JPS61259214A - Lens for optical disc - Google Patents
Lens for optical discInfo
- Publication number
- JPS61259214A JPS61259214A JP10045185A JP10045185A JPS61259214A JP S61259214 A JPS61259214 A JP S61259214A JP 10045185 A JP10045185 A JP 10045185A JP 10045185 A JP10045185 A JP 10045185A JP S61259214 A JPS61259214 A JP S61259214A
- Authority
- JP
- Japan
- Prior art keywords
- lens
- light source
- group
- lens group
- lenses
- 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.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 title claims description 18
- 230000005499 meniscus Effects 0.000 claims abstract description 4
- 230000004075 alteration Effects 0.000 description 8
- 239000000470 constituent Substances 0.000 description 4
- 239000006059 cover glass Substances 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 239000011521 glass Substances 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 201000009310 astigmatism Diseases 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
Landscapes
- Lenses (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、主としてレーザ光を微小スポットにまで集
光させ得るように回折限界以下に収差補正された大口径
レンズ、特にディジタルオーディオディスクやビデオデ
ィスク等の光ディスク用レンズに関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention is primarily concerned with large-diameter lenses whose aberrations are corrected to below the diffraction limit so as to be able to focus laser light down to a minute spot, particularly for digital audio discs and video discs. The present invention relates to lenses for optical discs such as discs.
ディジタルオーディオディスク用あるいはビデオディス
ク用のピックアップレンズとしての光ディスク用レンズ
は、ピックアップユニット等の小さなアクチュエーター
に装着され、フォーカシング等の制御駆動を受けるので
、まず小型、軽旦であることが要求される。さらに上記
駆動に対し、駆動時にレンズがディスク面に衝突しない
よう充分な作動距離を有することが要求されている。ま
た、レーザ光をディスク表面に微小スポットとして集光
させなければならないので、大きなNA(開口数)を保
ちながら光軸とその周辺にわたって、回折限界以下の程
度に良好に収差が補正されていることが必要である。そ
の池に、作り易いこと、低コストであること、安定した
性能、耐久性などが求められている。熱論これらの諸条
件を満足するレンズ系を提供するには、設計、製作の両
面で精密な技術が必要であることは言うまでもない。An optical disc lens used as a pickup lens for a digital audio disc or a video disc is attached to a small actuator such as a pickup unit, and is driven by control such as focusing, so it is first required to be small and lightweight. Furthermore, the above driving is required to have a sufficient working distance so that the lens does not collide with the disk surface during driving. In addition, since the laser beam must be focused as a minute spot on the disk surface, aberrations must be well corrected to below the diffraction limit while maintaining a large NA (numerical aperture). is necessary. The pond is required to be easy to make, low cost, stable performance, and durable. Thermal Theory It goes without saying that providing a lens system that satisfies these conditions requires precise technology in both design and manufacturing.
これら諸条件を満足する光ディスク用レンズは周知のよ
うに種々のタイプのレンズ系が報告されている。そして
その多くは入射するレーザ光束が、光軸に対して平行光
束であるという条件のもとで使用される集光レンズであ
る。As is well known, various types of lens systems have been reported as lenses for optical discs that satisfy these conditions. Most of these lenses are condensing lenses that are used under the condition that the incident laser beam is parallel to the optical axis.
(発明が解決しようとしている問題点)入射光束が、平
行光束であるという条件のもとで集光レンズが使用され
る場合、ピックアップを構成する光学系にはレーザ光を
所望の光束径に変換する光学系が必要である。特に光源
として半導体レーザを使用する場合には、半導体レーザ
からの発散光束を平行光束化させるコリメートレンズが
必要となる。一般にピックアップに用いられるコリメー
トレンズは小さなNAをカバーするだけで充分であるが
、最低2枚のレンズは必要であり、また集光レンズには
、概ね3枚構成のレンズが多いので一般的なピックアッ
プには略5枚のレンズが使用されていると言える。この
様に光束を平行光束化する部分を作っているピックアッ
プ光学系においては、フォーカシング及びトラッキング
靜1部駆動に対して、集光レンズのみを駆動させるのが
一般的であり、光源コリメートレンズ、集光レンズ等を
一体化させて制御駆動させることはしていない。その理
由は、一体化すると、必然的に駆動部分の重量が大きく
なって大きな駆動力が必要となったり、カットオフ周波
数が低下するなど好ましくない現象が生ずるからである
。(Problem to be solved by the invention) When a condenser lens is used under the condition that the incident light beam is a parallel light beam, the optical system that constitutes the pickup converts the laser beam into the desired beam diameter. An optical system is required. Particularly when a semiconductor laser is used as a light source, a collimating lens is required to convert the diverging light beam from the semiconductor laser into a parallel light beam. In general, it is sufficient for the collimating lens used for pickups to cover a small NA, but at least two lenses are required, and condensing lenses often have three lenses, so common pickups It can be said that approximately five lenses are used. In a pickup optical system that has a part that converts a light beam into a parallel light beam, it is common to drive only the condenser lens, while the focusing and tracking parts are driven. Optical lenses and the like are not integrated and controlled and driven. The reason for this is that when integrated, undesirable phenomena such as an increase in the weight of the driving part and the need for a large driving force, and a decrease in the cutoff frequency occur.
(問題点を解決するための手段)
本発明の目的は、コリメートレンズと集光レンズの機能
を1組のレンズに集約し、光源と集光スポットとの間を
有限倍率で結ぶことによって、構成枚数を減らして軽量
化をはかり、上記一体化して制御させ得る光学系に適し
た光ディスク用レンズを提供することにある。(Means for Solving the Problems) An object of the present invention is to integrate the functions of a collimating lens and a condensing lens into one set of lenses, and to connect a light source and a condensed spot with a finite magnification. It is an object of the present invention to provide an optical disk lens that is light in weight by reducing the number of lenses and is suitable for the optical system that can be integrated and controlled.
(発明の構成)
本発明に係るレンズ系は第1図に槙成図を示す如く、以
下のように構成されている。(Structure of the Invention) The lens system according to the present invention is structured as follows, as shown in the Makisei diagram in FIG.
即ち光源側から順に集光側に向って第18レンズ、第2
群レンズ及び第3群レンズの3つのレンズ群によって構
成されており、光源側から順に、第1群レンズは両凸面
の正レンズの第1レンズで構成されており、第2群レン
ズは正レンズの第2レンズと負レンズの第3レンズとの
接合レンズで構成されており、第3群レンズは光源側に
凸面を向けた正メニスカスレンズの第4レンズで構成さ
れている3群4枚構成のレンズ系であって、以下の条件
を満たすことを特徴としている。That is, from the light source side to the condensing side, the 18th lens, the 2nd lens, etc.
It is composed of three lens groups: a group lens and a third group lens. In order from the light source side, the first group lens is composed of a first lens that is a biconvex positive lens, and the second group lens is a positive lens. The lens is composed of a cemented lens consisting of a second lens and a third lens which is a negative lens, and the third lens group consists of a fourth lens which is a positive meniscus lens with its convex surface facing the light source side.It is composed of 4 elements in 3 groups. This lens system is characterized by satisfying the following conditions.
(1) 4.0<I23/f< 7.0(2>
0.5 <rs /f4< 0.7但し、ナは全系の
焦点距離、ftsは第2群レンズの焦点距離、I4は第
3群し°ンズの焦点距離、rsは第4レンズの光源側の
曲率半径である。(1) 4.0<I23/f<7.0(2>
0.5 <rs / f4 < 0.7 However, n is the focal length of the entire system, fts is the focal length of the second group lens, I4 is the focal length of the third group lens, and rs is the light source of the fourth lens. is the radius of curvature of the side.
上記条件式(1)は作動距離を良好に保つための条件で
ある。上限を越えると、第3群レンズの第4レンズの負
担するパワーが大きくなりずぎてしまい各収差を良好に
補正することが困難になる。The above conditional expression (1) is a condition for maintaining a good working distance. If the upper limit is exceeded, the power borne by the fourth lens of the third lens group becomes too large, making it difficult to satisfactorily correct each aberration.
また下限を越えると作動距離が小さくなりすぎ、フォー
カシングのflill@駆動に支障をきたす。Moreover, if the lower limit is exceeded, the working distance becomes too small, causing a problem in the focusing flill@ drive.
条件式(2)は正弦条件を良好に補正するための条件で
ある。上限を越えると正弦条件の補正不足、下限を越え
ると補正過剰となりともに軸外収差が悪化して軸外での
良好な集光性能の確保が困難になる。Conditional expression (2) is a condition for properly correcting the sine condition. If the upper limit is exceeded, the sine condition will be undercorrected, and if the lower limit is exceeded, the sine condition will be overcorrected, and off-axis aberrations will worsen, making it difficult to ensure good light collection performance off-axis.
上記構成と条件を満たすことにより、光源部と光学系等
を一体化して制御駆動を行なう場合に適した光ディスク
用レンズを実現できるとともに、有限系であるので枚数
を少なくすることができ、低コスト、コンパクト化をも
実現できる。By satisfying the above configuration and conditions, it is possible to realize an optical disc lens suitable for controlling drive by integrating the light source section and optical system, etc., and since it is a finite system, the number of lenses can be reduced, resulting in low cost. , it is also possible to realize compactness.
以下に本発明にもとず〈実施例を示す。 Examples based on the present invention will be shown below.
第1図で本発明の光ディスク用レンズの一実施例の構成
を示ずと、光源側から順に集光側に向って、第1群レン
ズI、第2群レンズ■及び第3群レンズ■の3つのレン
ズ群によって構成されており、光源側から順に第1群レ
ンズ■は両凸面の正レンズの第1レンズL1で構成され
ており、第2群レンズ■は正レンズの第2レンズL2と
負レンズの第3レンズL3との接合レンズによって構成
されており、第3群レンズ■は光源側に凸面を向けた正
メニスカスレンズの第4レンズL4で構成されている3
群4枚構成のレンズ系である。尚、符号1は光源側カバ
ーガラス、符号2は集光側ノコパーガラスを示す。第2
図は収差図である。If FIG. 1 does not show the structure of an embodiment of the optical disc lens of the present invention, the first lens group I, the second lens group ■, and the third lens group ■ are shown in order from the light source side toward the condensing side. It is composed of three lens groups, and in order from the light source side, the first group lens ■ consists of the first lens L1, which is a biconvex positive lens, and the second group lens ■ consists of the second lens L2, which is a positive lens. It is composed of a cemented lens with a third lens L3 which is a negative lens, and the third lens group (3) is composed of a fourth lens L4 which is a positive meniscus lens with its convex surface facing the light source side.
This is a lens system with a group of four elements. Note that the reference numeral 1 indicates a light source side cover glass, and the reference numeral 2 indicates a light condensing side cover glass. Second
The figure is an aberration diagram.
但し
rj 、r2・・・rj:各構成レンズの曲率半径d、
、d2・・・d6:各構成レンズの軸上厚みと軸上空
気間隔
nl、n2・・・n4=各構成レンズの波長780nR
+における屈折率
ν1、ν2・・・シ4:各構成レンズのアラへ数f
:全系の焦点距離
ft3 :第2群レンズの焦点距離
f4 :第3群レンズの焦点距離
NA :開口数
M :倍率
tdl :レンズの光源側7Jバーガラスの厚みt(
12:レンズの集光側7Jバーガラスの厚さtnl
:レンズの光源側カバーガラスの波長780 rvにお
ける屈折率
tnz :レンズの集光側カバーガラスの波長780
nIIlにおける屈折率
Y 二 m 高
実施例1
f=1 NA=0.45 M=−0,342r
1=30.7346 61=0.3202n 1
= 1,81961 ν、 =37,3r2 =−
2,6124d 2 = 0.0820r 3 = 2
.0490 d a = 0.4610n 2
= 1.55749 ν2 =60.8r 4
= −1,1525d 4 = 0.2049n 3
= 1.78571 し3 =25.5r 5
= −8,9284d 5 = 0.2049r 6
=0.8785 d B =0.3586n
4= 1,81961 シ、=37,3r 7 =
3.3501
td1=1゜1013 tn 1= 1.51
118td 2 = 0.3073 t
n 2 = 1.51f rs / f = 5.8
8
r s / f 4 =0.64
実施例2
f −I N A = 0.45 M = −
0,342r + =32.8731 d t
=0.2739n 、 = 1.81961 ν、
=37.3r 2 =−2,7942d 2 =0.
0877r 3 =2.1915 d 3 =
0.4794n 2 = 1.55749 シ2=
60.8r 4 = −1,2327d 4 = 0.
1507n 3 = 1,78571 ν3 =2
5.5r s = −9,549665= 0.027
4r 、 =0.8903 d 、 =0.3
698n 4 = 1.81961 ν4 =37
.3r 7 =2.5118
td1=1.1780 tn1=1.5111
8td2 = 0.3287 tn 2 =
1.51j n / f =6.29 r s
/ f 4 =0.58実施例3
f=1 N△=0.45 M=−0,36
4r 1 =68.4856 d l
=0.2739n 1 = 1.81961
ν1 =37.3r 2 =−2,4929d 2
=0.0274r 3 = 2.7668
d a = 0.4931n 2 = 1.5
5749 し2=eo、ar 4 = 1
.1232 d 4 =0.1507n 3
= 1,78571 ν3 ==25.
5r s =−3,8626d 5 = 0.02
74r 6 =0,8766 d b’
=0.3698r14 = 1,81961
シ4=37,3r 7 = 2.3230
td t = 1.1780 tn 1=
1.51118td 2 = 0.3287
tn 2 = 1.51fn/f=4.96
r5 /f4 =0.57実施例4
f=1 NA=0.45 M=−0,342r
1 =73.4819 d l =0.293
9n 1 = 1.8196+ シ1=37.3r
2 =−2,7923d 2 =0.0294r s
=2,9687 da =0.52
91n 2 = 1.55749 シ2=6
0.8r 4 = −1,205164= 0.16
17n 3 = 1,78571 ν3
=25.5r s = −4,144465=’0.
0294r 6 =0,9112 d
a =0.3968n 4 = 1.81961
シ4=37.3r7 =2.3103
tdl =L2639 tイ、=1.51
118td2 士0.3527 jn 2
= 1.55jn/j=5.32 rs
/f< =0.56〔発明の効果〕
以上の様に構成したことにより、本発明の光ディスク用
レンズは、光源部と光学系等を一体化してフォーカシン
グ及びトラッキング制御を行なう場合に適した光ディス
ク用レンズを実現できると共に有限系であるので枚数を
少なくづることができ、低コスト、コンパクト化をも実
現できる。However, rj, r2...rj: radius of curvature d of each component lens,
, d2...d6: Axial thickness and axial air spacing nl of each constituent lens, n2...n4 = wavelength 780nR of each constituent lens
+ refractive index ν1, ν2...C4: Number f of each constituent lens
: Focal length of the entire system ft3 : Focal length of the second group lens f4 : Focal length of the third group lens NA : Numerical aperture M : Magnification tdl : Thickness of the 7J bar glass on the light source side of the lens t(
12: Thickness tnl of 7J bar glass on condensing side of lens
: The wavelength of the cover glass on the light source side of the lens is 780. The refractive index at rv is tnz. The wavelength of the cover glass on the condensing side of the lens is 780.
Refractive index Y at nIIl High Example 1 f=1 NA=0.45 M=-0,342r
1=30.7346 61=0.3202n 1
= 1,81961 ν, =37,3r2 =-
2,6124d 2 = 0.0820r 3 = 2
.. 0490 d a = 0.4610n 2
= 1.55749 ν2 =60.8r 4
= −1,1525d 4 = 0.2049n 3
= 1.78571 3 = 25.5r 5
= -8,9284d 5 = 0.2049r 6
=0.8785 dB =0.3586n
4 = 1,81961 ci, = 37,3r 7 =
3.3501 td1=1゜1013 tn 1= 1.51
118td2 = 0.3073t
n2=1.51frs/f=5.8
8 r s / f 4 =0.64 Example 2 f −I N A = 0.45 M = −
0,342r + =32.8731 d t
=0.2739n, =1.81961ν,
=37.3r2=-2,7942d2=0.
0877r 3 =2.1915 d 3 =
0.4794n 2 = 1.55749 C2=
60.8r 4 = -1,2327d 4 = 0.
1507n 3 = 1,78571 ν3 = 2
5.5rs = -9,549665 = 0.027
4r, =0.8903 d, =0.3
698n 4 = 1.81961 ν4 = 37
.. 3r 7 =2.5118 td1=1.1780 tn1=1.5111
8td2 = 0.3287 tn2 =
1.51j n/f = 6.29 r s
/ f 4 =0.58 Example 3 f=1 N△=0.45 M=-0,36
4r 1 =68.4856 d l
=0.2739n 1 = 1.81961
ν1 = 37.3r 2 = -2,4929d 2
=0.0274r3=2.7668
d a = 0.4931n 2 = 1.5
5749 shi2=eo, ar4=1
.. 1232 d 4 =0.1507n 3
= 1,78571 ν3 ==25.
5rs = -3,8626d 5 = 0.02
74r 6 =0,8766 d b'
=0.3698r14 = 1,81961
C4=37,3r7=2.3230 td t=1.1780 tn 1=
1.51118td2 = 0.3287
tn 2 = 1.51fn/f = 4.96
r5 /f4 =0.57 Example 4 f=1 NA=0.45 M=-0,342r
1 =73.4819 d l =0.293
9n 1 = 1.8196+ Si1 = 37.3r
2 = -2,7923d 2 = 0.0294rs
=2,9687 da =0.52
91n 2 = 1.55749 C2 = 6
0.8r4=-1,205164=0.16
17n 3 = 1,78571 ν3
=25.5rs = -4,144465='0.
0294r 6 =0,9112d
a = 0.3968n 4 = 1.81961
C4=37.3r7=2.3103 tdl=L2639 ti,=1.51
118td2 shi0.3527 jn 2
= 1.55jn/j=5.32rs
/f<=0.56 [Effects of the Invention] With the above configuration, the optical disc lens of the present invention is suitable for optical discs where the light source unit, optical system, etc. are integrated to perform focusing and tracking control. In addition, since it is a finite system, the number of lenses can be reduced, making it possible to achieve low cost and compactness.
第1図は本発明に係る実施例におけるレンズ構成因、第
2図は実施例1の収差図で(イ)球面収差、(0)正弦
条件、〈ハ)非点収差を表わす。
(尚、実施例2〜4の収差図は実施例1に近似するので
省略する。)
rl・・・rl:各構成レンズの曲率半径、dl・・・
d8:各構成レンズの軸上厚みと軸上空気間隔、■=第
1群レンズ、■:第2群レンズ、■;第3群レンズ、し
1:第1レンズ、L2:第2レンズ、L3 :第3レン
ズ、L4:第4レンズ。FIG. 1 is an aberration diagram of the first embodiment, showing (a) spherical aberration, (0) sine condition, and (c) astigmatism. (The aberration diagrams of Examples 2 to 4 are omitted because they are similar to Example 1.) rl...rl: radius of curvature of each constituent lens, dl...
d8: Axial thickness and axial air spacing of each component lens, ■ = 1st group lens, ■: 2nd group lens, ■: 3rd group lens, 1: 1st lens, L2: 2nd lens, L3 : 3rd lens, L4: 4th lens.
Claims (1)
レンズ及び第3群レンズの3つのレンズ群によって構成
されており、光源側から順に第1群レンズは両凸面の正
レンズの第1レンズで構成されており、第2群レンズは
正レンズの第2レンズと負レンズの第3レンズとの接合
レンズで構成されており、第3群レンズは光源側に凸面
を向けた正メニスカスレンズの第4レンズで構成されて
いる3群4枚構成のレンズ系であって、以下の条件を満
たすことを特徴とする光ディスク用レンズ。 (1)4.0<f_2_3/f<7.0 (2)0.5<r_6/f_4<0.7 但し、fは全系の焦点距離、f_2_3は第2群レンズ
の焦点距離、f_4は第3群レンズの焦点距離、r_6
は第4レンズの光源側の曲率半径である。[Claims] It is composed of three lens groups, a first group lens, a second group lens, and a third group lens, in order from the light source side toward the condensing side.In order from the light source side, the first group lens is composed of a first lens which is a biconvex positive lens, a second lens group is composed of a cemented lens of a second positive lens and a third lens which is a negative lens, and the third lens group is a light source. A lens system for an optical disk, which is a lens system having four lenses in three groups, including a fourth lens that is a positive meniscus lens with a convex surface facing the side, and which satisfies the following conditions. (1) 4.0<f_2_3/f<7.0 (2) 0.5<r_6/f_4<0.7 However, f is the focal length of the entire system, f_2_3 is the focal length of the second group lens, and f_4 is Focal length of the third group lens, r_6
is the radius of curvature of the fourth lens on the light source side.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10045185A JPS61259214A (en) | 1985-05-14 | 1985-05-14 | Lens for optical disc |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10045185A JPS61259214A (en) | 1985-05-14 | 1985-05-14 | Lens for optical disc |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61259214A true JPS61259214A (en) | 1986-11-17 |
Family
ID=14274275
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10045185A Pending JPS61259214A (en) | 1985-05-14 | 1985-05-14 | Lens for optical disc |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61259214A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101974285B1 (en) * | 2017-11-29 | 2019-04-30 | 김도현 | Propjection potical system and lens assembly for low field of view |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5986018A (en) * | 1982-11-08 | 1984-05-18 | Konishiroku Photo Ind Co Ltd | Objective for reproduction of video disk or the like |
-
1985
- 1985-05-14 JP JP10045185A patent/JPS61259214A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5986018A (en) * | 1982-11-08 | 1984-05-18 | Konishiroku Photo Ind Co Ltd | Objective for reproduction of video disk or the like |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101974285B1 (en) * | 2017-11-29 | 2019-04-30 | 김도현 | Propjection potical system and lens assembly for low field of view |
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