JPH05114193A - Photomagnetic detector for optical head - Google Patents

Photomagnetic detector for optical head

Info

Publication number
JPH05114193A
JPH05114193A JP3302478A JP30247891A JPH05114193A JP H05114193 A JPH05114193 A JP H05114193A JP 3302478 A JP3302478 A JP 3302478A JP 30247891 A JP30247891 A JP 30247891A JP H05114193 A JPH05114193 A JP H05114193A
Authority
JP
Japan
Prior art keywords
optical
magneto
wollaston prism
optical system
light
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.)
Withdrawn
Application number
JP3302478A
Other languages
Japanese (ja)
Inventor
Kenji Fukui
健司 福井
Hiroyuki Wada
博之 和田
Musashirikarudo Okamoto
武蔵リカルド 岡本
Shohei Hashiguchi
昇平 橋口
Tadashi Takeda
正 武田
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel 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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP3302478A priority Critical patent/JPH05114193A/en
Publication of JPH05114193A publication Critical patent/JPH05114193A/en
Withdrawn legal-status Critical Current

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Abstract

PURPOSE:To provide a photomagnetic detector where the structure of an enclosure and the position adjustment of parts are simplified and the number of parts is reduced. CONSTITUTION:Optical axes of respective crystal of two optical uniaxial crystal members 10a, 10b constituting a Wollaston prism 10 are made orthogonal to each other when viewed from an optical axis A of a photomagnetic detection optical system 100, and the normal direction of a joint surface 10c is inclined at 45 deg. to irradiated laser light, and a fixed face 10d of the Wollaston prism is formed into a plane. Thus, the number of parts of the photomagnetic detector is reduced, and the enclosure structure is simplified and parts are easily adjusted because the Wollaston prism is only stuck to the flat enclosure to complete attachment at the time of fixing various optical parts to the optical head enclosure.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は光磁気記録再生装置の光
ヘッドなどに用いられる光磁気検出装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical detector used for an optical head of a magneto-optical recording / reproducing apparatus.

【0002】[0002]

【従来の技術】従来、コンパクトディスクやレーザディ
スクのように半導体レーザにより記録媒体上に記録され
た情報を読み取る装置がある。また、再生ばかりでな
く、一度だけ記録可能な記録媒体や何度でも記録再生可
能な記録媒体もあり、何度でも記録再生可能な記録媒体
として光磁気記録媒体がある。
2. Description of the Related Art Conventionally, there is an apparatus for reading information recorded on a recording medium by a semiconductor laser such as a compact disc or a laser disc. Further, not only reproduction but also a recording medium capable of recording only once and a recording medium capable of recording / reproducing many times are available, and a magneto-optical recording medium is a recording medium capable of recording / reproducing many times.

【0003】光磁気記録媒体にあっては、媒体に偏光し
たレーザ光を照射すると光磁気記録媒体上での磁化の向
きにより偏光方向が変化する磁気光学効果(カー効果)
を利用して光磁気記録媒体上に記録された情報を検出す
る光磁気記録再生装置が実用化されている。
In a magneto-optical recording medium, the polarization direction changes depending on the direction of magnetization on the magneto-optical recording medium when the medium is irradiated with polarized laser light. Magneto-optical effect (Kerr effect).
A magneto-optical recording / reproducing apparatus for detecting information recorded on a magneto-optical recording medium by utilizing the has been put into practical use.

【0004】このような光ヘッドの光磁気記録再生装置
の光学系の一例を図2に示す。半導体レーザ1から放射
された偏光光はコリメートレンズ2と対物レンズ4で構
成されたレーザ照射光学系100により光磁気記録媒体
5に照射される。光磁気記録媒体5からの反射光は、光
磁気記録媒体5上の記録ビットに応じた磁化の影響を受
け磁気光学効果により偏光方向が変調される。変調を受
けた偏光光はビームスプリッタ3により光磁気検出光学
系200へ導かれる。この光磁気検出光学系200は、
偏光方向を90度回転させるλ/2板6と、ウォーラス
トンプリズム7と、集光レンズ8と、二分割光検出器9
とから構成される。また、これを改良しλ/2板6を不
要とした光ヘッドが特開平2−113458号公報に記
載されている。この構造は図3に示すように、ウォーラ
ストンプリズム7を光軸を中心に45度回転させて配置
することにより、λ/2板を省略したものである。
An example of the optical system of the magneto-optical recording / reproducing apparatus of such an optical head is shown in FIG. The polarized light emitted from the semiconductor laser 1 is applied to the magneto-optical recording medium 5 by a laser irradiation optical system 100 including a collimator lens 2 and an objective lens 4. The reflected light from the magneto-optical recording medium 5 is influenced by the magnetization depending on the recording bit on the magneto-optical recording medium 5, and the polarization direction is modulated by the magneto-optical effect. The modulated polarized light is guided to the magneto-optical detection optical system 200 by the beam splitter 3. This magneto-optical detection optical system 200
A λ / 2 plate 6 for rotating the polarization direction by 90 degrees, a Wollaston prism 7, a condenser lens 8, and a two-part photodetector 9
Composed of and. Further, an optical head which is an improvement of this and eliminates the need for the λ / 2 plate 6 is described in Japanese Patent Application Laid-Open No. 2-113458. In this structure, as shown in FIG. 3, the Wollaston prism 7 is arranged so as to be rotated by 45 degrees about the optical axis, and the λ / 2 plate is omitted.

【0005】[0005]

【発明が解決しようとする課題】しかしながら上述の構
造にあっては、プリズムを光軸を中心に回転させる必要
があるため、光学系部品を保持する筐体構造及び各部品
の位置調整が複雑になる問題があった。
However, in the above-mentioned structure, since it is necessary to rotate the prism around the optical axis, the structure of the housing for holding the optical system parts and the position adjustment of each part are complicated. There was a problem.

【0006】上述したような従来技術の問題点に鑑み、
本発明の目的とするところは、筐体の構造及び部品の位
置調整が簡単であり、かつ部品点数も削減された光磁気
検出装置を提供することにある。
In view of the above-mentioned problems of the prior art,
An object of the present invention is to provide a magneto-optical detecting device in which the structure of the housing and the position of the parts are easily adjusted and the number of parts is reduced.

【0007】[0007]

【課題を解決するための手段】上記目的は、レーザ光源
及びレーザ光を光磁気記録媒体に照射する対物レンズか
ら構成されたレーザ照射光学系と、前記光磁気記録媒体
からの反射光を電気信号に変換するための光磁気検出光
学系とを有する光ヘッドの光磁気検出装置に於て、前記
光磁気検出光学系は、前記光磁気記録媒体からの反射光
を該光磁気検出光学系に導くためのビームスプリッタ
と、導かれた前記反射光の偏光方向に応じて第1の光束
及び第2の光束に分割するための第1及び第2の光学的
一軸性結晶部材を有するウォーラストンプリズムと、前
記第1の光束及び第2の光束を電気信号に変換する2分
割光検出器とを具備し、前記第1及び第2の光学的一軸
性結晶部材は、その結晶の光学軸同士が前記光磁気検出
光学系の光軸方向から見て互いに直交するように接合さ
れ、前記ウォーラストンプリズムは、前記各光学的一軸
性結晶部材の結晶の光学軸が前記レーザ照射光学系の前
記レーザ光の偏光方向に対して略45度傾くと共に前記
両光学的一軸性結晶部材の接合面の法線方向が前記光磁
気検出光学系の光軸方向から見て前記レーザ照射光学系
の前記レーザ光の偏光方向に対して略45度傾くように
配置され、かつ前記ウォーラストンプリズムの当該光磁
気検出装置に対する固定面が平面状をなすことを特徴と
する光ヘッドの光磁気検出装置を提供することにより達
成される。
The above object is to provide a laser irradiation optical system comprising a laser light source and an objective lens for irradiating a magneto-optical recording medium with a laser beam, and an electric signal for reflecting light from the magneto-optical recording medium. In a magneto-optical detection device for an optical head having a magneto-optical detection optical system for converting into a magneto-optical recording medium, the magneto-optical detection optical system guides reflected light from the magneto-optical recording medium to the magneto-optical detection optical system. Beam splitter, and a Wollaston prism having first and second optical uniaxial crystal members for splitting into a first light flux and a second light flux according to the polarization direction of the reflected light guided. A two-segment photodetector for converting the first light flux and the second light flux into an electric signal, wherein the first and second optical uniaxial crystal members have optical axes of the crystals which are the same as each other. Is it the direction of the optical axis of the magneto-optical detection optical system? The Wollaston prisms are joined so as to be orthogonal to each other when viewed, and the optical axis of the crystal of each of the optically uniaxial crystal members is inclined by about 45 degrees with respect to the polarization direction of the laser light of the laser irradiation optical system. The normal line direction of the joint surface of the both optically uniaxial crystal members is inclined by approximately 45 degrees with respect to the polarization direction of the laser light of the laser irradiation optical system when viewed from the optical axis direction of the magneto-optical detection optical system. The present invention is achieved by providing a magneto-optical detecting device for an optical head, characterized in that the fixed surface of the Wollaston prism with respect to the magneto-optical detecting device is planar.

【0008】[0008]

【作用】光磁気検出光学系の光軸から見てウォーラスト
ンプリズムを構成する2つの光学的一軸性結晶部材のそ
れぞれの結晶の光学軸を直交させ、その接合面の法線方
向を照射レーザ光に対し略45度傾け、ウォーラストン
プリズムの固定面を平面に形成することにより、λ/2
板を省略でき、光ヘッド筐体に各種光学部品を固定する
際に、平らな筐体にウォーラストンプリズムを貼り合わ
せるだけで取り付けが完了する。
Operation: The optical axes of the respective crystals of the two optically uniaxial crystal members constituting the Wollaston prism as viewed from the optical axis of the magneto-optical detection optical system are made orthogonal to each other, and the normal direction of the joint surface is irradiated with laser light. Approximately 45 degrees with respect to, and forming the fixing surface of the Wollaston prism into a flat surface,
The plate can be omitted, and when fixing various optical components to the optical head casing, the attachment is completed simply by attaching the Wollaston prism to the flat casing.

【0009】[0009]

【実施例】以下、本発明の実施例を図面を用いて説明す
る。
Embodiments of the present invention will be described below with reference to the drawings.

【0010】図1は、本発明の実施例を示す斜視図であ
る。図1の光ヘッドの光磁気検出装置は半導体レーザ1
から放射された偏光光はコリメートレンズ2と対物レン
ズ4で構成されたレーザ照射光学系100により光磁気
記録媒体5に照射される。
FIG. 1 is a perspective view showing an embodiment of the present invention. The magneto-optical detection device for the optical head shown in FIG.
The polarized light emitted from the laser irradiation optical system 100 including the collimator lens 2 and the objective lens 4 is applied to the magneto-optical recording medium 5.

【0011】レーザ照射光学系100により光磁気記録
媒体5に照射されるレーザ光はp偏光光となっており、
その反射光は磁気光学効果により光磁気記録媒体5に記
録された記録ビットの磁化方向に応じて偏光方向pを中
心に±θkだけ変調される。変調を受けた反射光はビー
ムスプリッタ3により光磁気検出光学系200へ導かれ
る。
The laser light applied to the magneto-optical recording medium 5 by the laser irradiation optical system 100 is p-polarized light,
Due to the magneto-optical effect, the reflected light is modulated by ± θk around the polarization direction p according to the magnetization direction of the recording bit recorded on the magneto-optical recording medium 5. The reflected light that has been modulated is guided to the magneto-optical detection optical system 200 by the beam splitter 3.

【0012】光磁気検出光学系200に導かれた反射光
はウォーラストンプリズム10に入射する。このウォー
ラストンプリズム10は図4に示すように第1の光学的
一軸性結晶部材10aと第2の光学的一軸性結晶部材1
0bとが接合面10cで貼り合わされたものからなる。
The reflected light guided to the magneto-optical detection optical system 200 enters the Wollaston prism 10. This Wollaston prism 10 includes a first optical uniaxial crystal member 10a and a second optical uniaxial crystal member 1 as shown in FIG.
0b and 0b are bonded together at the joint surface 10c.

【0013】ここで、ウォーラストンプリズム10は図
4に示すように、図5に示すように光磁気検出光学系2
00の光軸A方向から見て、各光学的一軸性結晶部材の
光学軸の向きは互いに直交している。また、光磁気検出
光学系200の光軸A方向から見て、接合面10cの法
線方向Nがレーザ照射光学系100のレーザ光の偏光方
向pに対して光軸Aを中心に45度傾いた位置となるよ
うに、第1の光学的一軸性結晶部材10aと第2の光学
的一軸性結晶部材10bとが成形されている。更に、ウ
ォーラストンプリズム10の不図示の光磁気検出光学系
200筐体に対する固定面10dは平面状をなすように
形成されている。
The Wollaston prism 10 has a magneto-optical detecting optical system 2 as shown in FIG. 4 and as shown in FIG.
The optical axes of the optically uniaxial crystal members are orthogonal to each other when viewed from the optical axis A direction of 00. Further, when viewed from the direction of the optical axis A of the magneto-optical detection optical system 200, the normal direction N of the joint surface 10c is inclined by 45 degrees about the optical axis A with respect to the polarization direction p of the laser light of the laser irradiation optical system 100. The first optical uniaxial crystal member 10a and the second optical uniaxial crystal member 10b are molded so as to be located at different positions. Further, the fixing surface 10d of the Wollaston prism 10 with respect to the casing of the magneto-optical detection optical system 200 (not shown) is formed to have a planar shape.

【0014】ビームスプリッタ3を介してウォーラスト
ンプリズム10に入射した、偏光方向pを中心に±θk
だけ変調された反射光は、偏光方向に応じて第1の光束
及び第2の光束に分割される。分割されたそれぞれの光
束は二分割光検出器9の2つの受光素子9a、9b上に
凸レンズ8により集光し、電気信号に変換される。そし
て、この二分割光検出器9の2つの受光素子9a、9b
の差動出力が光磁気信号として検出される。
The incident light on the Wollaston prism 10 through the beam splitter 3 is ± θk centered on the polarization direction p.
The reflected light that is modulated only is split into a first light flux and a second light flux according to the polarization direction. The respective divided light beams are condensed by the convex lens 8 on the two light receiving elements 9a and 9b of the two-divided photodetector 9 and converted into electric signals. Then, the two light receiving elements 9a, 9b of the two-divided photodetector 9 are
Is detected as a magneto-optical signal.

【0015】尚、図5で示されるようにウォーラストン
プリズム10を構成する稜、即ち幅と、高さと、奥行と
の比率を略1対1対1.414とすれば、奥行を最も短
くできるがこれに限定するものではない。
As shown in FIG. 5, if the ratio of the ridges that form the Wollaston prism 10, that is, the width, the height, and the depth is approximately 1: 1: 1.414, the depth can be minimized. However, it is not limited to this.

【0016】組み立てられた状態のウォーラストンプリ
ズム10は凸レンズ8の中心軸が合うように不図示の筐
体に固定するのみで良く、高い位置精度を必要としな
い。また筐体構造が簡単になると共に光軸合わせの調整
作業が容易になる。
The assembled Wollaston prism 10 need only be fixed to a housing (not shown) so that the central axes of the convex lenses 8 are aligned, and high positional accuracy is not required. In addition, the structure of the housing becomes simple and the adjustment work of the optical axis alignment becomes easy.

【0017】[0017]

【発明の効果】以上のように本発明の光磁気検出装置に
よれば、光磁気検出光学系の光軸から見てウォーラスト
ンプリズムを構成する2つの光学的一軸性結晶部材のそ
れぞれの結晶の光学軸を直交させ、その接合面の法線方
向を照射レーザ光に対し略45度傾け、ウォーラストン
プリズムの固定面を平面に形成することにより、光磁気
検出装置の部品点数が少なくなると共に、光ヘッド筐体
に各種光学部品を固定する際に平らな筐体にウォーラス
トンプリズムを貼り合わせるだけで取り付けが完了し、
筐体構造が簡単になると共に部品調整が容易になる。
As described above, according to the magneto-optical detecting apparatus of the present invention, the crystals of the two optical uniaxial crystal members constituting the Wollaston prism as viewed from the optical axis of the magneto-optical detecting optical system are formed. By making the optical axes orthogonal to each other and inclining the normal direction of the joining surface to the irradiation laser beam by about 45 degrees and forming the fixing surface of the Wollaston prism on a flat surface, the number of parts of the magneto-optical detection device is reduced, and When fixing various optical parts to the optical head housing, simply attach the Wollaston prism to the flat housing to complete the installation.
The case structure becomes simple and the parts adjustment becomes easy.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例の光磁気検出装置を示す斜視図
である。
FIG. 1 is a perspective view showing a magneto-optical detector according to an embodiment of the present invention.

【図2】従来の実施例の光磁気検出装置を示す斜視図で
ある。
FIG. 2 is a perspective view showing a magneto-optical detector of a conventional example.

【図3】従来の実施例の光磁気検出装置を示す斜視図で
ある。
FIG. 3 is a perspective view showing a conventional magneto-optical detector.

【図4】本発明の実施例に於ける光磁気検出装置に使用
するウォーラストンプリズムの構造を示す斜視図であ
る。
FIG. 4 is a perspective view showing the structure of a Wollaston prism used in the magneto-optical detecting device according to the embodiment of the invention.

【図5】図4のウォーラストンプリズムの光軸の構造を
示すちA方向について見た矢視図である。
5 is a view showing the structure of the optical axis of the Wollaston prism of FIG. 4 and is an arrow view seen in the A direction.

【符号の説明】[Explanation of symbols]

1 半導体レーザ 2 コリメートレンズ 3 ビームスプリッタ 4 対物レンズ 6 λ/2板 7 ウォーラストンプリズム 8 凸レンズ 9 2分割光検出器 10 ウォーラストンプリズム 10a 第1の光学的一軸性結晶部材 10b 第2の光学的一軸性結晶部材 10c 接合面 10d 固定面 1 Semiconductor Laser 2 Collimating Lens 3 Beam Splitter 4 Objective Lens 6 λ / 2 Plate 7 Wollaston Prism 8 Convex Lens 9 Two-Division Photo Detector 10 Wollaston Prism 10a First Optical Uniaxial Crystal Member 10b Second Optical Uniaxial Crystal member 10c Bonding surface 10d Fixed surface

───────────────────────────────────────────────────── フロントページの続き (72)発明者 橋口 昇平 相模原市淵野辺5丁目10番1号 新日本製 鐵株式会社エレクトロニクス研究所内 (72)発明者 武田 正 長野県諏訪郡下諏訪町5329番地 株式会社 三協精機製作所下諏訪工場内 ─────────────────────────────────────────────────── ─── Continued front page (72) Inventor Shohei Hashiguchi 5-10-1, Fuchinobe, Sagamihara-shi Nippon Steel Corporation Electronics Research Laboratory (72) Inventor Tadashi Takeda 5329 Shimosuwa-cho, Suwa-gun, Nagano Prefecture San Co., Ltd. Kyoseiki Seisakusho Shimosuwa factory

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 レーザ光源及びレーザ光を光磁気記録
媒体に照射する対物レンズから構成されたレーザ照射光
学系と、前記光磁気記録媒体からの反射光を電気信号に
変換するための光磁気検出光学系とを有する光ヘッドの
光磁気検出装置に於て、 前記光磁気検出光学系は、前記光磁気記録媒体からの反
射光を該光磁気検出光学系に導くためのビームスプリッ
タと、導かれた前記反射光の偏光方向に応じて第1の光
束及び第2の光束に分割するための第1及び第2の光学
的一軸性結晶部材を有するウォーラストンプリズムと、
前記第1の光束及び第2の光束を電気信号に変換する2
分割光検出器とを具備し、 前記第1及び第2の光学的一軸性結晶部材は、その結晶
の光学軸同士が前記光磁気検出光学系の光軸方向から見
て互いに直交するように接合され、 前記ウォーラストンプリズムは、前記各光学的一軸性結
晶部材の結晶の光学軸が前記レーザ照射光学系の前記レ
ーザ光の偏光方向に対して略45度傾くと共に前記両光
学的一軸性結晶部材の接合面の法線方向が前記光磁気検
出光学系の光軸方向から見て前記レーザ照射光学系の前
記レーザ光の偏光方向に対して略45度傾くように配置
され、かつ前記ウォーラストンプリズムの当該光磁気検
出装置に対する固定面が平面状をなすことを特徴とする
光ヘッドの光磁気検出装置。
1. A laser irradiation optical system comprising a laser light source and an objective lens for irradiating a magneto-optical recording medium with a laser beam, and a magneto-optical detection for converting reflected light from the magneto-optical recording medium into an electric signal. In a magneto-optical detection device for an optical head having an optical system, the magneto-optical detection optical system includes a beam splitter for guiding reflected light from the magneto-optical recording medium to the magneto-optical detection optical system. And a Wollaston prism having first and second optical uniaxial crystal members for splitting into a first light flux and a second light flux according to the polarization direction of the reflected light,
2 for converting the first light flux and the second light flux into electric signals
A split photodetector, and the first and second optical uniaxial crystal members are bonded so that the optical axes of the crystals are orthogonal to each other when viewed from the optical axis direction of the magneto-optical detection optical system. In the Wollaston prism, the optical axis of the crystal of each of the optically uniaxial crystal members is tilted by about 45 degrees with respect to the polarization direction of the laser light of the laser irradiation optical system, and the both optical uniaxial crystal members are provided. Is arranged so that the normal line direction of the joining surface of the optical disc is tilted by approximately 45 degrees with respect to the polarization direction of the laser light of the laser irradiation optical system when viewed from the optical axis direction of the magneto-optical detection optical system, and the Wollaston prism 2. A magneto-optical detecting device for an optical head, wherein a fixing surface of the magneto-optical detecting device is planar.
【請求項2】 前記ウォーラストンプリズムは、前記
ウォーラストンプリズムを構成する稜、即ち幅、高さ、
奥行の比率が略1対1対1.414となっていることを
特徴とする請求項1に記載の光ヘッドの光磁気検出装
置。
2. The Wollaston prism has ridges, that is, width, height,
The magneto-optical detection device for an optical head according to claim 1, wherein the depth ratio is approximately 1: 1: 1.414.
JP3302478A 1991-10-22 1991-10-22 Photomagnetic detector for optical head Withdrawn JPH05114193A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3302478A JPH05114193A (en) 1991-10-22 1991-10-22 Photomagnetic detector for optical head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3302478A JPH05114193A (en) 1991-10-22 1991-10-22 Photomagnetic detector for optical head

Publications (1)

Publication Number Publication Date
JPH05114193A true JPH05114193A (en) 1993-05-07

Family

ID=17909436

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3302478A Withdrawn JPH05114193A (en) 1991-10-22 1991-10-22 Photomagnetic detector for optical head

Country Status (1)

Country Link
JP (1) JPH05114193A (en)

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Effective date: 19990107