JPH0472202B2 - - Google Patents

Info

Publication number
JPH0472202B2
JPH0472202B2 JP1318187A JP1318187A JPH0472202B2 JP H0472202 B2 JPH0472202 B2 JP H0472202B2 JP 1318187 A JP1318187 A JP 1318187A JP 1318187 A JP1318187 A JP 1318187A JP H0472202 B2 JPH0472202 B2 JP H0472202B2
Authority
JP
Japan
Prior art keywords
double
multilayer film
prism
image prism
dielectric multilayer
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
Application number
JP1318187A
Other languages
Japanese (ja)
Other versions
JPS63180904A (en
Inventor
Nobuhisa Asanuma
Mitsuru Fujita
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.)
Toyo Communication Equipment Co Ltd
Original Assignee
Toyo Communication Equipment 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 Toyo Communication Equipment Co Ltd filed Critical Toyo Communication Equipment Co Ltd
Priority to JP1318187A priority Critical patent/JPS63180904A/en
Publication of JPS63180904A publication Critical patent/JPS63180904A/en
Publication of JPH0472202B2 publication Critical patent/JPH0472202B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は複像プリズム、殊に2個の結晶体の間
に誘電体多層膜を形成して接合した複像プリズム
に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a double-image prism, and particularly to a double-image prism in which a dielectric multilayer film is formed and bonded between two crystal bodies.

(従来技術) 周知の如く複像プリズムは第2図に示すように
光学軸が互に直交する結晶体プリズム1及び2を
接合したものであつて入射光3を偏波面が互に直
交する直線偏光に分離するものである。このよう
な複像プリズムを用いる光学系として第3図に示
す如き光磁気効果による偏波面回転検出装置があ
る。
(Prior art) As is well known, a double-image prism is a combination of crystal prisms 1 and 2 whose optical axes are orthogonal to each other, as shown in FIG. It separates into polarized light. As an optical system using such a double-image prism, there is a polarization plane rotation detecting device based on the magneto-optical effect as shown in FIG.

これは、例えば光磁気デイスク装置の記録再生
用光学系として用いるものであつて、光源(一般
には半導体レーザ)4を出射した直線偏光の光を
垂直磁化膜を有する記録媒体5表面で反射させカ
ー効果により偏波面が反射前の基準偏波面から少
し回転した反射光をビームスプリツタ6にて分割
しその反射光をセンサ9を用いて光量検出しサー
ボ信号として用いる。一方透過光については1/2
波長板7を通過させることによつてその偏波面を
次段に設ける複像プリズム8の入射面側の結晶体
の光学軸に対し45°傾けるようにし前記複像プリ
ズム8から出射する互に偏波面の直交した光出力
を光センサー10,11にて検出した後両出力の
差を出力差検出器12にて求めることによつて前
記記録媒体の情報を読み取るものである。
This is used, for example, as a recording/reproducing optical system in a magneto-optical disk device, and is used to reflect linearly polarized light emitted from a light source (generally a semiconductor laser) 4 on the surface of a recording medium 5 having a perpendicularly magnetized film. The reflected light whose polarization plane is slightly rotated from the reference polarization plane before reflection due to the effect is split by the beam splitter 6, and the amount of the reflected light is detected by the sensor 9 and used as a servo signal. On the other hand, for transmitted light, it is 1/2
By passing through the wavelength plate 7, the plane of polarization is tilted at 45 degrees with respect to the optical axis of the crystal on the incident surface side of the double-image prism 8 provided at the next stage, so that the polarized waves emitted from the double-image prism 8 are mutually polarized. Information on the recording medium is read by detecting optical outputs whose wavefronts are perpendicular to each other by optical sensors 10 and 11, and then determining the difference between the two outputs by an output difference detector 12.

しかしながら上述した如き複像プリズムを用い
た光学系は高価なビームスプリツタを必要として
光学系が大型高価となるという欠陥があつた。
However, the above-mentioned optical system using a double-image prism has the disadvantage that it requires an expensive beam splitter, making the optical system large and expensive.

(発明の目的) 本発明は上述した如き従来の複像プリズムを用
いた光学系の欠陥を除去すべくなされたものであ
つて従来必要とされたビームスプリツタを除去し
て所要の光学系を構成しうる複像プリズムを提供
することを目的とする。
(Object of the Invention) The present invention has been made in order to eliminate the defects of the optical system using the conventional double-image prism as described above. It is an object of the present invention to provide a double-image prism that can be configured.

(発明の概要) 上述の目的を達成する為、本発明に係る複像プ
リズムは少なくとも2個の結晶体を誘電体多層膜
を介して接合したものである。
(Summary of the Invention) In order to achieve the above-mentioned object, a double-image prism according to the present invention is made by joining at least two crystal bodies via a dielectric multilayer film.

(実施例) 以下本発明を図面に示した実施例に基づいて詳
細に説明する。
(Example) The present invention will be described in detail below based on an example shown in the drawings.

第1図aは複像プリズムとして従来から一般に
利用されていたウオーラストンプリズムの構成を
示す図であつて、これは2個の結晶体1,2の光
学軸を互に直交する如く接合したものであるが前
記結晶体1を入射側プリズムとし入射光3の偏波
面がその光学軸に対し45°傾いている場合出射光
は相互に直交する偏波面を有する光出力を得るこ
と前述のとうりである。
Figure 1a shows the configuration of a Wollaston prism, which has been commonly used as a double-image prism, and is made by joining two crystal bodies 1 and 2 so that their optical axes are perpendicular to each other. However, when the crystal body 1 is used as a prism on the incident side and the plane of polarization of the incident light 3 is inclined at 45 degrees with respect to its optical axis, the output light obtains an optical output having planes of polarization perpendicular to each other. It's uri.

而してこのウオーラストンプリズムの接合面に
適当な誘電体多層膜14を設け、2個の結晶体7
及び2を前記誘電体多層膜14を介して接合すれ
ば該部はハーフミラを構成するのでビームスプリ
ツタの機能を備えた複像プリズム13となること
が理解されよう。
Then, a suitable dielectric multilayer film 14 is provided on the joint surface of this Wallaston prism, and two crystal bodies 7 are formed.
It will be understood that if the parts 2 and 2 are joined together via the dielectric multilayer film 14, the part constitutes a half-mirror, resulting in a double-image prism 13 having the function of a beam splitter.

上述した如きビームスプリツタの機能を備えた
本発明の複像プリズムを用いて第3図に述べた如
き光学系を構成すれば第1図bのようになる。
If an optical system as shown in FIG. 3 is constructed using the double-image prism of the present invention having the function of a beam splitter as described above, the result will be as shown in FIG. 1b.

即ち、これは第1図に於けるビームスプリツタ
6を除去したものとなり、光源4を出射した直線
偏光の光を垂直磁化膜を有する記録媒体5表面で
反射させカー効果により偏波面が反射前の基準偏
波面から少し回転した反射光を1/2波長板7を通
過させることによつて次段に設ける本発明の複像
プリズム13の入射面側の結晶体の光学軸に対し
45°傾けるようにする。前記複像プリズム13を
構成する2個の結晶体の間には例えば透過率、反
射率がP偏光、S偏光によらず等しくなる機能を
有する誘電体多層膜14が形成されているので入
射した光の一部は反射するからセンサ9を用いて
光量検出してサーボ信号として用いる一方、透過
光については互に偏波面の直交した光出力を光セ
ンサー10,11にて検出した後、両出力の差を
出力差検出器12にて求めることによつて前記記
録媒体5の情報を読み取ることができ、高価なビ
ームスプリツタを用いることなく測定することが
できる。
In other words, in this case, the beam splitter 6 in FIG. 1 is removed, and the linearly polarized light emitted from the light source 4 is reflected on the surface of the recording medium 5 having a perpendicular magnetization film, and the plane of polarization is changed before reflection due to the Kerr effect. By passing the reflected light slightly rotated from the reference polarization plane of
Tilt it at 45 degrees. A dielectric multilayer film 14 is formed between the two crystals constituting the double-image prism 13, so that, for example, the transmittance and reflectance of the incident light are the same regardless of whether the light is P-polarized or S-polarized. Since a part of the light is reflected, a sensor 9 is used to detect the amount of light and used as a servo signal, while for transmitted light, optical sensors 10 and 11 detect optical outputs whose polarization planes are orthogonal to each other, and then output both outputs. The information on the recording medium 5 can be read by determining the difference between the two using the output difference detector 12, and measurement can be performed without using an expensive beam splitter.

以上、複像プリズムとして最も一般的なウオー
ラストンプリズムを例に挙げて本発明を説明した
が、本発明はこれのみに限定される必然性のない
ことは云うまでもあるまい。
Although the present invention has been described above using the Wallaston prism, which is the most common double-image prism, as an example, it goes without saying that the present invention is not necessarily limited to this.

(発明の効果) 本発明は以上説明した如く構成しかつ機能する
ものであるから光磁気効果に基づく偏波面の回転
を検出する光学系を少数の部品点数にて安価に構
成し得ると共にこれらの調整を容易にする上で著
しい効果がある。
(Effects of the Invention) Since the present invention is constructed and functions as described above, it is possible to construct an optical system for detecting the rotation of the plane of polarization based on the magneto-optical effect at low cost with a small number of parts, and also to use these components. This has a significant effect on facilitating adjustment.

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

第1図aは本発明に係る複像プリズムの一実施
例を示す構成図、同図bはこれを用いた光学系の
構成を示す図、第2図a及びbは夫々従来のウオ
ーラストンプリズムの構成を示す構成図及びA−
A断面図、第3図はこれを用いた従来の光学系の
一例を示す図である。 1,2……結晶体、14……誘電体多層膜。
FIG. 1a is a configuration diagram showing an embodiment of a double-image prism according to the present invention, FIG. 1b is a diagram showing the configuration of an optical system using this prism, and FIGS. A configuration diagram showing the configuration of the prism and A-
A sectional view and FIG. 3 are diagrams showing an example of a conventional optical system using this. 1, 2...Crystal, 14...Dielectric multilayer film.

Claims (1)

【特許請求の範囲】 1 少なくとも2個の結晶体の接合面に誘電体多
層膜を形成し、ビームスプリツタ機能を付与した
複像プリズム。 2 前記誘電体多層膜を形成することによつて三
個以上の分離光を得ることを特徴とする特許請求
の範囲1記載の複像プリズム。 3 少なくとも2個の結晶体の接合面に誘電体多
層膜を形成し、ビームスプリツタ機能を付与した
複像プリズムと、該プリズムの前記誘電体多層膜
にて反射する光線の出射面又は前記誘電体多層膜
を透過する光線の出射面に配置した受光素子とを
備えたことを特徴とする光磁気効果による偏波面
回転検出光学系。 4 前記複像プリズムの入射面に、垂直磁化膜を
有する記録媒体にて反射された光が入射するよう
構成したことを特徴とする特許請求の範囲3記載
の光磁気効果による偏波面回転検出光学系。
[Scope of Claims] 1. A double-image prism in which a dielectric multilayer film is formed on the joint surface of at least two crystal bodies to provide a beam splitter function. 2. The double-image prism according to claim 1, wherein three or more separated beams are obtained by forming the dielectric multilayer film. 3. A double-image prism in which a dielectric multilayer film is formed on the joint surface of at least two crystals to provide a beam splitter function, and a light exit surface of the prism that is reflected by the dielectric multilayer film or the dielectric 1. An optical system for detecting polarization plane rotation using a magneto-optical effect, comprising a light receiving element disposed on an output surface of a light beam transmitted through a multilayer film. 4. The polarization plane rotation detection optical system using the magneto-optical effect according to claim 3, characterized in that the optical system is configured such that light reflected by a recording medium having a perpendicularly magnetized film is incident on the incident surface of the double-image prism. system.
JP1318187A 1987-01-22 1987-01-22 Biprism Granted JPS63180904A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1318187A JPS63180904A (en) 1987-01-22 1987-01-22 Biprism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1318187A JPS63180904A (en) 1987-01-22 1987-01-22 Biprism

Publications (2)

Publication Number Publication Date
JPS63180904A JPS63180904A (en) 1988-07-26
JPH0472202B2 true JPH0472202B2 (en) 1992-11-17

Family

ID=11826011

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1318187A Granted JPS63180904A (en) 1987-01-22 1987-01-22 Biprism

Country Status (1)

Country Link
JP (1) JPS63180904A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011232481A (en) * 2010-04-27 2011-11-17 Disco Abrasive Syst Ltd Optical element

Also Published As

Publication number Publication date
JPS63180904A (en) 1988-07-26

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