JPH01211331A - Optical head - Google Patents

Optical head

Info

Publication number
JPH01211331A
JPH01211331A JP63038094A JP3809488A JPH01211331A JP H01211331 A JPH01211331 A JP H01211331A JP 63038094 A JP63038094 A JP 63038094A JP 3809488 A JP3809488 A JP 3809488A JP H01211331 A JPH01211331 A JP H01211331A
Authority
JP
Japan
Prior art keywords
light
rays
lens
optical head
elliptically
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
JP63038094A
Other languages
Japanese (ja)
Inventor
Yoshiaki Ikeda
義昭 池田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63038094A priority Critical patent/JPH01211331A/en
Publication of JPH01211331A publication Critical patent/JPH01211331A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To eliminate the need for a shaping prism so as to reduce the weight and cost of an optical head by using such a collimate lens that the minor axis of the elliptically diverged beam radiated from a semiconductor lens can become longer than the effective diameter of the collimate lens and the rays of light in the minor-axis direction can become parallel rays of light. CONSTITUTION:When the effective diameter 2a of collimate lens 2 is made shorter than the minor axis of the elliptically diverged rays of light from a semiconductor laser 1, the rays of light become parallel rays of light with a circular cross section. The parallel rays of light transmits through the 1/4-wave plate 5 of a polarization beam splitter and are allowed to form a beam spot on an information recording surface 7 by means of an object lens 6. Therefore, when the specifications and position of the collimate lens 2 are set so that the elliptically diverged rays of light can become parallel beams having a circular cross section, the necessity of an expensive shaping prism which shapes an elliptical beam to a circular beam can be eliminated and, as a result, an optical head which is small in size, light in weight, and low in cost can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、画像ファイル、文書ファイル、及びコンピュ
ータ用の外部メモリー装置等に用いられ、半導体レーザ
の光ビームを利用して、情報を記録再生する光学式記録
及び再生装置としての光学ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention is an optical system that is used for image files, document files, external memory devices for computers, etc., and records and reproduces information using a light beam of a semiconductor laser. The present invention relates to an optical head as a type recording and reproducing device.

従来の技術 近年、コンピュータ用外部メモリー装置として、高密度
大容量として光メモリー装置の開発が期待されているが
、原理的には半導体レーザから放射される光ビームを対
物レンズによシ、情報記録媒体上に集光させ、情報記録
膜に凹部を設ける等して情報を記録し、再生時には情報
記録面の平担部と凹部とで光量変化が生じることを利用
して、情報信号を取り出している。
Background of the Invention In recent years, high-density, large-capacity optical memory devices are expected to be developed as external memory devices for computers.In principle, a light beam emitted from a semiconductor laser is passed through an objective lens to record information. Information is recorded by condensing light onto the medium and creating recesses in the information recording film, and during reproduction, the information signal is extracted by taking advantage of the fact that the amount of light changes between the flat and recessed parts of the information recording surface. There is.

従来の光記録再生装置について第3図を用いて説明する
。1は半導体レーザであシ、この半導体レーザ1から放
射される光ビームは、発散かつ楕円ビームとなっている
。従ってこの発散ビームをコリメートレンズ2により平
行ビームに変換している。またこの平行ビームは楕円ビ
ームとなっているため、整形プリズム3にょシ円ビーム
に修正された後、偏光ビームスプリッタ−4と四分の一
波長板6を透過して、対物レンズ6にょシディスク情報
記録面T上に集光されている。この時、対物レンズ6に
入射される光ビームを対物レンズ6の有効径より大きく
して入射させれば、対物レンズ6によシ絞られたビーム
は回折効果によりエアリ−ディスク分布を示し、ビーム
の径は小さく絞られる。また絞られたビームがラジアル
方向1周方向とで均一なビーム径としようとすると対物
しンズ6に入射される平行ビーム径は円ビームとし、ラ
ジアル方向と周方向とで強度分布を均一にすることが必
要である。対物レンズ6により絞られたビームが小さく
絞ることができれば、レーザ光のエネルギーが集束され
、記録膜に凹部を設けることができる。また情報記録面
7上に照射された光ビームは反射され、再び対物レンズ
6に入射し平行ビームとなる。またこの平行ビームは再
び四分の一波長板6に入射され、偏向面が90°回転さ
れ、偏光ビームスプリッタ−4により反射全光量が反射
され、偏光ビームスプリッタ−8でP偏光とS偏光の光
ビームに分離され、反射され、反射されたS偏光のビー
ムは凸レンズ9により集光され、2分割フォトディテク
ター1oに結像され、トラッキングエラー信号を検出し
ている。一方透過されたP偏光のビームは凸レンズ11
によシ集光され、シリンドルカルレンズ12により非点
収差を発生させ、4分割フォトディテクター13に結像
し、フォーカスエラー信号を検出している。これらのフ
ォーカスエラー信号、トラッキングエラー信号により、
情報記録媒体が面振れ、偏芯がある程度あっても、フォ
ーカス方向に±1μm程度の集点深度内に、トラッキン
グ方向にも±0.1μm程度の位置決め制御をレンズ駆
動用コイルにより、対物レンズ7を駆動させることによ
り達成している。
A conventional optical recording/reproducing device will be explained using FIG. 3. 1 is a semiconductor laser, and the light beam emitted from this semiconductor laser 1 is a diverging and elliptical beam. Therefore, this diverging beam is converted into a parallel beam by the collimating lens 2. Also, since this parallel beam is an elliptical beam, it is modified into a circular beam by a shaping prism 3, and then transmitted through a polarizing beam splitter 4 and a quarter-wave plate 6, and then transmitted through an objective lens 6 and a circular beam. The light is focused on the information recording surface T. At this time, if the light beam incident on the objective lens 6 is made larger than the effective diameter of the objective lens 6, the beam focused by the objective lens 6 exhibits an Airy disk distribution due to the diffraction effect, and the beam diameter is narrowed down. In addition, if the narrowed beam is to have a uniform beam diameter in the radial direction and one circumferential direction, the parallel beam diameter incident on the objective lens 6 will be a circular beam, and the intensity distribution will be made uniform in the radial direction and the circumferential direction. It is necessary. If the beam narrowed by the objective lens 6 can be narrowed down to a small size, the energy of the laser beam can be focused, and a recess can be formed in the recording film. Further, the light beam irradiated onto the information recording surface 7 is reflected and enters the objective lens 6 again to become a parallel beam. This parallel beam is again incident on the quarter-wave plate 6, the polarization plane is rotated by 90 degrees, the total amount of light is reflected by the polarization beam splitter 4, and the polarization beam splitter 8 separates the P-polarized light and the S-polarized light. The S-polarized light beam is separated into light beams and reflected, and the reflected S-polarized light beam is focused by a convex lens 9 and imaged on a two-split photodetector 1o to detect a tracking error signal. On the other hand, the transmitted P-polarized beam is transmitted through the convex lens 11.
The light is focused by the cylindrical lens 12 to generate astigmatism, and an image is formed on a four-segment photodetector 13 to detect a focus error signal. With these focus error signals and tracking error signals,
Even if the information recording medium has some degree of surface wobbling or eccentricity, the objective lens 7 can be controlled within a focal depth of approximately ±1 μm in the focusing direction and within ±0.1 μm in the tracking direction using the lens drive coil. This is achieved by driving the

発明が解決しようとする課題 光記録再生装置及び消去可能型光記録再生装置の開発動
向としては、コンピュータ用外部メモリー装置代替市場
ねらいということで、小型大容量化、高速アクセス化が
検討されている。小型薄型化に対しても磁気記録用磁気
ヘッドに比較して第3図に示す光記録用光学ヘッドはは
るかに大きい。
Problems to be Solved by the Invention The development trend of optical recording and reproducing devices and erasable optical recording and reproducing devices is aimed at the replacement market for external memory devices for computers, and smaller size, larger capacity, and faster access are being considered. . In terms of miniaturization and thinning, the optical head for optical recording shown in FIG. 3 is much larger than the magnetic head for magnetic recording.

また高速アクセス化に対しても、固定磁気ディスク装置
と比較しても1桁近く遅い。その原因も光学ヘッドが磁
気ヘッドより2桁程近く重たいところにある。従って光
記録再生装置がコンピュータ用外部メモリー装置代替商
品となるには、この光学ヘッドの小型薄型軽量化及コス
トが最大の課題である。
Also, when it comes to high-speed access, it is nearly an order of magnitude slower than fixed magnetic disk drives. The reason for this is that the optical head is about two orders of magnitude heavier than the magnetic head. Therefore, in order for an optical recording/reproducing device to become a substitute for an external memory device for a computer, the biggest challenge is to make the optical head smaller, thinner, lighter, and more expensive.

課題を解決するための手段 前記問題点を解決するため本発明は半導体レーザか5放
射される楕円ビームを円ビームの平行光になる様にコリ
メートレンズの有効径を半導体レーザよシ放射される楕
円発散ビームの短軸方向長以下としたものである。
Means for Solving the Problems In order to solve the above-mentioned problems, the present invention changes the effective diameter of the collimating lens so that the elliptical beam emitted from the semiconductor laser becomes a parallel circular beam. The length of the diverging beam in the minor axis direction or less.

作用 前記した様に、コリメートレンズを半導体レーザから放
射される楕円発散ビームの短矩方向がコリメートレンズ
の有効径以上になる様に、かつ平行光になる様にするこ
とにより、コリメートレンズかの出射光は円ビームの平
行光になる。よって従来の整形プリズムが削除でき、そ
の分解量化。
Function As described above, by setting the collimating lens so that the short rectangular direction of the elliptically diverging beam emitted from the semiconductor laser is equal to or larger than the effective diameter of the collimating lens, and making the beam parallel, the output of the collimating lens can be improved. The emitted light becomes a circular beam of parallel light. Therefore, the conventional shaping prism can be removed and its decomposition can be achieved.

低コスト化が図れる。Cost reduction can be achieved.

実施例 本発明による実施例について、第1図を使って説明する
。第1図は本発明による光記録再生装置用光学ヘッドの
構成図を示す。記録再生の原理は従来例と全く同じであ
り、構成要素部品の一部、すなわち第3図の従来例にお
いてコリメートレンズ2後にある楕円ビームを円ビーム
に変換する整形プリズム3を削除することができる。第
1図において、半導体レーザ1から放射された楕円発散
光は、コリメートレンズ2を第2図aのごとくその有効
径21Lを半導体レーザ1の楕円ビームの短軸方向長以
下とすると、円ビームの平行光となり、偏光ビームスプ
リッタ−4の四分の一波長板5を透過し、対物レンズ6
により、情報記録面7上にビームスポットが結ばれる。
Embodiment An embodiment of the present invention will be described with reference to FIG. FIG. 1 shows a configuration diagram of an optical head for an optical recording/reproducing apparatus according to the present invention. The principle of recording and reproduction is exactly the same as in the conventional example, and some of the component parts, namely the shaping prism 3 that converts the elliptical beam into a circular beam located behind the collimating lens 2 in the conventional example shown in FIG. 3, can be deleted. . In FIG. 1, the elliptically diverging light emitted from the semiconductor laser 1 becomes a circular beam when the effective diameter 21L of the collimating lens 2 is set to be equal to or less than the short axis length of the elliptical beam of the semiconductor laser 1 as shown in FIG. 2a. It becomes parallel light, passes through the quarter-wave plate 5 of the polarizing beam splitter 4, and passes through the objective lens 6.
As a result, a beam spot is focused on the information recording surface 7.

(なお第2図すは従来例を示す。)照射された光ビーム
は再び情報記録面7で反射され四分の一波長板6を透過
し、偏光ビームスプリッタ−4で反射全光量が反射され
、偏光ビームスプリッタ−8でP偏光とS偏光の光ビー
ムに分離され、反射されたS偏光の光ビームは凸レンズ
9により集光され、2分割フォトディテクター10に結
像され、トラッキングエラー信号が検出される。一方透
過されたP偏光の光ビームは凸レンズ11により集光さ
れ、シリンドルカルレンズ12により非点収差が発生さ
れ、4分割フォトディテクター13に結像し、フォーカ
スエラー信号が検出される。
(Figure 2 shows a conventional example.) The irradiated light beam is reflected again by the information recording surface 7 and transmitted through the quarter-wave plate 6, and the total amount of reflected light is reflected by the polarizing beam splitter 4. The polarizing beam splitter 8 separates the light beam into P-polarized light and S-polarized light beam, and the reflected S-polarized light beam is focused by a convex lens 9 and imaged on a two-split photodetector 10 to detect a tracking error signal. be done. On the other hand, the transmitted P-polarized light beam is condensed by a convex lens 11, astigmatism is generated by a cylindrical lens 12, and an image is formed on a 4-split photodetector 13, where a focus error signal is detected.

発明の効果 以上の様に、本発明によりほとんど構成をかえず、半導
体レーザから放射される楕円発散ビームを、コリメート
レンズの仕様9位置を平行内ビームになる様に配置する
だけで、楕円ビームを円ビームに整形する高価な整形プ
リズムを削除でき、小型軽量かつローコストの光学ヘッ
ドを提供することができるものである。
As described above, the present invention makes it possible to convert an elliptical diverging beam emitted from a semiconductor laser into an elliptical beam by simply arranging the collimating lens so that the 9 positions of the collimating lens become parallel beams without changing the configuration. An expensive shaping prism for shaping a circular beam can be omitted, and a small, lightweight, and low-cost optical head can be provided.

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

第1図は本発明の一実施例における光記録再生装置用光
学ヘッドの構成図、第2図a、bにはコリメートレンズ
に入射するビーム形状を示す図である。第3図は従来の
光記録再生用光学ヘッドの構成図である。 1・・・・・・半導体レーザ、2・・・・・・コリメー
トレンズ、4・・・・・・偏光ビームスプリッタ−16
・・・・・・四分の一波長板、6・・・・・・対物レン
ズ、了・・・・・・情報記録面、8・・・・・・偏光ビ
ームスプリッタ−19・・・・・・凸レンズ、10・・
・・・・2分割フォトディテクター、11・・・・・・
凸レンズ、12・・・・・・シリンドルカルレンズ、1
3・・・・・・4分割フォトディテクター。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 (の       (b> t=*S株シープ・ 2− コリメートレンズ 第3r11
FIG. 1 is a block diagram of an optical head for an optical recording/reproducing apparatus according to an embodiment of the present invention, and FIGS. 2a and 2b are diagrams showing the shape of a beam incident on a collimating lens. FIG. 3 is a block diagram of a conventional optical recording/reproducing optical head. 1...Semiconductor laser, 2...Collimating lens, 4...Polarizing beam splitter-16
... Quarter wavelength plate, 6 ... Objective lens, End ... Information recording surface, 8 ... Polarizing beam splitter -19 ...・Convex lens, 10...
...2-split photodetector, 11...
Convex lens, 12... Cylindrical lens, 1
3...4-division photodetector. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Fig.2

Claims (1)

【特許請求の範囲】[Claims] 光源として半導体レーザを使用し、この半導体レーザか
らの楕円ビームが通過するコリメートレンズの有効径を
、半導体レーザより放射される楕円発散ビームの短軸方
向長以下にする光学ヘッド。
An optical head that uses a semiconductor laser as a light source and makes the effective diameter of a collimating lens through which an elliptical beam from the semiconductor laser passes equal to or less than the short-axis length of the elliptical diverging beam emitted from the semiconductor laser.
JP63038094A 1988-02-19 1988-02-19 Optical head Pending JPH01211331A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63038094A JPH01211331A (en) 1988-02-19 1988-02-19 Optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63038094A JPH01211331A (en) 1988-02-19 1988-02-19 Optical head

Publications (1)

Publication Number Publication Date
JPH01211331A true JPH01211331A (en) 1989-08-24

Family

ID=12515887

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63038094A Pending JPH01211331A (en) 1988-02-19 1988-02-19 Optical head

Country Status (1)

Country Link
JP (1) JPH01211331A (en)

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