JPH01269248A - Optical recording and reproducing device - Google Patents

Optical recording and reproducing device

Info

Publication number
JPH01269248A
JPH01269248A JP63097589A JP9758988A JPH01269248A JP H01269248 A JPH01269248 A JP H01269248A JP 63097589 A JP63097589 A JP 63097589A JP 9758988 A JP9758988 A JP 9758988A JP H01269248 A JPH01269248 A JP H01269248A
Authority
JP
Japan
Prior art keywords
lens
optical
light
reproducing device
optical member
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
Application number
JP63097589A
Other languages
Japanese (ja)
Inventor
Michihiro Tadokoro
通博 田所
Kazuo Okada
和夫 岡田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP63097589A priority Critical patent/JPH01269248A/en
Publication of JPH01269248A publication Critical patent/JPH01269248A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To unite an optical recording and reproducing device with another optical member by joining the both curved surfaces of a first lens, which has a plain surface and a projecting surface, and a second lens, whose refraction factor is different, to have a plain surface and the recessed surface of a radius of curvature, whose refraction factor is almost same as the above mentioned projecting surface. CONSTITUTION:A synthetic optical member 90 is formed by joining the respective projecting surface and recessed surface of equal radius of curvature R91 and R92. Then, respective refraction factors n91 and n92 have the relation of n91>n92 and the member 90 is optically operated as a convex lens. A diffusing light flux outgoing from a semiconductor laser 1 is passed through a collimator lens 2 and condensed on the recording film of an information carrier 8 through a united light flux shaping prism 3, a beam splitter (BS) 4, a reflection mirror 5, a lambda/4 board 6 and an objective lens 7. The reflected light reversely advances and passes through a synthetic optical member 90 to be connected to the BS4. Then, the light is divided into two lights by a half prism 10 and incoming to a two-dividing optical detector 11. After that, the light is incoming through a knife edge 12 to a two-dividing optical detector 13 and tracking and focusing control is respectively executed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は情報担体に情報を記録再生したり、あるいは
消去を行う光記録再生装置に係り、特にその装置に使用
する光学部材の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optical recording/reproducing device for recording, reproducing, or erasing information on an information carrier, and particularly relates to improvements in optical members used in the device.

〔従来の技術〕[Conventional technology]

第6図は例えば特開昭61−210541号公報に記載
された従来の光記録再生装置を示す斜視図で、特に光路
とその光路上に設けられた各光学部材の状況を説明する
ものである。図において、(1)は光源としての半導体
レーザ、(2)はコリメートレンズである。(3)は平
行光束を整形する光束整形プリズム、(4)は偏光ビー
ムスプリフタ、(5)は反射ミラー、(6)は1/4波
長板で、光束整形プリズム(3)、偏光ビームスプリッ
タ(4)、反射ミラー(5)および174波長板(6)
は相互に一体に構成されている。これら光学部材の一体
化構成については後に詳述する。(7)は対物レンズ、
(8)は記録膜(8a)が内部に形成された情報担体、
(9)は凸レンズ、Orjはハーフプリズム、θ0は2
分割光検知器で、トラック位置誤差検出用として対物レ
ンズ(7)の矢印Tの方向の位置制御のために使用され
る。(+2)は光束の一部を遮断するナイフェツジ、+
131は2分割光検知器で、焦点誤差検出用として対物
レンズ(7)の矢印Fの方向の位置制御のために使用さ
れる。
FIG. 6 is a perspective view showing a conventional optical recording/reproducing apparatus described in, for example, Japanese Patent Application Laid-Open No. 61-210541, and particularly illustrates the optical path and the state of each optical member provided on the optical path. . In the figure, (1) is a semiconductor laser as a light source, and (2) is a collimating lens. (3) is a beam shaping prism that shapes parallel beams, (4) is a polarizing beam splitter, (5) is a reflecting mirror, (6) is a quarter wavelength plate, and the beam shaping prism (3) is a polarizing beam splitter. (4), reflective mirror (5) and 174 wavelength plate (6)
are mutually integral. The integrated configuration of these optical members will be described in detail later. (7) is the objective lens,
(8) is an information carrier in which a recording film (8a) is formed;
(9) is a convex lens, Orj is a half prism, and θ0 is 2
The split photodetector is used to control the position of the objective lens (7) in the direction of arrow T for detecting track position errors. (+2) is a knife that blocks part of the luminous flux, +
A two-split photodetector 131 is used to control the position of the objective lens (7) in the direction of arrow F for detecting focus errors.

次に動作について説明する。半導体レーザ(1)から出
射した発散光束0→はコリメートレンズ(2)により収
束されて平行光束u9に変換される。平行光束(+51
は更に光束整形プリズム(3)に入射し、第7図にその
詳細を示すように、その光束径りは拡大されて光束径H
の拡大平行光束σ0となる。拡大平行光束ueは偏光ビ
ームスプリッタ(4)を通過して反射ミラー(5)で反
射され、1/4波長板(6)を経て対物レンツ旦 ズ(7)により情報柵体(8)の記録膜(8a)上に微
小な光ゴ且 スポットに集光される。次に、情報相体(8)からの1
反射光は、対物レンズ(7)および1/4波長板(6)
を通過して反射ミラー(5)で反射され、更に偏光ビー
ムスプリッタ(4)で反射されて反射光束(17]とな
る。反射光束u71は凸レンズ(9)により集光され、
その光量の略半分はハーフプリズムOlを透過してトラ
ック位置誤差検出用の2分割光検知器θ0に入射する。
Next, the operation will be explained. The diverging light beam 0→ emitted from the semiconductor laser (1) is converged by the collimating lens (2) and converted into a parallel light beam u9. Parallel luminous flux (+51
further enters the beam shaping prism (3), and as shown in detail in Figure 7, its beam diameter is expanded to a beam diameter H.
becomes an expanded parallel light flux σ0. The expanded parallel beam ue passes through a polarizing beam splitter (4), is reflected by a reflecting mirror (5), passes through a quarter-wave plate (6), and is recorded on an information frame (8) by an objective lens (7). The light is focused into a minute spot on the film (8a). Next, 1 from information phase (8)
The reflected light is transmitted through the objective lens (7) and the quarter-wave plate (6).
, is reflected by the reflecting mirror (5), and is further reflected by the polarizing beam splitter (4) to become a reflected beam (17).The reflected beam u71 is condensed by the convex lens (9),
Approximately half of the amount of light passes through the half prism Ol and enters the two-split photodetector θ0 for detecting a track position error.

この2分割光検知器00は凸レンズ(9)の集光点より
所定距離ずれた位置に配置されている。凸レンズ(9)
により集光された光束の他の半分はハーフプリ分割光検
知器0Jに入射する。この2分割光検知器03は凸レン
ズ(9)の焦点の位置に配置されている。
This two-split photodetector 00 is placed at a position shifted by a predetermined distance from the condensing point of the convex lens (9). Convex lens (9)
The other half of the luminous flux focused by is incident on the half pre-split photodetector 0J. This two-split photodetector 03 is placed at the focal point of the convex lens (9).

そして、2分割光検知器(+1)の出力信号の差からト
ラック位置誤差信号が得られ、この信号を入力した図示
しない制御回路およびアクチュエータにより、対物レン
ズ(7)を情報担体(8)の半径方向即ち第6図の矢印
Tに示す方向に駆動して、回転中心θ呻を軸に回転する
情報担体(8)の偏芯に光スポットを追従させるいわゆ
るトラッキング制御を行う。
A track position error signal is obtained from the difference between the output signals of the two-split photodetector (+1), and a control circuit and an actuator (not shown) to which this signal is input control the objective lens (7) to the radius of the information carrier (8). It is driven in the direction indicated by arrow T in FIG. 6 to perform so-called tracking control in which the light spot follows the eccentricity of the information carrier (8) rotating around the center of rotation θ.

また、2分割光検知器u3の出力信号の差から焦点誤差
信号が得られ、同様に制御回路およびアクチュエータに
より対物レンズ(7)をその焦点方向即ち第6図の矢印
Fに示す方向に駆動して、情報担体(8)の面振れに光
スポットを追従させるいわゆるフォーカシング制御を行
う。なお、情報担体(8)に記録されている情報を再生
するための再生信号は2分割光検出器01)の出力信号
の和から得ることができる。
Further, a focus error signal is obtained from the difference between the output signals of the two-split photodetector u3, and the control circuit and actuator similarly drive the objective lens (7) in its focal direction, that is, in the direction shown by arrow F in FIG. So-called focusing control is performed to cause the light spot to follow the surface deflection of the information carrier (8). Note that the reproduction signal for reproducing the information recorded on the information carrier (8) can be obtained from the sum of the output signals of the two-split photodetector 01).

以上、光記録再生装置に使用する各光学部材のうち、光
束整形プリズム(3)、偏光ビームスプリッタ(4)、
反射ミラー(5)および1/4波長板(6)は既述した
ように一体に構成されているが、これは以下の理由によ
る。即ち、本装置のこれら各光学部材は、それぞれに要
求された各光学的機能を満足する必要があることは勿論
であるが、半導体レーザ(1)、情報担体(8)および
光検知器α003の間にあって相互の光軸を所定の位置
関係に収めるよう特にその取付けにおいて高い寸法精度
面精度が要請される。
Among the optical members used in the optical recording and reproducing device, the beam shaping prism (3), the polarizing beam splitter (4),
The reflecting mirror (5) and the quarter-wave plate (6) are integrally constructed as described above, and this is for the following reason. That is, it goes without saying that each of these optical members of this device needs to satisfy each required optical function, but also the semiconductor laser (1), the information carrier (8), and the photodetector α003. High dimensional and surface accuracy is required, especially in the installation process, so that the mutual optical axes can be placed in a predetermined positional relationship.

この寸法精度等は本来各部材の相互間に要請されるもの
であるので、光記録再生装置の筐体に対する光学系全体
としての精度はある所定の誤差範囲内に収まっていれば
よい。しかし、各光学部材を個々独立に筐体に取付ける
構成とすると、全体として許容される誤差を各部材に割
り振ることになるため、個々の部材に要求される精度は
いきおい厳しくなる傾向となり、かつ個々の部材毎に筐
体に位置決め面を設ける必要があり、構造も複雑となり
困難な加工を伴うことになる。従って、複数の光学部材
を極カ一体化して、構造の簡単化と加工性の改善が図ら
れる訳である。
Since this dimensional accuracy is originally required between each member, the accuracy of the optical system as a whole with respect to the casing of the optical recording/reproducing device only needs to fall within a certain predetermined error range. However, if each optical component is individually attached to the housing, the overall allowable error will be allocated to each component, so the precision required for each component will tend to become even stricter, and It is necessary to provide a positioning surface on the casing for each member, which makes the structure complicated and requires difficult processing. Therefore, by integrating a plurality of optical members into one piece, it is possible to simplify the structure and improve workability.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

以上説明したように、各光学部材は極力多数のものを一
体化するのが望ましい。しかし、従来の光記録再生装置
では以上のように、光束整形プリズム(3)、偏光ビー
ムスプリッタ(4)、反射ミラー(5)および1/4波
長板(6)を一体止するにとどまっている。即ち、以上
の光学部材は、その光の入出面が平面であるので相互に
隣接する平面を接合することによって比較的容易に一体
化が可能となる。しかし、例えば凸レンズ(9)はその
光の入出面の一方が凸面であり、平面構造の上記一体上
部材との接合ができず、部材を個々に取付けた場合の上
述した欠点を解消できないという問題点があった。
As explained above, it is desirable to integrate as many optical members as possible. However, in conventional optical recording and reproducing devices, the beam shaping prism (3), the polarizing beam splitter (4), the reflecting mirror (5), and the quarter-wave plate (6) are only fixed together as described above. . That is, since the optical member described above has a flat surface through which light enters and exits, it can be relatively easily integrated by joining adjacent flat surfaces. However, for example, the convex lens (9) has a convex surface on one of its light entrance/exit surfaces, and cannot be joined to the above-mentioned integral member having a planar structure, making it impossible to eliminate the above-mentioned drawbacks when the members are attached individually. There was a point.

この発明は以上のような従来の問題点を解消するために
なされたもので、凸レンズ(9)のような曲面を有する
光学部材についても他の光学部材との一体化を可能とし
得る光記録再生装置を得ることを目的とする。
This invention was made in order to solve the above-mentioned conventional problems, and it is an optical recording and reproducing method that allows optical members with curved surfaces, such as the convex lens (9), to be integrated with other optical members. The purpose is to obtain equipment.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係る光記録再生装置は、一体止しようとする
光学部材の少なくとも1個を、光の入出面の一方が平面
に他方が凸面にそれぞれ形成された第1のレンズと、屈
折率が第1のレンズのそれと異なりかつ光の入出面の一
方が平面に他方が第1のレンズの凸面と略等しい曲率半
径を有し上記凸面と接合される凹面にそれぞれ形成され
た第2のレンズとの合成光学部材としたものである。
The optical recording/reproducing device according to the present invention is characterized in that at least one of the optical members to be integrally fixed is connected to a first lens in which one of the light entrance and exit surfaces is formed as a flat surface and the other as a convex surface, and a first lens having a refractive index as a first lens. A second lens, which is different from that of the first lens, has one of the light entrance and exit surfaces being flat and the other having a radius of curvature approximately equal to the convex surface of the first lens, and each formed on a concave surface joined to the convex surface. This is a synthetic optical member.

〔作 用〕[For production]

この発明における合成光学部材は、その第1および第2
の両レンズの屈折率の相異によって光学的には凸レンズ
または凹レンズとして機能するにもかかわらず、構造上
その光の入出面はいずれも平面に形成されることになる
ので、同じく平面に形成された他の光学部材と簡単に接
合でき、光学部材の一体化を一層徹底させることができ
る。
The synthetic optical member in this invention has its first and second
Although both lenses optically function as convex or concave lenses due to the difference in their refractive index, structurally speaking, both of their light entrance and exit surfaces are flat, so they are also formed flat. It can be easily joined to other optical members, and the optical members can be more thoroughly integrated.

〔発明の実施例〕[Embodiments of the invention]

第1図はこの発明の一実施例における光記録再生装置を
示す斜視図で、従来の第6図に相当するものである。図
において、(1)〜f81.Qtll〜0樽は従来の場
合と同一であるので説明を省略する。■は以下に詳述す
る第1のレンズT!J11と第2のレンズ(支)とを接
合してなる合成光学部材としての凸レンズで、従来から
の光学部材である光束整形プリズム(3)、偏光ビーム
スプリッタ(4)、反射ミラー(5)、1/4波長板(
6)およびハーフプリズムOIとをあわせて一体構造に
構成されている。
FIG. 1 is a perspective view showing an optical recording/reproducing apparatus according to an embodiment of the present invention, and corresponds to FIG. 6 of the prior art. In the figure, (1) to f81. Qtll~0 barrels are the same as in the conventional case, so the explanation will be omitted. ■ is the first lens T! detailed below! A convex lens as a composite optical member formed by joining J11 and a second lens (support), and includes conventional optical members such as a beam shaping prism (3), a polarizing beam splitter (4), a reflecting mirror (5), 1/4 wavelength plate (
6) and the half prism OI are combined into an integral structure.

第2図はこの凸レンズ■の全体および両レンズ(9Ll
1921をその光軸であるY軸の方向に離して示した斜
視図、第3図は第2図の凸レンズ■をY軸を含む平面で
切断しこれをXの方向から見た断面図である。図におい
て、(9Llは、そのY軸の方向の一方の端面がY軸と
直角の平面に、他方が中心がY軸上に存在する曲率半径
R9Iの球状の凸面にそれぞれ形成された第1のレンズ
で、その屈折率はnlである。これに対して、■はその
一方の端面がY軸と直角の平面に、他方が同じ(中心が
Y軸上に存在する曲率半径R92の球状の凹面にそれぞ
れ形成された第2のレンズで、その屈折率はn!である
Figure 2 shows the entire convex lens ■ and both lenses (9Ll
1921 is a perspective view showing the lens separated in the direction of the Y-axis, which is its optical axis, and FIG. 3 is a cross-sectional view of the convex lens ■ in FIG. 2 taken along a plane including the Y-axis and viewed from the X-direction. . In the figure, (9Ll is the first end face in the Y-axis direction formed on a plane perpendicular to the Y-axis, and the other on a spherical convex surface with a radius of curvature R9I whose center lies on the Y-axis. It is a lens whose refractive index is nl.On the other hand, ■ is a spherical concave surface with one end face on a plane perpendicular to the Y-axis and the other with a radius of curvature R92 whose center lies on the Y-axis. and a second lens formed respectively in the second lens, the refractive index of which is n!.

ここで曲率半径R,,、R,、および屈折率n91 e
 nl!はそれぞれ次の関係式が成立するように設定す
る。
Here, the radius of curvature R, , R, and the refractive index n91 e
nl! are set so that the following relational expressions hold true.

R91” R92・・・・・・・・・・・・・・・・・
・ (1)n9+ > 19g       ・・・・
・・・・・・・・・・・・・・ (2)即ち、R91”
 R9!とするから両レンズ(911(支)はその凸面
と凹面とが完全に当接し、両凸面を接着剤等で接合する
と全体としては完全な矩形形状の外形を有する1個のレ
ンズ、合成光学部材■となる。
R91” R92・・・・・・・・・・・・・・・・・・
・ (1) n9+ > 19g ・・・・
・・・・・・・・・・・・・・・ (2) That is, R91”
R9! Therefore, the convex and concave surfaces of both lenses (911 (support)) are in complete contact with each other, and when both convex surfaces are bonded together with an adhesive etc., the entire lens has a perfect rectangular outer shape, a composite optical member. ■It becomes.

次に、この合成光学部材t91が光学的に凸レンズとし
て機能することを第4図により説明する。
Next, it will be explained with reference to FIG. 4 that this composite optical member t91 optically functions as a convex lens.

第4図は本発明の主要光路部を第1図の矢印Zの方向か
ら見た図である。但し、便宜上、ナイフェツジ0乃およ
び2分割光検知器a3の部分はその光軸のまわりに90
°回転して描いている。
FIG. 4 is a view of the main optical path section of the present invention viewed from the direction of arrow Z in FIG. However, for convenience, the portion of the knife 0~ and the two-split photodetector a3 is placed 90 degrees around its optical axis.
°Drawing rotated.

しるレンズ作用これを焦点距離fで示すとその値は次式
のとおりとなる。
When this lens action is expressed by the focal length f, its value is as shown in the following equation.

ここで、屈折率の関係(2)式を考慮すると、(3)式
からf>Oとなる。
Here, considering the refractive index relationship (2), f>O from equation (3).

即ち、合成光学部材■は光学的にはf>o従って凸レン
ズとなって反射光束Oηを集光する。
That is, the synthetic optical member (2) optically serves as a convex lens since f>o and condenses the reflected light flux Oη.

従って、この実施例の場合においても従来の装置と全く
同一の動作を達成する。
Therefore, this embodiment also achieves the same operation as the conventional device.

もっとも、構成面では、光学部材の一体化が従来の凸レ
ンズ(9)に該当する凸レンズ■を含めてハーフプリズ
ムO■にまで拡大されたので、取付けのための寸法精度
や面精変更には筐体に設ける位置決め面の設定において
、特に条件の厳しいこの種光記録再生装置にあって、そ
れら精度が実質上緩和されまた筐体上の位置決め面の低
減を図ることができるので、装置全体として構造が簡単
になり加工性が向上し廉価となる。
However, in terms of construction, the integration of optical members has been expanded to include the convex lens (9), which corresponds to the conventional convex lens (9), to the half prism O■, so the dimensional accuracy and surface precision for installation need to be changed. In this type of optical recording/reproducing device, where the conditions for setting the positioning surface on the body are particularly severe, the precision of the setting is substantially reduced, and the number of positioning surfaces on the housing can be reduced, so the overall structure of the device is improved. This makes it easier to process, improves workability, and lowers the cost.

なお、上記実施例では第1のレンズ(9Dとして平面−
凸面のレンズ、第2のレンズωとして凹面−平面のレン
ズで構成したが、第5図に示すように、平面−凹面のレ
ンズ−と凸面−平面のレンズ■とざ を組合せる形にしても左い。但し、この場合にお:いて
、第4図に示す実施例と同様集光レンズとして機能させ
るには、両者の屈折率n(14およびn9sは以下の関
係式を満足するように設定する必要がある。
In the above embodiment, the first lens (9D is a flat surface).
Although the convex lens and the second lens ω are constructed with a concave-plane lens, as shown in Fig. 5, it is also possible to combine a plane-concave lens and a convex-plane lens. Left. However, in this case, in order to function as a condensing lens as in the example shown in FIG. be.

n114   <   nts           
 ・・・・・・・・・・・・・・・・・・   (4)
更に、他の応用例として合成光学部材を光束の拡大用と
して機能させたい場合には、第4図のものにあってはn
u < n92 *第5図のものにあってはnu4> 
nssの関係を満足するようにそれぞれの屈折率を設定
すればよい。
n114 < nts
・・・・・・・・・・・・・・・・・・ (4)
Furthermore, as another example of application, if you want to make the synthetic optical member function as a light beam enlarger, the one shown in Fig. 4 may be
u < n92 *nu4 for the one in Figure 5>
Each refractive index may be set so as to satisfy the relationship nss.

また、上記実施例では、両しンズall磯の曲率半径R
etとRHとを完全に等しくしたが、両曲面を接合する
接着剤を適当に選べば、両半径に若干の差異はあっても
それに基づく空隙を上記接着剤で充填することにより実
用上支障なく適用できる場合もある。
In addition, in the above embodiment, the radius of curvature R of all rocks is
et and RH are made completely equal, but if the adhesive used to join both curved surfaces is selected appropriately, even if there is a slight difference in both radii, the gap based on this difference can be filled with the above adhesive without causing any practical problems. It may be applicable in some cases.

なお、凸レンズ■とその隣接光学部材(4101との屈
折率の関係について考慮されるべき内容について以下に
説明する。即ち、第4図の例で説明するト、偏光ビーム
スプリッタ(4)の屈折率n4は第1のレンズallの
屈折率n91と等しく、また、ハーフプリズム0■の屈
折率nloは第2のレンズ(囮の屈折率n92と等しく
なるように設定するのが望ましい。
The following will explain what should be considered regarding the relationship between the refractive index of the convex lens (2) and its adjacent optical member (4101).In other words, the refractive index of the polarizing beam splitter (4) explained in the example of FIG. It is desirable that n4 be set equal to the refractive index n91 of the first lens all, and that the refractive index nlo of the half prism 02 be equal to the refractive index n92 of the second lens (decoy).

これは、それぞれの光学部材間の界面の前後で屈折率が
一定となるので、光束がこの界面で余分な反射を生じる
ことがなく、光束の減衰量を低減させる利点があるから
である。
This is because the refractive index is constant before and after the interface between each optical member, so the light flux does not undergo unnecessary reflection at this interface, which has the advantage of reducing the amount of attenuation of the light flux.

〔発明の効果〕〔Effect of the invention〕

この発明は以とのように、平面と凸面とを有する所定の
第1のレンズと、屈折率が第1のレンズと異なり、平面
と上記凸面とは略同−曲率半径の凹面とを有する第2の
レンズとを両曲面を接合して合成光学部材となし、これ
と他の光学部材とを接合するようにしたので、光学部材
の一体化がより広範囲に適用でき、装置製作上、その精
度が実質と緩和されまた筐体上の位置決め面が低減され
、装置全体としての構造が簡単になり加工性が向上して
廉価となる。
As described below, the present invention includes a predetermined first lens having a flat surface and a convex surface, and a concave surface having a refractive index different from that of the first lens, the flat surface and the convex surface having approximately the same radius of curvature. By joining both curved surfaces of lens 2 and 2 to form a composite optical member, and joining this to other optical members, the integration of optical members can be applied over a wider range, and the accuracy of the equipment can be improved. This substantially reduces the need for positioning surfaces on the casing, simplifies the overall structure of the device, improves workability, and lowers the cost.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例における光記録再生装置を
示す斜視図、第2図は第1図の合成光学部材の詳細を示
す斜視図、第3図は第2図をそのY軸を含む平面で切断
してそのXの方向から見た断面図、第4図は第1図の主
要光路部をそのZの方向からみた光路図、第5図はこの
発明の他の実施例における主要光路部を示す光路図、第
6図は従来の光記録再生装置を示す斜視図、第7図は第
6図の一部の光路部を示す光路図である。 図において、(1)は半導体レーザ、(8)は情報担体
、◇υαJは2分割光検知器、■は合成光学部材、■旧
よ第1のレンズ、■は第2のレンズである。 なお、各図中同一符号は同一または相当部分を示す。
FIG. 1 is a perspective view showing an optical recording/reproducing device according to an embodiment of the present invention, FIG. 2 is a perspective view showing details of the synthetic optical member shown in FIG. 1, and FIG. FIG. 4 is a cross-sectional view of the main optical path section of FIG. 1 viewed from the Z direction, and FIG. FIG. 6 is a perspective view showing a conventional optical recording/reproducing apparatus, and FIG. 7 is an optical path diagram showing a part of the optical path shown in FIG. 6. In the figure, (1) is a semiconductor laser, (8) is an information carrier, ◇υαJ is a two-split photodetector, ■ is a synthetic optical member, ■ is a first lens, and ■ is a second lens. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 光の入出面が平面に形成された光学部材を複数個、隣接
する上記光の入出面同士を接合して一体化したものを、
光源、情報担体および光検知器の間の光路上に設けて情
報の記録再生を行う光記録再生装置において、 上記光学部材の少なくとも1個を、光の入出面の一方が
平面に他方が凸面にそれぞれ形成された第1のレンズと
、屈折率が上記第1のレンズの屈折率と異なり、かつ光
の入出面の一方が平面に他方が上記第1のレンズの凸面
と略等しい曲率半径を有し上記凸面と接合される凹面に
それぞれ形成された第2のレンズとの合成光学部材とし
たことを特徴とする光記録再生装置。
[Claims] A plurality of optical members each having a flat light input/output surface are integrated by joining adjacent light input/output surfaces to each other,
In an optical recording and reproducing device that is installed on an optical path between a light source, an information carrier, and a photodetector to record and reproduce information, at least one of the optical members is configured such that one of the light input and output surfaces is flat and the other is a convex surface. The first lens formed respectively has a refractive index different from the refractive index of the first lens, and one of the light entrance and exit surfaces has a flat surface and the other has a radius of curvature that is approximately equal to the convex surface of the first lens. An optical recording/reproducing device characterized in that the optical recording/reproducing device is a composite optical member including second lenses formed on concave surfaces joined to the convex surface, respectively.
JP63097589A 1988-04-20 1988-04-20 Optical recording and reproducing device Pending JPH01269248A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63097589A JPH01269248A (en) 1988-04-20 1988-04-20 Optical recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63097589A JPH01269248A (en) 1988-04-20 1988-04-20 Optical recording and reproducing device

Publications (1)

Publication Number Publication Date
JPH01269248A true JPH01269248A (en) 1989-10-26

Family

ID=14196426

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63097589A Pending JPH01269248A (en) 1988-04-20 1988-04-20 Optical recording and reproducing device

Country Status (1)

Country Link
JP (1) JPH01269248A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009096280A1 (en) * 2008-01-28 2009-08-06 Konica Minolta Opto, Inc. Composite optical element and optical pickup device
JP2013525856A (en) * 2010-04-28 2013-06-20 ケーエルエー−テンカー コーポレイション Ring light illuminators and beam shapers for ring light illuminators

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009096280A1 (en) * 2008-01-28 2009-08-06 Konica Minolta Opto, Inc. Composite optical element and optical pickup device
JP2013525856A (en) * 2010-04-28 2013-06-20 ケーエルエー−テンカー コーポレイション Ring light illuminators and beam shapers for ring light illuminators

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