JPS58147821A - Optical head - Google Patents

Optical head

Info

Publication number
JPS58147821A
JPS58147821A JP2942582A JP2942582A JPS58147821A JP S58147821 A JPS58147821 A JP S58147821A JP 2942582 A JP2942582 A JP 2942582A JP 2942582 A JP2942582 A JP 2942582A JP S58147821 A JPS58147821 A JP S58147821A
Authority
JP
Japan
Prior art keywords
optical
reflected
section
tracking
disk
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
JP2942582A
Other languages
Japanese (ja)
Inventor
Koki Mineo
峰尾 弘毅
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co Ltd
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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP2942582A priority Critical patent/JPS58147821A/en
Publication of JPS58147821A publication Critical patent/JPS58147821A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/135Means for guiding the beam from the source to the record carrier or from the record carrier to the detector

Abstract

PURPOSE:To improve the tracking adjustment and focus adjustment of an optical head remarkably by separating reflected light from a disk into a center and a circumferential light beam through an optical part where a reflective and a transmissive part are formed nearly concentrically. CONSTITUTION:A reflected beam reflected by the recording surface of the optical disk is made into a parallel beam through a convergent lens and the parallel beam is sent to a polarization beam splitter 33 through a quarter-wavelength plate 34. Then, the reflected beam is portioned out by the beam splitter 33 and sent to the optical part 37 consisting of the reflective part 37a and transmissive part 37b. This optical part 37 is arranged at up to 45 degrees to the optical axis of an optical path of reflection as shown in the figure, and while the relatively gentle light intensity distribution in the section of the reflected beam due to an off-tracking phenomenon is considered, the reflected beam is separated into the center light beam near the optical axis and the circumferential light beam at the outside of the center light beam, which are distributed in two directions respectively.

Description

【発明の詳細な説明】 ス信号への混入を改善した光学式ヘッドに関する。[Detailed description of the invention] The present invention relates to an optical head that improves mixing of signals into signals.

〔背景技術〕[Background technology]

従来、ビデオディスクプレーヤーの光学式ヘッドにおい
て、トラッキング調整とフォーカス調整を行なうために
ディスクからの反射光を2分にするものとしてハーフミ
ラ−が用いられていた。この光学式ビデオディスクプレ
ーヤーの走査系を第1図を用いて説明する。レーザ光源
(半導体装置ザまたはHe−Neレーザ)1から発生し
たレーザビームは集光レンズ2によって平行光線に変え
られる。この平行光線は偏光性ビームスプリッタ3を抜
けてトラ、キングミラー(横方向の付蓋補正ミラー)4
に反射して収束レンズ5によりディスク6の記録面に焦
点が結ばれる。ディスク6の記録面で反射を受けたビー
ムは来た方向に逆戻りして偏光性ビームスプリッタ3で
振り分けられる。その後、ハーフミラ−7によってトラ
ッキング用光信号とフォーカス用光信号に2分され、ト
ラッキング用光信号は2個に分割されたホトダイオード
8番こ、またフォーカス用光信号は集光レンズ9aと円
筒レンズ9bにより構成した非点収差光学部9を介して
4個に分割されたホトダイオード10に送られる。
Conventionally, in the optical head of a video disc player, a half mirror has been used to divide the reflected light from the disc into two parts for tracking adjustment and focus adjustment. The scanning system of this optical video disc player will be explained with reference to FIG. A laser beam generated from a laser light source (semiconductor device laser or He-Ne laser) 1 is converted into a parallel beam by a condenser lens 2 . This parallel light beam passes through the polarizing beam splitter 3 and then passes through the tiger and king mirror (horizontal compensation mirror) 4.
The light is reflected by the converging lens 5 and focused on the recording surface of the disk 6. The beam reflected by the recording surface of the disk 6 returns in the direction in which it came and is distributed by the polarizing beam splitter 3. Thereafter, the optical signal for tracking is divided into two by the half mirror 7 into the optical signal for tracking and the optical signal for focusing. The light is sent to four divided photodiodes 10 through an astigmatism optical section 9 constructed by the following.

ここで、非点収差光学部によるフォーカス信号の検出に
ついて説明する。第2図は集光レンズ9aと円筒レンズ
9bからなる通常の非点収差光学部9である。図示例で
は説明の便宜上、光ディスク6の記録面からの反射光中
、光軸に沿って互いにて考察する。
Here, detection of a focus signal by the astigmatism optical section will be explained. FIG. 2 shows a normal astigmatism optical section 9 consisting of a condenser lens 9a and a cylindrical lens 9b. In the illustrated example, for convenience of explanation, the reflected light from the recording surface of the optical disc 6 will be considered along the optical axis.

光軸と円筒レンズ9bの円筒軸とで決まる面内の光線は
光軸上の遠方に集魚を結び、またそれと直交する面内の
ビームは近くに焦点を結ぶ。このことから、非点収差光
学部9を通過したビームは焦点FlとF、との間に結ば
れる。結果として非点収差光学部9を通過した光線は一
点に焦点を結ぶことがなく図に示すようにある大きさの
錯乱円を形成する。このとき、最小錯乱円の位置をあら
かじめ光学式ヘッドからディスク6の記録面へ出射する
読み取りレーザビームの焦点位置に対応させておけば、
最小錯乱円の位置変動からディスク6の変動を検出して
、Rみ取りレーザビームの焦点を常にディスク6の記録
面に合せる事ができる。
A ray of light in a plane determined by the optical axis and the cylindrical axis of the cylindrical lens 9b focuses the fish in a far distance on the optical axis, and a beam in a plane perpendicular to the ray focuses nearby. From this, the beam passing through the astigmatism optical section 9 is focused between the focal points Fl and F. As a result, the light beam passing through the astigmatism optical section 9 is not focused on one point, but forms a circle of confusion of a certain size as shown in the figure. At this time, if the position of the circle of least confusion is made to correspond in advance to the focal position of the reading laser beam emitted from the optical head to the recording surface of the disk 6,
By detecting the fluctuation of the disk 6 from the positional fluctuation of the circle of least confusion, the focus of the R-cutting laser beam can always be focused on the recording surface of the disk 6.

例えば、ディスク6が正常な位置にあり、入射ビームが
記録面に記録されたピット以外のところに照射された場
合1反射ビームが対物レンズ5゜トラッキングミラー4
 偏光性ビームスプリッタ3、ハーフミラ−7を通って
非点収差光学部9によりホトダイオード10に導かれる
。そして錯乱円は第3図に示すように4個のホトダイオ
ード10a10dと差動アンプ11によって構成したフ
ォーカス制御回路の4個のホトダイオード108〜10
dの中心lこ第4図(a)に示すように円形の像として
投影されるため、差動アンプ11から出る出力は零とな
りサーボ機構は停止状轢に保持される。
For example, if the disk 6 is in a normal position and the incident beam is irradiated to a place other than the pit recorded on the recording surface, the reflected beam will be reflected by the objective lens 5° and the tracking mirror 4.
The light passes through a polarizing beam splitter 3 and a half mirror 7 and is guided to a photodiode 10 by an astigmatism optical section 9. As shown in FIG.
Since the center l of d is projected as a circular image as shown in FIG. 4(a), the output from the differential amplifier 11 becomes zero and the servo mechanism is held in a stopped state.

また、ディスク6が光学式ヘッドlこ対しで近い位置に
ある場合、錯乱円は4個のホトダイオード10a〜10
dの中心に第4図(b)に示すように図示上下方向に細
長い横円形の澹として投影されるため、1対のホトダイ
オード10!、10cの出力が1対のホトダイオード1
0b、10dの出力に比べて大きくなる。このため差動
アンプ11から出る出力が十となり、この出力によりサ
ーボ機構が駆動し光学式ヘッドを正しい位置に修正する
Furthermore, when the disk 6 is located close to the optical head l, the circle of confusion is caused by the four photodiodes 10a to 10.
As shown in FIG. 4(b), a pair of photodiodes 10! is projected onto the center of d as an elongated horizontal circular ring in the vertical direction in the figure. , 10c output is a pair of photodiodes 1
The output is larger than that of 0b and 10d. Therefore, the output from the differential amplifier 11 is ten, and this output drives the servo mechanism to correct the optical head to the correct position.

さらに、ディスク6が光学式ヘッドiこ対して遠い位置
にある場合、錯乱円は4個のホトダイオード10a〜1
0dの中心にf44図1c)に示すように図示左右方向
に細長い楕円形の像として投影されるため。
Furthermore, when the disk 6 is located far away from the optical head i, the circle of confusion is caused by four photodiodes 10a to 1.
This is because it is projected at the center of 0d as an elongated elliptical image in the horizontal direction as shown in Figure 1c).

1対のホトダイオード10b、 10dの出力が1対の
ホトダイオード10a、 100の出力に比べて大きく
なる。
The output of the pair of photodiodes 10b and 10d is larger than the output of the pair of photodiodes 10a and 100.

このため、差動アンプ11から出る出力は−となる。こ
の出力によりフォーカスサーボ機構を制御して光学式ヘ
ッドを正しい位置に修正する。
Therefore, the output from the differential amplifier 11 becomes -. This output controls the focus servo mechanism to correct the optical head to the correct position.

次に1反射ビームをハーフミラ−7で2分したトラッキ
ング用光信号の検出について簡単に説明する。入射ビー
ムが記録面のトラックから外れると2反射ビーム断面内
の光強度分布が片寮るため。
Next, detection of a tracking optical signal obtained by dividing one reflected beam into two by the half mirror 7 will be briefly described. This is because when the incident beam deviates from the track on the recording surface, the light intensity distribution within the cross section of the two reflected beams becomes uneven.

このトラッキング用光信号を第5図に示すように2個の
ホトダイオード851.8bと差動アンプ21によって
構成したトラッキング制御回路の2個のホトダイオード
8a、8bに投影し、2分割にされたホトダイオードg
a、8bのダイオード出力差を差動アンプ21によって
検出する。この出力によりトラッキングサーボ機構を制
御して光学式ヘッドを正しい位置に修正する。
This tracking optical signal is projected onto two photodiodes 8a and 8b of a tracking control circuit constituted by two photodiodes 851.8b and a differential amplifier 21 as shown in FIG.
A differential amplifier 21 detects the diode output difference between a and 8b. This output controls the tracking servo mechanism to correct the optical head to the correct position.

しかし、ディスク6からの反射ビームは一様ではなく、
特にトラックが外れかけた状態では反射ビーム断面内の
光強度分布が生じる。このトラツス用光信号に混入する
ため、第4図(a)に示すように最小錯乱円が4個のホ
トダイオード10a〜10d or中心に投影されてい
るにもかかわらず、フォー膨lス制御回路の差動アンプ
11の出力が零にならず光学式ヘッドの焦点が外れる危
険性がある。
However, the reflected beam from the disk 6 is not uniform;
Particularly in a state where the track is about to come off, a light intensity distribution occurs within the cross section of the reflected beam. As shown in FIG. 4(a), even though the circle of least confusion is projected at the center of the four photodiodes 10a to 10d, the optical signal for the tratus control circuit is mixed with the optical signal. There is a risk that the output of the differential amplifier 11 will not become zero and the optical head will be out of focus.

〔発明の目的〕[Purpose of the invention]

この発明は上述の問題点に鑑みなされたもので。 This invention was made in view of the above-mentioned problems.

比較的簡単な構成によってトラッキング用光信号のフォ
ーカス用光信号への混入を減少させてトラッキング調整
およびフォーカス調整の精度を著しく向上させることが
できる光学式ヘッドを提供することを目的とする。
It is an object of the present invention to provide an optical head that can significantly improve the accuracy of tracking adjustment and focus adjustment by reducing the mixing of a tracking optical signal into a focusing optical signal with a relatively simple configuration.

〔発明のli[1 この発明は非点収差光学部を用いて光ディスク−ζ記録
された情報を読み取る光学式ヘッドの自動焦点合せ機構
に応用し、光ディスクからの反射光の党略内に反射部と
透過部を略同心円状に形成した光学部を反射光軸に対し
て斜めに配設して1反射光を光軸近傍の中心光線と、こ
の中心光線の外カス用光信号とし1周囲光線をトラッキ
ング用光信号として抽出するものである。
[li of the invention [1] This invention is applied to an automatic focusing mechanism of an optical head that reads information recorded on an optical disc using an astigmatism optical part, and a reflecting part is formed within the beam of reflected light from the optical disc. An optical section with a transmitting section formed approximately concentrically is arranged diagonally with respect to the reflected optical axis, and one reflected light is used as a central ray near the optical axis, and one surrounding ray is used as an optical signal for the outer rays of this central ray. This is extracted as a tracking optical signal.

〔発明の効果〕〔Effect of the invention〕

反射部と透過部を略同心円状に形成した光学部によりデ
ィスクからの反射光を中心光線と周囲光線に分離するこ
とができるため、トラッキング用光信号のフォーカス用
光信号への混入を減少させることができ、これにより光
学式ヘッドのトラッキング調整招よびフォーカス調整を
著しく向上させることができる。
The optical part in which the reflecting part and the transmitting part are formed in substantially concentric circles can separate the reflected light from the disk into a central ray and a surrounding ray, thereby reducing the mixing of the tracking optical signal into the focusing optical signal. This makes it possible to significantly improve the tracking adjustment and focus adjustment of the optical head.

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

以下図面を参照してこの発明の一実施例を説明する。第
6図において31はレーザ光源で、このレーザ光源31
から発生したレーザビームは集光レンズ32により平行
光線に変えられ、偏光用ビームスプリッタ33を抜けて
1/4波長板34を通して収束レンズ35により光ディ
スク36の記録面に焦点が結ばれる。この光ディスク3
6の記録面で反射を受けた反射ビームは収束レンズ35
にげよって平行光線に変えられ、1/4波長板34を通
して偏光性ビームスプリッタ−33に送られる。
An embodiment of the present invention will be described below with reference to the drawings. In FIG. 6, 31 is a laser light source, and this laser light source 31
The laser beam generated is converted into a parallel beam by a condensing lens 32, passes through a polarizing beam splitter 33, passes through a quarter-wave plate 34, and is focused on the recording surface of an optical disk 36 by a converging lens 35. This optical disc 3
The reflected beam that has been reflected on the recording surface of 6 is passed through the converging lens 35.
The beam is converted into a parallel beam by the beam and sent through a quarter-wave plate 34 to a polarizing beam splitter 33.

ここで反射ビームは偏光性ビームスプリッタ−33によ
り振り別けられ1反射部37aと透過部37bを略同心
円状に形成した光学部37に送られる。この光学部37
は第7図−こ示すように反射光路の光軸に対して45°
の角度で配設され、トラックの外れによって生じる反射
ビーム断面内の光強度分布する周囲光線に分離するとと
もに各光線を2方向に分別している。この実施例1ζ採
用された光学部37は、光学的に透明な材料例えばガラ
ス、アクリル等の平らな基板上に金、アルミ等の反射率
の高い金属膜を蒸着し、その中心部をホットエツチング
等の手段を用いて楕円形状に膜をエツチングして透過部
37bを形成する。このとき、透過部37m−の楕円形
状は長径と短径の比を(E : lに設定し、目官 状(先触に対して直交する面)が円形断面となると凹形
円筒レンズ38bにより構成した非点収差光学部38を
介して最小錯乱円の径を大きくして4個に分割したホト
ダイオード39に投影される。
Here, the reflected beam is separated by a polarizing beam splitter 33 and sent to an optical section 37 having a reflecting section 37a and a transmitting section 37b formed in substantially concentric circles. This optical section 37
is 45° to the optical axis of the reflected optical path as shown in Figure 7.
The beam is disposed at an angle of , and is separated into ambient light rays with a light intensity distribution in the cross section of the reflected beam caused by off-track, and each light ray is divided into two directions. The optical part 37 adopted in this embodiment 1ζ is made by depositing a highly reflective metal film such as gold or aluminum on a flat substrate made of an optically transparent material such as glass or acrylic, and then hot-etching the center of the film. The transparent portion 37b is formed by etching the membrane into an elliptical shape using a method such as etching. At this time, the elliptical shape of the transmitting part 37m- is set to have a ratio of the major axis to the minor axis (E:l), and when the eye shape (the surface perpendicular to the tip) has a circular cross section, it is formed by the concave cylindrical lens 38b. The image is projected through the constructed astigmatism optical section 38 onto a photodiode 39 which is divided into four parts by increasing the diameter of the circle of least confusion.

この最小錯乱円の位置をあらかじめ光学式ピックアップ
から光ディスク36の記録面へ入射する読み取りレーザ
ビームの焦点位置に対応させておけば、最小錯乱円の位
置変動から光ディスク36の変動を検出して読み取りレ
ーザビームの焦点を常に光ディスク36の記録面に合せ
ることができる。
If the position of this circle of least confusion is made to correspond in advance to the focal position of the reading laser beam that enters the recording surface of the optical disc 36 from the optical pickup, the fluctuation of the optical disc 36 can be detected from the positional fluctuation of the circle of least confusion, and the reading laser The beam can always be focused on the recording surface of the optical disc 36.

なお、非点収差光学部38におけるフォーカス信号の検
出原理は前に述べたのでここでは説明を省略する。
Note that the principle of detecting the focus signal in the astigmatism optical section 38 has been described above, so the explanation will be omitted here.

影される。ここで、入射ビームが光ディスク36のトラ
ックから外れたときに生じる反射ビーム断面内の光強度
分布の片寄りを1対のホトダイオード出力差を差動アン
プで検出している。この出力により、トラッキングサー
ボ機構を制御して光学式ピックアップを正しい位置に修
正する。
shadowed. Here, the deviation of the light intensity distribution in the cross section of the reflected beam that occurs when the incident beam deviates from the track of the optical disk 36 is detected by the difference in the outputs of a pair of photodiodes using a differential amplifier. This output controls the tracking servo mechanism to correct the optical pickup to the correct position.

したがって、トラックの外れによって生じる反射ビーム
断面内の光強度分布が比較的ゆるやかなことを利用して
、ディスク36からの反射ビームを光学s37の反射部
37aと透過部37bにより。
Therefore, by taking advantage of the fact that the light intensity distribution in the cross section of the reflected beam caused by off-track is relatively gentle, the reflected beam from the disk 36 is transmitted through the reflecting section 37a and the transmitting section 37b of the optical s37.

中心光線と周囲光線に分離することができるため。Because it can be separated into a central ray and an ambient ray.

簡単な4成でトラッキング用光信号のフォーカス信号へ
の混入を減少させることができ光学式ピックアップのト
ラッキング調整およびフォーカス調整を著しく向上させ
ることができる。
A simple four-component configuration can reduce the mixing of the tracking optical signal into the focus signal, and can significantly improve the tracking adjustment and focus adjustment of the optical pickup.

また、光学部37に形成した透過部37bの形状を光学
部37の配置角度に対応させて長径と短径の比をv/T
=1に設定し反射ビームの断面形状を円形゛にすること
により、正常状態時にホトダイオード39に投影される
最小錯乱円を円形にすることができるため、ホトダイオ
ード39のダイオード出力差を容易に零に合せることが
できる。
In addition, the shape of the transmitting part 37b formed in the optical part 37 is made to correspond to the arrangement angle of the optical part 37, and the ratio of the major axis and the minor axis is set to v/T.
By setting = 1 and making the cross-sectional shape of the reflected beam circular, the circle of least confusion projected onto the photodiode 39 in a normal state can be made circular, so the diode output difference of the photodiode 39 can be easily reduced to zero. Can be matched.

この発明はL記実施例に限定されるものではなく、要旨
を変更しない範囲において種々変形して実施することが
できる。
This invention is not limited to the embodiments described in L, and can be implemented with various modifications without changing the gist.

例えば上記実施例では透明な基板に反射率の高い金属膜
を蒸着させその中心部をエツチングして透過部と反射部
を形成したがこの発明はこれに限定されるものではなく
1例えば反射面を有する基板の中心を切欠いて透過部と
反射部を形成したり。
For example, in the above embodiment, a metal film with high reflectance is deposited on a transparent substrate and the central part is etched to form a transmitting part and a reflective part. However, the present invention is not limited to this. A transparent part and a reflective part can be formed by cutting out the center of the substrate.

または透明な基板の中心に金属膜をに状に蒸着して透過
部と反射部を形成することができる。
Alternatively, a metal film can be deposited in a rectangular shape at the center of a transparent substrate to form a transmissive part and a reflective part.

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

第1図は従来の光学式ヘッドの一列を示す概略的な構成
図、第2図は非点収差光学部の説明図、tx3図はフォ
ーカス制御回路の回路図、第4図(a)ないしくC1は
それぞれ異なる状態における非点収差光学部の錯乱円の
投影儂を示す説明図、第5図はトラッキング制御回路の
回路図、第6図はこの発明の一実施例を示す概略的な構
成図、第7図は同実施例の光学部の説明図である。 1・・・レーザ光源    2・・・集光レンズ3・・
・偏光性ビームスプリッタ 4・・・トラッキングミラー  5・・・収束レンズ6
・・・ディスク      7・・・ハーフミラ−8,
8m、 8b、 10.10a−10d=ホトダイオー
ド9・・・非点収差光学部  9a・・・集光レンズ9
b・・・円筒レンズ  11,21・・・差動アンプ3
1・・・レーザ光源  32・・・集光レンズ33・・
・偏光用ビームスプリッタ 34・・・1/4波長板  35・・・収束レンズ36
・・・光ディスク  37・・・光学部37s+・・・
反射部    37b・・・透過部38・・・非点収差
光学部  38a・・・集光レンズ38b・・・凹形円
筒レンズ 39.39a〜39d、 40a、40b−ホトダイオ
ード出願人 東京芝浦電気株式会社 代理人 弁理士 小宮幸−外1 li1WJ 第2図 ら 113図 第5図
Fig. 1 is a schematic configuration diagram showing a row of conventional optical heads, Fig. 2 is an explanatory diagram of the astigmatism optical section, Fig. tx3 is a circuit diagram of the focus control circuit, and Fig. 4 (a) or C1 is an explanatory diagram showing the projection of the circle of confusion of the astigmatism optical section in different states, FIG. 5 is a circuit diagram of a tracking control circuit, and FIG. 6 is a schematic configuration diagram showing an embodiment of the present invention. , FIG. 7 is an explanatory diagram of the optical section of the same embodiment. 1... Laser light source 2... Condensing lens 3...
・Polarizing beam splitter 4...Tracking mirror 5...Converging lens 6
...Disc 7...Half mirror 8,
8m, 8b, 10.10a-10d=Photodiode 9... Astigmatism optical section 9a... Condensing lens 9
b...Cylindrical lens 11, 21...Differential amplifier 3
1... Laser light source 32... Condensing lens 33...
・Polarizing beam splitter 34...1/4 wavelength plate 35...Converging lens 36
...Optical disc 37...Optical section 37s+...
Reflection section 37b... Transmission section 38... Astigmatic optical section 38a... Condensing lens 38b... Concave cylindrical lens 39. 39a to 39d, 40a, 40b - Photodiode applicant Tokyo Shibaura Electric Co., Ltd. Agent Patent Attorney Yuki Komiya - Outside 1 li1WJ Figure 2 et al. 113 Figure 5

Claims (1)

【特許請求の範囲】 (1)  光ディスクより情報を読み堆る光学式ヘッド
において、光ディスクに照射して得られた反射光の光路
内に反射部と透過部を略同心円状に形成した光学部を反
射光軸に対して斜めに配設し。 反射光を光軸近傍の中心光線とこの光線の外側に位置す
る周囲光線に分離するとともに中心光線をフォーカス用
光信号とし1周囲光線をトラッキング用光信号として抽
出することを特徴と−する光学式ヘッド。 囲第1項記載の光学式ヘッド。 13)光学部は中心に反射部を形成しその周囲に透過部
を形成したことを特徴とする特許請求の範囲fa1項記
載の光学式ヘッド。 (4)光学部により分別された中心光線は非点収差光学
部を介して4分割ホトダイオードに投影されフォーカス
信号に変換されることを特徴とする特許請求の範囲第1
項ないし第3項のいぐれかに記載の光学式ヘッド。 (5)光学部により分別された周囲光線は2分割ホトダ
イオードに投影されトラッキング信号に変換されること
を特徴とする特許請求の範囲第1項ないし第3項のいず
れかに記載の光学式ヘッド。
[Scope of Claims] (1) An optical head that reads information from an optical disk includes an optical section in which a reflecting section and a transmitting section are formed substantially concentrically in the optical path of reflected light obtained by irradiating the optical disk. Arranged diagonally to the reflected optical axis. An optical system characterized in that reflected light is separated into a central ray near the optical axis and peripheral rays located outside this ray, and the central ray is used as a focusing optical signal and one peripheral ray is extracted as a tracking optical signal. head. The optical head according to item 1 below. 13) The optical head according to claim fa1, wherein the optical part has a reflective part formed in the center and a transparent part formed around the reflective part. (4) The central ray separated by the optical section is projected onto a 4-split photodiode via an astigmatism optical section and converted into a focus signal.
The optical head according to any one of Items 1 to 3. (5) The optical head according to any one of claims 1 to 3, wherein the ambient light separated by the optical section is projected onto a two-split photodiode and converted into a tracking signal.
JP2942582A 1982-02-25 1982-02-25 Optical head Pending JPS58147821A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2942582A JPS58147821A (en) 1982-02-25 1982-02-25 Optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2942582A JPS58147821A (en) 1982-02-25 1982-02-25 Optical head

Publications (1)

Publication Number Publication Date
JPS58147821A true JPS58147821A (en) 1983-09-02

Family

ID=12275774

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2942582A Pending JPS58147821A (en) 1982-02-25 1982-02-25 Optical head

Country Status (1)

Country Link
JP (1) JPS58147821A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63173719U (en) * 1987-04-30 1988-11-11
JPH0447533A (en) * 1990-06-14 1992-02-17 Pioneer Electron Corp Optical pickup device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63173719U (en) * 1987-04-30 1988-11-11
JP2504893Y2 (en) * 1987-04-30 1996-07-24 株式会社ニコン Optical head
JPH0447533A (en) * 1990-06-14 1992-02-17 Pioneer Electron Corp Optical pickup device

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