JPH0810854Y2 - Magneto-optical recording medium reproducing device - Google Patents
Magneto-optical recording medium reproducing deviceInfo
- Publication number
- JPH0810854Y2 JPH0810854Y2 JP7080786U JP7080786U JPH0810854Y2 JP H0810854 Y2 JPH0810854 Y2 JP H0810854Y2 JP 7080786 U JP7080786 U JP 7080786U JP 7080786 U JP7080786 U JP 7080786U JP H0810854 Y2 JPH0810854 Y2 JP H0810854Y2
- Authority
- JP
- Japan
- Prior art keywords
- light
- magneto
- deflection
- optical
- recording medium
- 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.)
- Expired - Lifetime
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/1055—Disposition or mounting of transducers relative to record carriers
- G11B11/10576—Disposition or mounting of transducers relative to record carriers with provision for moving the transducers for maintaining alignment or spacing relative to the carrier
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/10—Beam splitting or combining systems
- G02B27/16—Beam splitting or combining systems used as aids for focusing
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
- G11B11/10532—Heads
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Recording Or Reproduction (AREA)
- Optical Head (AREA)
- Mechanical Optical Scanning Systems (AREA)
Description
【考案の詳細な説明】 「産業上の利用分野」 本考案は光磁気記録再生装置において、再生情報信号
と自動焦点制御信号とを得るようにした光学系構造に関
する。DETAILED DESCRIPTION OF THE INVENTION "Industrial application field" The present invention relates to an optical system structure for obtaining a reproduction information signal and an automatic focus control signal in a magneto-optical recording / reproducing apparatus.
「従来の技術」 従来の、この種の光学系構造例として第4図に示すよ
うなものがあった。図面において、1はレーザ光を発生
するレーザダイオード等のレーザ光源で、2はこのレー
ザ光源1の光束を平行光束とするためのコリメータ、3
は往路と復路の光束を分離するためのハーフミラー、4
は情報を垂直方向の磁化により記録する光磁気ディス
ク、5は該光磁気ディスク4の記録面上に光点を結ばせ
るための対物レンズ、6は偏光面の方位を変更するため
の1/2波長板、7は偏光を検出するための検光子、8Aと8
Bはレンズ、9は自動焦点の制御(誤差)信号を得るた
めの非点収差を発生させるシリンドリカルレンズ、10
A、10Bは記録情報検出のためのディテクタであり、ディ
テクタ10Bではフォーカスエラー信号の検出も行なって
いる。11、12は差動アンプである。"Prior Art" As an example of a conventional optical system structure of this type, there is one as shown in FIG. In the drawings, 1 is a laser light source such as a laser diode for generating a laser beam, 2 is a collimator for collimating the light flux of the laser light source 1, and 3 is a collimator.
Is a half mirror for separating the forward and return light beams, 4
Is a magneto-optical disk for recording information by perpendicular magnetization, 5 is an objective lens for forming a light spot on the recording surface of the magneto-optical disk 4, and 6 is 1/2 for changing the direction of the polarization plane. Wave plate, 7 is an analyzer for detecting polarized light, 8A and 8
B is a lens, 9 is a cylindrical lens that generates astigmatism for obtaining an autofocus control (error) signal, and 10
A and 10B are detectors for detecting recorded information, and the detector 10B also detects a focus error signal. 11 and 12 are differential amplifiers.
次に、動作について説明する。レーザ光源1で発生し
たレーザ光は、コリメータ2により平行光束となり、ハ
ーフミラー3を介し対物レンズ4により光磁気ディスク
4の記録面上に光点を結ばせる。一方、光磁気ディスク
4の記録面上で反射した光束は、ミラー3によって分離
され、1/2波長板6により検光子7の入射面に対し45°
方位となるよう偏光面回転を受ける。ここで、光磁気デ
ィスク4に記録された情報信号は、磁化方向が正逆反転
した形で記録されているため、カー効果により偏光面が
微少角回転するから、検光子7を通過する通過光と反射
光は光の強弱変動を受ける。この光の強弱変動が各々の
ディテクタ10A、10Bにより電気信号に変換され、両ディ
テクタ10A、10Bの差信号が差動アンプ11により生成され
て再生情報信号Sとなる。Next, the operation will be described. The laser light generated by the laser light source 1 becomes a parallel light flux by the collimator 2, and the objective lens 4 through the half mirror 3 forms a light spot on the recording surface of the magneto-optical disk 4. On the other hand, the light flux reflected on the recording surface of the magneto-optical disk 4 is separated by the mirror 3 and is 45 ° with respect to the incident surface of the analyzer 7 by the half-wave plate 6.
The plane of polarization is rotated so that it becomes azimuth. Here, since the information signal recorded on the magneto-optical disk 4 is recorded in the form in which the magnetization directions are reversed in normal and reverse directions, the plane of polarization is rotated by a slight angle due to the Kerr effect, so that the passing light passing through the analyzer 7 is transmitted. And the reflected light is subject to fluctuations in light intensity. The intensity fluctuations of the light are converted into electric signals by the respective detectors 10A and 10B, and the difference signal between the two detectors 10A and 10B is generated by the differential amplifier 11 and becomes the reproduction information signal S.
一方、シリンドリカルレンズ9により、非点収差を与
えられた光束の形状変化は、複数の受光素子で構成され
たディテクタ10Bにより電気信号に変換され、その差信
号が差動アンプ12で生成され、フォーカスエラー信号Sf
となる。On the other hand, the shape change of the light flux given astigmatism by the cylindrical lens 9 is converted into an electric signal by the detector 10B composed of a plurality of light receiving elements, and the difference signal is generated by the differential amplifier 12 to focus the light. Error signal Sf
Becomes
「考案が解決しようとする問題点」 従来の光磁気記録再生装置の光学系構造は、以上のよ
うに部品点数が多く、構成が複雑化するので、小型化で
きず、コストも高くなるという欠点があった。"Problems to be solved by the device" As described above, the conventional optical system structure of the magneto-optical recording / reproducing apparatus has a large number of parts and complicates the configuration, so that it cannot be downsized and the cost is high. was there.
本考案は、上記のような欠点を解決するために成され
たもので、装置を構成する各構成機能素子を集約化する
ことにより、単純な構成の光磁気記録再生装置の光学系
構造を提供するのが目的である。The present invention has been made to solve the above-mentioned drawbacks, and provides an optical system structure of a magneto-optical recording / reproducing apparatus having a simple structure by consolidating the functional elements constituting the apparatus. The purpose is to do.
「問題点を解決するための手段」 本考案は、上記のような欠点を解決する手段として、
次のように構成したものである。"Means for Solving Problems" The present invention provides means for solving the above-mentioned drawbacks.
It is configured as follows.
即ち、磁気光学的に信号を読取る光磁気再生装置にお
いて、光を放射する光源と、前記光源からの光を収束さ
せるレンズと、磁気記録媒体で反射され且つ前記レンズ
を通過した光をS偏向及びP偏向に分離すると共に、分
離された前記S偏向及びP偏向のうちいずれか一方に非
点収差を持たせる光学手段とを備え、前記光学手段は、
入射光に対して傾斜する第1の面と、該第1の面を通過
した光を更に通過させて前記光学手段の外部に導く第2
の面と、前記第1の面に施された偏向膜とを含み、前記
第1の面が前記偏向膜によって分離されたS偏向及びP
偏向のうち一方を反射し他方を通過させ、前記通過光を
用いてフォーカスエラー検出を行うようにしたものであ
る。That is, in a magneto-optical reproducing device that reads a signal magneto-optically, a light source that emits light, a lens that converges the light from the light source, and a light that is reflected by a magnetic recording medium and that has passed through the lens are S-polarized and Optical means for separating into P-deflection and for imparting astigmatism to one of the separated S-deflection and P-deflection, wherein the optical means comprises:
A first surface that is inclined with respect to the incident light; and a second surface that further transmits the light that has passed through the first surface and guides it to the outside of the optical means.
Surface and a deflecting film applied to the first surface, the first surface being separated by the deflecting film.
One of the deflections is reflected and the other is passed, and the focus light is detected using the passing light.
なお、上記の構成では、光源からの光をS偏向及びP
偏向の光に分離しその一方を非点収差を持たせる手段を
通過されるようにしてあるが、上記のレーザ光源の偏向
方向と、記録トラックとの方向とが平行もしくは直交状
態にあり、非点収差発生検光子の子午面及び入射面が上
記の偏向及びトラックの各方向に対しほぼ45°の方向に
配向されているように構成してもよい。In the above configuration, the light from the light source is S-polarized and P-polarized.
The polarized light is separated and passed through a means for imparting astigmatism to one of them, but the direction of deflection of the laser light source and the direction of the recording track are parallel or orthogonal to each other. The meridional surface and the incident surface of the point aberration generating analyzer may be oriented in a direction of approximately 45 ° with respect to the above-mentioned deflection and track directions.
すなわち、後述する第1図においてはレンズの前に1/
2波長板を配置して構成してあるが、後述する第2図に
示すように、1/2波長板を省略して、レーザ光源の偏向
方向とトラック方向とが非点収差発生検光子の入射面を
第2図紙面に対し45°に形成することにより、偏向面方
位と検光子入射面方位とが45°となり、光強度変動性ノ
イズが同相、同振幅となり、作動アンプで作動相殺され
ることとなる。That is, in FIG. 1 described later, 1 /
Although it is configured by arranging two wavelength plates, as shown in FIG. 2 described later, the half wavelength plate is omitted and the deflection direction of the laser light source and the track direction are astigmatism generating analyzers. By forming the incident surface at 45 ° with respect to the paper surface of Fig. 2, the deflection surface direction and the analyzer incident surface direction become 45 °, and the light intensity fluctuation noise becomes the same phase and the same amplitude, and the operation amplifier cancels it out. The Rukoto.
「実施例の構成」 以下、本考案を図面の実施例に基づいて説明する。第
1図は本考案に係る光磁気記録再生装置の光学系構造の
概略構成図である。Hereinafter, the present invention will be described with reference to the drawings. FIG. 1 is a schematic configuration diagram of an optical system structure of a magneto-optical recording / reproducing apparatus according to the present invention.
上記の図面において、21はレーザ光を発生するレーザ
ダイオード等のレーザ光源で、22はこのレーザ光源21の
光束を平行光束とするためのコリメータ、23は往路と復
路の光束を分離するためのハーフミラー、24は情報を垂
直方向の磁化により記録する光磁気ディスク、25は該光
磁気ディスク24の記録面上に交点を結ばせるための対物
レンズ、26は偏光面の方位を変更するための1/2波長
板、27はレンズである。In the above drawings, 21 is a laser light source such as a laser diode for generating a laser beam, 22 is a collimator for making the light flux of this laser light source 21 a parallel light flux, and 23 is a half for separating the forward and return light fluxes. A mirror, 24 is a magneto-optical disk for recording information by perpendicular magnetization, 25 is an objective lens for forming an intersection on the recording surface of the magneto-optical disk 24, and 26 is 1 for changing the direction of the polarization plane. / 2 wave plate, 27 is a lens.
28は自動焦点の制御(誤差)信号を非点収差効果で得
るための非点収差発生機能と、磁気光学的信号を検出す
るための検光子機能とを有する非点収差発生検光子で、
図面では両面平行板の片面に偏光膜を施したものであ
り、偏光ビームスプリッタと同様にP偏光成分はほぼ10
0%透過し、S偏光成分はほぼ100%反射するものであ
る。29A、29Bは記録情報検出のためのディテクタであ
り、ディテクタ29Bではフォーカスエラー信号の検出も
行なっている。30、31は差動アンプである。28 is an astigmatism generation analyzer having an astigmatism generation function for obtaining an autofocus control (error) signal by an astigmatism effect and an analyzer function for detecting a magneto-optical signal,
In the drawing, a polarizing film is applied to one side of a double-sided parallel plate, and the P-polarized component is almost 10 as in the polarization beam splitter.
It transmits 0% and reflects almost 100% of the S-polarized component. 29A and 29B are detectors for detecting recorded information, and the detector 29B also detects a focus error signal. Reference numerals 30 and 31 are differential amplifiers.
「実施例の作用」 次に、上記の実施例の作用について説明する。Next, the operation of the above embodiment will be described.
レーザ光源21で発生したレーザ光は、コリメータ22に
より平行光束となり、ハーフミラー23を介して対物レン
ズ25により光磁気ディスク24の記録面上に光点を結ばせ
る。また、光磁気ディスク24の記録面上で反射した光束
は、ミラー23によって分離され、1/2波長板26により非
点収差発生検光子28の入射面に対し45°方位となるよう
偏光面回転を受ける。ここで、光磁気ディスク24に記録
された情報信号は、磁化方向が正逆反転の形で記録され
ているため、カー効果により偏光面が微小角回転するか
ら、非点収差発生検光子28を通過する透過光(P偏光成
分)と反射光(S偏光成分)は光強弱変動を受け、磁化
の向きに応じた記録情報信号がディテクタ29A、29Bから
出力される。そして、上記の透過光と反射光の光強度変
化は、当然互いに逆相となっているので、ディテクタ29
A、29Bから出力される記録情報信号の差信号が差動アン
プ30に印加され再生情報信号Sとなる。The laser light generated by the laser light source 21 becomes a parallel light flux by the collimator 22, and the light spot is formed on the recording surface of the magneto-optical disk 24 by the objective lens 25 via the half mirror 23. Further, the light flux reflected on the recording surface of the magneto-optical disk 24 is separated by the mirror 23, and the polarization plane is rotated by the half-wave plate 26 so as to have a 45 ° azimuth with respect to the incident surface of the astigmatism generating analyzer 28. Receive. Here, since the information signal recorded on the magneto-optical disk 24 is recorded in a form in which the magnetization directions are forward / reverse inversion, the plane of polarization is rotated by a small angle due to the Kerr effect. The transmitted light (P-polarized component) and reflected light (S-polarized component) that pass through are subject to light intensity fluctuations, and the recording information signals corresponding to the direction of magnetization are output from the detectors 29A and 29B. The changes in the light intensities of the transmitted light and the reflected light are naturally opposite to each other, so the detector 29
The difference signal of the recording information signals output from A and 29B is applied to the differential amplifier 30 and becomes the reproduction information signal S.
一方、非点収差発生検光子28を通過した透過光は、フ
ォーカスエラーの検出に好適な非点収差を与えられ、デ
ィテクタ29Bにより記録情報信号とともに出力され、こ
の出力は差動アンプ31に印加されてフォーカスエラー信
号Sfが生成される。On the other hand, the transmitted light that has passed through the astigmatism generation analyzer 28 is given astigmatism suitable for detection of focus error, and is output together with the recording information signal by the detector 29B, and this output is applied to the differential amplifier 31. The focus error signal Sf is generated.
なお、上記の再生情報信号Sは一方のディテクタ29A
からの出力でも同様に得られるので、ディテクタ29Bは
必要不可欠の素子ということではない。It should be noted that the reproduction information signal S described above is generated by one detector 29A.
The detector 29B is not an indispensable element because the output from the same can be obtained in the same manner.
「他の実施例」 なお、上記の実施例では、レンズ27の前に1/2波長板2
6を配置したが、第2図で示すように構成すれば、1/2波
長板26を省略することができる。即ち、矢印Eで示すレ
ーザ光源1の偏光方向と矢印Tで示すトラック方向と
が、例えば、図面においてはともに紙面内にあり、非点
収差発生検光子28の入射面を紙面に対し45°とすること
により、1/2波長板26なしで、良好な情報再生信号Sが
得られると共に、トラック横切りノイズの少ないフォー
カスエラー信号Sfが得られる。Other Examples In the above example, the half-wave plate 2 is placed in front of the lens 27.
Although 6 is arranged, the half-wave plate 26 can be omitted if configured as shown in FIG. That is, the polarization direction of the laser light source 1 indicated by the arrow E and the track direction indicated by the arrow T are both within the plane of the drawing, for example, and the incident surface of the astigmatism generation analyzer 28 is 45 ° with respect to the plane of the paper. By doing so, a good information reproduction signal S can be obtained without the half-wave plate 26, and a focus error signal Sf with less track crossing noise can be obtained.
これは偏光面方位と検光子入射面方位とが45°となる
ことで、光強度変動性ノイズが同相、同振幅となるた
め、差動アンプ30で差動相殺されることと、トラックに
より発生する回折光パターンの対称軸が、ディテクタ29
Bの受光面分割線の1つと一致するため、トラック横切
りノイズが少なくなることによる。This is because the polarization plane azimuth and the analyzer entrance plane azimuth are 45 °, so that the light intensity fluctuation noise has the same phase and the same amplitude, so the differential amplifier 30 differentially cancels it and the track is generated. The symmetry axis of the diffracted light pattern
This is because the track crossing noise is reduced because it coincides with one of the light receiving surface dividing lines of B.
なお、図面では差動アンプ30、31は省略されている。 The differential amplifiers 30 and 31 are omitted in the drawing.
また、上記の実施例では、非点収差発生検光子28とし
て、両面平行平板を用いたが、その他種々の形状が考え
られ、その例を第3図(イ),(ロ)に示す。Further, in the above-mentioned embodiment, the double-sided parallel flat plate is used as the astigmatism generation analyzer 28, but other various shapes are conceivable, examples of which are shown in FIGS. 3 (a) and 3 (b).
まず、同図の(イ)はウエッジ基板32の一面に偏光膜
33を形成したものであり、同図の(ロ)は屈折率の異な
る基材n1≠n2を接合して形成した立方体形状の偏光ビー
ムスプリッタであり、上記の実施例と同様の効果を奏す
る。First, (a) in the figure shows a polarizing film on one surface of the wedge substrate 32.
33 is a cube-shaped polarization beam splitter formed by joining base materials n 1 ≠ n 2 having different refractive indexes, and (b) in the figure has the same effect as the above embodiment. Play.
「考案の効果」 本考案は叙上のように、磁気光学的に信号を読取る光
磁気再生装置において、光を放射する光源と、前記光源
からの光を収束させるレンズと、磁気記録媒体で反射さ
れ且つ前記レンズを通過した光をS偏向及びP偏向に分
離すると共に、分離された前記S偏向及びP偏向のうち
いずれか一方に非点収差を持たせる光学手段とを備え、
前記光学手段は、入射光に対して傾斜する第1の面と、
該第1の面を通過した光を更に通過させて前記光学手段
の外部に導く第2の面と、前記第1の面に施された偏向
膜とを含み、前記第1の面が前記偏向膜によって分離さ
れたS偏向及びP偏向のうち一方を反射し他方を通過さ
せ、前記通過光を用いてフォーカスエラー検出を行うよ
うにしたものである。[Advantages of the Invention] As described above, the present invention is a magneto-optical reproducing apparatus for reading a signal magneto-optically, in which a light source that emits light, a lens that converges the light from the light source, and a reflection on a magnetic recording medium. Optical means that separates the light that has been transmitted through the lens into S-deflection and P-deflection, and that has astigmatism in either of the separated S-deflection and P-deflection,
The optical means comprises a first surface inclined with respect to incident light;
The second surface further includes a second surface that further transmits the light that has passed through the first surface and guides the light to the outside of the optical unit, and a deflection film formed on the first surface, the first surface including the deflection film. One of the S-polarized light and the P-polarized light separated by the film is reflected and the other is passed, and the focus light is detected using the passing light.
即ち、1個の光学素子28に非点収差発生機能と検光子
機能とをもたせるように構成したので、光学ヘッド全体
を小型軽量化することができると共に、部品点数及びコ
ストを低減することができる。That is, since the single optical element 28 is configured to have the astigmatism generation function and the analyzer function, the entire optical head can be made compact and lightweight, and the number of parts and cost can be reduced. .
また、微弱な光変化を信号情報とする光磁気再生にお
いては、途中の光学部品による光量ロスは信号のS/Nに
大きな影響を与えるのであるが、上記のように光学部品
を削減できることによって、光量ロスの低減、したがっ
てS/Nの向上に寄与することができる。Also, in magneto-optical reproduction that uses weak light changes as signal information, the light amount loss due to the optical components in the middle has a great influence on the S / N of the signal, but by reducing the optical components as described above, It can contribute to the reduction of the light amount loss and therefore the improvement of the S / N.
第1図は本考案に係る光磁気記録再生装置の光学系構造
の概略構成図で、第2図は他の実施例の光学系構造の概
略構成図、第3図の(イ)、(ロ)は夫々上記の光学系
構造で使用される非点収差発生検光子の異なる実施例の
斜視図、第4図は従来の光磁気記録再生装置の光学系構
造の概略構成図である。 21……レーザ光源、22……コリメータ、23……ハーフミ
ラー、24……光磁気ディスク、25……対物レンズ、26…
…1/2波長板、28……非点収差発生検光子、29A、29B…
…ディテクタ、30、31……差動アンプ。FIG. 1 is a schematic configuration diagram of an optical system structure of a magneto-optical recording / reproducing apparatus according to the present invention, FIG. 2 is a schematic configuration diagram of an optical system structure of another embodiment, and (a) and (b) of FIG. 4) are perspective views of different embodiments of the astigmatism generating analyzer used in the above optical system structure, and FIG. 4 is a schematic configuration diagram of the optical system structure of the conventional magneto-optical recording / reproducing apparatus. 21 ... Laser light source, 22 ... Collimator, 23 ... Half mirror, 24 ... Magneto-optical disk, 25 ... Objective lens, 26 ...
... 1/2 wave plate, 28 ... Astigmatism generating analyzer, 29A, 29B ...
… Detectors, 30, 31… Differential amplifiers.
Claims (1)
装置において、光を放射する光源と、前記光源からの光
を収束させるレンズと、磁気記録媒体で反射され且つ前
記レンズを通過した光をS偏向及びP偏向に分離すると
共に、分離された前記S偏向及びP偏向のうちのいずれ
か一方に非点収差を持たせる光学手段とを備え、前記光
学手段は、入射光に対して傾斜する第1の面と、該第1
の面を通過した光を更に通過させて前記光学手段の外部
に導く第2の面と、前記第1の面に施された偏向膜とを
含み、前記第1の面が前記偏向膜によって分離されたS
偏向及びP偏向のうち一方を反射し他方を通過させ、前
記通過光を用いてフォーカスエラー検出を行うことを特
徴とする光磁気記録媒体再生装置。1. A magneto-optical recording / reproducing apparatus for reading a signal magneto-optically, a light source for emitting light, a lens for converging light from the light source, and light reflected by a magnetic recording medium and passing through the lens. Is divided into S-deflection and P-deflection, and optical means for imparting astigmatism to either of the separated S-deflection and P-deflection is provided, and the optical means is inclined with respect to incident light. And the first surface
A second surface that further passes light that has passed through the first surface and guides the light to the outside of the optical means, and a deflection film provided on the first surface, and the first surface is separated by the deflection film. The S
A magneto-optical recording medium reproducing apparatus characterized in that one of the polarized light and the P-polarized light is reflected and the other is passed, and a focus error is detected using the passing light.
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7080786U JPH0810854Y2 (en) | 1986-05-12 | 1986-05-12 | Magneto-optical recording medium reproducing device |
DE19873715443 DE3715443C2 (en) | 1986-05-12 | 1987-05-08 | Playback device for reading signals from a magneto-optical recording medium |
FR8706654A FR2598521B1 (en) | 1986-05-12 | 1987-05-12 | OPTICAL SYSTEM OF A PHOTO-ELECTRO-MAGNETIC RECORDING AND REPRODUCING DEVICE. |
US07/438,932 US5189651A (en) | 1986-05-12 | 1989-10-30 | Optical system in magneto-optical recording and reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7080786U JPH0810854Y2 (en) | 1986-05-12 | 1986-05-12 | Magneto-optical recording medium reproducing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS62186228U JPS62186228U (en) | 1987-11-26 |
JPH0810854Y2 true JPH0810854Y2 (en) | 1996-03-29 |
Family
ID=13442201
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7080786U Expired - Lifetime JPH0810854Y2 (en) | 1986-05-12 | 1986-05-12 | Magneto-optical recording medium reproducing device |
Country Status (3)
Country | Link |
---|---|
JP (1) | JPH0810854Y2 (en) |
DE (1) | DE3715443C2 (en) |
FR (1) | FR2598521B1 (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2624241B2 (en) * | 1986-07-31 | 1997-06-25 | 松下電器産業株式会社 | Magneto-optical disk device |
EP0331476A1 (en) * | 1988-03-03 | 1989-09-06 | Canon Kabushiki Kaisha | Magneto-optical information reproducing apparatus having a polarizing beam splitter disposed with an inclination of 45 |
US5132950A (en) * | 1989-05-02 | 1992-07-21 | Pioneer Electronic Corporation | Optical head having a prism for splitting a beam of light into two polarized light beams |
DE19645110A1 (en) | 1996-11-01 | 1998-05-07 | Thomson Brandt Gmbh | Recording or reproducing device and method for detecting a focus state |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
NL7907216A (en) * | 1979-09-28 | 1981-03-31 | Philips Nv | OPTICAL FOCUS ERROR DETECTION SYSTEM. |
JPS57147148A (en) * | 1981-03-05 | 1982-09-10 | Olympus Optical Co Ltd | Information reproducer with magnetooptic system |
DE3429382A1 (en) * | 1983-08-10 | 1985-02-28 | Canon K.K., Tokio/Tokyo | OPTICAL HEAD |
JPS61236035A (en) * | 1985-04-09 | 1986-10-21 | Sony Corp | Optical head |
-
1986
- 1986-05-12 JP JP7080786U patent/JPH0810854Y2/en not_active Expired - Lifetime
-
1987
- 1987-05-08 DE DE19873715443 patent/DE3715443C2/en not_active Expired - Fee Related
- 1987-05-12 FR FR8706654A patent/FR2598521B1/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
FR2598521A1 (en) | 1987-11-13 |
DE3715443A1 (en) | 1987-11-19 |
JPS62186228U (en) | 1987-11-26 |
DE3715443C2 (en) | 1998-02-26 |
FR2598521B1 (en) | 1991-11-08 |
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