JPH01307713A - Enlarging projection lens - Google Patents
Enlarging projection lensInfo
- Publication number
- JPH01307713A JPH01307713A JP13870688A JP13870688A JPH01307713A JP H01307713 A JPH01307713 A JP H01307713A JP 13870688 A JP13870688 A JP 13870688A JP 13870688 A JP13870688 A JP 13870688A JP H01307713 A JPH01307713 A JP H01307713A
- Authority
- JP
- Japan
- Prior art keywords
- lens
- positive
- curvature
- lens group
- group
- 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
Links
- 230000005499 meniscus Effects 0.000 claims description 4
- 238000010030 laminating Methods 0.000 claims 1
- 230000004075 alteration Effects 0.000 abstract description 21
- 201000009310 astigmatism Diseases 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000014509 gene expression Effects 0.000 description 2
- 206010010071 Coma Diseases 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Abstract
Description
[産業上の利用分野]
この発明は、例えば天体望遠鏡の対物レンズ等によって
形成された像を拡大投影するのに適用される拡大投影レ
ンズに関するものである。
[従来の技術]
一般的に天体望遠鏡の対物レンズ等によって形成された
像を拡大投影するためのレンズには、簡易的に接眼レン
ズが流用されている。しかし、接眼レンズは眼視用とし
てアフォーカル状態にて収差補正されたものであり、こ
れを拡大投影用として使用した場合には使用倍率が変化
することにより歪曲収差、像面湾曲、倍率色収差等の収
差が過度に発生するという問題点があった。
[発明の目的]
この発明は、Fナンバー1:6.O程度の対物レンズと
組み合わせて半画角1B’程度を含み、倍率−20倍以
上で周辺まで高い結像性能を有する拡大投影レンズを提
供することを目的とする。
[課題を解決するための手段]
この発明の拡大投影レンズは、上記目的を達成させるた
め、入射側より順に投影面に凸面を向けた正のメニスカ
スレンズである第1121群、正の第2レンズ群、入射
側に凸面を向けた正のメニスカスレンズである第3レン
ズ群より構成され、第2レンズ群は曲率の大きい方の面
を入射側へ向けた正の第1レンズと両凹の第2レンズと
両凸の第3レンズとを貼合わせて構成され、
■ n、 > 1.70
■ yl〉45.0
■ v * −y −> 16.0
■ f+/f>4.0
■ 1.3<−r+/ f< 1.7
但し、
f:全系の焦点距離
fI=第iレンズ群の焦点距離
rI=入射側から第1番目の面の曲率半径n、:第2.
第3レンズ群の正レンズの屈折率の平均V1:第iレン
ズのアツベ数
V、:第2.第3レンズ群の正レンズのアラへ数の平均
y−:第2.第3レンズ群の負レンズのアツベ数の平均
の各条件を満たすよう設定したことを特徴とする。
条件■は第2.第3レンズ群の正レンズの屈折率を大き
く保つことによってペッツバール和を小さく抑え、像面
を平坦化するための条件である0条件■の下限を下回る
とペッツバール和が過大となり、像面湾曲が過度に増加
する。
条件■、■は、色収差補正のための条件である。
条件■は正のパワーを持つ第1121群のアツベ数を大
きく保つことにより、倍率色収差を小さく抑えるための
条件であり、下限を下回ると倍率色収差が過大となる。
また、条件■は第2.第3レンズ群の正レンズのアツベ
数の平均と負レンズのアツベ数の平均との差を大きく保
つことにより色収差を小さく抑えるための条件であり、
下限を下回ると色収差が過大となる。
条件■、■は本発明の特徴とするところの弱いパワーを
持つ第1121群に関する。第1121群の作用は、対
物レンズによる集光光束の方向及び集光位置を弱いパワ
ーによって補正することにより、倍率色収差を発生させ
ることなく歪曲収差と像面湾曲とを補正することにある
。
条件■は第1121群のパワーを与えるもので。
下限を下回るとパワーが過大となり、倍率色収差が過度
に発生し、第2.第3レンズ群で補正しきれなくなる。
条件■は第1レンズの第1面の曲率半径を適切に設定す
ることにより、第3レンズ群で発生する歪曲収差を予め
補正し、かつ、他の収差の発生を抑えるための条件であ
る0条件■の上限を越えると歪曲収差の補正が過小とな
り、下限を下回るとコマ収差、その他の高次の収差が過
度に発生すると共に、曲率半径が小さくなり過ぎて研磨
加工のコストが嵩むこととなる。
[実施例]
以下、この発明に係る拡大投影レンズの実施例を説明す
る。
第1図は、この発明の第1実施例に係る拡大投影レンズ
の配置構成を示したものであり、具体的な数値構成は第
8ページの表に示される通りである。
表中の符号Fnoは上記の拡大投影レンズと組み合わせ
て使用する対物レンズのFナンバー、fは拡大投影レン
ズ全系の焦点距離、rは各レンズ面の曲率半径、dは面
間の距III(レンズ厚及び空気間隔)、nハd線(5
88nm)における屈折率、y−はアラへ数をそれぞれ
表わしている。
第2〜第6実施例については、レンズ構成は第1図とほ
ぼ同様であるので省略し、数値構成のみを第8.9ペー
ジの6表に示す。
なお、各実施例と条件式■〜■との関係は次ページの表
に示した通りである。
(以下余白)[Industrial Application Field] The present invention relates to an enlarged projection lens that is applied to enlarge and project an image formed by, for example, an objective lens of an astronomical telescope. [Prior Art] Generally, an eyepiece lens is simply used as a lens for enlarging and projecting an image formed by an objective lens or the like of an astronomical telescope. However, the eyepiece lens has aberrations corrected in the afocal state for visual viewing, and when used for enlarged projection, distortion, curvature of field, lateral chromatic aberration, etc. occur due to changes in the magnification used. There was a problem in that excessive aberrations occurred. [Object of the invention] This invention provides an F number of 1:6. It is an object of the present invention to provide an enlarged projection lens that includes a half angle of view of about 1 B' in combination with an objective lens of about 0.0 and has high imaging performance up to the periphery at a magnification of -20 times or more. [Means for Solving the Problems] In order to achieve the above object, the magnifying projection lens of the present invention includes, in order from the incident side, a 1121st group which is a positive meniscus lens with a convex surface facing the projection surface, and a positive second lens. The third lens group is a positive meniscus lens with its convex surface facing the incident side, and the second lens group consists of a positive first lens with its surface with greater curvature facing the incident side, and a biconcave lens group. Consisting of two lenses and a biconvex third lens, ■ n, > 1.70 ■ yl>45.0 ■ v * -y -> 16.0 ■ f+/f>4.0 ■ 1 .3<-r+/f<1.7 However, f: Focal length of the entire system fI = Focal length of the i-th lens group rI = Radius of curvature n of the first surface from the incident side,: Second.
Average refractive index of the positive lens of the third lens group V1: Atsube number V of the i-th lens: 2nd. Average y- of the positive lens numbers of the third lens group: 2nd. It is characterized in that it is set to satisfy each condition of the average Atsube number of the negative lenses of the third lens group. Condition ■ is the second condition. By keeping the refractive index of the positive lens in the third lens group large, the Petzval sum can be kept small and the field curvature can be reduced below the lower limit of the 0 condition (2), which is a condition for flattening the field. Increase excessively. Conditions (2) and (2) are conditions for correcting chromatic aberration. Condition (2) is a condition for keeping the chromatic aberration of magnification small by keeping the Abbe number of the 1121st lens group, which has positive power, large; below the lower limit, the chromatic aberration of magnification becomes excessive. Also, condition (■) is the second condition. This is a condition for keeping chromatic aberrations small by keeping a large difference between the average Atsube number of the positive lens in the third lens group and the average Atsube number of the negative lens.
Below the lower limit, chromatic aberration becomes excessive. Conditions (1) and (2) relate to the 1121st group having weak power, which is a feature of the present invention. The function of the 1121st lens group is to correct distortion and field curvature without producing lateral chromatic aberration by correcting the direction and focusing position of the light beam focused by the objective lens with weak power. Condition ■ gives the power of the 1121st group. Below the lower limit, the power becomes excessive and lateral chromatic aberration occurs excessively. The third lens group will no longer be able to compensate. Condition (2) is a condition for correcting the distortion aberration occurring in the third lens group in advance and suppressing the occurrence of other aberrations by appropriately setting the radius of curvature of the first surface of the first lens. If the upper limit of condition (■) is exceeded, distortion aberration will be undercorrected, and if it is below the lower limit, coma and other higher-order aberrations will occur excessively, and the radius of curvature will become too small, increasing the cost of polishing. Become. [Example] Hereinafter, an example of the magnifying projection lens according to the present invention will be described. FIG. 1 shows the arrangement of the magnifying projection lens according to the first embodiment of the present invention, and the specific numerical structure is as shown in the table on page 8. The symbol Fno in the table is the F number of the objective lens used in combination with the above magnifying projection lens, f is the focal length of the entire magnifying projection lens system, r is the radius of curvature of each lens surface, and d is the distance between the surfaces III ( lens thickness and air spacing), n-d line (5
The refractive index at 88 nm), y- represents the number. As for the second to sixth embodiments, the lens configurations are almost the same as those shown in FIG. 1, so they are omitted, and only the numerical configurations are shown in Table 6 on page 8.9. The relationship between each embodiment and conditional expressions (1) to (2) is as shown in the table on the next page. (Margin below)
これらの拡大投影レンズの収差特性は、第2図〜第7図
に示す通りである。何れも対物レンズのFナンバー1
: 6.0、焦点距@3.8rrtn、 倍率−27
倍、半画角18′としたときの状態を示している6図中
の球面収差SAが実線、正弦条件SCが破線で示されて
おり、軸上の色収差及び倍率色収差では、d−Line
(588nm)、g−Line(436nm)、C−L
ine(656nm)の3つのデータを示している。非
点収差はサジタル方向Sを実線、メリディオナル方向H
を破線で示している。
何れの実施例においても、■から■の条件を満たすこと
により、良好な性能が得られる。
(以下、金白)
第1実施例
第2実施例
第3実施例
第4実施例
第5実施例
第6実施例
[効果]
以上説明した通り、この発明によれば、Fナンに−1+
6.0程度の大口径の対物レンズと組み合わせて使用で
きる拡大投影レンズであって、倍$ −20倍1度の高
倍率で歪曲収差、倍率色収差、非点収差、象面湾曲が良
好に補正されたレンズを提供するここができる。
しかも、このレンズは接眼レンズとしても使用すること
ができる。The aberration characteristics of these magnifying projection lenses are as shown in FIGS. 2 to 7. Both objective lenses have F number 1
: 6.0, focal length @3.8rrtn, magnification -27
In Figure 6, which shows the state when the magnification and half angle of view is 18', the spherical aberration SA is shown as a solid line, the sine condition SC is shown as a broken line, and the axial chromatic aberration and lateral chromatic aberration are
(588nm), g-Line (436nm), C-L
Three data of ine (656 nm) are shown. For astigmatism, the sagittal direction S is a solid line, and the meridional direction H is a solid line.
is shown with a broken line. In any of the examples, good performance can be obtained by satisfying the conditions (1) to (4). (Hereinafter referred to as "Kinpaku") 1st embodiment 2nd embodiment 3rd embodiment 4th embodiment 5th embodiment 6th embodiment [Effects] As explained above, according to this invention, -1+
This is a magnifying projection lens that can be used in combination with an objective lens with a large aperture of about 6.0, and can effectively correct distortion, chromatic aberration of magnification, astigmatism, and curvature of the field at a high magnification of $ -20x 1 degree. We can provide lenses here. Furthermore, this lens can also be used as an eyepiece.
第1図はこの発明に係る拡大投影レンズの第1実1例の
構成図、第2図〜第7図はこの発明の第1〜第実施例に
係る拡大投影レンズの収差図である。FIG. 1 is a block diagram of a first example of a magnifying projection lens according to the present invention, and FIGS. 2 to 7 are aberration diagrams of the magnifying projection lenses according to the first to first embodiments of the present invention.
Claims (1)
ンズである第1レンズ群、正の第2レンズ群、入射側に
凸面を向けた正のメニスカスレンズである第3レンズ群
より構成され、前記第2レンズ群は曲率の大きい方の面
を入射側へ向けた正の第1レンズと両凹の第2レンズと
両凸の第3レンズとを貼合わせて構成され、 (1)n_+>1.70 (2)ν_i>45.0 (3)ν_+−ν_−>16.0 (4)f_1/f>4.0 (5)1.3<−r_i/f<1.7 但し、 f:全系の焦点距離 f_i:第iレンズ群の焦点距離 r_i:入射側から第i番目の面の曲率半径 n_+:第2、第3レンズ群の正レンズの屈折率の平均 ν_i:第iレンズのアツベ数 ν_+:第2、第3レンズ群の正レンズのアツベ数の平
均 ν_−:第2、第3レンズ群の負レンズのアツベ数の平
均 の各条件を満たすことを特徴とする拡大投影レンズ。[Claims] In order from the incident side, the first lens group is a positive meniscus lens with a convex surface facing the projection surface, the second positive lens group, and the third lens group is a positive meniscus lens with a convex surface facing the incident side. It is composed of a lens group, and the second lens group is constructed by laminating together a positive first lens with its surface with a larger curvature facing the incident side, a biconcave second lens, and a biconvex third lens. , (1) n_+>1.70 (2) ν_i>45.0 (3) ν_+-ν_->16.0 (4) f_1/f>4.0 (5) 1.3<-r_i/f< 1.7 However, f: focal length of the entire system f_i: focal length of the i-th lens group r_i: radius of curvature of the i-th surface from the incident side n_+: refractive index of the positive lens of the second and third lens groups Average ν_i: Atsube number of the i-th lens ν_+: Average Atsube number of the positive lenses in the second and third lens groups ν_-: Satisfy each condition of the average Atsube number of the negative lenses in the second and third lens groups A magnifying projection lens featuring
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13870688A JP2652662B2 (en) | 1988-06-06 | 1988-06-06 | Magnifying projection lens |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13870688A JP2652662B2 (en) | 1988-06-06 | 1988-06-06 | Magnifying projection lens |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH01307713A true JPH01307713A (en) | 1989-12-12 |
JP2652662B2 JP2652662B2 (en) | 1997-09-10 |
Family
ID=15228224
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13870688A Expired - Fee Related JP2652662B2 (en) | 1988-06-06 | 1988-06-06 | Magnifying projection lens |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2652662B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016126133A (en) * | 2014-12-26 | 2016-07-11 | 日本電産コパル株式会社 | Imaging lens and optical device |
-
1988
- 1988-06-06 JP JP13870688A patent/JP2652662B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016126133A (en) * | 2014-12-26 | 2016-07-11 | 日本電産コパル株式会社 | Imaging lens and optical device |
Also Published As
Publication number | Publication date |
---|---|
JP2652662B2 (en) | 1997-09-10 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
LAPS | Cancellation because of no payment of annual fees |