JPS63228423A - Optical information processor - Google Patents

Optical information processor

Info

Publication number
JPS63228423A
JPS63228423A JP6102287A JP6102287A JPS63228423A JP S63228423 A JPS63228423 A JP S63228423A JP 6102287 A JP6102287 A JP 6102287A JP 6102287 A JP6102287 A JP 6102287A JP S63228423 A JPS63228423 A JP S63228423A
Authority
JP
Japan
Prior art keywords
light
optical
reflected
polarizing
dividing
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.)
Granted
Application number
JP6102287A
Other languages
Japanese (ja)
Other versions
JP2594929B2 (en
Inventor
Shigeru Nakamura
滋 中村
Teiji Machida
町田 貞次
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP62061022A priority Critical patent/JP2594929B2/en
Priority to US07/130,637 priority patent/US4873678A/en
Publication of JPS63228423A publication Critical patent/JPS63228423A/en
Application granted granted Critical
Publication of JP2594929B2 publication Critical patent/JP2594929B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To minimize the number of optical parts by using polarized separated film to a dividing optical element to divide a reflecting optical flux from an information medium into two semicircle light fluxes for detecting a reflecting light flux, dividing it for a focus dislocation detection, simultaneously, separating it into two polarized components and obtaining even a magneto-optical signal from the difference of the light strength of two polarized components. CONSTITUTION:A P-polarizing component to the polarizing separating surface of a dividing prism 50 transmits polarizing separating films 55, 56 and 57 and comes to be a circular light flux 65 focused to a point 70. The right side half of an optical axis out of S-polarizing components of a reflecting light 5 is reflected by the polarizing separating film 55, comes to be a semicircle light flux 66, reflected by whole reflecting surfaces 59 and 60 of a rectangular triangular prism 58 and further, reflected by the polarizing separating film 57. The left side half of the optical axis out of S polarizing components of the reflecting light 5 is reflected by the polarizing separating film 56, comes to be a semicircle light flux 67 and further, reflected by the polarizing separating film 55. When the dividing prism 50 and the rectangular triangular prism 58 are used, three light fluxes 65, 66 and 67 can be arranged in the same direction. Thus, one photodetector to receive these light fluxes may be sufficient.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、光学的情報処理装置に係り、特に、光デイス
ク装置や光カード装置などに好適な、光ヘッドの構成を
改良した光学的情報処理装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an optical information processing device, and in particular to an optical information processing device with an improved structure of an optical head, suitable for optical disk devices, optical card devices, etc. It relates to a processing device.

〔従来の技術〕[Conventional technology]

光デイスク装置や光カード装置などでは、情報媒体が回
転や移動によって面ぶれが生・しるため焦点ずれ検出系
が必要である。従来からいろいろな焦点ずれ検出方式が
提案されており、その−例として特開昭60−5954
5号に記載のように、情報媒体からの反射光束をビーム
スプリッタで光源からの光束と分離した後、ミラーなど
で半円形の2つの光束に分割し、それらの分割光束の各
焦束点の一方は前方に他方は後方に2つの2分割光検出
器を配置する方式がある。この方式では、情報媒体の面
ぶれによって光検出器面上の半円形光束の大きさが変化
することを用いて、焦点ずれ検出信号を2分割光検出器
から得る。一方の焦点ずれ検出信号だけでは、検出信号
が情報媒体の面ぶれ方向に対し非対称であるため1両方
の焦点ずれ検出信号を加えることにより焦点ずれ検出信
号を対称的にすることができる。
In optical disk devices, optical card devices, and the like, a defocus detection system is required because rotation and movement of the information medium cause surface blur. Various defocus detection methods have been proposed in the past, and an example is Japanese Patent Application Laid-Open No. 60-5954.
As described in No. 5, after the reflected light beam from the information medium is separated from the light beam from the light source by a beam splitter, it is split into two semicircular light beams by a mirror, etc., and the focal point of each of the divided light beams is There is a method in which two split photodetectors are arranged, one in front and the other in rear. In this method, a defocus detection signal is obtained from a two-split photodetector by using the fact that the size of the semicircular light beam on the photodetector surface changes due to surface wobbling of the information medium. If only one of the defocus detection signals is used, the detection signal is asymmetrical with respect to the direction of surface wobbling of the information medium. Therefore, by adding both defocus detection signals, the defocus detection signals can be made symmetrical.

この従来例の光ヘッドでは、反射光をミラーなどで2つ
に分割する分割方向を情報媒体のトラック方向に合わせ
ることにより、各々の2分割光検出器受光量の差信号か
らトラックずれ検出信号を得ることができる。また、各
々の2分割光検出器受光量の和信号から、穴あけ型や位
相型、相変化型の情報ビットを再生することもできる。
In this conventional optical head, by aligning the dividing direction in which the reflected light is divided into two parts with a mirror or the like to match the track direction of the information medium, a track deviation detection signal can be obtained from the difference signal of the amount of light received by each two-split photodetector. Obtainable. Furthermore, it is also possible to reproduce hole-type, phase-type, and phase-change type information bits from the sum signal of the amount of light received by each of the two-split photodetectors.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ミラーなどで反射光束を2つに分割する上記従来例の光
ヘッドでは、光磁気ディスク装置のように情報媒体から
の反射光の偏光方向の回転を検出して情報を再生する点
については配慮がされていなかった。そのため、光磁気
信号検出用の光束を分離するためのビームスプリッタや
光磁気信号検出用の光学部品や光検出器を必要とし、光
ヘツド全体の光学部品点数が増し、高価になり1寸法が
大きく、重量が重くなる、という問題があった。
In the conventional optical head described above, which uses a mirror or the like to split the reflected light beam into two, consideration is given to detecting the rotation of the polarization direction of the reflected light from the information medium and reproducing information, as in a magneto-optical disk device. It had not been done. Therefore, a beam splitter for separating the light flux for magneto-optical signal detection, optical components and photodetectors for detecting magneto-optical signals are required, which increases the number of optical components in the entire optical head, making it expensive and larger in size. , there was a problem of increased weight.

本発明の目的は、穴あけ型や位相型・相変化型の情報信
号再生に限らず光磁気信号再生をも焦点ずれ検出やトラ
ックずれ検出を行なう同一の光学系によって行なうこと
により、光学部品点数が少なく、安価で、小型軽量の光
ヘッドを提供することにある。
An object of the present invention is to reduce the number of optical parts by performing not only hole-drilling type, phase type, and phase change type information signal reproduction but also magneto-optical signal reproduction using the same optical system that detects defocus and track deviation. The object of the present invention is to provide an optical head that is small in size, inexpensive, and lightweight.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的は、情報媒体からの反射光束を焦点ずれ検出用
の2つの半円形光束に分割する分割光学素子に偏光分離
膜を用い、焦点ずれ検出のために分割すると同時に、2
つの偏光成分に分離して。
The above purpose is to use a polarization separation film in the splitting optical element that splits the reflected light beam from the information medium into two semicircular light beams for defocus detection, and simultaneously splits the light beam into two semicircular beams for defocus detection.
separated into two polarized components.

その2つの偏光成分の光強度の差から光磁気信号も得る
ことによって、達成される。
This is achieved by also obtaining a magneto-optical signal from the difference in light intensity of the two polarized components.

〔作用〕[Effect]

本発明で用いる焦点ずれの検出原理及び光磁気信号の再
生原理を第10図〜第12図を用いて説明する。第10
図は本発明による光ヘッドの構成図で、半導体レーザ1
から出射したレーザ光は、絞り込みレンズ2で光磁気デ
ィスク3上に微小スポットとして結像する。第10図の
紙面内にX軸方向をとり、紙面に垂直な方向°をy軸方
向とする。
The principle of detecting defocus and the principle of reproducing magneto-optical signals used in the present invention will be explained with reference to FIGS. 10 to 12. 10th
The figure is a configuration diagram of an optical head according to the present invention, in which a semiconductor laser 1
The laser beam emitted from the diaphragm is imaged as a minute spot on the magneto-optical disk 3 by the aperture lens 2. The X-axis direction is taken in the paper plane of FIG. 10, and the direction perpendicular to the paper plane is taken as the y-axis direction.

半導体レーザ1の偏光方向をX軸方向として、第12図
(a)の矢印21で示す、光磁気ディスク3の未記録領
域の磁化方向は、例えば矢印22aで示す方向に向いて
おり、この未記録領域で反射したレーザ光束の偏光方向
は第12図(a゛)の矢印21aで示す方向に回転する
。一方、情報が記録されているドメインの磁化方向は、
矢印22bで示す方向に反転しており、ディスク反射光
の偏光は第12図(a)の矢印21bで示す方向に回転
する。光磁気ディスク3からの反射光束は、ビームスプ
リッタ4で半導体レーザ1の出射光と分離される。その
分離光束5の光束中に2分の1波長板23を置き、X軸
からの方位角を22.5度にすると、2分の1波長板2
3を透過した光の偏光方向は、第12K(b)に示すよ
うに45度回転する9次に偏光ビームスプリッタ24a
と24bをそれぞれ光束5の約半分まで挿入する。偏光
分離膜25aと25bは、X方向の偏光成分を透過し、
y方向の偏光成分を反射する。そこで、絞り込みスポッ
トが未記録領域から記録ドメインに移ると、偏光ビーム
スプリッタ24a、24bの透過光束26の光量は第1
2図(b)の矢印21axから矢印21bxへと減少し
、偏光ビームスプリッタ24aによる反射光束27aと
偏光ビームスプリッタ24bによる反射光束27bを加
えた光量は矢印21ayから矢印21byへと増加する
Assuming that the polarization direction of the semiconductor laser 1 is the X-axis direction, the magnetization direction of the unrecorded area of the magneto-optical disk 3, indicated by the arrow 21 in FIG. 12(a), is directed, for example, in the direction indicated by the arrow 22a. The polarization direction of the laser beam reflected from the recording area rotates in the direction shown by the arrow 21a in FIG. 12(a'). On the other hand, the magnetization direction of the domain where information is recorded is
It is reversed in the direction shown by arrow 22b, and the polarization of the disk reflected light is rotated in the direction shown by arrow 21b in FIG. 12(a). The reflected light flux from the magneto-optical disk 3 is separated from the light emitted from the semiconductor laser 1 by a beam splitter 4. If the half-wave plate 23 is placed in the separated light beam 5 and the azimuth angle from the X axis is 22.5 degrees, the half-wave plate 23
The polarization direction of the light transmitted through the 9th-order polarizing beam splitter 24a is rotated by 45 degrees as shown in 12K(b).
and 24b are inserted up to about half of the luminous flux 5, respectively. The polarized light separation films 25a and 25b transmit polarized light components in the X direction,
Reflects the polarized light component in the y direction. Therefore, when the focused spot moves from the unrecorded area to the recorded domain, the light intensity of the transmitted light beam 26 of the polarizing beam splitters 24a and 24b becomes the first
The amount of light decreases from arrow 21ax to arrow 21bx in FIG. 2(b), and the amount of light, which is the sum of the reflected light beam 27a by polarizing beam splitter 24a and the reflected light beam 27b by polarizing beam splitter 24b, increases from arrow 21ay to arrow 21by.

よって透過光束26の光量を光検出器28で受光し、反
射光束27aと27bをそれぞれ光検出器29と30で
受光し、光検出器29及び30の出力の和と光検出器2
8の出力との差をとることにより光磁気信号を再生でき
る。
Therefore, the light quantity of the transmitted light beam 26 is received by the photodetector 28, the reflected light beams 27a and 27b are received by the photodetectors 29 and 30, respectively, and the sum of the outputs of the photodetectors 29 and 30 and the photodetector 2
The magneto-optical signal can be reproduced by taking the difference from the output of 8.

また、光検出器29.30はそれぞれ受光面が2分割さ
れており、反射光束27aと27bの焦束点31aと3
1bの一方は前方へ、他方は後方へほぼ等しい距離だけ
離して配置しておく、ディスク3が焦点位置にある場合
、光検出器29と30の検出面上における光束形状は、
第11図(b)の半円形32aと32bで示すように等
しい大きさであtやイスク3が絞り込みレンズ2の方向
にずれると、第11図(a)に示すように光検出器29
面上の半円形状32aの方が大きくなり、光検出器30
面上の半円形状32bの方が小さくなる。逆にディスク
3がレンズ2から離れる方向にずれると、第11図(c
)に示すように光検出1130面上の半円形状32bの
方が大きくなる。よって、光検出器29の2分割受光部
29′と29′の出力を差動回路33aで、光検出器3
0の2分割受光部30′と30’の出力を差動回路33
bでとることにより、それぞれ焦点ずれ信号を得ること
ができる。しかし、光検出器29又は30から得られる
焦点ずれ検出信号は、ディスク3のずれ方向に対して非
対称であるため、さらに差動回路33aと33bの出力
を加算回路34で加えることによって、対称的な焦点ず
れ検出信号を得ることができる。
In addition, each of the photodetectors 29 and 30 has a light-receiving surface divided into two parts, and the focal points 31a and 3 of the reflected light beams 27a and 27b are divided into two parts.
One of the disks 1b is placed forward and the other is placed approximately equal distances apart from the rear. When the disk 3 is at the focal position, the shape of the light flux on the detection surfaces of the photodetectors 29 and 30 is as follows.
When the semicircles 32a and 32b of FIG. 11(b) have the same size and the isk 3 is shifted in the direction of the stop lens 2, the photodetector 29 as shown in FIG. 11(a)
The semicircular shape 32a on the surface is larger, and the photodetector 30
The semicircular shape 32b on the surface is smaller. On the other hand, if the disk 3 shifts away from the lens 2, as shown in Fig. 11(c).
), the semicircular shape 32b on the light detection surface 1130 is larger. Therefore, the outputs of the two divided light receiving sections 29' and 29' of the photodetector 29 are sent to the photodetector 3 by the differential circuit 33a.
The outputs of the two divided light receiving sections 30' and 30' of 0 are connected to a differential circuit 33.
By taking the image at b, defocus signals can be obtained. However, since the defocus detection signal obtained from the photodetector 29 or 30 is asymmetrical with respect to the direction of displacement of the disk 3, the defocus detection signal obtained from the photodetector 29 or 30 is asymmetrical with respect to the direction of displacement of the disk 3. A defocus detection signal can be obtained.

〔実施例〕〔Example〕

以下、本発明の一実施例を第1図により説明する。第1
図は、本発明による光デイスク装置の光ヘッドの構成図
である。1は半導体レーザ、2は絞り込みレンズ、3は
光磁気ディスク、4はビームスプリッタ、23は2分の
1波長板であり、これらの作用は前に述べであるので省
略する。光磁気ディスク3からの反射光5は、分割プリ
ズム50と直角三角プリズム58によって3つの光束6
5と66と67に分割される。第2図は、分割プリズム
50と直角三角プリズム58の構成を詳しく説明するた
めの図である1分割プリズム50は、三角プリズム51
.平行ガラス板52.三角プリズム53.三角プリズム
54と、偏光分離膜55.56および57とから成る。
An embodiment of the present invention will be described below with reference to FIG. 1st
The figure is a configuration diagram of an optical head of an optical disk device according to the present invention. 1 is a semiconductor laser, 2 is a focusing lens, 3 is a magneto-optical disk, 4 is a beam splitter, and 23 is a 1/2 wavelength plate, and since their functions have been described previously, their explanation will be omitted. The reflected light 5 from the magneto-optical disk 3 is divided into three light beams 6 by a dividing prism 50 and a right triangular prism 58.
It is divided into 5, 66 and 67. FIG. 2 is a diagram for explaining in detail the configuration of the divided prism 50 and the right triangular prism 58.
.. Parallel glass plate 52. Triangular prism 53. It consists of a triangular prism 54 and polarization separation films 55, 56 and 57.

所定の寸法にプリズム51,52.53および54を研
摩した後、偏光分離膜55,56.57をそれぞれプリ
ズム51,53.54に蒸着し、紫外線硬化樹脂で接着
する。ディスク3からの反射光5の紙面内の偏光成分、
即ち、分割プリズム50の偏光分離面に対するP偏光成
分は、偏光分離膜55と56と57を透過して、点70
に集束する円形光束65になる0反射光5のS偏光成分
のうち光軸の右側半分は、偏光分離膜55で反射されて
半円形光束66となり、直角三角プリズム58の全反射
面59と60で反射され、さらに偏光分離It1157
で反射される。また反射光5のS偏光成分のうち(i 光軸の左側半分蓼、偏光分離膜56で反射されて半円形
光束67となり、さらに偏光分離膜55で反射される0
分離プリズム50と直角三角プリズム58を用いると、
3つの光束65と66と67を同一方向にそろえること
ができるので、これらの光束を受光する光検出器は一つ
でよい、半円形光束66と67の集束点68と69の光
路上の中点に光検出[I71を配置する。第4図は、光
検出器71の受光面を示し、左側に配置された分割受光
素子71aと71bで半円形光束66を受光し。
After the prisms 51, 52, 53, and 54 are polished to predetermined dimensions, polarization separation films 55, 56, and 57 are deposited on the prisms 51, 53, and 54, respectively, and bonded with ultraviolet curing resin. Polarized light component in the plane of the paper of the reflected light 5 from the disk 3,
That is, the P-polarized light component with respect to the polarization separation surface of the splitting prism 50 passes through the polarization separation films 55, 56, and 57, and reaches the point 70.
The right half of the S-polarized light component of the reflected light 5 is reflected by the polarization separation film 55 and becomes a semicircular light flux 66, which is focused on the total reflection surfaces 59 and 60 of the right triangular prism 58. It is reflected by the polarization separation It1157
reflected. Also, among the S-polarized components of the reflected light 5 (i), the left half of the optical axis is reflected by the polarization separation film 56 to become a semicircular beam 67, and is further reflected by the polarization separation film 55.
Using the separation prism 50 and the right triangular prism 58,
Since the three light beams 65, 66, and 67 can be aligned in the same direction, only one photodetector is required to receive these light beams. A photodetector [I71 is placed at the point. FIG. 4 shows the light-receiving surface of the photodetector 71, in which a semicircular light beam 66 is received by divided light-receiving elements 71a and 71b arranged on the left side.

右側に配置された分割受光素子71dと7ieで半円形
光束67を受光することにより、前述した焦点ずれ検出
原理に従って焦点ずれ検出信号が得られる。又、P偏光
成分の円形光束65を中央に配置された分割受光素子7
1cで受光し、S偏光成分を受光している受光素子71
a、71b。
By receiving the semicircular light beam 67 with the divided light receiving elements 71d and 7ie arranged on the right side, a defocus detection signal is obtained according to the defocus detection principle described above. Further, a divided light receiving element 7 arranged at the center receives a circular light beam 65 of the P polarized light component.
1c, and the light receiving element 71 receives the S polarized light component.
a, 71b.

71d及び71θの出力の和と受光素子71との出力と
の差から光磁気信号を再生することができる。穴あけ型
や位相型、相変化型のビットは、光検出器71の全出力
信号の和から再生することができる。ディスク3のトラ
ック方向が第1図の紙面に垂直な方向であれば、受光素
子71aと71bの出力の和信号と、受光素子71dと
71eの出力の和信号との差から、トラックずれ検出信
号が得られる。一方、ディスク3のトラック方向が第1
図の紙面内であれば、光束65を受光する受光素子71
oを第5図の71c′と71c′で示すように2分割し
て、それらの差信号からトラックずれ検出信号が得られ
る。直角三角プリズム58を第1図の上下方向に移動さ
せると、光検出器71面上の半円形光束66と67の間
隔を任意に調整することができる。このことは、光学部
品の加工精度をゆるめ、調整によって加工組立誤差を吸
収するのに役立つ、しかし、その必要がなければ1分割
プリズム50と直角三角プリズムを一体化して、第3図
に示す分割プリズム61を、用いても良い0図中台形の
プリズム62は、第2図の三角プリズム51と58を一
体化したものであり、その他は、第2図と同じものであ
る。ビームスプリッタ4と2分の一波長板23と分割プ
リズム50や61は、接着により一体化することにより
A magneto-optical signal can be reproduced from the difference between the sum of the outputs of 71d and 71θ and the output of the light receiving element 71. The drilling type, phase type, and phase change type bits can be reproduced from the sum of all output signals of the photodetector 71. If the track direction of the disk 3 is perpendicular to the plane of the paper in FIG. is obtained. On the other hand, the track direction of disk 3 is
If it is within the paper plane of the figure, a light receiving element 71 that receives the luminous flux 65
o is divided into two parts as shown by 71c' and 71c' in FIG. 5, and a track deviation detection signal is obtained from the difference signal between them. By moving the right triangular prism 58 in the vertical direction in FIG. 1, the interval between the semicircular light beams 66 and 67 on the surface of the photodetector 71 can be adjusted as desired. This is useful for loosening the machining precision of the optical parts and absorbing machining and assembly errors through adjustment.However, if this is not necessary, the one-segment prism 50 and the right triangular prism can be integrated, and the split prism 50 shown in FIG. Prism 61 may be used. The trapezoidal prism 62 in Figure 0 is a combination of the triangular prisms 51 and 58 in Figure 2, and the other parts are the same as in Figure 2. The beam splitter 4, the half-wave plate 23, and the splitting prisms 50 and 61 are integrated by adhesive.

組立が容易になることは言うまでもない、また、2分の
1波長板23を用いるかわりに1分割プリズム、光検出
器などを45度回転しても良い。
Needless to say, assembly becomes easier, and instead of using the half-wave plate 23, the one-split prism, photodetector, etc. may be rotated by 45 degrees.

第6図は1本発明を光磁気ディスク装置の光へラドに用
いた他の実施例で、同一の番号で示したものは同じ作用
をするので説明を省略する。分割プリズム80は、光磁
気ディスク3からの反射光5を3つの光束65と66と
67に分割する。第の間及び82と83の間に偏光分離
膜84と85をそれぞれ蒸着しである0反射光5のP偏
光成分は、偏光分離膜84と85を透過して円形光束6
5となる。反射光5のS偏光成分のうち光軸の右側半分
は、偏光分離膜85で反射して半円形光束66となり全
反射面86で反射する。一方、S偏光成分のうち光軸の
左側半分は、偏光分離膜84で反射し、さらに偏光分離
膜85で反射して半円形光束67になる。前述の第1の
実施例と同様に、分割プリズム80を用いると、3つの
光束65と66と67を同一方向にそろえることができ
るので、第8図に示すような受光素子90aと90bと
90cと90dと90eを持つ一つの光検出器90から
全ての信号を得ることができるゆ即ち、各受光素子の出
力を添子に対してSa。
FIG. 6 shows another embodiment in which the present invention is applied to an optical disc drive of a magneto-optical disk device. Items denoted by the same numbers have the same functions, so a description thereof will be omitted. The splitting prism 80 splits the reflected light 5 from the magneto-optical disk 3 into three beams 65, 66, and 67. Polarization separation films 84 and 85 are deposited between the 0-th and 82-83 spaces, respectively.
It becomes 5. Of the S-polarized light component of the reflected light 5, the right half of the optical axis is reflected by the polarization separation film 85 and becomes a semicircular light beam 66, which is reflected by the total reflection surface 86. On the other hand, the left half of the S-polarized light component on the optical axis is reflected by the polarization separation film 84 and further reflected by the polarization separation film 85 to become a semicircular light beam 67. As in the first embodiment described above, when the splitting prism 80 is used, the three light beams 65, 66, and 67 can be aligned in the same direction, so that the light receiving elements 90a, 90b, and 90c as shown in FIG. All the signals can be obtained from one photodetector 90 having 90d and 90e, that is, the output of each light receiving element is Sa with respect to the splint.

Sb、Sc、Sd、Ssとすれば、焦点ずれ検出信号は
、(Sb−8c)+ (Sd−8s) 、光磁気信号は
S a −(S b + S c + S d + S
 e ) 、六あけ型や位相型、相変化型のピット再生
信号は(Sa+Sb+Sc+Sd+Ss) 、である、
トラック方向が紙面に垂直な方向であれば、トラックず
れ検出信号は(Sb+5c)−(Sd+Se)で得られ
る。一方、トラック方向が紙面内であれば、受光素子9
0aを第9図に示すように2分割して90a′と90a
’の出力信号の差から得られる。
Assuming Sb, Sc, Sd, and Ss, the defocus detection signal is (Sb-8c) + (Sd-8s), and the magneto-optical signal is S a - (S b + S c + S d + S
e) The six-open type, phase type, and phase change type pit reproduction signal is (Sa+Sb+Sc+Sd+Ss),
If the track direction is perpendicular to the paper surface, the track deviation detection signal is obtained as (Sb+5c)-(Sd+Se). On the other hand, if the track direction is within the plane of the paper, the light receiving element 9
0a is divided into two as shown in Figure 9, 90a' and 90a.
' is obtained from the difference between the output signals of '.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、穴あけ型や位相型・相変化型などの情
報信号再生に限らず光磁気信号も、焦点ずれ検出やトラ
ックずれ検出を行なう同一の光学系によって再生するこ
とができ、しかも一つの光検出器から上記全ての信号を
得ることができ、光学部品点数が少なく、小型で、安価
で、軽量な光ヘッドを得ることができる。
According to the present invention, not only information signal reproduction of the drilling type, phase type, and phase change type, but also magneto-optical signals can be reproduced by the same optical system that detects defocus and track deviation. All of the above signals can be obtained from one photodetector, and an optical head that is small, inexpensive, and lightweight can be obtained with a small number of optical parts.

【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を示す構成図、第2図、第3
図、第4図及び第5図は、それぞれ第1図の実施例を詳
しく説明するための図、第6図は本発明の他の一実施例
を示す構成図、第7図、第8図及び第9図はそれぞれ第
6図の実施例を詳しく説明するための図、第10図、第
11図及び第12図は、本発明の詳細な説明するための
図である。 1・・・半導体レーザ、2・・・絞り込みレンズ、3・
・・光磁気ディスク、4・・・ビームスプリッタ、23
・・・2分の1波長板、50.80・・・分割プリズム
、58・・・直角三角プリズム、71.90・・・光検
出器。
Fig. 1 is a configuration diagram showing one embodiment of the present invention, Fig. 2, Fig. 3
4 and 5 are diagrams for explaining in detail the embodiment of FIG. 1, respectively. FIG. 6 is a configuration diagram showing another embodiment of the present invention, and FIGS. 7 and 8. and FIG. 9 are diagrams for explaining the embodiment of FIG. 6 in detail, and FIGS. 10, 11, and 12 are diagrams for explaining the present invention in detail. 1... Semiconductor laser, 2... Stop lens, 3...
... Magneto-optical disk, 4... Beam splitter, 23
...half wavelength plate, 50.80...dividing prism, 58...right triangular prism, 71.90...photodetector.

Claims (1)

【特許請求の範囲】 1、光源と、前記光源からの出射光束を情報媒体面上に
結像する結像光学手段を、前記情報媒体からの反射光束
の少なくとも一部を前記光源の出射光束から分離する分
離手段と、前記分離手段によつて分離された分離光束を
分割する分割手段と、前記分割手段によつて分割された
分割光束の集束点の前方及び後方に配置された2つの光
検出器とからなり、前記分割手段が偏光分離膜を有する
ことを特徴とする光学的情報処理装置。 2、特許請求の範囲第1項において、前記分割手段が少
なくとも2つの略平行な偏光分離膜を有することを特徴
とする光学的情報処理装置。 3、特許請求の範囲第2項において、前記分割手段が前
記偏光分離膜に略平行な全反射面を有することを特徴と
する光学的情報処理装置。 4、特許請求の範囲第3項において、前記分割手段が、
前記偏光分離膜に略直角な偏光分離膜を有するプリズム
と、前記全反射面を有する直角プリズムとから成ること
を特徴とする光学的情報処理装置。 5、特許請求の範囲第3項又は第4項において、前記2
つの光検出器を一体型としたことを特徴とする光学的情
報処理装置。 6、特許請求の範囲第5項において、前記光検出器が6
つ以上に分割された受光領域を有することを特徴とする
光学的情報処理装置。
[Scope of Claims] 1. A light source and an imaging optical means for forming an image of the light beam emitted from the light source onto the information medium surface, and a light source that converts at least a portion of the light beam reflected from the information medium from the light beam emitted from the light source. a separating means for separating, a dividing means for dividing the separated beam separated by the separating means, and two photodetectors arranged in front and behind a convergence point of the divided beam divided by the dividing means. an optical information processing device, characterized in that the dividing means has a polarization separation film. 2. The optical information processing device according to claim 1, wherein the dividing means has at least two substantially parallel polarization separation films. 3. The optical information processing device according to claim 2, wherein the dividing means has a total reflection surface substantially parallel to the polarization separation film. 4. In claim 3, the dividing means comprises:
An optical information processing device comprising: a prism having a polarization separation film substantially perpendicular to the polarization separation film; and a right-angle prism having the total reflection surface. 5. In claim 3 or 4, the above-mentioned 2.
An optical information processing device characterized by integrating two photodetectors. 6. In claim 5, the photodetector is 6.
An optical information processing device characterized by having a light receiving area divided into three or more parts.
JP62061022A 1986-12-10 1987-03-18 Optical information processing device Expired - Lifetime JP2594929B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP62061022A JP2594929B2 (en) 1987-03-18 1987-03-18 Optical information processing device
US07/130,637 US4873678A (en) 1986-12-10 1987-12-09 Optical head and optical information processor using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62061022A JP2594929B2 (en) 1987-03-18 1987-03-18 Optical information processing device

Publications (2)

Publication Number Publication Date
JPS63228423A true JPS63228423A (en) 1988-09-22
JP2594929B2 JP2594929B2 (en) 1997-03-26

Family

ID=13159266

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62061022A Expired - Lifetime JP2594929B2 (en) 1986-12-10 1987-03-18 Optical information processing device

Country Status (1)

Country Link
JP (1) JP2594929B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0440632A (en) * 1990-06-05 1992-02-12 Matsushita Electric Ind Co Ltd Optical head

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61206944A (en) * 1985-03-11 1986-09-13 Hitachi Ltd Photomagnetic disc device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61206944A (en) * 1985-03-11 1986-09-13 Hitachi Ltd Photomagnetic disc device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0440632A (en) * 1990-06-05 1992-02-12 Matsushita Electric Ind Co Ltd Optical head

Also Published As

Publication number Publication date
JP2594929B2 (en) 1997-03-26

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