=42.7 r12=36.888 d12=可変 r13=(絞り) d13=2.20 *r14=41.177 d14=1.80 n8=1.58313 ν8=59.4 r15=-29.537 d15=可変 r16=-39.851 d16=0.70 n9=1.84666 ν9=23.9 r17=19.986 d17=2.80 n10=1.67790 ν10=54.9 *r18=-20.589 d18=0.50 r19=22.582 d19=1.95 n11=1.77250 ν11=49.6 r20=-116.734 d20=5.00 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=4.11772D+01 k=-3.06458D+01 B=1.49123D-05 C=-9.25985D-08 D=1.59599D-08 E=1.57343D-09 F=-1.66189D-10 r18面 r=-2.05892D+01 k=-1.61879D-01 B=2.46942D-07 C=2.33996D-07 D=-6.83658D-09 E=2.80776D-11 F=1.30665D-12Numerical Example 6 f = 6.01 to 59.00 fno = 1: 2.89 to 2.93 2ω = 59.2 ° to 6.4 ° r1 = 70.577 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 28.102 d2 = 5.25 n2 = 1.48749 ν2 = 70.2 r3 = -135.912 d3 = 0.20 r4 = 25.710 d4 = 3.20 n3 = 1.83481 ν3 = 42.7 r5 = 85.671 d5 = variable r6 = 48.172 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.784 d7 = 2.81 r8 = -34.302 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 41.261 d9 = 0.60 r10 = 13.312 d10 = 2.70 n6 = 1.84666 ν6 = 23.9 r11 = -35.939 d11 = 0.60 n7 = 1.83481 ν7 = 42.7 r12 = 36.888 d12 = variable r13 = (aperture) d13 = 2.20 * r14 = 41.177 d14 = 1.80 n8 = 1.58313 ν8 = 59.4 r15 = -29.537 d15 = variable r16 = -39.851 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 19.986 d17 = 2.80 n10 = 1.67790 ν10 = 54.9 * r18 =- 20.589 d18 = 0.50 r19 = 22.582 d19 = 1.95 n11 = 1.77250 ν11 = 49.6 r20 = -116.734 d20 = 5.00 r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 4.11772D + 01 k = -3.06458D + 01 B = 1.49123D-05 C = -9.25985D-08 D = 1.59599D-08 E = 1.57343D-09 F = -1.66189D-10 r18 surface r = -2.05892D + 01 k =- 1.61879D-01 B = 2.46942D-07 C = 2.33996D-07 D = -6.83658D-09 E = 2.80776D-11 F = 1.30665D-12

【0074】[0074]

【表6】 [Table 6]

【0075】 数値実施例7 f=6.03〜59.02 fno=1:2.87〜2.89 2ω=59.0°〜6.4° r1=62.095 d1=1.30 n1=1.84666 ν1=23.9 r2=28.268 d2=4.70 n2=1.48749 ν2=70.2 r3=-228.219 d3=0.20 r4=25.507 d4=2.95 n3=1.83481 ν3=42.7 r5=67.193 d5=可変 r6=26.771 d6=0.80 n4=1.88300 ν4=40.8 r7=6.365 d7=3.15 r8=-23.692 d8=0.70 n5=1.88300 ν5=40.8 r9=74.962 d9=0.60 r10=13.790 d10=2.50 n6=1.84666 ν6=23.9 r11=-49.225 d11=0.60 n7=1.77250 ν7=49.6 r12=33.632 d12=可変 r13=(絞り) d13=3.00 *r14=41.241 d14=2.00 n8=1.58313 ν8=59.4 r15=-25.592 d15=可変 r16=-29.471 d16=0.70 n9=1.84666 ν9=23.9 r17=25.818 d17=2.85 n10=1.67790 ν10=54.9 r18=-17.943 d18=0.50 r19=28.075 d19=1.80 n11=1.77250 ν11=49.6 r20=-137.571 d20=5.00 r21=∞ d21=3.17 n12=1.51680 ν12=64.2 r22=∞ 非球面係数 r14面 r=4.12412D+01 k=-2.09653D+01 B=-9.81742D-06 C=-2.33933D-07 D=7.49268D-09 E=2.16763D-09 F=-1.21645D-10Numerical Example 7 f = 6.03-59.02 fno = 1: 2.87-2.89 2ω = 59.0 ° -6.4 ° r1 = 62.095 d1 = 1.30 n1 = 1.84666 ν1 = 23.9 r2 = 28.268 d2 = 4.70 n2 = 1.48749 ν2 = 70.2 r3 = -228.219 d3 = 0.20 r4 = 25.507 d4 = 2.95 n3 = 1.83481 ν3 = 42.7 r5 = 67.193 d5 = variable r6 = 26.771 d6 = 0.80 n4 = 1.88300 ν4 = 40.8 r7 = 6.365 d7 = 3.15 r8 = -23.692 d8 = 0.70 n5 = 1.88300 ν5 = 40.8 r9 = 74.962 d9 = 0.60 r10 = 13.790 d10 = 2.50 n6 = 1.84666 ν6 = 23.9 r11 = -49.225 d11 = 0.60 n7 = 1.77250 ν7 = 49.6 r12 = 33.632 d12 = variable r13 = (aperture) d13 = 3.00 * r14 = 41.241 d14 = 2.00 n8 = 1.58313 ν8 = 59.4 r15 = -25.592 d15 = variable r16 = -29.471 d16 = 0.70 n9 = 1.84666 ν9 = 23.9 r17 = 25.818 d17 = 2.85 n10 = 1.67790 ν10 = 54.9 r18 = -17.943 d18 = 0.50 r19 = 28.075 d19 = 1.80 n11 = 1.77250 ν11 = 49.6 r20 = -137.571 d20 = 5.00 r21 = ∞ d21 = 3.17 n12 = 1.51680 ν12 = 64.2 r22 = ∞ Aspheric coefficient r14 surface r = 4.12412D + 01 k = -2.09653D + 01 B = -9.81742D-06 C = -2.33933D-07 D = 7.49268D-09 E = 2.16763D-09 F = -1.21645D-10

【0076】[0076]

【表7】 [Table 7]

【0077】[0077]

【表8】 [Table 8]

【0078】[0078]

【発明の効果】本発明によれば、レンズ系全体を小型化
し、高変倍比であるにもかかわらず高い光学性能を有
し、かつレンズの構成枚数を減らした簡易な構成のレン
ズ全長の短いズームレンズ及びそれを用いた光学機器を
達成することができる。
According to the present invention, the entire lens system is reduced in size, has a high optical performance in spite of a high zoom ratio, and has a simple total lens length with a reduced number of lenses. A short zoom lens and an optical device using the same can be achieved.

【0079】この他、本発明によれば変倍比10倍に及
ぶ高変倍比でありながら、小型軽量の全変倍範囲に渡り
良好に収差補正を行った高い光学性能を有したリアーフ
ォーカス式ズームレンズを達成する事ができる。
In addition, according to the present invention, a rear focus having a high zoom ratio as high as 10 times, and having a high optical performance which is excellent in correcting aberrations over the entire zoom range with a small size and light weight. Type zoom lens can be achieved.

【図面の簡単な説明】[Brief description of the drawings]

【図1】 本発明の数値実施例1のレンズ断面図FIG. 1 is a sectional view of a lens according to a numerical example 1 of the present invention.

【図2】 本発明の数値実施例1の広角端の収差図FIG. 2 is an aberration diagram at a wide-angle end according to Numerical Embodiment 1 of the present invention.

【図3】 本発明の数値実施例1の中間の収差図FIG. 3 is an intermediate aberration diagram of the numerical example 1 of the present invention.

【図4】 本発明の数値実施例1の望遠端の収差図FIG. 4 is an aberration diagram at a telephoto end in Numerical Embodiment 1 of the present invention.

【図5】 本発明の数値実施例2のレンズ断面図FIG. 5 is a sectional view of a lens according to a numerical example 2 of the present invention.

【図6】 本発明の数値実施例2の広角端の収差図FIG. 6 is an aberration diagram at a wide angle end according to Numerical Example 2 of the present invention.

【図7】 本発明の数値実施例2の中間の収差図FIG. 7 is an intermediate aberration diagram of the numerical example 2 of the present invention.

【図8】 本発明の数値実施例2の望遠端の収差図FIG. 8 is an aberration diagram at a telephoto end in Numerical Example 2 of the present invention.

【図9】 本発明の数値実施例3のレンズ断面図FIG. 9 is a sectional view of a lens according to a numerical example 3 of the present invention.

【図10】 本発明の数値実施例3の広角端の収差図FIG. 10 is an aberration diagram at a wide angle end according to Numerical Example 3 of the present invention.

【図11】 本発明の数値実施例3の中間の収差図FIG. 11 is an intermediate aberration diagram of the numerical example 3 of the present invention.

【図12】 本発明の数値実施例3の望遠端の収差図FIG. 12 is an aberration diagram at a telephoto end in Numerical Example 3 of the present invention.

【図13】 本発明の数値実施例4のレンズ断面図FIG. 13 is a sectional view of a lens according to a numerical example 4 of the present invention.

【図14】 本発明の数値実施例4の広角端の収差図FIG. 14 is an aberration diagram at a wide angle end according to Numerical Example 4 of the present invention.

【図15】 本発明の数値実施例4の中間の収差図FIG. 15 is an intermediate aberration diagram of the numerical example 4 of the present invention.

【図16】 本発明の数値実施例4の望遠端の収差図FIG. 16 is an aberration diagram at a telephoto end in Numerical Example 4 of the present invention.

【図17】 本発明の数値実施例5のレンズ断面図FIG. 17 is a lens sectional view of a numerical example 5 of the present invention;

【図18】 本発明の数値実施例5の広角端の収差図FIG. 18 is an aberration diagram at a wide angle end according to Numerical Example 5 of the present invention.

【図19】 本発明の数値実施例5の中間の収差図FIG. 19 is an intermediate aberration diagram of the numerical example 5 of the present invention.

【図20】 本発明の数値実施例5の望遠端の収差図FIG. 20 is an aberration diagram at a telephoto end in Numerical Example 5 of the present invention.

【図21】 本発明の数値実施例6のレンズ断面図FIG. 21 is a sectional view of a lens according to a numerical example 6 of the present invention.

【図22】 本発明の数値実施例6の広角端の収差図FIG. 22 is an aberration diagram at a wide angle end according to Numerical Example 6 of the present invention.

【図23】 本発明の数値実施例6の中間の収差図FIG. 23 is an intermediate aberration diagram of the numerical example 6 of the present invention.

【図24】 本発明の数値実施例6の望遠端の収差図FIG. 24 is an aberration diagram at a telephoto end in Numerical Example 6 of the present invention.

【図25】 本発明の数値実施例7のレンズ断面図FIG. 25 is a sectional view of a lens according to a numerical example 7 of the present invention.

【図26】 本発明の数値実施例7の広角端の収差図FIG. 26 is an aberration diagram at a wide angle end according to Numerical Example 7 of the present invention.

【図27】 本発明の数値実施例7の中間の収差図FIG. 27 is an intermediate aberration diagram of the numerical example 7 of the present invention.

【図28】 本発明の数値実施例7の望遠端の収差図FIG. 28 is an aberration diagram at a telephoto end in Numerical Example 7 of the present invention.

【図29】 本発明の光学機器の要部概略図FIG. 29 is a schematic diagram of a main part of the optical apparatus of the present invention.

【符号の説明】[Explanation of symbols]

L1 第1群 L2 第2群 L3 第3群 L4 第4群 SP 絞り G ガラスブロック IP 像面 d d線 g g線 ΔM メリディオナル像面 ΔS サジタル像面 L1 First group L2 Second group L3 Third group L4 Fourth group SP Aperture G Glass block IP Image plane d d line g g line ΔM Meridional image plane ΔS Sagittal image plane

───────────────────────────────────────────────────── フロントページの続き Fターム(参考) 2H087 KA02 KA03 MA15 PA08 PA20 PB11 QA02 QA07 QA17 QA21 QA25 QA34 QA41 QA46 RA05 RA12 RA13 RA32 RA41 RA42 RA43 SA23 SA27 SA29 SA32 SA63 SA65 SA72 SA74 SB04 SB15 SB22 SB34  ──────────────────────────────────────────────────続 き Continued on the front page F term (reference) 2H087 KA02 KA03 MA15 PA08 PA20 PB11 QA02 QA07 QA17 QA21 QA25 QA34 QA41 QA46 RA05 RA12 RA13 RA32 RA41 RA42 RA43 SA23 SA27 SA29 SA32 SA63 SA65 SA72 SA74 SB04 SB15 SB22 SB34

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 物体側より順に正の屈折力の第1群、負
の屈折力の第2群、絞り正の屈折力の第3群、そして正
の屈折力の第4群の4つのレンズ群を有し、広角端から
望遠端への変倍の際には、該第2群を像面側へ移動させ
ると共に第4群を物体側に凸状の軌跡を有するように移
動させ、合焦の際には該第4群を移動させて行い、該第
2群を物体側から順に、物体側に凸面を向けたメニスカ
ス状の負の第21レンズ、両レンズ面が凹面の負の第2
2レンズ、両レンズ面が凸面の正の第23レンズと負の
第24レンズとを接合した貼合わせレンズより構成し、
該第3群は非球面を有する正の1枚のレンズにより構成
したことを特徴とするリヤーフォーカス式のズームレン
ズ。
1. Four lenses of a first lens unit having a positive refractive power, a second lens unit having a negative refractive power, a third lens unit having a positive refractive power, and a fourth lens unit having a positive refractive power in order from the object side. When zooming from the wide-angle end to the telephoto end, the second unit is moved to the image plane side, and the fourth unit is moved to have a locus convex toward the object side. In focusing, the fourth unit is moved, and the second unit is sequentially moved from the object side to the negative second meniscus lens having a convex surface facing the object side, and both lens surfaces having a concave concave surface. 2
Two lenses, each composed of a cemented lens in which a positive twenty-third lens and a negative twenty-fourth lens whose both lens surfaces are convex are joined;
A rear focus type zoom lens, wherein the third group is constituted by a single positive lens having an aspheric surface.
【請求項2】 前記第22レンズの像側のレンズ面の曲
率半径をR222、前記第23レンズの物体側のレンズ
面の曲率半径をR231とするとき 【数1】 なる条件を満足することを特徴とする請求項1のリヤー
フォーカス式のズームレンズ。
2. When the radius of curvature of the lens surface on the image side of the 22nd lens is R222, and the radius of curvature of the lens surface on the object side of the 23rd lens is R231. 2. The rear focus type zoom lens according to claim 1, wherein the following condition is satisfied.
【請求項3】 前記第23レンズの材質のアッベ数をν
23、前記第24レンズの材質のアッベ数をν24とす
るとき 15<(ν24−ν23)<30 なる条件を満足することを特徴とする請求項1又は2の
リヤーフォーカス式のズームレンズ。
3. The Abbe number of the material of the 23rd lens is ν.
23. The rear focus type zoom lens according to claim 1, wherein a condition of 15 <(ν24−ν23) <30 is satisfied when an Abbe number of a material of the 24th lens is ν24.
【請求項4】 前記第2レンズ群の焦点距離をf2、前
記第23レンズと前記第24レンズとの接合レンズ面の
曲率半径をR234とするとき 【数2】 なる条件を満足することを特徴とする請求項1,2又は
3のリヤーフォーカス式のズームレンズ。
4. When the focal length of the second lens group is f2 and the radius of curvature of the cemented lens surface between the 23rd lens and the 24th lens is R234. 4. The rear focus type zoom lens according to claim 1, wherein the following condition is satisfied.
【請求項5】 請求項1から4のいずれか1項のリヤー
フォーカス式のズームレンズを有することを特徴とする
光学機器。
5. An optical apparatus comprising the rear focus type zoom lens according to claim 1.
JP2000041671A 2000-02-18 2000-02-18 Rear focus zoom lens and optical apparatus using the same Expired - Fee Related JP4593716B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000041671A JP4593716B2 (en) 2000-02-18 2000-02-18 Rear focus zoom lens and optical apparatus using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000041671A JP4593716B2 (en) 2000-02-18 2000-02-18 Rear focus zoom lens and optical apparatus using the same

Publications (3)

Publication Number Publication Date
JP2001228395A true JP2001228395A (en) 2001-08-24
JP2001228395A5 JP2001228395A5 (en) 2010-07-08
JP4593716B2 JP4593716B2 (en) 2010-12-08

Family

ID=18564869

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP4593716B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7106521B2 (en) 2001-09-28 2006-09-12 Canon Kabushiki Kaisha Zoom lens and camera with the zoom lens
JP2010066661A (en) * 2008-09-12 2010-03-25 Fujinon Corp Zoom lens and imaging apparatus
US7715113B2 (en) 2007-11-15 2010-05-11 Fujinon Corporation Zoom lens and imaging apparatus
CN114624869A (en) * 2022-03-10 2022-06-14 长春通视光电技术有限公司 High-resolution and large-zoom-ratio optical system and zoom lens adopting same

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04208912A (en) * 1990-12-03 1992-07-30 Nikon Corp High magnifying power zoom lens
JPH1144845A (en) * 1997-07-25 1999-02-16 Canon Inc Rear focus type zoom lens provided with vibration-proof function and image pickup device using the same
JPH11258502A (en) * 1998-03-10 1999-09-24 Canon Inc Zoom lens and optical unit using the same

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04208912A (en) * 1990-12-03 1992-07-30 Nikon Corp High magnifying power zoom lens
JPH1144845A (en) * 1997-07-25 1999-02-16 Canon Inc Rear focus type zoom lens provided with vibration-proof function and image pickup device using the same
JPH11258502A (en) * 1998-03-10 1999-09-24 Canon Inc Zoom lens and optical unit using the same

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7106521B2 (en) 2001-09-28 2006-09-12 Canon Kabushiki Kaisha Zoom lens and camera with the zoom lens
US7715113B2 (en) 2007-11-15 2010-05-11 Fujinon Corporation Zoom lens and imaging apparatus
JP2010066661A (en) * 2008-09-12 2010-03-25 Fujinon Corp Zoom lens and imaging apparatus
CN114624869A (en) * 2022-03-10 2022-06-14 长春通视光电技术有限公司 High-resolution and large-zoom-ratio optical system and zoom lens adopting same
CN114624869B (en) * 2022-03-10 2024-03-29 长春通视光电技术股份有限公司 High-resolution and large-zoom-ratio optical system and zoom lens adopting same

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