JPH0341623A - Optical information recording and reproducing device - Google Patents
Optical information recording and reproducing deviceInfo
- Publication number
- JPH0341623A JPH0341623A JP17558989A JP17558989A JPH0341623A JP H0341623 A JPH0341623 A JP H0341623A JP 17558989 A JP17558989 A JP 17558989A JP 17558989 A JP17558989 A JP 17558989A JP H0341623 A JPH0341623 A JP H0341623A
- Authority
- JP
- Japan
- Prior art keywords
- beam splitter
- information recording
- optical
- semiconductor laser
- optical axis
- 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
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 38
- 239000004065 semiconductor Substances 0.000 claims abstract description 16
- 238000001514 detection method Methods 0.000 claims description 6
- 230000001678 irradiating effect Effects 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 5
- 230000004907 flux Effects 0.000 description 4
- 238000002834 transmittance Methods 0.000 description 4
- 230000002411 adverse Effects 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
Landscapes
- Moving Of The Head For Recording And Reproducing By Optical Means (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、光学的情報記録再生装置に関し、もう少し
詳しくいうと、情報記録媒体にレーザビームを集光して
光スポットを形成する光学系を有する光学的情報記録再
生装置に関するものである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an optical information recording/reproducing device, and more specifically, an optical system that focuses a laser beam on an information recording medium to form a light spot. The present invention relates to an optical information recording/reproducing device having the following.
第3図は従来のこの種の光学的情報記録再生装置を示し
、図において、レーザ光源(1〉からのレーザ光の出射
方向に、反射面(3〉のある偏光ビームスプリッタ(2
)、コリメータレンズ(4)、1/4波長板(5)、対
物レンズ(6)が順次に配設されており、情報記録媒体
(7)の案内溝(8)にレーザビームが集光される。ま
た、信号検出手段(lO〉は情報記録媒体(7)に記録
された信号の再生、および焦点ずれ、トラックずれなど
の信号を検出するものであり、概略、信号検出用光学素
子(11)と光検知器(12)とからなっている。FIG. 3 shows a conventional optical information recording/reproducing device of this type. In the figure, a polarizing beam splitter (2) with a reflective surface (3) is located in the direction of emission of laser light from a laser light source (1).
), a collimator lens (4), a quarter-wave plate (5), and an objective lens (6) are arranged in sequence, and the laser beam is focused on the guide groove (8) of the information recording medium (7). Ru. In addition, the signal detection means (lO) is for reproducing signals recorded on the information recording medium (7) and detecting signals such as defocus and track deviation, and generally consists of an optical element for signal detection (11). It consists of a photodetector (12).
かかる構成により、レーザ光源(1)から出射した発散
光束は偏光ビームスプリッタ(2〉の特性により、−開
光方向、P偏光の光束だけが透過される。この光束はコ
リメータレンズ〈4)により平行光となり1/4波長板
(5)および対物レンズ(6)を介して、情報記録媒体
(7)上に照射され、光スポット(9)を形成する。光
スポット(9)は情報記録媒体(7〉で反射され、再び
対物レンズ(6)および1/4波長板(5〉を透過する
が、1/4波長板(5)を往復することによって偏光方
向が90°回転してS fti光になるため、偏光ビー
ムスプリッタ(2)で反射される。続いて、光束は信号
検出用光学素子(11)、光検知器(12)からなる信
号検出手段(10)に入り、情報記録媒体〈7)に記録
された信号の再生および焦点ずれ、トラックずれなどの
信号検出を行う。With this configuration, due to the characteristics of the polarizing beam splitter (2), only the light beam in the -opening direction and P polarization is transmitted from the diverging light beam emitted from the laser light source (1).This light beam is converted into parallel light by the collimator lens (4). The information recording medium (7) is irradiated with the light through the quarter-wave plate (5) and the objective lens (6) to form a light spot (9). The light spot (9) is reflected by the information recording medium (7>) and passes through the objective lens (6) and the 1/4 wavelength plate (5>) again, but the light spot (9) is polarized by going back and forth through the 1/4 wavelength plate (5). Since the direction is rotated by 90° to become S fti light, it is reflected by the polarizing beam splitter (2).Then, the light beam is passed through a signal detection means consisting of a signal detection optical element (11) and a photodetector (12). At step (10), the signal recorded on the information recording medium (7) is reproduced and signals such as defocus and track deviation are detected.
従来の光学的情報記録再生装置は以上のように構成され
ているので、次のような問題があった。Since the conventional optical information recording/reproducing apparatus is configured as described above, it has the following problems.
これを第4図から第7図を用いて説明する。第3図に示
すように偏光ビームスプリッタ(2)へ入射する光束は
半導体レンズ(1)からの出射光束が直接入射するため
、発散光束になる。従って、光の任意の発散角θに対し
て、偏光ビームスプリッタ(2)の反射面(3)への入
射角δは全て異なる。その様子を第4図に示す。発散角
θ1.θ2.θ、に対して偏光膜への入射角δ、δ2.
δ、が対応する。このように入射角度は発散角に依存す
る。第5図に一般の偏光ビームスプリッタ(2)の光学
特性の一例を示す、グラフはP偏光に対するもので、横
軸は発散角θを示し、符号はビームスプリッタに対する
発散光の光軸からの傾き方向を示す、縦軸は透過率Tで
ある。このグラフにより発散角θに対して透過率Tが不
規則に変わり、透過光強度が不均一になることがわかる
。そこで、第6図に、膜設針により、発散角に対する依
存性を小さくした偏光ビームスプリッタの特性の一例を
示す。このグラフはP(I光に対するもので横軸、縦軸
は第5図と同じである。これから0°付近の発散角に対
する透過率の変化が小さくなること、および発散角θが
大きくなる一方の方向に対して急激に透過率が低くなる
ことがわかる。このような特性を示すビームスプリッタ
(2)を透過した光束の光スポットは、第7図に示すよ
うに、発散角が+θ測の光強度が強い、光軸に関して非
対称な光強度分布となり良好な光スポットを得ることが
できない。This will be explained using FIGS. 4 to 7. As shown in FIG. 3, the light flux incident on the polarizing beam splitter (2) becomes a diverging light flux because the light flux emitted from the semiconductor lens (1) is directly incident thereon. Therefore, for any divergence angle θ of light, the incident angle δ on the reflective surface (3) of the polarizing beam splitter (2) is different. The situation is shown in Figure 4. Divergence angle θ1. θ2. The angle of incidence on the polarizing film δ, δ2.
δ corresponds. The angle of incidence thus depends on the angle of divergence. Figure 5 shows an example of the optical characteristics of a general polarizing beam splitter (2). The graph is for P-polarized light, the horizontal axis indicates the divergence angle θ, and the sign indicates the inclination of the divergent light from the optical axis with respect to the beam splitter. The vertical axis indicating the direction is the transmittance T. It can be seen from this graph that the transmittance T changes irregularly with respect to the divergence angle θ, and the transmitted light intensity becomes non-uniform. Therefore, FIG. 6 shows an example of the characteristics of a polarizing beam splitter whose dependence on the divergence angle is reduced by using a film needle. This graph is for P(I light, and the horizontal and vertical axes are the same as in Figure 5. From this point on, the change in transmittance with respect to the divergence angle near 0° will become smaller, and the divergence angle θ will continue to increase. It can be seen that the transmittance decreases rapidly with respect to the direction.The light spot of the light beam transmitted through the beam splitter (2) exhibiting such characteristics is a light spot with a divergence angle of +θ, as shown in Figure 7. The intensity is strong and the light intensity distribution is asymmetrical with respect to the optical axis, making it impossible to obtain a good light spot.
また同様の問題が情報記録媒体で良好された光束がビー
ムスプリッタで反射する際にも発生し、信号再生および
焦点ずれ、トラックずれなどの信号検出特性にも悪影響
を与える。A similar problem also occurs when a light beam that has been improved by an information recording medium is reflected by a beam splitter, which adversely affects signal reproduction and signal detection characteristics such as defocus and track deviation.
この発明は上記の課題を解決するためになされたもので
、良好な光スポットを生じさせることができる光学的情
報記録再生装置を得ることを目的とする。The present invention was made to solve the above problems, and an object of the present invention is to obtain an optical information recording/reproducing device that can generate a good light spot.
この発明に係る光学的情報記録再生装置は、半導体レー
ザを、ビームスプリッタの光軸と反射面の法線を含む面
内方向に傾けることができるようにしたものである。The optical information recording/reproducing device according to the present invention is capable of tilting a semiconductor laser in an in-plane direction including the optical axis of a beam splitter and the normal line of a reflecting surface.
この発明においては、半導体レーザをビームスプリッタ
の光軸とハーフミラ−面の法線を含む面内方向に傾ける
ことにより、光スポットの強度分布の偏りを補正して光
軸に対称な光強度分布とする。In this invention, by tilting the semiconductor laser in an in-plane direction including the optical axis of the beam splitter and the normal to the half mirror surface, the bias in the intensity distribution of the light spot is corrected and the light intensity distribution is symmetrical about the optical axis. do.
第1図はこの発明の一実施例を示し、図において符号〈
1〉〜(12)は第3図におけると同様の部分であり、
基本的動作は同じである。FIG. 1 shows an embodiment of the present invention, and in the figure, reference numeral 〈
1> to (12) are the same parts as in Fig. 3,
The basic operation is the same.
半導体レーザ(1)は、ビームスプリッタ(2)の光軸
と、ビームスプリッタ<2)の反射面(3)の法線を含
む面内方向に傾けることができる。(13)は傾は角φ
を示す。The semiconductor laser (1) can be tilted in an in-plane direction including the optical axis of the beam splitter (2) and the normal to the reflective surface (3) of the beam splitter <2. (13) has an angle φ
shows.
次に動作について第2図で説明する。第2図は各構成の
2面における光強度分布を示す。同図(a)は従来装置
の場合で、偏光ビームスプリッタ(2)に半導体レーザ
(1)からの発散光が入射する場合の光強度分布を示す
。同図(b)は半導体レーザ(1〉をビームスプリッタ
(2)の光軸と法線を含む面内で−θ傾けたときの強度
分布を示す。これにより半導体レーザの傾き角φ(13
)を調節して、光軸に対する光強度分布の清りを補正し
、同図(e)のように、光強度分布を光軸に対してほぼ
対称に近付けることができる。Next, the operation will be explained with reference to FIG. FIG. 2 shows the light intensity distribution on two sides of each configuration. FIG. 5A shows a light intensity distribution in the case of a conventional device in which diverging light from the semiconductor laser (1) is incident on the polarizing beam splitter (2). Figure (b) shows the intensity distribution when the semiconductor laser (1) is tilted by −θ in a plane that includes the optical axis and normal line of the beam splitter (2).
), it is possible to correct the clarity of the light intensity distribution with respect to the optical axis, and to make the light intensity distribution nearly symmetrical with respect to the optical axis, as shown in FIG.
以上のように、この発明によれば、半導体レーザをビー
ムスプリッタの光軸とビームスプリッタ反射面の法線を
含む面内で傾けられるようにしたので、傾き角を調節し
て、光軸に対する光強度分布を対称に近付け、良好な光
スポットを得ることができる。As described above, according to the present invention, the semiconductor laser can be tilted within a plane that includes the optical axis of the beam splitter and the normal to the beam splitter reflecting surface, so that the tilt angle can be adjusted to It is possible to make the intensity distribution symmetrical and obtain a good light spot.
第1図はこの発明の一実施例の概略正面図、第2図は当
該実施例における光強度分布の補正の説明図、第3図は
従来の光学的情報記録再生装置の概略斜視図、第4図は
第3図のものの発散光束とビームスプリッタの関係を示
す模式図、第5図は第3図におけるビームスプリッタの
光学特性線図、第6図は第3図のものの入射角度依存性
を小さくしたビームスプリッタの光学特性線図、第7図
は第3図のもののビームスプリッタの発散角に対する光
強度分布特性線図である。
(1)・・半導体レーザ、(2)・・ビームスプリッタ
、(3)・・反射面、(7)・・情報記録媒体、(8)
・・案内溝、(13)・・半導体レーザの傾は角。
なお、各図中、同一符号は同−又は相当部分を示す。
晃2図
昂3図
昂5図
昂6図FIG. 1 is a schematic front view of an embodiment of the present invention, FIG. 2 is an explanatory diagram of the correction of light intensity distribution in the embodiment, and FIG. 3 is a schematic perspective view of a conventional optical information recording/reproducing device. Figure 4 is a schematic diagram showing the relationship between the divergent luminous flux and the beam splitter of the one in Figure 3, Figure 5 is an optical characteristic diagram of the beam splitter in Figure 3, and Figure 6 shows the incident angle dependence of the one in Figure 3. FIG. 7 is an optical characteristic diagram of a smaller beam splitter, and FIG. 7 is a light intensity distribution characteristic diagram with respect to the divergence angle of the beam splitter of FIG. 3. (1)...Semiconductor laser, (2)...Beam splitter, (3)...Reflecting surface, (7)...Information recording medium, (8)
...Guide groove, (13)...The inclination of the semiconductor laser is an angle. In each figure, the same reference numerals indicate the same or corresponding parts. Figure 2, figure 3, figure 5, figure 6
Claims (1)
的に情報の記録、再生を行う光学的情報記録再生装置に
おいて、 前記半導体レーザから出射した発散光束を反射光と透過
光とに分割するビームスプリッタと、前記情報記録媒体
に記録された信号の再生および焦点ずれ、トラックずれ
などの信号を検出する信号検出手段と、 を備え、かつ、前記半導体レーザを前記ビームスプリッ
タの光軸と反射面の法線を含む面内に傾けることができ
る光学的情報記録再生装置。[Scope of Claims] An optical information recording and reproducing device that optically records and reproduces information by irradiating an information recording medium with a light beam from a semiconductor laser, wherein a diverging light beam emitted from the semiconductor laser is reflected light and transmitted. a beam splitter that splits the semiconductor laser into the beam splitter, and a signal detection means that reproduces the signal recorded on the information recording medium and detects signals such as defocus and track misalignment, and An optical information recording/reproducing device that can be tilted in a plane that includes the optical axis and the normal to the reflective surface.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17558989A JPH0341623A (en) | 1989-07-10 | 1989-07-10 | Optical information recording and reproducing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP17558989A JPH0341623A (en) | 1989-07-10 | 1989-07-10 | Optical information recording and reproducing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0341623A true JPH0341623A (en) | 1991-02-22 |
Family
ID=15998725
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP17558989A Pending JPH0341623A (en) | 1989-07-10 | 1989-07-10 | Optical information recording and reproducing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0341623A (en) |
-
1989
- 1989-07-10 JP JP17558989A patent/JPH0341623A/en active Pending
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